Sample records for c4997 seismic records

  1. Interpretation of two compact planetary nebulae, IC 4997 and NGC 6572, with aid of theoretical models.

    PubMed Central

    Hyung, S; Aller, L H

    1993-01-01

    Observations of two dense compact planetary nebulae secured with the Hamilton Echelle spectrograph at Lick Observatory combined with previously published UV spectra secured with the International Ultraviolet Explorer enable us to probe the electron densities and temperatures (plasma diagnostics) and ionic concentrations in these objects. The diagnostic diagrams show that no homogenous model will work for these nebulae. NGC 6572 may consist of an inner torordal ring of density 25,000 atoms/cm3 and an outer conical shell of density 10,000 atoms/cm3. The simplest model of IC 4997 suggests a thick inner shell with a density of about 107 atoms/cm3 and an outer envelope of density 10,000 atoms/cm3. The abundances of all elements heavier than He appear to be less than the solar values in NGC 6572, whereas He, C, N, and O may be more abundant in IC 4997 than in the sun. IC 4997 presents puzzling problems. PMID:11607347

  2. Method of migrating seismic records

    DOEpatents

    Ober, Curtis C.; Romero, Louis A.; Ghiglia, Dennis C.

    2000-01-01

    The present invention provides a method of migrating seismic records that retains the information in the seismic records and allows migration with significant reductions in computing cost. The present invention comprises phase encoding seismic records and combining the encoded seismic records before migration. Phase encoding can minimize the effect of unwanted cross terms while still allowing significant reductions in the cost to migrate a number of seismic records.

  3. The spectrum of the variable planetary nebula IC 4997

    NASA Technical Reports Server (NTRS)

    Hyung, Siek; Aller, Lawrence H.; Feibelman, Walter A.

    1994-01-01

    The compact, dusty, presumably young planetary nebula (PN) IC 4997 has been studied extensively since the variability of the lambda 4363/lambda 4340 ratio was established in 1956. Since 1938, other nebular lines have shown changes. IC 4997 is also unique because of the great density range revealed by its spectrum which goes in excitation from Mg I to (Ar IV). We present a detailed listing of spectral lines from 360 to 1005 nm. The diagnostic diagram shows that the spectrum can be interpreted only in terms of strata with a huge density gamut. Essential spectral features can be reproduced approximately by a model consisting of a geometrically thin shell of density around 10(exp 7) atoms cm(exp -3), surrounded by a much larger shell with a density of about 10(exp 4) atoms cm(exp -3). The actual, certainly more complex structure can be evaluated only when high resolution spatial imaging is at hand. The usual method of getting abundances from N(ion)/N(H(+)) and ionization correction factors (ICFs) cannot be applied here. It is argued that a reasonable theoretical model that represents the spectrum provides a valid initial approximation to nebular abundances. We propose that the chemical composition of IC 4997 does not differ greatly from that of the Sun. The finally adopted model suggests that the ejection of the material destined to form the inner shell occurred between 1900 and 1960, but observational evidence of such an ejection event is lacking. Perhaps the shell was accelerated. A need for further study is emphasized, especially the role of dust which appears to contribute 2% of the total mass. More attention to this object is recommended. An accurate measurement of its distance is especially desirable.

  4. Five-day recorder seismic system

    USGS Publications Warehouse

    Criley, Ed; Eaton, Jerry P.; Ellis, Jim

    1978-01-01

    The 10-day recorder seismic system used by the USGS since 1965 has been modified substantially to improve its dynamic range and frequency response, to decrease its power consumption and physical complexity, and to make its recordings more compatible with other NCER systems to facilitate data processing. The principal changes include: 1. increasing tape speed from 15/160 ips to 15/80 ips (reducing running time from 10 days to 5 days with a 14' reel of 1 mil tape), 2. increasing the FM center frequency by a factor of 4, from 84.4 Hz to 337.6 Hz, 3. replacing the original amplifiers and FM modulators with new low-power units, 4. replacing the chronometer with a higher quality time code generator (with IRIG-C) to permit automation of data retrieval, 5. eliminating the amplifier/WWVB radio field case by incorporating these elements, along with the new TCG, in the weatherproof tape-recorder box, 6. reducing the power consumption of the motor-drive circuit by removal of a redundant component. In the new system, the tape-recorder case houses all components except the seismometers, the WWVB antenna, the 70-amp-hour 12-VDC battery (which powers the system for 5 days), and the cables to connect these external elements to the recorder box. The objectives of this report are: 1. to describe the new 5-day-recorder seismic system in terms of its constituent parts and their functions, 2. to describe modifications to parts of the original system that were retained and to document new or replacement components with appropriate circuit diagrams and constructional details, 3. to provide detailed instructions for the correct adjustment or alignment of the system in the laboratory, and 4. to provide detailed instructions for installing and operating the system in the field.

  5. Design and development of digital seismic amplifier recorder

    DOE Office of Scientific and Technical Information (OSTI.GOV)

    Samsidar, Siti Alaa; Afuar, Waldy; Handayani, Gunawan, E-mail: gunawanhandayani@gmail.com

    2015-04-16

    A digital seismic recording is a recording technique of seismic data in digital systems. This method is more convenient because it is more accurate than other methods of seismic recorders. To improve the quality of the results of seismic measurements, the signal needs to be amplified to obtain better subsurface images. The purpose of this study is to improve the accuracy of measurement by amplifying the input signal. We use seismic sensors/geophones with a frequency of 4.5 Hz. The signal is amplified by means of 12 units of non-inverting amplifier. The non-inverting amplifier using IC 741 with the resistor values 1KΩmore » and 1MΩ. The amplification results were 1,000 times. The results of signal amplification converted into digital by using the Analog Digital Converter (ADC). Quantitative analysis in this study was performed using the software Lab VIEW 8.6. The Lab VIEW 8.6 program was used to control the ADC. The results of qualitative analysis showed that the seismic conditioning can produce a large output, so that the data obtained is better than conventional data. This application can be used for geophysical methods that have low input voltage such as microtremor application.« less

  6. 6C polarization analysis - seismic direction finding in coherent noise, automated event identification, and wavefield separation

    NASA Astrophysics Data System (ADS)

    Schmelzbach, C.; Sollberger, D.; Greenhalgh, S.; Van Renterghem, C.; Robertsson, J. O. A.

    2017-12-01

    Polarization analysis of standard three-component (3C) seismic data is an established tool to determine the propagation directions of seismic waves recorded by a single station. A major limitation of seismic direction finding methods using 3C recordings, however, is that a correct propagation-direction determination is only possible if the wave mode is known. Furthermore, 3C polarization analysis techniques break down in the presence of coherent noise (i.e., when more than one event is present in the analysis time window). Recent advances in sensor technology (e.g., fibre-optical, magnetohydrodynamic angular rate sensors, and ring laser gyroscopes) have made it possible to accurately measure all three components of rotational ground motion exhibited by seismic waves, in addition to the conventionally recorded three components of translational motion. Here, we present an extension of the theory of single station 3C polarization analysis to six-component (6C) recordings of collocated translational and rotational ground motions. We demonstrate that the information contained in rotation measurements can help to overcome some of the main limitations of standard 3C seismic direction finding, such as handling multiple arrivals simultaneously. We show that the 6C polarisation of elastic waves measured at the Earth's free surface does not only depend on the seismic wave type and propagation direction, but also on the local P- and S-wave velocities just beneath the recording station. Using an adaptation of the multiple signal classification algorithm (MUSIC), we demonstrate how seismic events can univocally be identified and characterized in terms of their wave type. Furthermore, we show how the local velocities can be inferred from single-station 6C data, in addition to the direction angles (inclination and azimuth) of seismic arrivals. A major benefit of our proposed 6C method is that it also allows the accurate recovery of the wave type, propagation directions, and phase

  7. Automated Processing Workflow for Ambient Seismic Recordings

    NASA Astrophysics Data System (ADS)

    Girard, A. J.; Shragge, J.

    2017-12-01

    Structural imaging using body-wave energy present in ambient seismic data remains a challenging task, largely because these wave modes are commonly much weaker than surface wave energy. In a number of situations body-wave energy has been extracted successfully; however, (nearly) all successful body-wave extraction and imaging approaches have focused on cross-correlation processing. While this is useful for interferometric purposes, it can also lead to the inclusion of unwanted noise events that dominate the resulting stack, leaving body-wave energy overpowered by the coherent noise. Conversely, wave-equation imaging can be applied directly on non-correlated ambient data that has been preprocessed to mitigate unwanted energy (i.e., surface waves, burst-like and electromechanical noise) to enhance body-wave arrivals. Following this approach, though, requires a significant preprocessing effort on often Terabytes of ambient seismic data, which is expensive and requires automation to be a feasible approach. In this work we outline an automated processing workflow designed to optimize body wave energy from an ambient seismic data set acquired on a large-N array at a mine site near Lalor Lake, Manitoba, Canada. We show that processing ambient seismic data in the recording domain, rather than the cross-correlation domain, allows us to mitigate energy that is inappropriate for body-wave imaging. We first develop a method for window selection that automatically identifies and removes data contaminated by coherent high-energy bursts. We then apply time- and frequency-domain debursting techniques to mitigate the effects of remaining strong amplitude and/or monochromatic energy without severely degrading the overall waveforms. After each processing step we implement a QC check to investigate improvements in the convergence rates - and the emergence of reflection events - in the cross-correlation plus stack waveforms over hour-long windows. Overall, the QC analyses suggest that

  8. Detecting Seismic Activity with a Covariance Matrix Analysis of Data Recorded on Seismic Arrays

    NASA Astrophysics Data System (ADS)

    Seydoux, L.; Shapiro, N.; de Rosny, J.; Brenguier, F.

    2014-12-01

    Modern seismic networks are recording the ground motion continuously all around the word, with very broadband and high-sensitivity sensors. The aim of our study is to apply statistical array-based approaches to processing of these records. We use the methods mainly brought from the random matrix theory in order to give a statistical description of seismic wavefields recorded at the Earth's surface. We estimate the array covariance matrix and explore the distribution of its eigenvalues that contains information about the coherency of the sources that generated the studied wavefields. With this approach, we can make distinctions between the signals generated by isolated deterministic sources and the "random" ambient noise. We design an algorithm that uses the distribution of the array covariance matrix eigenvalues to detect signals corresponding to coherent seismic events. We investigate the detection capacity of our methods at different scales and in different frequency ranges by applying it to the records of two networks: (1) the seismic monitoring network operating on the Piton de la Fournaise volcano at La Réunion island composed of 21 receivers and with an aperture of ~15 km, and (2) the transportable component of the USArray composed of ~400 receivers with ~70 km inter-station spacing.

  9. Development of a 300°C 3C Fiber Optic Downhole Seismic Receiver Array for Surveying and Monitoring of Geothermal Reservoirs

    DOE Office of Scientific and Technical Information (OSTI.GOV)

    Paulsson, Bjorn N.P.

    2016-06-29

    To address the critical site characterization and monitoring needs for Enhance Geothermal Systems (EGS) programs, US Department of Energy (DOE) awarded Paulsson, Inc. in 2011 a contract to design, build and test a high temperature fiber optic based ultra-large bandwidth clamped borehole seismic vector array capable of deploying a large number of 3C sensor pods suitable for deployment into high temperature and high pressure boreholes. Paulsson, Inc. has completed a design or a unique borehole seismic system consisting of a novel drill pipe based deployment system that includes a hydraulic clamping mechanism for the sensor pods, a new sensor podmore » design and most important – a unique fiber optic seismic vector sensor with technical specifications and capabilities that far exceed the state of the art seismic sensor technologies. These novel technologies were all applied to the new borehole seismic system. In combination these technologies will allow for the deployment of up to 1,000 3C sensor pods in vertical, deviated or horizontal wells. Laboratory tests of the fiber optic seismic vector sensors developed during this project have shown that the new borehole seismic sensor technology is capable of generating outstanding high vector fidelity data with extremely large bandwidth: 0.01 – 6,000 Hz. Field tests have shown that the system can record events at magnitudes much smaller than M-4.0 at frequencies over 2,000 Hz. The sensors have also proved to be about 100 times more sensitive than the regular coil geophones that are used in borehole seismic systems today. The fiber optic seismic sensors have furthermore been qualified to operate at temperatures over 300°C (572°F). The data telemetry fibers used for the seismic vector sensors in the system are also used to simultaneously record Distributed Temperature Sensor (DTS) and Distributed Acoustic Sensor (DAS) data allowing additional value added data to be recorded simultaneously with the seismic vector

  10. Extraction of Pn seismic signals from air-gun shots recorded by the Cascadia Amphibious seismic experiment

    NASA Astrophysics Data System (ADS)

    Rathnayaka, S.; Gao, H.

    2017-12-01

    The goal of this study is to extract Pn (head wave) seismic waveforms recorded by both offshore and onshore (broadband and short period) seismic stations and evaluate the data quality. Two offshore active-source seismic experiments, MGL 1211 and MGL 1212, were conducted from 13th June to 24th July 2012, during the first year deployment of the Cascadia Initiative Amphibious Array. In total, we choose 110 ocean bottom seismometers and 209 inland stations that are located along the entire Cascadia subduction zone. We first remove the instrument response, and then explore the potential frequency ranges and the diurnal effect. We make the common receiver gathering for each seismic station and filter the seismic waveforms at multiple frequency bands, ranging from 3-5 Hz, 5-10 Hz, 10-20 Hz, to 20-40 Hz, respectively. To quantitatively evaluate the data quality, we calculate the signal-to-noise ratio (SNR) of the waveforms for usable stations that record clear Pn arrivals at multiple frequency bands. Our results show that most offshore stations located at deep water (>1.5 km) record clear air-gun shot signals at frequencies higher than 3 Hz and up to 550 km away from the source. For most stations located on the shallow continental shelf, the seismic recordings appear much noisier at all the frequencies compared to stations at deep water. Three general trends are observed for the SNR distribution; First, the SNR ratio increases from lower to higher frequency bands; Second, the ratio decreases with the increasing source-to-receiver distance; And third, the ratio increases from shallow to deep water. We also observe a rough negative relationship of the signal-to-noise ratio with the thickness of the marine sediment. Only 5 inland stations record clear air-gun shot arrivals up to 200 km away from the source. More detailed data quality analysis with more results will also be present.

  11. Preliminary consideration on the seismic actions recorded during the 2016 Central Italy seismic sequence

    NASA Astrophysics Data System (ADS)

    Carlo Ponzo, Felice; Ditommaso, Rocco; Nigro, Antonella; Nigro, Domenico S.; Iacovino, Chiara

    2017-04-01

    After the Mw 6.0 mainshock of August 24, 2016 at 03.36 a.m. (local time), with the epicenter located between the towns of Accumoli (province of Rieti), Amatrice (province of Rieti) and Arquata del Tronto (province of Ascoli Piceno), several activities were started in order to perform some preliminary evaluations on the characteristics of the recent seismic sequence in the areas affected by the earthquake. Ambient vibration acquisitions have been performed using two three-directional velocimetric synchronized stations, with a natural frequency equal to 0.5Hz and a digitizer resolution of equal to 24bit. The activities are continuing after the events of the seismic sequence of October 26 and October 30, 2016. In this paper, in order to compare recorded and code provision values in terms of peak (PGA, PGV and PGD), spectral and integral (Housner Intensity) seismic parameters, several preliminary analyses have been performed on accelerometric time-histories acquired by three near fault station of the RAN (Italian Accelerometric Network): Amatrice station (station code AMT), Norcia station (station code NRC) and Castelsantangelo sul Nera station (station code CNE). Several comparisons between the elastic response spectra derived from accelerometric recordings and the elastic demand spectra provided by the Italian seismic code (NTC 2008) have been performed. Preliminary results retrieved from these analyses highlight several apparent difference between experimental data and conventional code provision. Then, the ongoing seismic sequence appears compatible with the historical seismicity in terms of integral parameters, but not in terms of peak and spectral values. It seems appropriate to reconsider the necessity to revise the simplified design approach based on the conventional spectral values. Acknowledgements This study was partially funded by the Italian Department of Civil Protection within the project DPC-RELUIS 2016 - RS4 ''Seismic observatory of structures and

  12. Response to long-period seismic waves recorded by broadband seismometer and pore pressure sensor at IODP Site C0002, Nankai Trough

    NASA Astrophysics Data System (ADS)

    Kitada, K.; Araki, E.; Kimura, T.; Saffer, D. M.

    2013-12-01

    Long term in situ monitoring of seismic activity, slow slip event, and pore fluid behavior around mega earthquake zone is important for understanding the processes of earthquake generation and strain accumulation. In order to characterize the response to long-period seismic waves, we compared waveforms and hydroseismograms recorded by broadband seismometer and pore pressure transducers, respectively, which were installed at IODP Site C0002 in the Nankai Trough Kumano Basin. The borehole monitoring system sensor array at Site C0002 is designed to collect multiparameter observations covering a dynamic range of events, including local microearthquakes, low frequency earthquakes, and large-scale earthquakes similar to the Tonankai earthquake. The suite of sensors for the downhole portion of the observatory includes a broadband seismometer (CMG3TBD, Guralp Systems Ltd.) with sampling rate of 100Hz at the depth of 907mbsf, and four pressure ports connected to pressure gauges located at 948mbsf, 917mbsf, 766mbsf, and at the seafloor. The sampling rate of the data logger was set to 1Hz after successful connection to the DONET seafloor cable network for real-time monitoring on 24 Jan 2013. Since then, we processed 12 earthquakes between a moment magnitude of 6.5 to 8.3. In addition to the comparison of long-period surface waves waveform and pressure data, we compared the records with theoretical strain seismograms. The latter were calculated by normal mode summation using the earth model PREM of Dziewonski and Anderson (1981). A Butterworth bandpass filter was applied to the records with cut-off frequencies of 0.003 and 0.1 Hz. Our initial results indicate that the hydroseismograms correspond well with the vertical rather than the horizontal (radial and transverse) components in seismic data. The observed hydroseismogram have a good correlation with the predicted volumetric strain seismogram, especially for the Okhotsk (2013/05/24 14:17UT, Mw8.3, 632km depth), the Chishima

  13. Wide-angle seismic recordings from the 1998 Seismic Hazards Investigation of Puget Sound (SHIPS), western Washington and British Columbia

    USGS Publications Warehouse

    Brocher, Thomas M.; Parsons, Tom; Creager, Ken C.; Crosson, Robert S.; Symons, Neill P.; Spence, George D.; Zelt, Barry C.; Hammer, Philip T.C.; Hyndman, Roy D.; Mosher, David C.; Tréhu, Anne M.; Miller, Kate C.; ten Brink, Uri S.; Fisher, Michael A.; Pratt, Thomas L.; Alvarez, Marcos G.; Beaudoin, Bruce C.; Louden, Keith E.; Weaver, Craig S.

    1999-01-01

    This report describes the acquisition and processing of deep-crustal wide-angle seismic reflection and refraction data obtained in the vicinity of Puget Lowland, the Strait of Juan de Fuca, and Georgia Strait, western Washington and southwestern British Columbia, in March 1998 during the Seismic Hazards Investigation of Puget Sound (SHIPS). As part of a larger initiative to better understand lateral variations in crustal structure along the Cascadia margin, SHIPS participants acquired 1000 km of deep-crustal multichannel seismic-reflection profiles and 1300 km of wideangle airgun shot lines in this region using the R/V Thompson and R/V Tully. The Tully was used to record airgun shots fired by the Thompson in two different geometries: (1) expanding spread profiles (ESPs) and (2) constant offset profiles (COPs). Prior to this reflection survey, we deployed 257 Reftek and 15 ocean-bottom seismic recorders to record the airgun signals at far offsets. All data were recorded digitally on large-capacity hard disks. Although most of these stations only recorded the vertical component of motion, 95 of these seismographs recorded signals from an oriented 3-component seismometer. By recording signals generated by the Thompson's marine air gun array, operated in two differing geometries having a total volume of 110 and 79 liters (6730 and 4838 cu. in.), respectively, the arrays of wide-angle recorders were designed to (1) image the crustal structure, particularly in the vicinity of crustal faults and Cenozoic sedimentary basins, (2) determine the geometry of the Moho, and (3) image the subducting Gorda and Juan de Fuca plates. Nearly 33,300 air gun shots were recorded along several seismic lines. In this report, we illustrate the expanding spread profiles acquired using the Thompson and Tully, describe the land and ocean-bottom recording of the air gun signals, discuss the processing of the land recorder data into common receiver gathers, and illustrate the processed wide

  14. Digital processing of array seismic recordings

    USGS Publications Warehouse

    Ryall, Alan; Birtill, John

    1962-01-01

    This technical letter contains a brief review of the operations which are involved in digital processing of array seismic recordings by the methods of velocity filtering, summation, cross-multiplication and integration, and by combinations of these operations (the "UK Method" and multiple correlation). Examples are presented of analyses by the several techniques on array recordings which were obtained by the U.S. Geological Survey during chemical and nuclear explosions in the western United States. Seismograms are synthesized using actual noise and Pn-signal recordings, such that the signal-to-noise ratio, onset time and velocity of the signal are predetermined for the synthetic record. These records are then analyzed by summation, cross-multiplication, multiple correlation and the UK technique, and the results are compared. For all of the examples presented, analysis by the non-linear techniques of multiple correlation and cross-multiplication of the traces on an array recording are preferred to analyses by the linear operations involved in summation and the UK Method.

  15. Factors limiting the sensitivity and dynamic range of a seismic system employing analog magnetic tape recording and a seismic amplifier with adjustable gain settings and several output levels

    USGS Publications Warehouse

    Eaton, Jerry P.; Van Schaack, John R.

    1977-01-01

    In the course of modernizing the low-speed-tape-recorder portable seismic systems and considering the possibilities for the design of a cassette-tape-recorder seismic refraction system, the factors that limit the sensitivity and dynamic range of such systems have been reviewed. These factors will first be stated briefly, and then their influence on systems such as the new 5-day-tape seismic system will be examined in more detail. To fix ideas, we shall assume that the system consists of the following elements: 1. A seismic sensor: usually a moving coil inertial seismometer with a period of about 1 second, a coil resistance of about 5000 ohms, and an effective motor constant of 1.0 V/cm/sec (across a 10K load terminating the seismometer sensitivity-and-damping-adjustment resistive network). 2. A seismic amplifier/voltage controlled oscillator unit made up of the following components: a) A fixed gain preamplifier with an input resistance of 10K and an internal noise level of 0.5 muVpp referred to the preamp input (0.1 Hz <= freq. <= 30 hz). b) An adjustable gain (0 to 42 db in 6 db steps) intermediate amplifier c) One or more fixed gain output amplifiers. d) Two sections of 6 db/octave bandpass filter serving to couple the 3 amplifier stages together. e) Voltage controlled oscillators for each output amplifier to produce modulated FM carriers for recording on separate tape tracks or modulated FM subcarriers for subsequent multiplexing and direct recording on tape in the California Network format. 3. An analog magnetic tape recorder: e.g. the PI 5100 (15/80 ips recording in the FM mode or in the direct mode with the 'broad-band' variant-of the Cal Net multiplex system, or 15/16 ips recording in the direct mode with the standard Cal Net multiplex system), or the Sony TC-126 cassette recorder operating in the direct record mode with the standard Cal Net multiplex system. 4. Appropriate magnetic tape playback equipment: e.g., the Bell and Howell 3700-B for the PI-5100 or

  16. Development and Test of a 1,000 Level 3C Fiber Optic Borehole Seismic Receiver Array Applied to Carbon Sequestration

    DOE Office of Scientific and Technical Information (OSTI.GOV)

    Paulsson, Bjorn N.P.

    2015-02-28

    To address the critical site characterization and monitoring needs for CCS programs, US Department of Energy (DOE) awarded Paulsson, Inc. in 2010 a contract to design, build and test a fiber optic based ultra-large bandwidth clamped borehole seismic vector array capable of deploying up to one thousand 3C sensor pods suitable for deployment into high temperature and high pressure boreholes. Paulsson, Inc. has completed a design or a unique borehole seismic system consisting of a novel drill pipe based deployment system that includes a hydraulic clamping mechanism for the sensor pods, a new sensor pod design and most important –more » a unique fiber optic seismic vector sensor with technical specifications and capabilities that far exceed the state of the art seismic sensor technologies. These novel technologies were all applied to the new borehole seismic system. In combination these technologies will allow for the deployment of up to 1,000 3C sensor pods in vertical, deviated or horizontal wells. Laboratory tests of the fiber optic seismic vector sensors developed during this project have shown that the new borehole seismic sensor technology is capable of generating outstanding high vector fidelity data with extremely large bandwidth: 0.01 – 6,000 Hz. Field tests have shown that the system can record events at magnitudes much smaller than M-2.3 at frequencies up to 2,000 Hz. The sensors have also proved to be about 100 times more sensitive than the regular coil geophones that are used in borehole seismic systems today. The fiber optic seismic sensors have furthermore been qualified to operate at temperatures over 300°C (572°F). The fibers used for the seismic sensors in the system are used to record Distributed Temperature Sensor (DTS) data allowing additional value added data to be recorded simultaneously with the seismic vector sensor data.« less

  17. Joint seismic-infrasonic processing of recordings from a repeating source of atmospheric explosions.

    PubMed

    Gibbons, Steven J; Ringdal, Frode; Kvaerna, Tormod

    2007-11-01

    A database has been established of seismic and infrasonic recordings from more than 100 well-constrained surface explosions, conducted by the Finnish military to destroy old ammunition. The recorded seismic signals are essentially identical and indicate that the variation in source location and magnitude is negligible. In contrast, the infrasonic arrivals on both seismic and infrasound sensors exhibit significant variation both with regard to the number of detected phases, phase travel times, and phase amplitudes, which would be attributable to atmospheric factors. This data set provides an excellent database for studies in sound propagation, infrasound array detection, and direction estimation.

  18. Fracturing and Transformation Into Veins Beneath the Crustal Scale Brittle Ductile Transition - a Record of Co-seismic Loading and Post-seismic Relaxation

    NASA Astrophysics Data System (ADS)

    Nüchter, J. A.; Stöckhert, B.

    2005-12-01

    Metamorphic rocks approaching the crustal scale brittle-ductile transition (BDT) during exhumation are expected to become increasingly affected by short term stress fluctuations related to seismic activity in the overlying seismogenic layer (schizosphere), while still residing in a long-term viscous environment (plastosphere). The structural and microstructural record of quartz veins in low grade - high pressure metamorphic rocks from southern Evia, Greece, yields insight into the processes and conditions just beneath the long-term BDT at temperatures of about 300 to 350°C, which switches between brittle failure and viscous flow as a function of imposed stress or strain rate. The following features are characteristic: (1) The veins have formed from tensile fractures, with a typical length on the order of 10-1 to 101 m; (2) The veins are discordant with respect to foliation and all pre-existing structures, with a uniform orientation over more than 500 km2; (3) The veins show a low aspect ratio of about 10 to 100 and an irregular or characteristic flame shape, which requires distributed ductile deformation of the host rock; (4) Fabrics of the sealing vein quartz indicate that - at a time - the veins were wide open cavities; (5) The sealing quartz crystals reveal a broad spectrum of microstructural features indicative of crystal plastic deformation at high stress and temperatures of about 300 to 350°C. These features indicate that opening and sealing of the fractures commenced immediately after brittle failure, controlled by ductile deformation of the host rock. Vein-parallel shortening was generally less than about 2%. Crystals formed early during sealing were plastically deformed upon progressive deformation and opening of the vein. The structural and microstructural record is interpreted as follows: Brittle failure is proposed to be a consequence of short term co-seismic loading. Subsequent opening of the fracture and sealing to become a vein is interpreted to

  19. Seismic Signals Recorded During Artificial and Natural Karst Recharge Events

    NASA Astrophysics Data System (ADS)

    Bilek, S. L.; Luhmann, A. J.; Diniakos, R. S.; Morton, E.; Rinehart, A. J.; Alexander, E. C., Jr.; Alexander, S. C.; Larsen, M.; Green, J. A.

    2016-12-01

    Seismology has recently been used to explore a variety of surficial processes, including tracking landslides, glaciers, and river flow. The seismic data collected can provide useful information about these flow processes, particularly in areas where other flow-related observations are difficult to make. Underground flow through karst aquifers is an area of significant interest, where most of the flow occurs through preferential flow conduits whose locations are largely unknown. We investigate seismic signals generated by both controlled and natural recharge into a karst aquifer system located near Bear Spring, near Eyota, MN, USA. The controlled recharge experiments involved injecting a pool full of water ( 13,000 L) into a dry overflow spring, which then flowed underground until it was discharged at Bear Spring. The natural recharge fortuitously involved a large rainstorm that supplied over 2 inches of rain in a few hour period, which caused the overflow spring to start flowing and total discharge to increase from a background of 100 L/s to 300 L/s. These events were recorded by 12 seismometers (11 short period and 1 broadband with 500 Hz sampling rate) all placed within the 4500 m2 area containing the dry overflow spring and predicted underground flow path. Spectrograms for the artificial and natural recharge events show significant seismic energy over a broad frequency range (few to nearly 220 Hz) during the periods of artificial recharge, largely contained during the period of water injection. Stations closest to Bear Spring see peak seismic energy in the 20-30 Hz range during these tests, likely related to changes in the underground water flow. During the natural recharge event, we find much longer duration of seismic energy over the broad frequency range. We compare these seismic results with discharge measurements conducted during all tests at Bear Spring, as well as with rainfall measurements recorded for the natural recharge event.

  20. Surface seismic measurements of near-surface P-and S-wave seismic velocities at earthquake recording stations, Seattle, Washington

    USGS Publications Warehouse

    Williams, R.A.; Stephenson, W.J.; Frankel, A.D.; Odum, J.K.

    1999-01-01

    We measured P-and S-wave seismic velocities to about 40-m depth using seismic-refraction/reflection data on the ground surface at 13 sites in the Seattle, Washington, urban area, where portable digital seismographs recently recorded earthquakes. Sites with the lowest measured Vs correlate with highest ground motion amplification. These sites, such as at Harbor Island and in the Duwamish River industrial area (DRIA) south of the Kingdome, have an average Vs in the upper 30 m (V??s30) of 150 to 170 m/s. These values of V??s30 place these sites in soil profile type E (V??s30 < 180 m/s). A "rock" site, located at Seward Park on Tertiary sedimentary deposits, has a V??S30 of 433 m/s, which is soil type C (V??s30: 360 to 760 m/s). The Seward Park site V??s30 is about equal to, or up to 200 m/s slower than sites that were located on till or glacial outwash. High-amplitude P-and S-wave seismic reflections at several locations appear to correspond to strong resonances observed in earthquake spectra. An S-wave reflector at the Kingdome at about 17 to 22 m depth probably causes strong 2-Hz resonance that is observed in the earthquake data near the Kingdome.

  1. Development and programming of Geophonino: A low cost Arduino-based seismic recorder for vertical geophones

    NASA Astrophysics Data System (ADS)

    Soler-Llorens, J. L.; Galiana-Merino, J. J.; Giner-Caturla, J.; Jauregui-Eslava, P.; Rosa-Cintas, S.; Rosa-Herranz, J.

    2016-09-01

    The commercial data acquisition systems used for seismic exploration are usually expensive equipment. In this work, a low cost data acquisition system (Geophonino) has been developed for recording seismic signals from a vertical geophone. The signal goes first through an instrumentation amplifier, INA155, which is suitable for low amplitude signals like the seismic noise, and an anti-aliasing filter based on the MAX7404 switched-capacitor filter. After that, the amplified and filtered signal is digitized and processed by Arduino Due and registered in an SD memory card. Geophonino is configured for continuous registering, where the sampling frequency, the amplitude gain and the registering time are user-defined. The complete prototype is an open source and open hardware system. It has been tested by comparing the registered signals with the ones obtained through different commercial data recording systems and different kind of geophones. The obtained results show good correlation between the tested measurements, presenting Geophonino as a low-cost alternative system for seismic data recording.

  2. The Seismicity activity toward east of Bogotá D. C., Colombia

    NASA Astrophysics Data System (ADS)

    Chicangana, G.; Vargas, C. A.; Gomez-Capera, A.; Pedraza, P.; Mora-Paez, H.; Salcedo, E.; Caneva, A.

    2013-12-01

    In the eastern flank of Eastern Cordillera very close to Bogotá D.C metropolitan area at least in last 450 years five magnitude 5.0 or higher earthquakes has occur. These were confirmed by both historical and instrumental seismicity information. Among these earthquakes, the first one in Colombian historical times was occur at March 16th, 1644 and was sense toward south of Santa Fé de Bogotá. Then on October 18th, 1743 occurred with a current probabilistic magnitude greater than 6.5 an earthquake that transcended in this region due to the economic slump and loss of lives that it caused. Recently the Quetame Earthquake with M = 5.9 occur on May 24th, 2008, that destroyed the Quetame town. This last earthquake was registered locally by Colombian Seismological Network (RSNC). In this study we realized an analysis over this seismicity activity both by historical chronicles with macroseismic estimation data, the seismicity record obtained mainly by the Colombian National Seismological Network (RSNC) data for the 1993-2012 lapse, for searching the seismogenics sources that produced this seismicity activity. So, with these results we show the tectonic panorama of this region indicating of this manner the faults that possibility can be potentially seismic actives. For this we have considered mainly geomorphologic features associated to the faults activity additionally corroborated with GPS velocities data of GEORED project of Colombian Geological Survey.

  3. Finding Trapped Miners by Using a Prototype Seismic Recording System Made from Music-Recording Hardware

    USGS Publications Warehouse

    Pratt, Thomas L.

    2009-01-01

    The goal of this project was to use off-the-shelf music recording equipment to build and test a prototype seismic system to listen for people trapped in underground chambers (mines, caves, collapsed buildings). Previous workers found that an array of geophones is effective in locating trapped miners; displaying the data graphically, as well as playing it back into an audio device (headphones) at high speeds, was found to be effective for locating underground tapping. The desired system should record the data digitally to allow for further analysis, be capable of displaying the data graphically, allow for rudimentary analysis (bandpass filter, deconvolution), and allow the user to listen to the data at varying speeds. Although existing seismic reflection systems are adequate to record, display and analyze the data, they are relatively expensive and difficult to use and do not have an audio playback option. This makes it difficult for individual mines to have a system waiting on the shelf for an emergency. In contrast, music recording systems, like the one I used to construct the prototype system, can be purchased for about 20 percent of the cost of a seismic reflection system and are designed to be much easier to use. The prototype system makes use of an ~$3,000, 16-channel music recording system made by Presonus, Inc., of Baton Rouge, Louisiana. Other manufacturers make competitive systems that would serve equally well. Connecting the geophones to the recording system required the only custom part of this system - a connector that takes the output from the geophone cable and breaks it into 16 microphone inputs to be connected to the music recording system. The connector took about 1 day of technician time to build, using about $300 in off-the-shelf parts. Comparisons of the music recording system and a standard seismic reflection system (A 24-channel 'Geode' system manufactured by Geometrics, Inc., of San Jose, California) were carried out at two locations. Initial

  4. Experimental investigation of the seismic performance of the R/C frames with reinforced masonry infills

    NASA Astrophysics Data System (ADS)

    Tanjung, Jafril; Maidiawati, Nugroho, Fajar

    2017-10-01

    Intensive studies regarding the investigation of seismic performance of reinforced concrete (R/C) frames which are infilled with brick masonry walls have been carried out by several researchers within the last three-decades. According to authors' field and experimentally experiences conclude that the unreinforced brick masonry infills significantly contributes to increase the seismic performance of the R/C frame structure. Unfortunately, the presence of brick masonry infill walls causes several undesirable effects such as short column, soft-storey, torsion and out of plane collapse. In this study, a strengthening technique for the brick masonry infills were experimentally investigated to improve the seismic performance of the R/C frame structures. For this purpose, four experimental specimens have been prepared, i.e. one of bare R/C frame (BF), one of R/C frame infilled with unreinforced brick-masonry wall (IFUM) and two of R/C frames were infilled with reinforced brick-masonry wall (IFRM-1 and IFRM-2). The bare frame and R/C frame infilled with unreinforced brick-masonry wall represents the typical R/C buildings' construction in Indonesia assuming the brick-masonry wall as the non-structural elements. The brick-masonry wall infills in specimens IFRM-1 and IFRM-2 were strengthened by using embedded ϕ4 plain steel bar on their diagonal and center of brick-masonry wall, respectively. All specimens were laterally pushed-over. The lateral loading and its lateral displacement, failure mechanism and their crack pattern were recorded during experimental works. Comparison of the experimental results of these four specimens conclude that the strengthening of the brick-masonry infills wall gave the significantly increasing of the seismic performance of the R/C frame. The seismic performance was evaluated based on the lateral strength of the R/C specimen. The embedded plain steel bar on brick-masonry also reduces the diagonal crack on the brick-masonry wall. It seems that

  5. Broad Halpha Wing Formation in the Planetary Nebula IC 4997.

    PubMed

    Lee; Hyung

    2000-02-10

    The young and compact planetary nebula IC 4997 is known to exhibit very broad wings with a width exceeding 5000 km s-1 around Halpha. We propose that the broad wings are formed through Rayleigh-Raman scattering that involves atomic hydrogen, by which Lybeta photons with a velocity width of a few 102 km s-1 are converted to optical photons and fill the Halpha broad wing region. The conversion efficiency reaches 0.6 near the line center, where the scattering optical depth is much larger than 1, and rapidly decreases in the far wings. Assuming that close to the central star there exists an unresolved inner compact core of high density, nH approximately 109-1010 cm-3, we use the photoionization code "CLOUDY" to show that sufficient Lybeta photons for scattering are produced. Using a top-hat-incident profile for the Lybeta flux and a scattering region with a H i column density NHi=2x1020 cm-2 and a substantial covering factor, we perform a profile-fitting analysis in order to obtain a satisfactory fit to the observed flux. We briefly discuss the astrophysical implications of the Rayleigh-Raman processes in planetary nebulae and other emission objects.

  6. Historic and Instrumental Records of Repeating Seismicity in the Gyeongju Area, Southeastern Korea

    NASA Astrophysics Data System (ADS)

    HAN, M.; Kim, K. H.; Kang, S. Y.; Son, M.; Park, J. H.; LI, Z.

    2015-12-01

    Gyeongju area located in southeastern Korea has experienced repeated seismicity. Historic records during the last 2000 years in the area indicate the earthquake with magnitude 6.7 caused damages of human life and property in 779. During the period of modern instrumental seismic records, the area also experienced numerous small- and moderate-magnitude earthquakes. For example, an earthquake with magnitude 4.3 occurring in 1997 provided a chance for nationwide evaluations of earthquake safety and the renewal of earthquake monitoring system in Korea. The area is still experiencing small earthquakes including magnitude 3.5 in September 2014. We applied waveform correlation detector to continuously recorded seismic data from July 2014 to December 2014 to identify any repeating earthquakes. Detected waveforms are carefully inspected and more than 230 potential events are identified. Eighty three earthquakes among them have been selected for precise determination of earthquake hypocenters. Focal mechanism solutions for representative events were also determined. We further compared the results with those obtained using earthquakes prior to 2013. It has been confirmed the earthquakes in the area are clustered in space. Similar waveforms, earthquake locations, and focal mechanism solutions identified in the study indicates an active faults in the area. Since the area hosts many critical infra-structures, micro-seismicity in the area requires extensive study to address earthquake hazard issues.

  7. Past seismic slip-to-the-trench recorded in Central America megathrust

    NASA Astrophysics Data System (ADS)

    Vannucchi, Paola; Spagnuolo, Elena; Aretusini, Stefano; Di Toro, Giulio; Ujiie, Kohtaro; Tsutsumi, Akito; Nielsen, Stefan

    2017-12-01

    The 2011 Tōhoku-Oki earthquake revealed that co-seismic displacement along the plate boundary megathrust can propagate to the trench. Co-seismic slip to the trench amplifies hazards at subduction zones, so its historical occurrence should also be investigated globally. Here we combine structural and experimental analyses of core samples taken offshore from southeastern Costa Rica as part of the Integrated Ocean Drilling Program (IODP) Expedition 344, with three-dimensional seismic reflection images of the subduction zone. We document a geologic record of past co-seismic slip to the trench. The core passed through a less than 1.9-million-year-old megathrust frontal ramp that superimposes older Miocene biogenic oozes onto late Miocene-Pleistocene silty clays. This, together with our stratigraphic analyses and geophysical images, constrains the position of the basal decollement to lie within the biogenic oozes. Our friction experiments show that, when wet, silty clays and biogenic oozes are both slip-weakening at sub-seismic and seismic slip velocities. Oozes are stronger than silty clays at slip velocities of less than or equal to 0.01 m s-1, and wet oozes become as weak as silty clays only at a slip velocity of 1 m s-1. We therefore suggest that the geological structures found offshore from Costa Rica were deformed during seismic slip-to-the-trench events. During slower aseismic creep, deformation would have preferentially localized within the silty clays.

  8. Recordings from the deepest borehole in the New Madrid Seismic Zone

    USGS Publications Warehouse

    Wang, Z.; Woolery, E.W.

    2006-01-01

    The recordings at the deepest vertical strong-motion array (VSAS) from three small events, the 21 October 2004 Tiptonville, Tennessee, earthquake; the 10 February 2005 Arkansas earthquake; and the 2 June 2005 Ridgely, Tennessee, earthquake show some interesting wave-propagation phenomena through the soils: the S-wave is attenuated from 260 m to 30 m depth and amplified from 30 m to the surface. The S-wave arrival times from the three events yielded different shear-wave velocity estimates for the soils. These different estimates may be the result of different incident angles of the S-waves due to different epicentral distances. The epicentral distances are about 22 km, 110 km, and 47 km for the Tiptonville, Arkansas, and Ridgely earthquakes, respectively. These recordings show the usefulness of the borehole strong-motion array. The vertical strong-motion arrays operated by the University of Kentucky have started to accumulate recordings that will provide a database for scientists and engineers to study the effects of the near-surface soils on the strong ground motion in the New Madrid Seismic Zone. More information about the Kentucky Seismic and Strong-Motion Network can be found at www.uky.edu/KGS/geologichazards. The digital recordings are available at ftp://kgsweb.uky.edu.

  9. High-resolution seismic-reflection profiles and sidescan-sonar records collected on Block Island Sound by U.S. Geological Survey, R/V ASTERIAS, cruise AST 81-2

    USGS Publications Warehouse

    Needell, S. W.; Lewis, R.S.

    1982-01-01

    Cruise AST 81-2 was conducted aboard the R/V ASTERIAS during September 10-18, 1981, in Block Island Sound by the U.S. Geological Survey. It was funded in part by the Connecticut Geological and Natural History Survey. The purpose of the study was to define and map the geology and shallow structure, to determine the geologic framework and late Tertiary to Holocene history, and to identify and map any potential geologic hazards of Block Island Sound.The survey was conducted using an EG&G Uniboom seismic system and an EDO Western sidescan-sonar system. Seismic signals were band-passed between 400 and 4,000 Hz and were recorded at a quarter-second sweep rate. Sidescan sonographs were collected at a 100-m scan range to each side of the ship track. In all, 702 km of seismic-reflection profiles and 402 km of sidescan-sonar records were collected. Navigation was by Loran-C, and the ship position was recorded at 5-minute intervals. Seismic-reflection profiling is continuous and good in quality. Sidescan-sonar records are varied in quality; coverage was intermittent and eventu­ally terminated owing to difficulties with the recorder.Original records can be seen and studied at the U.S. Geological Survey Data Library at Woods Hole, MA 02543. Microfilm copies of the seismic-reflection pro­files and the sidescan sonographs can be purchased only from the National Geo­physical and Solar-Terrestrial Data Center, NOAA/EDIS/NGSDC, Code D621, 325 Broad­way, Boulder, CO 80303 (telephone 303-497-6338).

  10. Seismic signal and noise on Europa

    NASA Astrophysics Data System (ADS)

    Panning, Mark; Stähler, Simon; Bills, Bruce; Castillo Castellanos, Jorge; Huang, Hsin-Hua; Husker, Allen; Kedar, Sharon; Lorenz, Ralph; Pike, William T.; Schmerr, Nicholas; Tsai, Victor; Vance, Steven

    2017-10-01

    Seismology is one of our best tools for detailing interior structure of planetary bodies, and a seismometer is included in the baseline and threshold mission design for the upcoming Europa Lander mission. Guiding mission design and planning for adequate science return, though, requires modeling of both the anticipated signal and noise. Assuming ice seismicity on Europa behaves according to statistical properties observed in Earth catalogs and scaling cumulative seismic moment release to the moon, we can simulate long seismic records and estimate background noise and peak signal amplitudes (Panning et al., 2017). This suggests a sensitive instrument comparable to many broadband terrestrial instruments or the SP instrument from the InSight mission to Mars will be able to record signals, while high frequency geophones are likely inadequate. We extend this analysis to also begin incorporation of spatial and temporal variation due to the tidal cycle, which can help inform landing site selection. We also begin exploration of how chaotic terrane at the bottom of the ice shell and inter-ice heterogeneities (i.e. internal melt structures) may affect anticipated seismic observations using 2D numerical seismic simulations.M. P. Panning, S. C. Stähler, H.-H. Huang, S. D. Vance, S. Kedar, V. C. Tsai, W. T. Pike, R. D. Lorenz, “Expected seismicity and the seismic noise environment of Europa,” J. Geophys. Res., in revision, 2017.

  11. Interferometric Seismic Sources on the Core Mantle Boundary Revealed by Seismic Coda Crosscorrelation

    NASA Astrophysics Data System (ADS)

    Pham, T. S.; Tkalcic, H.; Sambridge, M.

    2017-12-01

    The crosscorrelation of earthquake coda can be used to extract seismic body waves which are sensitive to deep Earth interior. The retrieved peaks in crosscorrelation of two seismic records are commonly interpreted as seismic phases that originate at a point source collocated with the first recorder (Huygens-Fresnel principle), reflected upward from prominent underground reflectors and reaching the second recorder. From the time shift of these peaks measured at different interstation distances, new travel time curves can be constructed. This study focuses on a previously unexplained interferometric phase (named temporarily a ghost or "G phase") observed in crosscorrelogram stack sections utilizing seismic coda. In particular, we deploy waveforms recorded by two regional seismic networks, one in Australia and another in Alaska. We show that the G phase cannot be explained by as a reflection. Moreover, we demonstrate that the G phase is explained through the principle of energy partitioning, and specifically, conversions from compressional to shear motions at the core-mantle boundary (CMB). This can be thought of in terms of a continuous distribution of Huygens sources across the CMB that are "activated" in long-range wavefield coda following significant earthquakes. The newly explained phase is renamed to cPS, to indicate a CMB origin and the P to S conversion. This mechanism explains a range of newly observed global interferometric phases that can be used in combination with existing phases to constrain Earth structure.

  12. Catalogs of micro-seismicity recorded at the Pechgraben landslide (Upper Austria)

    NASA Astrophysics Data System (ADS)

    Provost, Floriane; Hibert, Clément; Vouillamoz, Naomi; Malet, Jean-Philippe; Ottowitz, David; Jochum, Birgit

    2017-04-01

    The microseismicity activity of soft-rock landslides (i.e. developed in clays and clay-shales) present various types of seismic event associated with the slope deformation. They are assumed to be linked to the slip at the interface with the bedrock or at the boundaries of the landslide, to material failures, to fissure openings or to fluid transfers within the medium. It is currently necessary to document the microseismicity generated by soft-rock landslides on a larger amount of instrumented slopes in order to validate the current seismic typology and understand the source mechanisms in relation with the deformation. Previous studies have shown the interest of the Pechgraben (Upper Austria) clay-shale landslide for such documentation. This landslide was reactivated in summer 2013 after heavy rainfalls and is characterized by a shallow bedrock (<10m) and varying displacement rates in space and time (from mm.day-1 to cm.day-1). A short pilot seismic campaign (<9 days) was carried out in 2015 and micro-earthquakes as well as episodic tremor-like signals were recorded. A new passive seismic campaign was conducted during one month in November-December 2016. Two broadband three-component seismometers were installed facing each other on the two stable borders of the slope with one tripartite seismic array deployed in the center, on top of the most active area of the landslide. The deformation pattern of the slope was monitored remotely with a ground-based InSAR at a high frequency (10 min). This study aims to present the variety of seismic sources generated by the landslide, using supervised machine learning algorithms for event detection and classification, and to correlate the resulting micro-seismic catalog with the changes in time of the slope deformation.

  13. Acoustic signature of thunder from seismic records

    NASA Astrophysics Data System (ADS)

    Kappus, Mary E.; Vernon, Frank L.

    1991-06-01

    Thunder, the sound wave through the air associated with lightning, transfers sufficient energy to the ground to trigger seismometers set to record regional earthquakes. The acoustic signature recorded on seismometers, in the form of ground velocity as a function of time, contains the same type features as pressure variations recorded with microphones in air. At a seismic station in Kislovodsk, USSR, a nearly direct lightning strike caused electronic failure of borehole instruments while leaving a brief impulsive acoustic signature on the surface instruments. The peak frequency of 25-55 Hz is consistent with previously published values for cloud-to-ground lightning strikes, but spectra from this station are contaminated by very strong wind noise in this band. A thunderstorm near a similar station in Karasu triggered more than a dozen records of individual lightning strikes during a 2-hour period. The spectra for these events are fairly broadband, with peaks at low frequencies, varying from 6 to 13 Hz. The spectra were all computed by multitaper analysis, which deals appropriately with the nonstationary thunder signal. These independent measurements of low-frequency peaks corroborate the occasional occurrences in traditional microphone records, but a theory concerning the physical mechanism to account for them is still in question. Examined separately, the individual claps in each record have similar frequency distributions, discounting a need for multiple mechanisms to explain different phases of the thunder sequence. Particle motion, determined from polarization analysis of the three-component records, is predominantly vertical downward, with smaller horizontal components indicative of the direction to the lightning bolt. In three of the records the azimuth to the lightning bolt changes with time, confirming a significant horizontal component to the lightning channel itself.

  14. Data report for onshore-offshore wide-angle seismic recordings in the Bering-Chukchi Sea, Western Alaska and eastern Siberia

    USGS Publications Warehouse

    Brocher, Thomas M.; Allen, Richard M.; Stone, David B.; Wolf, Lorraine W.; Galloway, Brian K.

    1995-01-01

    This report presents fourteen deep-crustal wide-angle seismic reflection and refraction profiles recorded onland in western Alaska and eastern Siberia from marine air gun sources in the Bering-Chukchi Seas. During a 20-day period in August, 1994, the R/V Ewing acquired two long (a total of 3754 km) deep-crustal seismic-reflection profiles on the continental shelf of the Bering and Chukchi Seas, in a collaborative project between Stanford University and the United States Geological Survey (USGS). The Ewing's 137.7 liter (8355 cu. in.) air gun array was the source for both the multichannel reflection and the wide-angle seismic data. The Ewing, operated by the Lamont-Doherty Earth Observatory, steamed northward from Nunivak Island to Barrow, and returned, firing the air gun array at intervals of either 50 m or 75 m. About 37,700 air gun shots were fired along the northward directed Lines 1 and 2, and more than 40,000 air gun shots were fired along the southward directed Line 3. The USGS and the University of Alaska, Fairbanks (UAF), deployed an array of twelve 3-component REFTEK and PDAS recorders in western Alaska and eastern Siberia which continuously recorded the air gun signals fired during the northward bound Lines 1 and 2. Seven of these recorders also continuously recorded the southward bound Line 3. These wide-angle seismic data were acquired to: (1) image reflectors in the upper to lower crust, (2) determine crustal and upper mantle refraction velocities, and (3) provide important constraints on the geometry of the Moho along the seismic lines. In this report, we describe the land recording of wide-angle data conducted by the USGS and the UAF, describe in detail how the wide-angle REFTEK and PDAS data were reduced to common receiver gather seismic sections, and illustrate the wide-angle seismic data obtained by the REFTEKs and PDAS's. Air gun signals were observed to ranges in excess of 400 km, and crustal and upper /mantle refractions indicate substantial

  15. Seismic gradiometry using ambient seismic noise in an anisotropic Earth

    NASA Astrophysics Data System (ADS)

    de Ridder, S. A. L.; Curtis, A.

    2017-05-01

    We introduce a wavefield gradiometry technique to estimate both isotropic and anisotropic local medium characteristics from short recordings of seismic signals by inverting a wave equation. The method exploits the information in the spatial gradients of a seismic wavefield that are calculated using dense deployments of seismic arrays. The application of the method uses the surface wave energy in the ambient seismic field. To estimate isotropic and anisotropic medium properties we invert an elliptically anisotropic wave equation. The spatial derivatives of the recorded wavefield are evaluated by calculating finite differences over nearby recordings, which introduces a systematic anisotropic error. A two-step approach corrects this error: finite difference stencils are first calibrated, then the output of the wave-equation inversion is corrected using the linearized impulse response to the inverted velocity anomaly. We test the procedure on ambient seismic noise recorded in a large and dense ocean bottom cable array installed over Ekofisk field. The estimated azimuthal anisotropy forms a circular geometry around the production-induced subsidence bowl. This conforms with results from studies employing controlled sources, and with interferometry correlating long records of seismic noise. Yet in this example, the results were obtained using only a few minutes of ambient seismic noise.

  16. Thermal Alteration of Pyrite to Pyrrhotite During Earthquakes: New Evidence of Seismic Slip in the Rock Record

    NASA Astrophysics Data System (ADS)

    Yang, Tao; Dekkers, Mark J.; Chen, Jianye

    2018-02-01

    Seismic slip zones convey important information on earthquake energy dissipation and rupture processes. However, geological records of earthquakes along exhumed faults remain scarce. They can be traced with a variety of methods that establish the frictional heating of seismic slip, although each has certain assets and disadvantages. Here we describe a mineral magnetic method to identify seismic slip along with its peak temperature through examination of magnetic mineral assemblages within a fault zone in deep-sea sediments cored from the Japan Trench—one of the seismically most active regions around Japan—during the Integrated Ocean Drilling Program Expedition 343, the Japan Trench Fast Drilling Project. Fault zone sediments and adjacent host sediments were analyzed mineral magnetically, supplemented by scanning electron microscope observations with associated energy dispersive X-ray spectroscopy analyses. The presence of the magnetic mineral pyrrhotite appears to be restricted to three fault zones occurring at 697, 720, and 801 m below sea floor in the frontal prism sediments, while it is absent in the adjacent host sediments. Elevated temperatures and coseismic hot fluids as a consequence of frictional heating during earthquake rupture induced partial reaction of preexisting pyrite to pyrrhotite. The presence of pyrrhotite in combination with pyrite-to-pyrrhotite reaction kinetics constrains the peak temperature to between 640 and 800°C. The integrated mineral-magnetic, microscopic, and kinetic approach adopted here is a useful tool to identify seismic slip along faults without frictional melt and establish the associated maximum temperature.

  17. Seismic Observation of Infrasonic Signals

    DTIC Science & Technology

    1984-11-01

    The implication of these results is that an infra - sonic monitoring capability already exists in the current seismic network and... infra - sonic signal recorded by the microbarographs. This arrival is linearly polarized, with a near-vertical orientation of the state vector. The...TECHNICAL REPORT NO. 84-7 cn "^ SEISMIC OBSERVATION p INFRASONIC SIGNALS D < FINAL REPORT by JACK C. SWANSON and J. CRAIG WOERPEL The views and

  18. Paleoseismic potential of sublacustrine landslide records in a high-seismicity setting (south-central Alaska)

    USGS Publications Warehouse

    Praet, Nore; Moernaut, Jasper; Van Daele, Maarten; Boes, Evelien; Haeussler, Peter J.; Strupler, Michael; Schmidt, Sabine; Loso, Michael G.; De Batist, Marc

    2017-01-01

    Sublacustrine landslide stratigraphy is considered useful for quantitative paleoseismology in low-seismicity settings. However, as the recharging of underwater slopes with sediments is one of the factors that governs the recurrence of slope failures, it is not clear if landslide deposits can provide continuous paleoseismic records in settings of frequent strong shaking. To test this, we selected three lakes in south-central Alaska that experienced a strong historical megathrust earthquake (the 1964 Mw9.2 Great Alaska Earthquake) and exhibit high sedimentation rates in their main basins (0.2 cm yr-1 -1.0 cm yr-1). We present high-resolution reflection seismic data (3.5 kHz) and radionuclide data from sediment cores in order to investigate factors that control the establishment of a reliable landslide record. Seismic stratigraphy analysis reveals the presence of several landslide deposits in the lacustrine sedimentary infill. Most of these landslide deposits can be attributed to specific landslide events, as multiple landslide deposits sourced from different lacustrine slopes occur on a single stratigraphic horizon. We identify numerous events in the lakes: Eklutna Lake proximal basin (14 events), Eklutna Lake distal basin (8 events), Skilak Lake (7 events) and Kenai Lake (7 events). The most recent event in each basin corresponds to the historic 1964 megathrust earthquake. All events are characterized by multiple landslide deposits, which hints at a regional trigger mechanism, such as an earthquake (the synchronicity criterion). This means that the landslide record in each basin represents a record of past seismic events. Based on extrapolation of sedimentation rates derived from radionuclide dating, we roughly estimate a mean recurrence interval in the Eklutna Lake proximal basin, Eklutna Lake distal basin, Skilak Lake and Kenai Lake, at ~ 250 yrs, ~ 450 yrs, ~ 900 yrs and ~ 450 yrs, respectively. This distinct difference in recording can be explained by variations

  19. Landslide caracteristics determination using bayesian inversion and seismic recording

    NASA Astrophysics Data System (ADS)

    Mangeney, A.; Moretti, L.; Capdeville, Y.; Stutzmann, E.; Bodin, T.; Bouchut, F.

    2014-12-01

    Gravitational instabilities, such as landslides, avalanches, or debris flows, play a key role in erosional processes and represent one of the major natural hazards in mountainous, coastal, and volcanic regions. Despite the great amount of field, experimental and numerical work devoted to this problem, the understanding of the physical processes at work in gravitational flows is still an open issue, in particular due to the lack of observations relevant to their dynamics. In this context, the seismic signal generated by gravitational flows is a unique opportunity to obtain information on their dynamics and characteristics. Here we present the study of the 1997 Boxing Day landslide that occurred in Montserrat. We accessed the force applied by the landslide to the ground surface responsible of the seismic waves by inverting the seismic waveform recorded (force-time function). This force was then used as a constraint in a bayesian inversion problem where the forward problem is the force-time function calculation obtained by simulating the landslide with the SHALTOP model (mangeney et al., 2007). With this method, we are able to give an estimate of the rheology (friction coefficient) and the initial shape of the collapsing mass. The volume retrieved is very similar to that obtained by field observations. The friction coefficient determined is also similar to that constrained by former studies or to that predicted by empirical laws (Lucas et al., 2014). Furthermore the method permits to give an estimate of the error made on these parameters.

  20. Expected Seismicity and the Seismic Noise Environment of Europa

    NASA Astrophysics Data System (ADS)

    Panning, Mark P.; Stähler, Simon C.; Huang, Hsin-Hua; Vance, Steven D.; Kedar, Sharon; Tsai, Victor C.; Pike, William T.; Lorenz, Ralph D.

    2018-01-01

    Seismic data will be a vital geophysical constraint on internal structure of Europa if we land instruments on the surface. Quantifying expected seismic activity on Europa both in terms of large, recognizable signals and ambient background noise is important for understanding dynamics of the moon, as well as interpretation of potential future data. Seismic energy sources will likely include cracking in the ice shell and turbulent motion in the oceans. We define a range of models of seismic activity in Europa's ice shell by assuming each model follows a Gutenberg-Richter relationship with varying parameters. A range of cumulative seismic moment release between 1016 and 1018 Nm/yr is defined by scaling tidal dissipation energy to tectonic events on the Earth's moon. Random catalogs are generated and used to create synthetic continuous noise records through numerical wave propagation in thermodynamically self-consistent models of the interior structure of Europa. Spectral characteristics of the noise are calculated by determining probabilistic power spectral densities of the synthetic records. While the range of seismicity models predicts noise levels that vary by 80 dB, we show that most noise estimates are below the self-noise floor of high-frequency geophones but may be recorded by more sensitive instruments. The largest expected signals exceed background noise by ˜50 dB. Noise records may allow for constraints on interior structure through autocorrelation. Models of seismic noise generated by pressure variations at the base of the ice shell due to turbulent motions in the subsurface ocean may also generate observable seismic noise.

  1. Calibration Shots Recorded for the Salton Seismic Imaging Project, Salton Trough, California

    NASA Astrophysics Data System (ADS)

    Murphy, J. M.; Rymer, M. J.; Fuis, G. S.; Stock, J. M.; Goldman, M.; Sickler, R. R.; Miller, S. A.; Criley, C. J.; Ricketts, J. W.; Hole, J. A.

    2009-12-01

    The Salton Seismic Imaging Project (SSIP) is a collaborative venture between the U.S. Geological Survey, California Institute of Technology, and Virginia Polytechnic Institute and State University, to acquire seismic reflection/wide angle refraction data, and currently is scheduled for data acquisition in 2010. The purpose of the project is to get a detailed subsurface 3-D image of the structure of the Salton Trough (including both the Coachella and Imperial Valleys) that can be used for earthquake hazards analysis, geothermal studies, and studies of the transition from ocean-ocean to continent-continent plate-boundary. In June 2009, a series of calibration shots were detonated in the southern Imperial Valley with specific goals in mind. First, these shots were used to measure peak particle velocity and acceleration at various distances from the shots. Second, the shots were used to calibrate the propagation of energy through sediments of the Imperial Valley. Third, the shots were used to test the effects of seismic energy on buried clay drainage pipes, which are abundant throughout the irrigated parts of the Salton Trough. Fourth, we tested the ODEX drilling technique, which uses a down-hole casing hammer for a tight casing fit. Information obtained from the calibration shots will be used for final planning of the main project. The shots were located in an unused field adjacent to Hwy 7, about 6 km north of the U.S. /Mexican border (about 18 km southeast of El Centro). Three closely spaced shot points (16 meters apart) were aligned N-S and drilled to 21-m, 23.5-m, and 27-m depth. The holes were filled with 23-kg, 68-kg, and 123-kg of ammonium-nitrate explosive, respectively. Four instrument types were used to record the seismic energy - six RefTek RT130 6-channel recorders with a 3-component accelerometer and a 3-component 2-Hz velocity sensor, seven RefTek RT130 3-channel recorders with a 3-component 4.5-Hz velocity sensor, 35 Texans with a vertical component 4

  2. Infrasound and Seismic Recordings of Rocket Launches from Kennedy Space Center, 2016-2017

    NASA Astrophysics Data System (ADS)

    McNutt, S. R.; Thompson, G.; Brown, R. G.; Braunmiller, J.; Farrell, A. K.; Mehta, C.

    2017-12-01

    We installed a temporary 3-station seismic-infrasound network at Kennedy Space Center (KSC) in February 2016 to test sensor calibrations and train students in field deployment and data acquisitions techniques. Each station featured a single broadband 3-component seismometer and a 3-element infrasound array. In May 2016 the network was scaled back to a single station due to other projects competing for equipment. To date 8 rocket launches have been recorded by the infrasound array, as well as 2 static tests, 1 aborted launch and 1 rocket explosion (see next abstract). Of the rocket launches recorded 4 were SpaceX Falcon-9, 2 were ULA Atlas-5 and 2 were ULA Delta-IV. A question we attempt to answer is whether the rocket engine type and launch trajectory can be estimated with appropriate travel-time, amplitude-ratio and spectral techniques. For example, there is a clear Doppler shift in seismic and infrasound spectrograms from all launches, with lower frequencies occurring later in the recorded signal as the rocket accelerates away from the array. Another question of interest is whether there are relationships between jet noise frequency, thrust and/or nozzle velocity. Infrasound data may help answer these questions. We are now in the process of deploying a permanent seismic and infrasound array at the Astronaut Beach House. 10 more rocket launches are schedule before AGU. NASA is also conducting a series of 33 sonic booms over KSC beginning on Aug 21st. Launches and other events at KSC have provided rich sources of signals that are useful to characterize and gain insight into physical processes and wave generation from man-made sources.

  3. 15/16 ips Operation of the Precision Instrument Company Model P15100 tape recorder to record the standard (30 Hz) NCER seismic data multiplex system

    USGS Publications Warehouse

    Eaton, Jerry P.

    1976-01-01

    In recent months the need has arisen to record special seismic networks consisting of a dozen or more standard NCER seismic systems telemetered to a central collection point on a reliable, portable, low-power tape recorder. Because of its simplicity and the ease with which it can be adapted for the purpose, the PI 5100 field recorder should be considered for such use. In the tests described here, a PI 5100 was speeded up to run at 15/16 inches per second (ips) and signals from the standard multiplex system test modulator bank were recorded on one tape track by means of a simple, improvised AM record amplifier. The results of these tests are extremely encouraging: the dynamic range of the system when played back on the Bell and Howell Model 3700 B reproduce machine, with subtractive compensation, is nearly as high as for the system employing the B&H 3700 B for recording. These notes indicate the principle employed to speed up the recorder, outline the circuit required to drive the tape heads in the AM record mode, and describe the tests carried out to evaluate the system's performance.

  4. UK National Data Centre archive of seismic recordings of (presumed) underground nuclear tests 1964-1996

    NASA Astrophysics Data System (ADS)

    Young, John; Peacock, Sheila

    2016-04-01

    The year 1996 has particular significance for forensic seismologists. This was the year when the Comprehensive Test Ban Treaty (CTBT) was signed in September at the United Nations, setting an international norm against nuclear testing. Blacknest, as a long time seismic centre for research into detecting and identifying underground explosions using seismology, provided significant technical advice during the CTBT negotiations. Since 1962 seismic recordings of both presumed nuclear explosions and earthquakes from the four seismometer arrays Eskdalemuir, Scotland (EKA), Yellowknife, Canada (YKA), Gauribidanur, India (GBA), and Warramunga, Australia (WRA) have been copied, digitised, and saved. There was a possibility this archive would be lost. It was decided to process the records and catalogue them for distribution to other groups and institutions. This work continues at Blacknest but the archive is no longer under threat. In addition much of the archive of analogue tape recordings has been re-digitised with modern equipment, allowing sampling rates of 100 rather than 20 Hz.

  5. Very-long-period seismic signals - filling the gap between deformation and seismicity

    NASA Astrophysics Data System (ADS)

    Neuberg, Jurgen; Smith, Paddy

    2013-04-01

    Good broadband seismic sensors are capable to record seismic transients with dominant wavelengths of several tens or even hundreds of seconds. This allows us to generate a multi-component record of seismic volcanic events that are located in between the conventional high to low-frequency seismic spectrum and deformation signals. With a much higher temporal resolution and accuracy than e.g. GPS records, these signals fill the gap between seismicity and deformation studies. In this contribution we will review the non-trivial processing steps necessary to retrieve ground deformation from the original velocity seismogram and explore which role the resulting displacement signals have in the analysis of volcanic events. We use examples from Soufriere Hills volcano in Montserrat, West Indies, to discuss the benefits and shortcomings of such methods regarding new insights into volcanic processes.

  6. Catalog of seismic records obtained in support of the ERDA/Nevada Operations Office, October 1963 through June 1976

    USGS Publications Warehouse

    Navarro, R.; Sembera, E.D.; Jungblut, W.L.

    1977-01-01

    The United States Geological Survey (USGS), Branch of Earthquake Hazards (BEH), Las Vegas, Nevada has provided ERDA, Nevada Operations Office, with seismic monitoring support to the underground nuclear weapons test program conducted at the Nevada Test Site (NTS) since September 1961. Activities from September 15, 1961 to September 13, 1963 are summarized in the report, "Seismic Dats Summary Nuclear Detonation Program, 1961 thru 1963", (Mickey and Shugart 1964) which lists seismic records obtained from all announced underground nuclear tests conducted during that period.

  7. A one year long continuous record of seismic activity and surface motion at the tongue of Rhonegletscher (Valais, Switzerland)

    NASA Astrophysics Data System (ADS)

    Dalban Canassy, Pierre; Röösli, Claudia; Walter, Fabian; Gabbi, Jeannette

    2014-05-01

    A critical gap in our current understanding of glaciers is how high sub-glacial water pressure controls the coupling of the glacier to its bed. Processes at the base of a glacier are inherently difficult to investigate due to their remoteness. Investigation of the sub-glacial environment with passive seismic methods is an innovative, rapidly growing interdisciplinary and promising endeavor. In combination with observations of surface motion and basal water pressure, this method is ideally suited to localize and quantify frictional and fracture processes which occur during periods of rapidly changing sub-glacial water pressure with consequent stress redistribution at the contact interface between ice and bed. Here we present the results of the first one-year-long glacier seismic monitoring performed on an Alpine glacier to our knowledge. Together with records of surface motion and hydrological measurements, we examine whether seasonal changes can be captured by seismic recording. Experiments were carried out from June 2012 to July 2013 on Rhonegletscher (Valais, Switzerland), by means of 3 three-components seismometers settled close to the tongue in 2 meters boreholes. An additional array of eleven sensors installed at the ice surface was also maintained during September 2012, in order to achieve more accurate icequakes locations. A high seismic emission is observed on Rhonegletscher, with icequakes located close to the surface or in the vicinity of the bedrock. The temporal distribution of seismic activity is shown to nicely reflect the seasonal evolution of the glacier hydrology, with a dramatic seismic release in early spring. During summer, released seismic activity is generally driven by diurnal ice/snow melting cycle. In winter, snow-cover conditions are associated with a reduced seismic release, with nevertheless some unexpected activity possibly related to snow-pack metamorphism. Based on icequake locations derived from data recorded in September, we discuss

  8. Seismicity in 2010 and major earthquakes recorded and located in Costa Rica from 1983 until 2012, by the local OVSICORI-UNA seismic network

    NASA Astrophysics Data System (ADS)

    Ronnie, Q.; Segura, J.; Burgoa, B.; Jimenez, W.; McNally, K. C.

    2013-05-01

    This work is the result of the analysis of existing information in the earthquake database of the Observatorio Sismológico y Vulcanológico de Costa Rica, Universidad Nacional (OVSICORI-UNA), and seeks disclosure of basic seismological information recorded and processed in 2010. In this year there was a transition between the software used to record, store and locate earthquakes. During the first three months of 2010, we used Earthworm (http://folkworm.ceri.memphis.edu/ew-doc), SEISAN (Haskov y Ottemoller, 1999) and Hypocenter (Lienert y Haskov, 1995) to capture, store and locate the earthquakes, respectively; in April 2010, ANTELOPE (http://www.brtt.com/software.html) start to be used for recording and storing and GENLOC (Fan at al, 2006) and LOCSAT (Bratt and Bache 1988), to locate earthquakes. GENLOC was used for local events and LOCSAT for regional and distant earthquakes. The local earthquakes were located using the 1D velocity model of Quintero and Kissling (2001) and for regional and distant earthquakes IASPEI91 (Kennett and Engdahl, 1991) was used. All the events for 2010 and shown in this work were rechecked by the authors. We located 3903 earthquakes in and around Costa Rica and 746 regional and distant seismic events were recorded (see Figure 1). In this work we also give a summary of major earthquakes recorded and located by OVSICORI-UNA network between 1983 and 2012. Seismicity recorded by OVSICORI-UNA network in 2010

  9. Strong Motion Network of Medellín and Aburrá Valley: technical advances, seismicity records and micro-earthquake monitoring

    NASA Astrophysics Data System (ADS)

    Posada, G.; Trujillo, J. C., Sr.; Hoyos, C.; Monsalve, G.

    2017-12-01

    The tectonics setting of Colombia is determined by the interaction of Nazca, Caribbean and South American plates, together with the Panama-Choco block collision, which makes a seismically active region. Regional seismic monitoring is carried out by the National Seismological Network of Colombia and the Accelerometer National Network of Colombia. Both networks calculate locations, magnitudes, depths and accelerations, and other seismic parameters. The Medellín - Aburra Valley is located in the Northern segment of the Central Cordillera of Colombia, and according to the Colombian technical seismic norm (NSR-10), is a region of intermediate hazard, because of the proximity to seismic sources of the Valley. Seismic monitoring in the Aburra Valley began in 1996 with an accelerometer network which consisted of 38 instruments. Currently, the network consists of 26 stations and is run by the Early Warning System of Medellin and Aburra Valley (SIATA). The technical advances have allowed the real-time communication since a year ago, currently with 10 stations; post-earthquake data is processed through operationally near-real-time, obtaining quick results in terms of location, acceleration, spectrum response and Fourier analysis; this information is displayed at the SIATA web site. The strong motion database is composed by 280 earthquakes; this information is the basis for the estimation of seismic hazards and risk for the region. A basic statistical analysis of the main information was carried out, including the total recorded events per station, natural frequency, maximum accelerations, depths and magnitudes, which allowed us to identify the main seismic sources, and some seismic site parameters. With the idea of a more complete seismic monitoring and in order to identify seismic sources beneath the Valley, we are in the process of installing 10 low-cost shake seismometers for micro-earthquake monitoring. There is no historical record of earthquakes with a magnitude

  10. MSNoise: a Python Package for Monitoring Seismic Velocity Changes using Ambient Seismic Noise

    NASA Astrophysics Data System (ADS)

    Lecocq, T.; Caudron, C.; Brenguier, F.

    2013-12-01

    Earthquakes occur every day all around the world and are recorded by thousands of seismic stations. In between earthquakes, stations are recording "noise". In the last 10 years, the understanding of this noise and its potential usage have been increasing rapidly. The method, called "seismic interferometry", uses the principle that seismic waves travel between two recorders and are multiple-scattered in the medium. By cross-correlating the two records, one gets an information on the medium below/between the stations. The cross-correlation function (CCF) is a proxy to the Green Function of the medium. Recent developments of the technique have shown those CCF can be used to image the earth at depth (3D seismic tomography) or study the medium changes with time. We present MSNoise, a complete software suite to compute relative seismic velocity changes under a seismic network, using ambient seismic noise. The whole is written in Python, from the monitoring of data archives, to the production of high quality figures. All steps have been optimized to only compute the necessary steps and to use 'job'-based processing. We present a validation of the software on a dataset acquired during the UnderVolc[1] project on the Piton de la Fournaise Volcano, La Réunion Island, France, for which precursory relative changes of seismic velocity are visible for three eruptions betwee 2009 and 2011.

  11. Seismic waves triggering slow slip event on the pressure gauge records in the Hikurangi subducting margin

    NASA Astrophysics Data System (ADS)

    Ito, Y.; Wallace, L. M.; Henrys, S. A.; Kaneko, Y.; Webb, S. C.; Muramoto, T.; Ohta, K.; Mochizuki, K.; Suzuki, S.; Kido, M.; Hino, R.

    2017-12-01

    The two M7-class earthquakes struck in New Zealand in 2016. One is the M7.1 Te Araroa earthquake on 1st September, and the other is the M7.8 Kaikoura earthquake on 14th November. The M7.1 earthquake struck offshore, following a sequence of the Hikurangi slow slip event on the northern Hikurangi Margin. The M7.8 Kaikoura earthquake has triggered a shallow slow slip event of northern Hikurangi subduction margin. We present seismic and tsunami waves radiated from two large earthquakes of M7.8 Kaikoura and M7.1 Te Araroa earthquakes in 2016 using a network of absolute pressure gauges (APG) deployed at the Hikurangi subduction margin offshore New Zealand. We deployed 5 APG on the accretionary wedge at the northen part of the Hikurangi margnin in June 2016 at the northern part of Hikurangi subducting margin, and were recovered in June 2015. The pressure gauge recorded data continuously for one year, with a logging interval of 1 or 2 s. Our processing of the APG data to identify seismic is a band pass filter with a range of 10-100 s is applied for seismic signals. We observed seismic waves radiated from both the M7.8 Kaikoura and M7.1 Te Araroa earthquakes. The pressure fluctuation more than 20 hPa from the arrivals of seismic waves was observed on two both earthquakes. It should be noted that marine pressure records are nearly equivalent to vertical acceleration measurements [Webb, 1998]. Specifically, on the M7.8 Kaikoura earthquake, the characteristic seismic signals with large amplitude more than 20 hPa lasting more than 300 s was observed on the all of four APGs. The long duration seismic waves with relatively large amplitude observed after the 7.8 Kaikoura earthquake would dynamically trigger the Hikurangi slow slip event; the dynamic triggering and characteristic seismic waves in the accretionary wedge has been predicted from a wave-field modeling using a 3D velocity model with a low-velocity sedimentary basin [Wallace et al., 2017].

  12. Seismic reading taken at MSC recording impact of Apollo 13 S-IVB with surface

    NASA Technical Reports Server (NTRS)

    1970-01-01

    A seismic reading taken from instruments at the Manned Spacecraft Center (MSC) recording impact of the Apollo 13 S-IVB/Instrument Unit with lunar surface. The expended Saturn third stage and instrument unit impacted the lunar surface at 7:09 p.m., April 14, 1970. The location of the impact was 2.4 degrees south latitude and 27.9 degrees west longitude, about 76 nautical miles west-northwest of the Apollo 12 Lunar Surface Experiment package deployment site. The S-IVB/IU impact was picked up by the Passive Seismic Experiment, a component of the package and transmitted to instruments at the Mission Control Center.

  13. Progressive Seismic Failure, Seismic Gap, and Great Seismic Risk across the Densely Populated North China Basin

    NASA Astrophysics Data System (ADS)

    Yin, A.; Yu, X.; Shen, Z.

    2014-12-01

    Although the seismically active North China basin has the most complete written records of pre-instrumentation earthquakes in the world, this information has not been fully utilized for assessing potential earthquake hazards of this densely populated region that hosts ~200 million people. In this study, we use the historical records to document the earthquake migration pattern and the existence of a 180-km seismic gap along the 600-km long right-slip Tangshan-Hejian-Cixian (THC) fault zone that cuts across the North China basin. The newly recognized seismic gap, which is centered at Tianjin with a population of 11 million people and ~120 km from Beijing (22 million people) and Tangshan (7 million people), has not been ruptured in the past 1000 years by M≥6 earthquakes. The seismic migration pattern in the past millennium suggests that the epicenters of major earthquakes have shifted towards this seismic gap along the THC fault, which implies that the 180- km gap could be the site of the next great earthquake with M≈7.6 if it is ruptured by a single event. Alternatively, the seismic gap may be explained by aseismic creeping or seismic strain transfer between active faults.

  14. Discriminating Induced-Microearthquakes Using New Seismic Features

    NASA Astrophysics Data System (ADS)

    Mousavi, S. M.; Horton, S.

    2016-12-01

    We studied characteristics of induced-microearthquakes on the basis of the waveforms recorded on a limited number of surface receivers using machine-learning techniques. Forty features in the time, frequency, and time-frequency domains were measured on each waveform, and several techniques such as correlation-based feature selection, Artificial Neural Networks (ANNs), Logistic Regression (LR) and X-mean were used as research tools to explore the relationship between these seismic features and source parameters. The results show that spectral features have the highest correlation to source depth. Two new measurements developed as seismic features for this study, spectral centroids and 2D cross-correlations in the time-frequency domain, performed better than the common seismic measurements. These features can be used by machine learning techniques for efficient automatic classification of low energy signals recorded at one or more seismic stations. We applied the technique to 440 microearthquakes-1.7Reference: Mousavi, S.M., S.P. Horton, C. A. Langston, B. Samei, (2016) Seismic features and automatic discrimination of deep and shallow induced-microearthquakes using neural network and logistic regression, Geophys. J. Int. doi: 10.1093/gji/ggw258.

  15. On the importance of changes in the gravity field on seismic recording at ultralong periods

    PubMed Central

    Okal, Emile A.

    1981-01-01

    The effect of changes in gravity induced by the Earth's deformation on seismic recording at ultralong periods is studied quantitatively for the low-order spheroidal modes of the Earth. Because this effect can either enhance or reduce the recorded amplitude of a mode, depending on its geometry, it may become nontrivial at the longest free-oscillation periods, and contribute to relative deviations of up to 17%. PMID:16592943

  16. Investigations of Periodic Disturbances on Seismic Aftershock Recordings

    NASA Astrophysics Data System (ADS)

    Liebsch, Mattes; Gorschlüter, Felix; Knoop, Jan-Frederik; Altmann, Jürgen

    2013-04-01

    The Comprehensive Nuclear Test-Ban Treaty Organisation (CTBTO) runs the International Monitoring System (IMS) to detect possible violations of the treaty. The seismic sensors of the IMS are set up to detect every underground explosion with a yield of 1 kT TNT equivalent or even better everywhere on the world. Under consideration of all IMS data the hypocentre of a large underground explosion is located within an area of about 1000 sq km. To verify if it was a violation of the Test-Ban Treaty the CTBTO (after CTBT entry into force) is allowed to carry out an on-site inspection (OSI) in the area of suspicion. During an OSI the hypocentre is to be located much more precisely; for this a local seismic aftershock monitoring system (SAMS) can be installed to detect small seismic events caused as a consequence of the explosion, such as relaxation of the rock around the cavity. However the magnitude of these aftershock signals is extremely weak. Other difficulties arise from other seismic signals in the inspection area, for example caused by vehicles of the inspectors, from coupling of airborne signals to the ground, or even by intended attempts to disturb the OSI. While the aftershock signals have a pulsed shape, man-made seismic signals (primarily created by engines) usually show periodic characteristics and thus are representable as a sum of sine functions and their harmonics. A mathematical expression for the Hann-windowed discrete Fourier transform of the underlying sine is used to characterise every such disturbance by the amplitude, frequency and phase. The contributions of these sines are computed and subtracted from the complex spectrum sequentially. Synthetic sines superposed to real signals, orders of magnitude stronger than the latter, can be removed successfully. Removal of periodic content from the signals of a helicopter overflight reduces the amplitude by a factor 3.3 when the frequencies are approximately constant. To reduce or prevent disturbing seismic

  17. Implosion, earthquake, and explosion recordings from the 2000 Seattle Kingdome Seismic Hazards Investigation of Puget Sound (SHIPS), Washington

    USGS Publications Warehouse

    Brocher, Thomas M.; Pratt, Thomas L.; Weaver, Craig S.; Snelson, Catherine M.; Frankel, Arthur D.

    2002-01-01

    This report describes seismic data obtained in Seattle, Washington, March 24-28, 2000, during a Seismic Hazards Investigation of Puget Sound (SHIPS). The seismic recordings obtained by this SHIPS experiment, nicknamed Kingdome SHIPS, were designed to (1) measure site responses throughout Seattle and to (2) help define the location of the Seattle fault. During Kingdome SHIPS, we recorded the Kingdome implosion, four 150-lb (68-kg) shots, and a Mw = 7.6 teleseism using a dense network of seismographs deployed throughout Seattle. The seismographs were deployed at a nominal spacing of 1 km in a hexagonal grid extending from Green Lake in the north to Boeing Field in the south. The Seattle Kingdome was a domed sports stadium located in downtown Seattle near the Seattle fault. The Seattle Kingdome was imploded (demolished) at 8:32 AM local time (16:32 UTC) on March 26 (JD 086), 2000. The seismic energy produced by implosion of the Kingdome was equivalent to a local earthquake magnitude of 2.3. Strong impacts produced by the implosion of the Kingdome generated seismic arrivals to frequencies as low as 0.1 Hz. Two shots located north of the Seattle fault, where the charges were detonated within the ground water column (Discovery and Magnuson Parks), were much more strongly coupled than were the two shots to the south of the Seattle fault, where the shots were detonated above the water table (Lincoln and Seward Parks). Thirty-eight RefTek stations, scattered throughout Seattle, recorded the Mw = 7.6 Japan Volcano Islands earthquake (22.4°N, 143.6°E, 104 km depth) of 28 March 2000 (JD 088). This teleseism produced useful signals for periods between 4 and 7 seconds. Only a few recordings of small magnitude local earthquakes were made, and these recordings are not presented. In this report, we describe the acquisition of these data, discuss the processing and merging of the data into common shot gathers, and illustrate the acquired data. We also describe the format and

  18. Analysis of recently digitized continuous seismic data recorded during the March-May, 1980, eruption sequence at Mount St. Helens

    NASA Astrophysics Data System (ADS)

    Moran, S. C.; Malone, S. D.

    2013-12-01

    The May 18, 1980, eruption of Mount St. Helens (MSH) was an historic event, both for society and for the field of volcanology. However, our knowledge of the eruption and the precursory period leading up it is limited by the fact that most of the data, particularly seismic recordings, were not kept due to severe limitations in the amount of digital data that could be handled and stored using 1980 computer technology. Because of these limitations, only about 900 digital event files have been available for seismic studies of the March-May seismic sequence out of a total of more than 4,000 events that were counted using paper records. Fortunately, data from a subset of stations were also recorded continuously on a series of 24 analog 14-track IRIG magnetic tapes. We have recently digitized these tapes and time-corrected and cataloged the resultant digital data streams, enabling more in-depth studies of the (almost) complete pre-eruption seismic sequence using modern digital processing techniques. Of the fifteen seismic stations operating near MSH for at least a part of the two months between March 20 and May 18, six stations have relatively complete analog recordings. These recordings have gaps of minutes to days because of radio noise, poor tape quality, or missing tapes. In addition, several other stations have partial records. All stations had short-period vertical-component sensors with very limited dynamic range and unknown response details. Nevertheless, because the stations were at a range of distances and were operated at a range of gains, a variety of earthquake sizes were recorded on scale by at least one station, and therefore a much more complete understanding of the evolution of event types, sizes and character should be achievable. In our preliminary analysis of this dataset we have found over 10,000 individual events as recorded on stations 35-40 km from MSH, spanning a recalculated coda-duration magnitude range of ~1.5 to 4.1, including many M < 3

  19. Local Seismicity Recorded by ChilePEPPER: Implications for Dynamic Accretionary Prism Response and Long-term Prism Evolution

    NASA Astrophysics Data System (ADS)

    de Moor, A.; Trehu, A. M.; Tryon, M. D.

    2015-12-01

    To investigate the dynamic response of the outer accretionary wedge updip from the patch of greatest slip during the Mw8.8 2010 Maule earthquake, 10 Ocean Bottom Seismometers (OBS) were deployed from May 2012 to March 2013 in a small array with an inter-instrument spacing of ~12 km . Nine instruments were recovered, with 4 recording data on 3 intermediate-band 3-component seismometers and a differential pressure gauge and 5 recording data from absolute pressure gauges. [note: All instruments were also equipped with a fluid flow meter sensitive to flow rates as low as 0.0001 cm/yr in or out of the sediments. However, no flow signal was detected.] Here we present hypocenters for 569 local events that have S-P times less than 17 seconds (i.e. within ~125 km of the array) using hand-picked arrival times and a 1D velocity model derived from a 2D seismic refraction profile through the region (Moscoso et al 2011, EPSL). We analyze the distribution of seismicity in the context of published slip models, ChilePEPPER high-resolution seismic reflection data, critical taper analysis done by Cubas et al 2013 (EPSL), and offshore gravity data. The data show distinct segmentation within the outer prism. The northern section of the study area is characterized by a lack of seismicity, accretion of nearly all incoming sediment and a prism at critical taper. In contrast, abundant seismicity, significant sediment underthrusting at the deformation front and a prism below critical taper angle characterize the southern part of the study area. Both coseismic slip and post-rupture local seismicity can be related to density anomalies within the upper plate as revealed by free air gravity data corrected for the effects of bathymetry and the subducting plate. [ChilePEPPER - Project Evaluating Prism Post-Earthquake Response

  20. Thirty years of seismic network recording in South Australia: Selected results

    NASA Astrophysics Data System (ADS)

    Greenhalgh, S. A.; Love, D.; Sinadinovski, C.

    1994-11-01

    The year 1993 marks 30 years of seismic network recording of earthquakes in South Australia. The network currently comprises 17 short-period instruments, of which six use digital recording and five employ triaxial sensors. Approximately 350 earthquakes are located within the State each year using a computerized seismic analysis system developed by the Phillip Institute of Technology. A duration-based magnitude scale, equivalent to the Richter M(sub L) scale, has been developed for most stations. The pre-network (historical) record of earthquake activity in South Australia dates back to 1837. Epicenters are available for just 45 earthquakes. Of these, ten are of magnitude five or greater. The instrumental data over the last 30 years show a similar trend in epicentral pattern to the historical earthquakes, with the major zones being the Flinders Ranges, Eyre Peninsula and the Southeast. There have been 40 earthquakes of magnitude four or greater since 1963, the largest earthquake being of magnitude six in the Musgrave Ranges during 1986. Mine and quarry blasts within the State have been useful in calibration of the network, both in terms of hypocentral location and amplitude studies. The explosions have also furnished valuable information on the crustal velocity distribution. Epicentral co-ordinates of mine blasts are generally good to within 3-5 km. The explosions yield Richter magnitudes of one (charge size 1 or 2 tons) to 2.5 (charge size 50 tons). The crustal S waves, used in earthquake magnitude determinations, exhibit an amplitude-distance decay coefficient of 1.2. The P-wave velocity function of the crust increases non-linearly with depth, from about 5.0 km /s near the surface to 6.4 km /s at 20 km depth, where the gradient reduces, with the velocity reaching a value of about 7.4 km /s at a depth of 40 km.

  1. Seismic signal and noise on Europa and how to use it

    NASA Astrophysics Data System (ADS)

    Panning, M. P.; Stähler, S. C.; Bills, B. G.; Castillo, J.; Huang, H. H.; Husker, A. L.; Kedar, S.; Lorenz, R. D.; Pike, W. T.; Schmerr, N. C.; Tsai, V. C.; Vance, S.

    2017-12-01

    Seismology is one of our best tools for detailing interior structure of planetary bodies, and a seismometer is included in the baseline and threshold mission design for a potential Europa lander mission. Guiding mission design and planning for adequate science return, though, requires modeling of both the anticipated signal and noise. Assuming ice seismicity on Europa behaves according to statistical properties observed in Earth catalogs and scaling cumulative seismic moment release to the moon, we simulate long seismic records and estimate background noise and peak signal amplitudes (Panning et al., 2017). This suggests a sensitive instrument comparable to many broadband terrestrial instruments or the SP instrument from the InSight mission to Mars will be able to record signals, while high frequency geophones are likely inadequate. We extend this analysis to also begin incorporation of spatial and temporal variation due to the tidal cycle, which can help inform landing site selection. We also begin exploration of how chaotic terrane at the bottom of the ice shell and inter-ice heterogeneities (i.e. internal melt structures) may affect predicted seismic observations using 2D numerical seismic simulations. We also show some of the key seismic observations to determine interior properties of Europa (Stähler et al., 2017). M. P. Panning, S. C. Stähler, H.-H. Huang, S. D. Vance, S. Kedar, V. C. Tsai, W. T. Pike, R. D. Lorenz, "Expected seismicity and the seismic noise environment of Europa," J. Geophys. Res., in revision, 2017. S. C. Stähler, M. P. Panning, S. D. Vance, R. D. Lorenz, M. van Driel, T. Nissen-Meyer, S. Kedar, "Seismic wave propagation in icy ocean worlds," J. Geophys. Res., in revision, 2017.

  2. Deep Downhole Seismic Testing at the Waste Treatment Plant Site, Hanford, WA. Volume IV S-Wave Measurements in Borehole C4993 Seismic Records, Wave-Arrival Identifications and Interpreted S-Wave Velocity Profile.

    DOE Office of Scientific and Technical Information (OSTI.GOV)

    Stokoe, Kenneth H.; Li, Song Cheng; Cox, Brady R.

    2007-06-06

    In this volume (IV), all S-wave measurements are presented that were performed in Borehole C4993 at the Waste Treatment Plant (WTP) with T-Rex as the seismic source and the Lawrence Berkeley National Laboratory (LBNL) 3-D wireline geophone as the at-depth borehole receiver. S-wave measurements were performed over the depth range of 370 to 1300 ft, typically in 10-ft intervals. However, in some interbeds, 5-ft depth intervals were used, while below about 1200 ft, depth intervals of 20 ft were used. Shear (S) waves were generated by moving the base plate of T-Rex for a given number of cycles at amore » fixed frequency as discussed in Section 2. This process was repeated so that signal averaging in the time domain was performed using 3 to about 15 averages, with 5 averages typically used. In addition, a second average shear wave record was recorded by reversing the polarity of the motion of the T-Rex base plate. In this sense, all the signals recorded in the field were averaged signals. In all cases, the base plate was moving perpendicular to a radial line between the base plate and the borehole which is in and out of the plane of the figure shown in Figure 1.1. The definition of “in-line”, “cross-line”, “forward”, and “reversed” directions in items 2 and 3 of Section 2 was based on the moving direction of the base plate. In addition to the LBNL 3-D geophone, called the lower receiver herein, a 3-D geophone from Redpath Geophysics was fixed at a depth of 22 ft in Borehole C4993, and a 3-D geophone from the University of Texas (UT) was embedded near the borehole at about 1.5 ft below the ground surface. The Redpath geophone and the UT geophone were properly aligned so that one of the horizontal components in each geophone was aligned with the direction of horizontal shaking of the T-Rex base plate. This volume is organized into 12 sections as follows. Section 1: Introduction, Section 2: Explanation of Terminology, Section 3: Vs Profile at Borehole C

  3. Earthquake recordings from the 2002 Seattle Seismic Hazard Investigation of Puget Sound (SHIPS), Washington State

    USGS Publications Warehouse

    Pratt, Thomas L.; Meagher, Karen L.; Brocher, Thomas M.; Yelin, Thomas; Norris, Robert; Hultgrien, Lynn; Barnett, Elizabeth; Weaver, Craig S.

    2003-01-01

    This report describes seismic data obtained during the fourth Seismic Hazard Investigation of Puget Sound (SHIPS) experiment, termed Seattle SHIPS . The experiment was designed to study the influence of the Seattle sedimentary basin on ground shaking during earthquakes. To accomplish this, we deployed seismometers over the basin to record local earthquakes, quarry blasts, and teleseisms during the period of January 26 to May 27, 2002. We plan to analyze the recordings to compute spectral amplitudes at each site, to determine the variability of ground motions over the basin. During the Seattle SHIPS experiment, seismometers were deployed at 87 sites in a 110-km-long east-west line, three north-south lines, and a grid throughout the Seattle urban area (Figure 1). At each of these sites, an L-22, 2-Hz velocity transducer was installed and connected to a REF TEK Digital Acquisition System (DAS), both provided by the Program for Array Seismic Studies of the Continental Lithosphere (PASSCAL) of the Incorporated Research Institutes for Seismology (IRIS). The instruments were installed on January 26 and 27, and were retrieved gradually between April 18 and May 27. All instruments continuously sampled all three components of motion (velocity) at a sample rate of 50 samples/sec. To ensure accurate computations of amplitude, we calibrated the geophones in situ to obtain the instrument responses. In this report, we discuss the acquisition of these data, we describe the processing and merging of these data into 1-hour long traces and into windowed events, we discuss the geophone calibration process and its results, and we display some of the earthquake recordings.

  4. Structure of the southern Juan de Fuca Ridge from seismic reflection records

    USGS Publications Warehouse

    Morton, Janet L.; Sleep, Norman H.; Normark, William R.; Tompkins, Donald H.

    1987-01-01

    Twenty-four-channel seismic reflection records were obtained from the axial region of the southern Juan de Fuca Ridge. Two profiles are normal to the strike of the spreading center and intersect the ridge at latitude 44°40′N and 45°05′N; a third profile extends south along the ridge axis from latitude 45°20′N and crosses the Blanco Fracture Zone. Processing of the axial portions of the cross-strike lines resolved a weak reflection centered beneath the axis. The reflector is at a depth similar to seismically detected magma chambers on the East Pacific Rise and a Lau Basin spreading center; we suggest that the reflector represents the top of an axial magma chamber. In the migrated sections the top of the probable magma chamber is relatively flat and 1–2 km wide, and the subbottom depth of the chamber is greater where the depth to the ridge axis is greater.

  5. Based on records of Three Gorge Telemetric Seismic Network to analyze Vibration process of micro fracture of rock landslide

    NASA Astrophysics Data System (ADS)

    WANG, Q.

    2017-12-01

    Used the finite element analysis software GeoStudio to establish vibration analysis model of Qianjiangping landslide, which locates at the Three Gorges Reservoir area. In QUAKE/W module, we chosen proper Dynamic elasticity modulus and Poisson's ratio of soil layer and rock stratum. When loading, we selected the waveform data record of Three Gorge Telemetric Seismic Network as input ground motion, which includes five rupture events recorded of Lujiashan seismic station. In dynamic simulating, we mainly focused on sliding process when the earthquake date record was applied. The simulation result shows that Qianjiangping landslide wasn't not only affected by its own static force, but also experienced the dynamic process of micro fracture-creep-slip rupture-creep-slip.it provides a new approach for the early warning feasibility of rock landslide in future research.

  6. Active seismic experiment

    NASA Technical Reports Server (NTRS)

    Kovach, R. L.; Watkins, J. S.; Talwani, P.

    1972-01-01

    The Apollo 16 active seismic experiment (ASE) was designed to generate and monitor seismic waves for the study of the lunar near-surface structure. Several seismic energy sources are used: an astronaut-activated thumper device, a mortar package that contains rocket-launched grenades, and the impulse produced by the lunar module ascent. Analysis of some seismic signals recorded by the ASE has provided data concerning the near-surface structure at the Descartes landing site. Two compressional seismic velocities have so far been recognized in the seismic data. The deployment of the ASE is described, and the significant results obtained are discussed.

  7. Imaging a Fault Boundary System Using Controlled-Source Data Recorded on a Large-N Seismic Array

    NASA Astrophysics Data System (ADS)

    Paschall, O. C.; Chen, T.; Snelson, C. M.; Ralston, M. D.; Rowe, C. A.

    2016-12-01

    The Source Physics Experiment (SPE) is a series of chemical explosions conducted in southern Nevada with an objective of improving nuclear explosion monitoring. Five chemical explosions have occurred thus far in granite, the most recent being SPE-5 on April 26, 2016. The SPE series will improve our understanding of seismic wave propagation (primarily S-waves) due to explosions, and allow better discrimination of background seismicity such as earthquakes and explosions. The Large-N portion of the project consists of 996 receiver stations. Half of the stations were vertical component and the other half were three-component geophones. All receivers were deployed for 30 days and recorded the SPE-5 shot, earthquakes, noise, and an additional controlled-source: a large weight-drop, which is a 13,000 kg modified industrial pile driver. In this study, we undertake reflection processing of waveforms from the weight-drop, as recorded by a line of sensors extracted from the Large-N array. The profile is 1.2 km in length with 25 m station spacing and 100 m shot point spacing. This profile crosses the Boundary Fault that separates granite body and an alluvium basin, a strong acoustic impedance boundary that scatters seismic energy into S-waves and coda. The data were processed with traditional seismic reflection processing methods that include filtering, deconvolution, and stacking. The stack will be used to extract the location of the splays of the Boundary Fault and provide geologic constraints to the modeling and simulation teams within the SPE project.

  8. Unsupervised seismic facies analysis with spatial constraints using regularized fuzzy c-means

    NASA Astrophysics Data System (ADS)

    Song, Chengyun; Liu, Zhining; Cai, Hanpeng; Wang, Yaojun; Li, Xingming; Hu, Guangmin

    2017-12-01

    Seismic facies analysis techniques combine classification algorithms and seismic attributes to generate a map that describes main reservoir heterogeneities. However, most of the current classification algorithms only view the seismic attributes as isolated data regardless of their spatial locations, and the resulting map is generally sensitive to noise. In this paper, a regularized fuzzy c-means (RegFCM) algorithm is used for unsupervised seismic facies analysis. Due to the regularized term of the RegFCM algorithm, the data whose adjacent locations belong to same classification will play a more important role in the iterative process than other data. Therefore, this method can reduce the effect of seismic data noise presented in discontinuous regions. The synthetic data with different signal/noise values are used to demonstrate the noise tolerance ability of the RegFCM algorithm. Meanwhile, the fuzzy factor, the neighbour window size and the regularized weight are tested using various values, to provide a reference of how to set these parameters. The new approach is also applied to a real seismic data set from the F3 block of the Netherlands. The results show improved spatial continuity, with clear facies boundaries and channel morphology, which reveals that the method is an effective seismic facies analysis tool.

  9. Six-degree-of-freedom local seismic records from micro-earthquakes and anthropogenic events

    NASA Astrophysics Data System (ADS)

    Brokešová, J.; Málek, J.

    2012-04-01

    Full ground motion description, including both translational and rotational components, attracts still more attention in modern seismology. There is a need for portable rotational sensors, easily installed and operated in the field, sensitive enough to provide 6DOF records in a wide range of amplitudes excited not only by strong but also weak motion events. A new prototype of our rotational seismic sensor system (Rotaphone) designed to measure three rotation rate and three ground velocity components is presented. Our method is based on measurements of the differential motions between paired low-frequency geophones attached to a rigid skeleton, the size of which is much smaller than the wavelength of interest. This approach is conditioned by a precise calibration of each paired geophone in the system. A method of our in-situ calibration is explained and demonstrated. The device was thoroughly tested at the Albuquerque Seismological Laboratory, U.S. Geological Survey, with focus on linearity and cross-axis errors. Results of these tests confirm its proper function. The Rotaphone operates in the frequency range 2-40 Hz and its dynamic range is at least 120 dB. It was successfully applied to measure 6DOF ground motions from local shallow micro-earthquakes in the West Bohemia swarm area (Czech Republic), at Hronov-Pozíčí fault zone in East Bohemia (Czech Republic), and in the vicinity of the salt-works of Provadia (Bulgaria). It was also used to obtain records from anthropogenic sources (blasts, rockbursts). Three-axial rotation rate records for these types of events are shown and discussed. Their peak amplitudes reach values from 10-7 rad/s to 10-4 rad/s. To characterize the significance of rotation we define the rotation to translation ratio (RTR) relating peak amplitudes of rotation rate and translational velocity. The RTR factor for different types of local events is discussed in view of its dependence on hypocentral distance, source type and probably on

  10. Seabed topography beneath Larsen C Ice Shelf from seismic soundings

    NASA Astrophysics Data System (ADS)

    Brisbourne, A. M.; Smith, A. M.; King, E. C.; Nicholls, K. W.; Holland, P. R.; Makinson, K.

    2013-08-01

    Seismic reflection soundings of ice thickness and seabed depth were acquired on the Larsen C Ice Shelf in order to test a sub-shelf bathymetry model derived from the inversion of IceBridge gravity data. A series of lines were collected, from the Churchill Peninsula in the north to the Joerg Peninsula in the south, and also towards the ice front. Sites were selected using the bathymetry model derived from the inversion of free-air gravity data to indicate key regions where sub-shelf oceanic circulation may be affected by ice draft and sub-shelf cavity thickness. The seismic velocity profile in the upper 100 m of firn and ice was derived from shallow refraction surveys at a number of locations. Measured temperatures within the ice column and at the ice base were used to define the velocity profile through the remainder of the ice column. Seismic velocities in the water column were derived from previous in situ measurements. Uncertainties in ice and water cavity thickness are in general <10 m. Compared with the seismic measurements, the root-mean-square error in the gravimetrically derived bathymetry at the seismic sites is 162 m. The seismic profiles prove the non-existence of several bathymetric features that are indicated in the gravity inversion model, significantly modifying the expected oceanic circulation beneath the ice shelf. Similar features have previously been shown to be highly significant in affecting basal melt rates predicted by ocean models. The discrepancies between the gravity inversion results and the seismic bathymetry are attributed to the assumption of uniform geology inherent in the gravity inversion process and also the sparsity of IceBridge flight lines. Results indicate that care must be taken when using bathymetry models derived by the inversion of free-air gravity anomalies. The bathymetry results presented here will be used to improve existing sub-shelf ocean circulation models.

  11. Metamorphic records of multiple seismic cycles during subduction

    PubMed Central

    Hacker, Bradley R.; Seward, Gareth G. E.; Kelley, Chris S.

    2018-01-01

    Large earthquakes occur in rocks undergoing high-pressure/low-temperature metamorphism during subduction. Rhythmic major-element zoning in garnet is a common product of such metamorphism, and one that must record a fundamental subduction process. We argue that rhythmic major-element zoning in subduction zone garnets from the Franciscan Complex, California, developed in response to growth-dissolution cycles driven by pressure pulses. Using electron probe microanalysis and novel techniques in Raman and synchrotron Fourier transform infrared microspectroscopy, we demonstrate that at least four such pressure pulses, of magnitude 100–350 MPa, occurred over less than 300,000 years. These pressure magnitude and time scale constraints are most consistent with the garnet zoning having resulted from periodic overpressure development-dissipation cycles, related to pore-fluid pressure fluctuations linked to earthquake cycles. This study demonstrates that some metamorphic reactions can track individual earthquake cycles and thereby opens new avenues to the study of seismicity. PMID:29568800

  12. Pre-instrumental seismicity in Central Africa using felt seisms recorded mainly at the meteorological stations of DRC, Rwanda and Burundi during the colonial period

    NASA Astrophysics Data System (ADS)

    Mulumba, J.-L.; Delvaux, D.

    2012-04-01

    Seismic hazard assessment and mitigation of catastrophes are primarily based on the identification and characterization of seismically active zones. These tasks still rely heavily on the existing knowledge of the seismic activity over the longest possible time period. The first seismic network in Equatorial Africa (IRSAC network) was operated from the Lwiro scientific base on the western shores of Lake Kivu between 1953 and 1963. Before this installation, the historical record of seismic activity in Central Africa is sparse. Even for the relatively short period concerned, spanning only 50-60 years, the historical record is far from being complete. A first attempt has been made by Herrinckx (1959) who compiled a list 960 felt seisms recorded at the meteorological stations between 1915 and 1954 in Congo, Rwanda and Burundi. They were used to draw a density map of felt seisms per square degree. We completed this data base by exploiting the meteorological archives and any available historical report to enlarge the database which now reaches 1513 entries between 1900 and 1959. These entries have been exanimate in order to identify possible historical seismic events. Those are defined by 3 or more quasi-simultaneous records observed over a relatively short distance (a few degrees of latitude/longitude) within a short time difference (few hours). A preliminary list of 115 possible historical seisms has been obtained, identified by 3 to 15 different stations. The proposed location is taken as the average latitude and longitude of the stations where the felt seisms were recorded. Some of the most important ones are associated to aftershocks that have been felt at some stations after the main shocks. The most recent felt seisms have been also recorded instrumentally, which helps to validate the procedure followed. The main difficulties are the magnitude estimation and the possible spatial incompleteness of the recording of felt seism evidence at the margin of the observation

  13. Numerical modeling and characterization of rock avalanches and associated seismic signal

    NASA Astrophysics Data System (ADS)

    Moretti, L.; Mangeney, A.; Capdeville, Y.; Stutzmann, E.; Lucas, A.; Huggel, C.; Schneider, D.; Crosta, G. B.; Bouchut, F.

    2012-04-01

    recorded seismic signal depends on the characteristics of the landslide (volume, mass, friction coefficient…) and on the earth model (seismic waves velocity, number of layers…) used to calculate wave propagation. Favreau, P., Mangeney, A., Lucas, A., Crosta, G.B., and F. Bouchut, Numerical modeling of landquakes. Geophysical Research Letters, VOL. 37, L15305, doi:10.1029/2010GL043512, 2010 Huggel, C., Caplan-Auerbach, J., Molnia, B. and Wessels R. (2008), The 2005 Mt. Steller, Alaska, rock-ice avalanche: A large slope failure in cold permafrost, Proceedings of the Ninth International Conference on Permafrost, vol. 1., p. 747-752, Univ. of Alaska Fairbanks

  14. Automatic Processing and Interpretation of Long Records of Endogenous Micro-Seismicity: the Case of the Super-Sauze Soft-Rock Landslide.

    NASA Astrophysics Data System (ADS)

    Provost, F.; Malet, J. P.; Hibert, C.; Doubre, C.

    2017-12-01

    The Super-Sauze landslide is a clay-rich landslide located the Southern French Alps. The landslide exhibits a complex pattern of deformation: a large number of rockfalls are observed in the 100 m height main scarp while the deformation of the upper part of the accumulated material is mainly affected by material shearing along stable in-situ crests. Several fissures are locally observed. The shallowest layer of the accumulated material tends to behave in a brittle manner but may undergo fluidization and/or rapid acceleration. Previous studies have demonstrated the presence of a rich endogenous micro-seismicity associated to the deformation of the landslide. However, the lack of long-term seismic records and suitable processing chains prevented a full interpretation of the links between the external forcings, the deformation and the recorded seismic signals. Since 2013, two permanent seismic arrays are installed in the upper part of the landslide. We here present the methodology adopted to process this dataset. The processing chain consists of a set of automated methods for automatic and robust detection, classification and location of the recorded seismicity. Thousands of events are detected and further automatically classified. The classification method is based on the description of the signal through attributes (e.g. waveform, spectral content properties). These attributes are used as inputs to classify the signal using a Random Forest machine-learning algorithm in four classes: endogenous micro-quakes, rockfalls, regional earthquakes and natural/anthropogenic noises. The endogenous landslide sources (i.e. micro-quake and rockfall) are further located. The location method is adapted to the type of event. The micro-quakes are located with a 3D velocity model derived from a seismic tomography campaign and an optimization of the first arrival picking with the inter-trace correlation of the P-wave arrivals. The rockfalls are located by optimizing the inter

  15. Seismic Noise Analysis and Reduction through Utilization of Collocated Seismic and Atmospheric Sensors at the GRO Chile Seismic Network

    NASA Astrophysics Data System (ADS)

    Farrell, M. E.; Russo, R. M.

    2013-12-01

    The installation of Earthscope Transportable Array-style geophysical observatories in Chile expands open data seismic recording capabilities in the southern hemisphere by nearly 30%, and has nearly tripled the number of seismic stations providing freely-available data in southern South America. Through the use of collocated seismic and atmospheric sensors at these stations we are able to analyze how local atmospheric conditions generate seismic noise, which can degrade data in seismic frequency bands at stations in the ';roaring forties' (S latitudes). Seismic vaults that are climate-controlled and insulated from the local environment are now employed throughout the world in an attempt to isolate seismometers from as many noise sources as possible. However, this is an expensive solution that is neither practical nor possible for all seismic deployments; and also, the increasing number and scope of temporary seismic deployments has resulted in the collection and archiving of terabytes of seismic data that is affected to some degree by natural seismic noise sources such as wind and atmospheric pressure changes. Changing air pressure can result in a depression and subsequent rebound of Earth's surface - which generates low frequency noise in seismic frequency bands - and even moderate winds can apply enough force to ground-coupled structures or to the surface above the seismometers themselves, resulting in significant noise. The 10 stations of the permanent Geophysical Reporting Observatories (GRO Chile), jointly installed during 2011-12 by IRIS and the Chilean Servicio Sismológico, include instrumentation in addition to the standard three seismic components. These stations, spaced approximately 300 km apart along the length of the country, continuously record a variety of atmospheric data including infrasound, air pressure, wind speed, and wind direction. The collocated seismic and atmospheric sensors at each station allow us to analyze both datasets together, to

  16. Detection of Temporally and Spatially Limited Periodic Earthquake Recurrence in Synthetic Seismic Records

    NASA Astrophysics Data System (ADS)

    Zielke, O.; Arrowsmith, R. J.

    2005-12-01

    The nonlinear dynamics of fault behavior are dominated by complex interactions among the multiple processes controlling the system. For example, temporal and spatial variations in pore pressure, healing effects, and stress transfer cause significant heterogeneities in fault properties and the stress-field at the sub-fault level. Numerical and laboratory fault models show that the interaction of large systems of fault elements causes the entire system to develop into a state of self-organized criticality. Once in this state, small perturbations of the system may result in chain reactions (i.e., earthquakes) which can affect any number of fault segments. This sensitivity to small perturbations is strong evidence for chaotic fault behavior, which implies that exact event prediction is not possible. However, earthquake prediction with a useful accuracy is nevertheless possible. Studies of other natural chaotic systems have shown that they may enter states of metastability, in which the system's behavior is predictable. Applying this concept to earthquake faults, these windows of metastable behavior should be characterized by periodic earthquake recurrence. The observed periodicity of the Parkfield, CA (M= 6) events may resemble such a window of metastability. I am statistically analyzing numerically generated seismic records to study these phases of periodic behavior. In this preliminary study, seismic records were generated using a model introduced by Nakanishi [Phys. Rev. A, 43, 6613-6621, 1991]. It consists of a one-dimensional chain of blocks (interconnected by springs) with a relaxation function that mimics velocity-weakened frictional behavior. The earthquakes occurring in this model show generally a power-law frequency-size distribution. However, for large events the distribution has a shoulder where the frequency of events is higher than expected from the power law. I have analyzed time-series of single block motions within the system. These time-series include

  17. Seabed topography beneath Larsen C Ice Shelf from seismic soundings

    NASA Astrophysics Data System (ADS)

    Brisbourne, A. M.; Smith, A. M.; King, E. C.; Nicholls, K. W.; Holland, P. R.; Makinson, K.

    2014-01-01

    Seismic reflection soundings of ice thickness and seabed depth were acquired on the Larsen C Ice Shelf in order to test a sub-ice shelf bathymetry model derived from the inversion of IceBridge gravity data. A series of lines was collected, from the Churchill Peninsula in the north to the Joerg Peninsula in the south, and also towards the ice front. Sites were selected using the bathymetry model derived from the inversion of free-air gravity data to indicate key regions where sub-ice shelf oceanic circulation may be affected by ice draft and seabed depth. The seismic velocity profile in the upper 100 m of firn and ice was derived from shallow refraction surveys at a number of locations. Measured temperatures within the ice column and at the ice base were used to define the velocity profile through the remainder of the ice column. Seismic velocities in the water column were derived from previous in situ measurements. Uncertainties in ice and water cavity thickness are in general < 10 m. Compared with the seismic measurements, the root-mean-square error in the gravimetrically derived bathymetry at the seismic sites is 162 m. The seismic profiles prove the non-existence of several bathymetric features that are indicated in the gravity inversion model, significantly modifying the expected oceanic circulation beneath the ice shelf. Similar features have previously been shown to be highly significant in affecting basal melt rates predicted by ocean models. The discrepancies between the gravity inversion results and the seismic bathymetry are attributed to the assumption of uniform geology inherent in the gravity inversion process and also the sparsity of IceBridge flight lines. Results indicate that care must be taken when using bathymetry models derived by the inversion of free-air gravity anomalies. The bathymetry results presented here will be used to improve existing sub-ice shelf ocean circulation models.

  18. Rescaled Range analysis of Induced Seismicity: rapid classification of clusters in seismic crisis

    NASA Astrophysics Data System (ADS)

    Bejar-Pizarro, M.; Perez Lopez, R.; Benito-Parejo, M.; Guardiola-Albert, C.; Herraiz, M.

    2017-12-01

    Different underground fluid operations, mainly gas storing, fracking and water pumping, can trigger Induced Seismicity (IS). This seismicity is normally featured by small-sized earthquakes (M<2.5), although particular cases reach magnitude as great as 5. It has been up for debate whether earthquakes greater than 5 can be triggered by IS or this level of magnitude only corresponds to tectonic earthquakes caused by stress change. Whatever the case, the characterization of IS for seismic clusters and seismic series recorded close but not into the gas storage, is still under discussion. Time-series of earthquakes obey non-linear patterns where the Hurst exponent describes the persistency or anti-persistency of the sequence. Natural seismic sequences have an H-exponent close to 0.7, which combined with the b-value time evolution during the time clusters, give us valuable information about the stationarity of the phenomena. Tectonic earthquakes consist in a main shock with a decay of time-occurrence of seismic shocks obeying the Omori's empirical law. On the contrary, IS does not exhibit a main shock and the time occurrence depends on the injection operations instead of on the tectonic energy released. In this context, the H-exponent can give information about the origin of the sequence. In 2013, a seismic crisis was declared from the Castor underground gas storing located off-shore in the Mediterranean Sea, close to the Northeastern Spanish cost. The greatest induced earthquake was 3.7. However, a 4.2 earthquake, probably of tectonic origin, occurred few days after the operations stopped. In this work, we have compared the H-exponent and the b-value time evolution according to the timeline of gas injection. Moreover, we have divided the seismic sequence into two groups: (1) Induced Seismicity and (2) Triggered Seismicity. The rescaled range analysis allows the differentiation between natural and induced seismicity and gives information about the persistency and long

  19. Crustal migration of CO2-rich magmatic fluids recorded by tree-ring radiocarbon and seismicity at Mammoth Mountain, CA, USA

    USGS Publications Warehouse

    Lewicki, Jennifer L.; Hilley, George E.; Shelly, David R.; King, John C.; McGeehin, John P.; Mangan, Margaret T.; Evans, William C.

    2014-01-01

    Unrest at Mammoth Mountain over the past several decades, manifest by seismicity, ground deformation, diffuse CO2 emissions, and elevated 3He/4He ratios in fumarolic gases has been driven by the release of CO2-rich fluids from basaltic intrusions in the middle to lower crust. Recent unrest included the occurrence of three lower-crustal (32–19 km depth) seismic swarms beneath Mammoth Mountain in 2006, 2008 and 2009 that were consistently followed by peaks in the occurrence rate of shallow (≤10 km depth) earthquakes. We measured 14C in the growth rings (1998–2012) of a tree growing in the largest (∼0.3 km2) area of diffuse CO2 emissions on Mammoth Mountain (the Horseshoe Lake tree kill; HLTK) and applied atmospheric CO2 concentration source area modeling to confirm that the tree was a reliable integrator of magmatic CO2 emissions over most of this area. The tree-ring 14C record implied that magmatic CO2 emissions from the HLTK were relatively stable from 1998 to 2009, nearly doubled from 2009 to 2011, and then declined by the 2012 growing season. The initial increase in CO2 emissions was detected during the growing season that immediately followed the largest (February 2010) peak in the occurrence rate of shallow earthquakes. Migration of CO2-rich magmatic fluids may have driven observed patterns of elevated deep, then shallow seismicity, while the relationship between pore fluid pressures within a shallow (upper 3 km of crust) fluid reservoir and permeability structure of the reservoir cap rock may have controlled the temporal pattern of surface CO2 emissions.

  20. Seismic Strong Motion Array Project (SSMAP) to Record Future Large Earthquakes in the Nicoya Peninsula area, Costa Rica

    NASA Astrophysics Data System (ADS)

    Simila, G.; McNally, K.; Quintero, R.; Segura, J.

    2006-12-01

    The seismic strong motion array project (SSMAP) for the Nicoya Peninsula in northwestern Costa Rica is composed of 10 13 sites including Geotech A900/A800 accelerographs (three-component), Ref-Teks (three- component velocity), and Kinemetric Episensors. The main objectives of the array are to: 1) record and locate strong subduction zone mainshocks [and foreshocks, "early aftershocks", and preshocks] in Nicoya Peninsula, at the entrance of the Nicoya Gulf, and in the Papagayo Gulf regions of Costa Rica, and 2) record and locate any moderate to strong upper plate earthquakes triggered by a large subduction zone earthquake in the above regions. Our digital accelerograph array has been deployed as part of our ongoing research on large earthquakes in conjunction with the Earthquake and Volcano Observatory (OVSICORI) at the Universidad Nacional in Costa Rica. The country wide seismographic network has been operating continuously since the 1980's, with the first earthquake bulletin published more than 20 years ago, in 1984. The recording of seismicity and strong motion data for large earthquakes along the Middle America Trench (MAT) has been a major research project priority over these years, and this network spans nearly half the time of a "repeat cycle" (50 years) for large (Ms 7.5- 7.7) earthquakes beneath the Nicoya Peninsula, with the last event in 1950. Our long time co-collaborators include the seismology group OVSICORI, with coordination for this project by Dr. Ronnie Quintero and Mr. Juan Segura. Numerous international investigators are also studying this region with GPS and seismic stations (US, Japan, Germany, Switzerland, etc.). Also, there are various strong motion instruments operated by local engineers, for building purposes and mainly concentrated in the population centers of the Central Valley. The major goal of our project is to contribute unique scientific information pertaining to a large subduction zone earthquake and its related seismic activity when

  1. A frequency-domain seismic blind deconvolution based on Gini correlations

    NASA Astrophysics Data System (ADS)

    Wang, Zhiguo; Zhang, Bing; Gao, Jinghuai; Huo Liu, Qing

    2018-02-01

    In reflection seismic processing, the seismic blind deconvolution is a challenging problem, especially when the signal-to-noise ratio (SNR) of the seismic record is low and the length of the seismic record is short. As a solution to this ill-posed inverse problem, we assume that the reflectivity sequence is independent and identically distributed (i.i.d.). To infer the i.i.d. relationships from seismic data, we first introduce the Gini correlations (GCs) to construct a new criterion for the seismic blind deconvolution in the frequency-domain. Due to a unique feature, the GCs are robust in their higher tolerance of the low SNR data and less dependent on record length. Applications of the seismic blind deconvolution based on the GCs show their capacity in estimating the unknown seismic wavelet and the reflectivity sequence, whatever synthetic traces or field data, even with low SNR and short sample record.

  2. Short-Period Seismic Noise in Vorkuta (Russia)

    DOE Office of Scientific and Technical Information (OSTI.GOV)

    Kishkina, S B; Spivak, A A; Sweeney, J J

    Cultural development of new subpolar areas of Russia is associated with a need for detailed seismic research, including both mapping of regional seismicity and seismic monitoring of specific mining enterprises. Of special interest are the northern territories of European Russia, including shelves of the Kara and Barents Seas, Yamal Peninsula, and the Timan-Pechora region. Continuous seismic studies of these territories are important now because there is insufficient seismological knowledge of the area and an absence of systematic data on the seismicity of the region. Another task of current interest is the necessity to consider the seismic environment in the design,more » construction, and operation of natural gas extracting enterprises such as the construction of the North European Gas Pipeline. Issues of scientific importance for seismic studies in the region are the complex geodynamical setting, the presence of permafrost, and the complex tectonic structure. In particular, the Uralian Orogene (Fig. 1) strongly affects the propagation of seismic waves. The existing subpolar seismic stations [APA (67,57{sup o}N; 33,40{sup o}E), LVZ (67,90{sup o}N; 34,65{sup o}E), and NRIL (69,50{sup o}N; 88,40{sup o}E)] do not cover the extensive area between the Pechora and Ob Rivers (Fig. 1). Thus seismic observations in the Vorkuta area, which lies within the area of concern, represent a special interest. Continuous recording at a seismic station near the city of Vorkuta (67,50{sup o}N; 64,11{sup o}E) [1] has been conducted since 2005 for the purpose of regional seismic monitoring and, more specifically, detection of seismic signals caused by local mining enterprises. Current surveys of local seismic noise [7,8,9,11], are particularly aimed at a technical survey for the suitability of the site for installation of a small-aperture seismic array, which would include 10-12 recording instruments, with the Vorkuta seismic station as the central element. When constructed, this

  3. Wide-angle seismic recording from the 2002 Georgia Basin Geohazards Initiative, northwestern Washington and British Columbia

    USGS Publications Warehouse

    Brocher, Thomas M.; Pratt, Thomas L.; Spence, George D.; Riedel, Michael; Hyndman, Roy D.

    2003-01-01

    This report describes the acquisition and processing of shallow-crustal wide-angle seismicreflection and refraction data obtained during a collaborative study in the Georgia Strait, western Washington and southwestern British Columbia. The study, the 2002 Georgia Strait Geohazards Initiative, was conducted in May 2002 by the Pacific Geoscience Centre, the U.S. Geological Survey, and the University of Victoria. The wide-angle recordings were designed to image shallow crustal faults and Cenozoic sedimentary basins crossing the International Border in southern Georgia basin and to add to existing wide-angle recordings there made during the 1998 SHIPS experiment. We recorded, at wide-angle, 800 km of shallow penetration multichannel seismic-reflection profiles acquired by the Canadian Coast Guard Ship (CCGS) Tully using an air gun with a volume of 1.967 liters (120 cu. in.). Prior to this reflection survey, we deployed 48 Refteks onshore to record the airgun signals at wide offsets. Three components of an oriented, 4.5 Hz seismometer were digitally recorded at all stations. Nearly 160,300 individual air gun shots were recorded along 180 short seismic reflection lines. In this report, we illustrate the wide-angle profiles acquired using the CCGS Tully, describe the land recording of the air gun signals, and summarize the processing of the land recorder data into common-receiver gathers. We also describe the format and content of the archival tapes containing the SEGY-formated, common-receiver gathers for the Reftek data. Data quality is variable but the experiment provided useful data from 42 of the 48 stations deployed. Three-fourths of all stations yielded useful first-arrivals to source-receiver offsets beyond 10 km: the average maximum source-receiver offset for first arrivals was 17 km. Six stations yielded no useful data and useful firstarrivals were limited to offsets less than 10 km at five stations. We separately archived our recordings of 86 local and regional

  4. Deepwater seismic acquisition technology

    DOE Office of Scientific and Technical Information (OSTI.GOV)

    Caldwell, J.

    1996-09-01

    Although truly new technology is not required for successful acquisition of seismic data in deep Gulf of Mexico waters, it is helpful to review some basic aspects of these seismic surveys. Additionally, such surveys are likely to see early use of some emerging new technology which can improve data quality. Because such items as depth imaging, borehole seismic, 4-D and marine 3-component recording were mentioned in the May 1996 issue of World Oil, they are not discussed again here. However, these technologies will also play some role in the deepwater seismic activities. What is covered in this paper are somemore » new considerations for: (1) longer data records needed in deeper water, (2) some pros and cons of very long steamer use, and (3) two new commercial systems for quantifying data quality.« less

  5. Passive seismic imaging based on seismic interferometry: method and its application to image the structure around the 2013 Mw6.6 Lushan earthquake

    NASA Astrophysics Data System (ADS)

    Gu, N.; Zhang, H.

    2017-12-01

    Seismic imaging of fault zones generally involves seismic velocity tomography using first arrival times or full waveforms from earthquakes occurring around the fault zones. However, in most cases seismic velocity tomography only gives smooth image of the fault zone structure. To get high-resolution structure of the fault zones, seismic migration using active seismic data needs to be used. But it is generally too expensive to conduct active seismic surveys, even for 2D. Here we propose to apply the passive seismic imaging method based on seismic interferometry to image fault zone detailed structures. Seismic interferometry generally refers to the construction of new seismic records for virtual sources and receivers by cross correlating and stacking the seismic records on physical receivers from physical sources. In this study, we utilize seismic waveforms recorded on surface seismic stations for each earthquake to construct zero-offset seismic record at each earthquake location as if there was a virtual receiver at each earthquake location. We have applied this method to image the fault zone structure around the 2013 Mw6.6 Lushan earthquake. After the occurrence of the mainshock, a 29-station temporary array is installed to monitor aftershocks. In this study, we first select aftershocks along several vertical cross sections approximately normal to the fault strike. Then we create several zero-offset seismic reflection sections by seismic interferometry with seismic waveforms from aftershocks around each section. Finally we migrate these zero-offset sections to create seismic structures around the fault zones. From these migration images, we can clearly identify strong reflectors, which correspond to major reverse fault where the mainshock occurs. This application shows that it is possible to image detailed fault zone structures with passive seismic sources.

  6. Seismic and Infrasound Recordings from Kilauea Volcano: Volcanic Tremor, Lava Outbreaks, and Fissure Eruptions

    NASA Astrophysics Data System (ADS)

    Fee, D.; Garces, M.; Orr, T.

    2007-12-01

    The continuous effusion from the Pu'u 'O'o crater complex, the active vent of Kilauea Volcano, Hawaii, produced nearly continuous tremor for years. Recently this tremor was recorded by two infrasound arrays, one at 12.5 km and one at 2.5 km, as well as a broadband seismometer at the closer array. These recordings exhibit significant temporal changes. A sharp, complex spectral peak of ~0.6 Hz is present in nearly the entire dataset, and tends to bifurcate and shift frequency over time. Although the seismic wavefield at Kilauea is complex and path effects appear to play a significant role, this spectral peak is also weakly manifested in the seismic recordings. Array processing of the infrasonic data reveals an abundance of broadband signal as well. Most of the signal appears to originate from the main crater region. However, the 2.5 km array detected the presence of a skylight with growing hornitos ~400 m south of Pu'u 'O'o on the active lava tube system. On June 19th, 2007, the magmatic system at Pu'u 'O'o changed. An intrusion of magma reached the surface 6 km west of the crater complex. The timing and location of the lava outbreak were determined acoustically using array processing. Two distinct acoustic pulses were recorded from the correct azimuth, both exhibiting harmonics. The 7/21 fissure eruption also produced clear infrasound signals. The onset of the fissure eruption east of P'u' 'O'o was apparent beginning around midnight on 7/21 and was focused between ~1.5-5 Hz. Although the fissure eruption continued to produce infrasound, the character of the recorded signal changes over time. A third infrasound array was placed closer to P'u' 'O'o and the fissure to help further constrain the eruption. More detailed results on acoustic signals from the Father's Day Intrusion and Fissure eruption will be presented.

  7. Development of the Multi-Level Seismic Receiver (MLSR)

    NASA Astrophysics Data System (ADS)

    Sleefe, G. E.; Engler, B. P.; Drozda, P. M.; Franco, R. J.; Morgan, Jeff

    1995-02-01

    The Advanced Geophysical Technology Department (6114) and the Telemetry Technology Development Department (2664) have, in conjunction with the Oil Recovery Technology Partnership, developed a Multi-Level Seismic Receiver (MLSR) for use in crosswell seismic surveys. The MLSR was designed and evaluated with the significant support of many industry partners in the oil exploration industry. The unit was designed to record and process superior quality seismic data operating in severe borehole environments, including high temperature (up to 200 C) and static pressure (10,000 psi). This development has utilized state-of-the-art technology in transducers, data acquisition, and real-time data communication and data processing. The mechanical design of the receiver has been carefully modeled and evaluated to insure excellent signal coupling into the receiver.

  8. Seismic Strong Motion Array Project (SSMAP) to Record Future Large Earthquakes in the Nicoya Peninsula area, Costa Rica

    NASA Astrophysics Data System (ADS)

    Simila, G.; Lafromboise, E.; McNally, K.; Quintereo, R.; Segura, J.

    2007-12-01

    The seismic strong motion array project (SSMAP) for the Nicoya Peninsula in northwestern Costa Rica is composed of 10 - 13 sites including Geotech A900/A800 accelerographs (three-component), Ref-Teks (three- component velocity), and Kinemetric Episensors. The main objectives of the array are to: 1) record and locate strong subduction zone mainshocks [and foreshocks, "early aftershocks", and preshocks] in Nicoya Peninsula, at the entrance of the Nicoya Gulf, and in the Papagayo Gulf regions of Costa Rica, and 2) record and locate any moderate to strong upper plate earthquakes triggered by a large subduction zone earthquake in the above regions. Our digital accelerograph array has been deployed as part of our ongoing research on large earthquakes in conjunction with the Earthquake and Volcano Observatory (OVSICORI) at the Universidad Nacional in Costa Rica. The country wide seismographic network has been operating continuously since the 1980's, with the first earthquake bulletin published more than 20 years ago, in 1984. The recording of seismicity and strong motion data for large earthquakes along the Middle America Trench (MAT) has been a major research project priority over these years, and this network spans nearly half the time of a "repeat cycle" (~ 50 years) for large (Ms ~ 7.5- 7.7) earthquakes beneath the Nicoya Peninsula, with the last event in 1950. Our long time co- collaborators include the seismology group OVSICORI, with coordination for this project by Dr. Ronnie Quintero and Mr. Juan Segura. The major goal of our project is to contribute unique scientific information pertaining to a large subduction zone earthquake and its related seismic activity when the next large earthquake occurs in Nicoya. We are now collecting a database of strong motion records for moderate sized events to document this last stage prior to the next large earthquake. A recent event (08/18/06; M=4.3) located 20 km northwest of Samara was recorded by two stations (Playa Carrillo

  9. MyShake: Building a smartphone seismic network

    NASA Astrophysics Data System (ADS)

    Kong, Q.; Allen, R. M.; Schreier, L.

    2014-12-01

    We are in the process of building up a smartphone seismic network. In order to build this network, we did shake table tests to evaluate the performance of the smartphones as seismic recording instruments. We also conducted noise floor test to find the minimum earthquake signal we can record using smartphones. We added phone noises to the strong motion data from past earthquakes, and used these as an analogy dataset to test algorithms and to understand the difference of using the smartphone network and the traditional seismic network. We also built a prototype system to trigger the smartphones from our server to record signals which can be sent back to the server in near real time. The phones can also be triggered by our developed algorithm running locally on the phone, if there's an earthquake occur to trigger the phones, the signal recorded by the phones will be sent back to the server. We expect to turn the prototype system into a real smartphone seismic network to work as a supplementary network to the existing traditional seismic network.

  10. Seismic Symphonies

    NASA Astrophysics Data System (ADS)

    Strinna, Elisa; Ferrari, Graziano

    2015-04-01

    The project started in 2008 as a sound installation, a collaboration between an artist, a barrel organ builder and a seismologist. The work differs from other attempts of sound transposition of seismic records. In this case seismic frequencies are not converted automatically into the "sound of the earthquake." However, it has been studied a musical translation system that, based on the organ tonal scale, generates a totally unexpected sequence of sounds which is intended to evoke the emotions aroused by the earthquake. The symphonies proposed in the project have somewhat peculiar origins: they in fact come to life from the translation of graphic tracks into a sound track. The graphic tracks in question are made up by copies of seismograms recorded during some earthquakes that have taken place around the world. Seismograms are translated into music by a sculpture-instrument, half a seismograph and half a barrel organ. The organ plays through holes practiced on paper. Adapting the documents to the instrument score, holes have been drilled on the waves' peaks. The organ covers about three tonal scales, starting from heavy and deep sounds it reaches up to high and jarring notes. The translation of the seismic records is based on a criterion that does match the highest sounds to larger amplitudes with lower ones to minors. Translating the seismogram in the organ score, the larger the amplitude of recorded waves, the more the seismogram covers the full tonal scale played by the barrel organ and the notes arouse an intense emotional response in the listener. Elisa Strinna's Seismic Symphonies installation becomes an unprecedented tool for emotional involvement, through which can be revived the memory of the greatest disasters of over a century of seismic history of the Earth. A bridge between art and science. Seismic Symphonies is also a symbolic inversion: the instrument of the organ is most commonly used in churches, and its sounds are derived from the heavens and

  11. A Fiber-Optic Borehole Seismic Vector Sensor System for Geothermal Site Characterization and Monitoring

    DOE Office of Scientific and Technical Information (OSTI.GOV)

    Paulsson, Bjorn N.P.; Thornburg, Jon A.; He, Ruiqing

    2015-04-21

    Seismic techniques are the dominant geophysical techniques for the characterization of subsurface structures and stratigraphy. The seismic techniques also dominate the monitoring and mapping of reservoir injection and production processes. Borehole seismology, of all the seismic techniques, despite its current shortcomings, has been shown to provide the highest resolution characterization and most precise monitoring results because it generates higher signal to noise ratio and higher frequency data than surface seismic techniques. The operational environments for borehole seismic instruments are however much more demanding than for surface seismic instruments making both the instruments and the installation much more expensive. The currentmore » state-of-the-art borehole seismic instruments have not been robust enough for long term monitoring compounding the problems with expensive instruments and installations. Furthermore, they have also not been able to record the large bandwidth data available in boreholes or having the sensitivity allowing them to record small high frequency micro seismic events with high vector fidelity. To reliably achieve high resolution characterization and long term monitoring of Enhanced Geothermal Systems (EGS) sites a new generation of borehole seismic instruments must therefore be developed and deployed. To address the critical site characterization and monitoring needs for EGS programs, US Department of Energy (DOE) funded Paulsson, Inc. in 2010 to develop a fiber optic based ultra-large bandwidth clamped borehole seismic vector array capable of deploying up to one thousand 3C sensor pods suitable for deployment into ultra-high temperature and high pressure boreholes. Tests of the fiber optic seismic vector sensors developed on the DOE funding have shown that the new borehole seismic sensor technology is capable of generating outstanding high vector fidelity data with extremely large bandwidth: 0.01 – 6,000 Hz. Field tests have

  12. Seismo-volcano source localization with triaxial broad-band seismic array

    NASA Astrophysics Data System (ADS)

    Inza, L. A.; Mars, J. I.; Métaxian, J. P.; O'Brien, G. S.; Macedo, O.

    2011-10-01

    Seismo-volcano source localization is essential to improve our understanding of eruptive dynamics and of magmatic systems. The lack of clear seismic wave phases prohibits the use of classical location methods. Seismic antennas composed of one-component (1C) seismometers provide a good estimate of the backazimuth of the wavefield. The depth estimation, on the other hand, is difficult or impossible to determine. As in classical seismology, the use of three-component (3C) seismometers is now common in volcano studies. To determine the source location parameters (backazimuth and depth), we extend the 1C seismic antenna approach to 3Cs. This paper discusses a high-resolution location method using a 3C array survey (3C-MUSIC algorithm) with data from two seismic antennas installed on an andesitic volcano in Peru (Ubinas volcano). One of the main scientific questions related to the eruptive process of Ubinas volcano is the relationship between the magmatic explosions and long-period (LP) swarms. After introducing the 3C array theory, we evaluate the robustness of the location method on a full wavefield 3-D synthetic data set generated using a digital elevation model of Ubinas volcano and an homogeneous velocity model. Results show that the backazimuth determined using the 3C array has a smaller error than a 1C array. Only the 3C method allows the recovery of the source depths. Finally, we applied the 3C approach to two seismic events recorded in 2009. Crossing the estimated backazimuth and incidence angles, we find sources located 1000 ± 660 m and 3000 ± 730 m below the bottom of the active crater for the explosion and the LP event, respectively. Therefore, extending 1C arrays to 3C arrays in volcano monitoring allows a more accurate determination of the source epicentre and now an estimate for the depth.

  13. Continuous Seismic Threshold Monitoring

    DTIC Science & Technology

    1992-05-31

    Continuous threshold monitoring is a technique for using a seismic network to monitor a geographical area continuously in time. The method provides...area. Two approaches are presented. Site-specific monitoring: By focusing a seismic network on a specific target site, continuous threshold monitoring...recorded events at the site. We define the threshold trace for the network as the continuous time trace of computed upper magnitude limits of seismic

  14. A tree fell in the forest, and SPREE heard it: seismic recording of the 2011 St. Croix Valley Blowdown

    NASA Astrophysics Data System (ADS)

    Wolin, E.; van der Lee, S.

    2016-12-01

    As part of the Superior Province Rifting Earthscope Experiment (SPREE), 82 broadband seismic stations from the EarthScope Flexible Array pool were deployed by the SPREE team from April 2011 through October 2013, to explore the deep structure of the Mid-Continent Rift System (Stein et al., 2011). The deployment included two crosslines with approximate station spacing of 10 km centered near the northern Minnesota-Wisconsin border. Analysis of long-period noise reveals strong seasonal and diurnal variations (Wolin et al., 2015). On 1 July 2011, a severe thunderstorm system swept over the St. Croix Valley, passing directly over the dense SPREE array. This storm system was accompanied by a series of downbursts that generated straight-line winds in excess of 100 km/hr, resulting in extensive damage to hundreds of thousands of acres of forest. Seven SPREE stations were located in the path of the storm, with two stations in the center of areas that were heavily damaged by downbursts. The stations remained in operation throughout this extreme weather event, capturing a unique record of ground noise generated by the storm system. We compare available radar reflectivity data with seismic noise power spectra throughout the event and show that storm cells generated significant broadband seismic signals as they passed over the region. Relative to typical background seismic noise levels, power between 0.05-10 Hz increased by 5-20 dB during the storm. Seismic noise levels can be compared to available wind speed data to provide a detailed record of wind speeds during the weather event. We also explore the long-period coherence of energy across the array, which is potentially useful to help constrain near-surface velocity structure at the array sites as well as to better characterize how atmospheric processes couple into the solid earth during severe weather events.

  15. Cultural noise and the night-day asymmetry of the seismic activity recorded at the Bunker-East (BKE) Vesuvian Station

    NASA Astrophysics Data System (ADS)

    Scafetta, Nicola; Mazzarella, Adriano

    2018-01-01

    Mazzarella and Scafetta (2016) showed that the seismic activity recorded at the Bunker-East (BKE) Vesuvian station from 1999 to 2014 suggests a higher nocturnal seismic activity. However, this station is located at about 50 m from the main road to the volcano's crater and since 2009 its seismograms also record a significant diurnal cultural noise due mostly to tourist tours to Mt. Vesuvius. Herein, we investigate whether the different seismic frequency between day and night times could be an artifact of the peculiar cultural noise that affects this station mostly from 9:00 am to 5:00 pm from spring to fall. This time-distributed cultural noise should evidently reduce the possibility to detect low magnitude earthquakes during those hours but not high magnitude events. Using hourly distributions referring to different magnitude thresholds from M = 0.2 to M = 2.0, the Gutenberg-Richter magnitude-frequency diagram applied to the day and night-time sub-catalogs and Montecarlo statistical modeling, we demonstrate that the day-night asymmetry persists despite an evident disruption induced by cultural noise during day-hours. In particular, for the period 1999-2017, and for earthquakes with M ≥ 2 we found a Gutenberg-Richter exponent b = 1.66 ± 0.07 for the night-time events and b = 2.06 ± 0.07 for day-time events. Moreover, we repeat the analysis also for an older BKE catalog covering the period from 1992 to 2000 when cultural noise was not present. The analysis confirms a higher seismic nocturnal activity that is also characterized by a smaller Gutenberg-Richter exponent b for M ≥ 2 earthquakes relative to the day-time activity. Thus, the found night-day seismic asymmetric behavior is likely due to a real physical feature affecting Mt. Vesuvius.

  16. Applying the seismic interferometry method to vertical seismic profile data using tunnel excavation noise as source

    NASA Astrophysics Data System (ADS)

    Jurado, Maria Jose; Teixido, Teresa; Martin, Elena; Segarra, Miguel; Segura, Carlos

    2013-04-01

    In the frame of the research conducted to develop efficient strategies for investigation of rock properties and fluids ahead of tunnel excavations the seismic interferometry method was applied to analyze the data acquired in boreholes instrumented with geophone strings. The results obtained confirmed that seismic interferometry provided an improved resolution of petrophysical properties to identify heterogeneities and geological structures ahead of the excavation. These features are beyond the resolution of other conventional geophysical methods but can be the cause severe problems in the excavation of tunnels. Geophone strings were used to record different types of seismic noise generated at the tunnel head during excavation with a tunnelling machine and also during the placement of the rings covering the tunnel excavation. In this study we show how tunnel construction activities have been characterized as source of seismic signal and used in our research as the seismic source signal for generating a 3D reflection seismic survey. The data was recorded in vertical water filled borehole with a borehole seismic string at a distance of 60 m from the tunnel trace. A reference pilot signal was obtained from seismograms acquired close the tunnel face excavation in order to obtain best signal-to-noise ratio to be used in the interferometry processing (Poletto et al., 2010). The seismic interferometry method (Claerbout 1968) was successfully applied to image the subsurface geological structure using the seismic wave field generated by tunneling (tunnelling machine and construction activities) recorded with geophone strings. This technique was applied simulating virtual shot records related to the number of receivers in the borehole with the seismic transmitted events, and processing the data as a reflection seismic survey. The pseudo reflective wave field was obtained by cross-correlation of the transmitted wave data. We applied the relationship between the transmission

  17. Recorded seismic response of Pacific Park Plaza. II. System identification

    USGS Publications Warehouse

    Safak, F.; Celebi, M.

    1992-01-01

    This is the second of two companion papers on the recorded seismic response of the Pacific Park Plaza building, in Emeryville, Calif., during the October 17, 1989, Ms = 7.1 (surface-wave magnitude) Loma Prieta earthquake. In this second part, the recorded data are analyzed in more detail by using system-identification techniques. The three-dimensional behavior and the coupled modes of the building are determined, and the effects of soil-structure interaction are investigated. The study shows that the response of the building is nonlinear at the beginning, and becomes linear after 17 sec into the earthquake. The dominant motion of the building follows an elliptical path oriented in the southeast-northwest direction. Some of the modes are complex, with nonproportional damping, and there are phase differences among modal response components. The fundamental mode of the building is a translation in the southeast-northwest direction at 0.4 Hz, with 13% damping. The wing displacements relative to the center core are large, about 50% of the center core displacements, and indicate significant torsion in the center core. The soil-structure interaction is characterized by a vibration at 0.7 Hz. This is believed to be the fundamental frequency of the surrounding soil medium. The rocking motions of the building are negligible.

  18. Advanced Seismic While Drilling System

    DOE Office of Scientific and Technical Information (OSTI.GOV)

    Robert Radtke; John Fontenot; David Glowka

    by TII. An APS Turbine Alternator powered the SeismicPULSER{trademark} to produce two Hz frequency peak signals repeated every 20 seconds. Since the ION Geophysical, Inc. (ION) seismic survey surface recording system was designed to detect a minimum downhole signal of three Hz, successful performance was confirmed with a 5.3 Hz recording with the pumps running. The two Hz signal generated by the sparker was modulated with the 3.3 Hz signal produced by the mud pumps to create an intense 5.3 Hz peak frequency signal. The low frequency sparker source is ultimately capable of generating selectable peak frequencies of 1 to 40 Hz with high-frequency spectra content to 10 kHz. The lower frequencies and, perhaps, low-frequency sweeps, are needed to achieve sufficient range and resolution for realtime imaging in deep (15,000 ft+), high-temperature (150 C) wells for (a) geosteering, (b) accurate seismic hole depth, (c) accurate pore pressure determinations ahead of the bit, (d) near wellbore diagnostics with a downhole receiver and wired drill pipe, and (e) reservoir model verification. Furthermore, the pressure of the sparker bubble will disintegrate rock resulting in an increased overall rates of penetration. Other applications for the SeismicPULSER{trademark} technology are to deploy a low-frequency source for greater range on a wireline for Reverse Vertical Seismic Profiling (RVSP) and Cross-Well Tomography. Commercialization of the technology is being undertaken by first contacting stakeholders to define the value proposition for rig site services utilizing SeismicPULSER{trademark} technologies. Stakeholders include national oil companies, independent oil companies, independents, service companies, and commercial investors. Service companies will introduce a new Drill Bit SWD service for deep HTHP wells. Collaboration will be encouraged between stakeholders in the form of joint industry projects to develop prototype tools and initial field trials. No barriers have been

  19. Correlation of offshore seismic profiles with onshore New Jersey Miocene sediments

    USGS Publications Warehouse

    Monteverde, D.H.; Miller, K.G.; Mountain, Gregory S.

    2000-01-01

    The New Jersey passive continental margin records the interaction of sequences and sea-level, although previous studies linking seismically defined sequences, borehole control, and global ??18O records were hindered by a seismic data gap on the inner-shelf. We describe new seismic data from the innermost New Jersey shelf that tie offshore seismic stratigraphy directly to onshore boreholes. These data link the onshore boreholes to existing seismic grids across the outer margin and to boreholes on the continental slope. Surfaces defined by age; facies, and log signature in the onshore boreholes at the base of sequences Kw2b, Kw2a, Kw1c, and Kw0 are now tied to seismic sequence boundaries m5s, m5.2s, m5.4s, and m6s, respectively, defined beneath the inner shelf. Sequence boundaries recognized in onshore boreholes and inner shelf seismic profiles apparently correlate with reflections m5, m5.2, m5.4, and m6, respectively, that were dated at slope boreholes during ODP Leg 150. We now recognize an additional sequence boundary beneath the shelf that we name m5.5s and correlate to the base of the onshore sequence Kw1b. The new seismic data image prograding Oligocene clinoforms beneath the inner shelf, consistent with the results from onshore boreholes. A land-based seismic profile crossing the Island Beach borehole reveals reflector geometries that we tie to Lower Miocene litho- and bio-facies in this borehole. These land-based seismic profiles image well-defined sequence boundaries, onlap and downlap truncations that correlate to Transgressive Systems Tracts (TST) and Highstand Systems Tracts (HST) identified in boreholes. Preliminary analysis of CH0698 data continues these system tract delineations across the inner shelf The CH0698 seismic profiles tie seismically defined sequence boundaries with sequences identified by lithiologic and paleontologic criteria. Both can now be related to global ??18O increases and attendant glacioeustatic lowerings. This integration of core

  20. Seismic and Geodetic Monitoring of the Nicoya, Costa Rica, Seismic Gap

    NASA Astrophysics Data System (ADS)

    Protti, M.; Gonzalez, V.; Schwartz, S.; Dixon, T.; Kato, T.; Kaneda, Y.; Simila, G.; Sampson, D.

    2007-05-01

    The Nicoya segment of the Middle America Trench has been recognized as a mature seismic gap with potential to generate a large earthquake in the near future (it ruptured with large earthquakes in 1853, 1900 and 1950). Low level of background seismicity and fast crustal deformation of the forearc are indicatives of strong coupling along the plate interface. Given its high seismic potential, the available data and especially the fact that the Nicoya peninsula extends over large part of the rupture area, this gap was selected as one of the two sites for a MARGINS-SEIZE experiment. With the goal of documenting the evolution of loading and stress release along this seismic gap, an international effort involving several institutions from Costa Rica, the United States and Japan is being carried out for over a decade in the region. This effort involves the installation of temporary and permanent seismic and geodetic networks. The seismic network includes short period, broad band and strong motion instruments. The seismic monitoring has provided valuable information on the geometry and characteristics of the plate interface. The geodetic network includes temporary and permanent GPS stations as well as surface and borehole tiltmeters. The geodetic networks have helped quantify the extend and degree of coupling. A continuously recording, three- station GPS network on the Nicoya Peninsula, Costa Rica, recorded what we believe is the first slow slip event observed along the plate interface of the Costa Rica subduction zone. We will present results from these monitoring networks. Collaborative international efforts are focused on expanding these seismic and geodetic networks to provide improved resolution of future creep events, to enhanced understanding of the mechanical behavior of the Nicoya subduction segment of the Middle American Trench and possibly capture the next large earthquake and its potential precursor deformation.

  1. Applications of seismic spatial wavefield gradient and rotation data in exploration seismology

    NASA Astrophysics Data System (ADS)

    Schmelzbach, C.; Van Renterghem, C.; Sollberger, D.; Häusler, M.; Robertsson, J. O. A.

    2017-12-01

    Seismic spatial wavefield gradient and rotation data have the potential to open up new ways to address long-standing problems in land-seismic exploration such as identifying and separating P-, S-, and surface waves. Gradient-based acquisition and processing techniques could enable replacing large arrays of densely spaced receivers by sparse spatially-compact receiver layouts or even one single multicomponent station with dedicated instruments (e.g., rotational seismometers). Such approaches to maximize the information content of single-station recordings are also of significant interest for seismic measurements at sites with limited access such as boreholes, the sea bottom, and extraterrestrial seismology. Arrays of conventional three-component (3C) geophones enable measuring not only the particle velocity in three dimensions but also estimating their spatial gradients. Because the free-surface condition allows to express vertical derivatives in terms of horizontal derivatives, the full gradient tensor and, hence, curl and divergence of the wavefield can be computed. In total, three particle velocity components, three rotational components, and divergence, result seven-component (7C) seismic data. Combined particle velocity and gradient data can be used to isolate the incident P- or S-waves at the land surface or the sea bottom using filtering techniques based on the elastodynamic representation theorem. Alternatively, as only S-waves exhibit rotational motion, rotational measurements can directly be used to identify S-waves. We discuss the derivations of the gradient-based filters as well as their application to synthetic and field data, demonstrating that rotational data can be of particular interest to S-wave reflection and P-to-S-wave conversion imaging. The concept of array-derived gradient estimation can be extended to source arrays as well. Therefore, source arrays allow us to emulate rotational (curl) and dilatational (divergence) sources. Combined with 7C

  2. Composition and variation of noise recorded at the Yellowknife Seismic Array, 1991-2007

    USGS Publications Warehouse

    Koper, K.D.; De Foy, B.; Benz, H.

    2009-01-01

    We analyze seismic noise recorded on the 18 short-period, vertical component seismometers of the Yellowknife Seismic Array (YKA). YKA has an aperture of 23 km and is sited on cratonic lithosphere in an area with low cultural noise. These properties make it ideal for studying natural seismic noise at periods of 1-3 s. We calculated frequency-wave number spectra in this band for over 6,000 time windows that were extracted once per day for 17 years (1991-2007). Slowness analysis reveals a rich variety of seismic phases originating from distinct source regions: Rg waves from the Great Slave Lake; Lg waves from the Atlantic, Pacific, and Arctic Oceans; and teleseismic P waves from the north Pacific and equatorial mid-Atlantic regions. The surface wave energy is generated along coastlines, while the body wave energy is generated at least in part in deep-water, pelagic regions. Surface waves tend to dominate at the longer periods and, just as in earthquake seismograms, Lg is the most prominent arrival. Although the periods we study are slightly shorter than the classic double-frequency microseismic band of 4-10 s, the noise at YKA has clear seasonal behavior that is consistent with the ocean wave climate in the Northern Hemisphere. The temporal variation of most of the noise sources can be well fit using just two Fourier components: yearly and biyearly terms that combine to give a fast rise in microseismic power from mid-June through mid-October, followed by a gradual decline. The exception is the Rg energy from the Great Slave Lake, which shows a sharp drop in noise power over a 2-week period in November as the lake freezes. The L g noise from the east has a small but statistically significant positive slope, perhaps implying increased ocean wave activity in the North Atlantic over the last 17 years. Copyright 2009 by the American Geophysical Union.

  3. Improvement of real-time seismic magnitude estimation by combining seismic and geodetic instrumentation

    NASA Astrophysics Data System (ADS)

    Goldberg, D.; Bock, Y.; Melgar, D.

    2017-12-01

    Rapid seismic magnitude assessment is a top priority for earthquake and tsunami early warning systems. For the largest earthquakes, seismic instrumentation tends to underestimate the magnitude, leading to an insufficient early warning, particularly in the case of tsunami evacuation orders. GPS instrumentation provides more accurate magnitude estimations using near-field stations, but isn't sensitive enough to detect the first seismic wave arrivals, thereby limiting solution speed. By optimally combining collocated seismic and GPS instruments, we demonstrate improved solution speed of earthquake magnitude for the largest seismic events. We present a real-time implementation of magnitude-scaling relations that adapts to consider the length of the recording, reflecting the observed evolution of ground motion with time.

  4. Tree-ring 14C links seismic swarm to CO2 spike at Yellowstone, USA

    USGS Publications Warehouse

    Evans, William C.; Bergfeld, D.; McGeehin, J.P.; King, J.C.; Heasler, H.

    2010-01-01

    Mechanisms to explain swarms of shallow seismicity and inflation-deflation cycles at Yellowstone caldera (western United States) commonly invoke episodic escape of magma-derived brines or gases from the ductile zone, but no correlative changes in the surface efflux of magmatic constituents have ever been documented. Our analysis of individual growth rings in a tree core from the Mud Volcano thermal area within the caldera links a sharp ~25% drop in 14C to a local seismic swarm in 1978. The implied fivefold increase in CO2 emissions clearly associates swarm seismicity with upflow of magma-derived fluid and shows that pulses of magmatic CO2 can rapidly traverse the 5-kmthick brittle zone, even through Yellowstone's enormous hydrothermal reservoir. The 1978 event predates annual deformation surveys, but recognized connections between subsequent seismic swarms and changes in deformation suggest that CO2 might drive both processes. ?? 2010 Geological Society of America.

  5. Non Linear Analyses for the Evaluation of Seismic Behavior of Mixed R.C.-Masonry Structures

    DOE Office of Scientific and Technical Information (OSTI.GOV)

    Liberatore, Laura; Tocci, Cesare; Masiani, Renato

    2008-07-08

    In this work the seismic behavior of masonry buildings with mixed structural system, consisting of perimeter masonry walls and internal r.c. frames, is studied by means of non linear static (pushover) analyses. Several aspects, like the distribution of seismic action between masonry and r.c. elements, the local and global behavior of the structure, the crisis of the connections and the attainment of the ultimate strength of the whole structure are examined. The influence of some parameters, such as the masonry compressive and tensile strength, on the structural behavior is investigated. The numerical analyses are also repeated on a building inmore » which the r.c. internal frames are replaced with masonry walls.« less

  6. On the variations of O III forbidden line intensities in the spectrum of the planetary nebula IC 4997

    NASA Astrophysics Data System (ADS)

    Egikyan, A. G.

    1997-10-01

    The causes of asynchronous variations in the intensities of forbidden O III lines in the spectrum of the planetary nebula IC 4997 are considered. It is shown that the strengthening of the 4363-A line with a simultaneous weakening of the N1 and N2 lines can be explained by a severalfold increase of the mass-loss rate from the nucleus, up to 1-2 x 10 exp -7 solar mass/yr, over several years. The ionization model of the nebula under the combined effect of nucleus emission and the emission from a variable hot stellar wind with electron temperature of 500,000 K is used to calculate the theoretical line intensities. The calculations included 12 levels of O III. In the region of O III line formation, the electron density of 10 exp 6/cu cm and Te, which varies from 12,000 to 15,000 K, yield theoretical line intensities that are in best agreement with observations. The X-ray luminosity of the stellar wind from the nucleus at energies not less than 0.2 keV is on the order of 10 exp 35 erg/s, but the interstellar extinction rules out the possibility of observing this object.

  7. DigiSeis—A software component for digitizing seismic signals using the PC sound card

    NASA Astrophysics Data System (ADS)

    Amin Khan, Khalid; Akhter, Gulraiz; Ahmad, Zulfiqar

    2012-06-01

    An innovative software-based approach to develop an inexpensive experimental seismic recorder is presented. This approach requires no hardware as the built-in PC sound card is used for digitization of seismic signals. DigiSeis, an ActiveX component is developed to capture the digitized seismic signals from the sound card and deliver them to applications for processing and display. A seismic recorder application software SeisWave is developed over this component, which provides real-time monitoring and display of seismic events picked by a pair of external geophones. This recorder can be used as an educational aid for conducting seismic experiments. It can also be connected with suitable seismic sensors to record earthquakes. The software application and the ActiveX component are available for download. This component can be used to develop seismic recording applications according to user specific requirements.

  8. The performance of the stations of the Romanian seismic network in monitoring the local seismic activity

    NASA Astrophysics Data System (ADS)

    Ardeleanu, Luminita Angela; Neagoe, Cristian

    2014-05-01

    The seismic survey of the territory of Romania is mainly performed by the national seismic network operated by the National Institute for Earth Physics of Bucharest. After successive developments and upgrades, the network consists at present of 123 permanent stations equipped with high quality digital instruments (Kinemetrics K2, Quantera Q330, Quantera Q330HR, PS6-24 and Basalt digitizers) - 102 real time and 20 off-line stations - which cover the whole territory of the country. All permanent stations are supplied with 3 component accelerometers (episenzor type), while the real time stations are in addition provided with broadband (CMG3ESP, CMG40T, KS2000, KS54000, KS2000, CMG3T, STS2) or short period (SH-1, S13, Mark l4c, Ranger, GS21, L22_VEL) velocity sensors. Several communication systems are currently used for the real time data transmission: an analog line in UHF band, a line through GPRS (General Packet Radio Service), a dedicated line through satellite, and a dedicated line provided by the Romanian Special Telecommunication Service. During the period January 1, 2006 - June 30, 2013, 5936 shallow depth seismic events - earthquakes and quarry blasts - with local magnitude ML ≥ 1.2 were localized on the Romanian territory, or in its immediate vicinity, using the records of the national seismic network; 1467 subcrustal earthquakes (depth ≥ 60 km) with magnitude ML ≥ 1.9 were also localized in the Vrancea region, at the bend of the Eastern Carpathians. The goal of the present study is to evaluate the individual contribution of the real time seismic stations to the monitoring of the local seismicity. The performance of each station is estimated by taking into consideration the fraction of events that are localised using the station records, compared to the total number of events of the catalogue, occurred during the time of station operation. Taking into account the nonuniform space distribution of earthquakes, the location of the site and the recovery

  9. Ship Noise in the SW Indian Ocean Recorded by Ocean Bottom Seismic and Hydroacoustic Sensors

    NASA Astrophysics Data System (ADS)

    Barruol, G.; Dreo, R.; Fontaine, F. R.; Scholz, J. R.; Sigloch, K.

    2016-12-01

    In the frame of the RHUM-RUM project (Réunion Hotspot and Upper Mantle - Réunions Unterer Mantel, www.rhum-rum.net), a network of 57 ocean-bottom seismometers (OBS) has been installed on the ocean floor around La Réunion Island, but also on the neighbouring Southwest and Central Indian Ridges. The OBS were equipped by wide- and broad-band three-components seismic and hydroacoustic sensors. They were deployed in Nov. 2012, and depending on the configuration, they recorded for 8 to 13 months. Interestingly, part of the network was located beneath a NE-SW trending lane of very dense ship traffic connecting SE-Asia and the South-Atlantic region. By combining the vessel position - provided by AIS GPS data - and our geophysical data recorded on the ocean floor, we analyze the seismic and hydroacoustic ship signatures. From spectral analyzes, we show clear signals over the whole high-frequency range available from our instruments (between 1 and 50 Hz). The RHUM-RUM network covering latitude between 17 and 34° South, this allows to detect numerous vessels and to compare the noise characteristics (frequency content, polarization) of each vessel. We also investigate the possibility of using the polarization of the noise emitted by ships passing above an ocean-bottom seismometer, to help retrieving the orientation of the OBS horizontal components on the ocean floor in the geographic reference frame.

  10. Classifying elephant behaviour through seismic vibrations.

    PubMed

    Mortimer, Beth; Rees, William Lake; Koelemeijer, Paula; Nissen-Meyer, Tarje

    2018-05-07

    Seismic waves - vibrations within and along the Earth's surface - are ubiquitous sources of information. During propagation, physical factors can obscure information transfer via vibrations and influence propagation range [1]. Here, we explore how terrain type and background seismic noise influence the propagation of seismic vibrations generated by African elephants. In Kenya, we recorded the ground-based vibrations of different wild elephant behaviours, such as locomotion and infrasonic vocalisations [2], as well as natural and anthropogenic seismic noise. We employed techniques from seismology to transform the geophone recordings into source functions - the time-varying seismic signature generated at the source. We used computer modelling to constrain the propagation ranges of elephant seismic vibrations for different terrains and noise levels. Behaviours that generate a high force on a sandy terrain with low noise propagate the furthest, over the kilometre scale. Our modelling also predicts that specific elephant behaviours can be distinguished and monitored over a range of propagation distances and noise levels. We conclude that seismic cues have considerable potential for both behavioural classification and remote monitoring of wildlife. In particular, classifying the seismic signatures of specific behaviours of large mammals remotely in real time, such as elephant running, could inform on poaching threats. Copyright © 2018 The Authors. Published by Elsevier Ltd.. All rights reserved.

  11. Using strain rates to forecast seismic hazards

    USGS Publications Warehouse

    Evans, Eileen

    2017-01-01

    One essential component in forecasting seismic hazards is observing the gradual accumulation of tectonic strain accumulation along faults before this strain is suddenly released as earthquakes. Typically, seismic hazard models are based on geologic estimates of slip rates along faults and historical records of seismic activity, neither of which records actively accumulating strain. But this strain can be estimated by geodesy: the precise measurement of tiny position changes of Earth’s surface, obtained from GPS, interferometric synthetic aperture radar (InSAR), or a variety of other instruments.

  12. Writing user selectable data on the extended header of seismic recordings made on the Texas Instruments DFS-V

    USGS Publications Warehouse

    Robinson, W.C.

    1996-01-01

    A circuit has been developed to allow the writing of up to 192 digits of user-selectable data on a portion of tape called extended header, which is always available for use before each DFS-V seismic record is written. Such data could include navigation information, air gun and streamer depth and shot times.

  13. Building a Smartphone Seismic Network

    NASA Astrophysics Data System (ADS)

    Kong, Q.; Allen, R. M.

    2013-12-01

    We are exploring to build a new type of seismic network by using the smartphones. The accelerometers in smartphones can be used to record earthquakes, the GPS unit can give an accurate location, and the built-in communication unit makes the communication easier for this network. In the future, these smartphones may work as a supplement network to the current traditional network for scientific research and real-time applications. In order to build this network, we developed an application for android phones and server to record the acceleration in real time. These records can be sent back to a server in real time, and analyzed at the server. We evaluated the performance of the smartphone as a seismic recording instrument by comparing them with high quality accelerometer while located on controlled shake tables for a variety of tests, and also the noise floor test. Based on the daily human activity data recorded by the volunteers and the shake table tests data, we also developed algorithm for the smartphones to detect earthquakes from daily human activities. These all form the basis of setting up a new prototype smartphone seismic network in the near future.

  14. Submarine seismic monitoring of El Hierro volcanic eruption with a 3C-geophone string: applying new acquisition and data processing techniques to volcano monitoring

    NASA Astrophysics Data System (ADS)

    Jurado, Maria Jose; Ripepe, Maurizio; Lopez, Carmen; Blanco, Maria Jose; Crespo, Jose

    2015-04-01

    A submarine volcanic eruption took place near the southernmost emerged land of the El Hierro Island (Canary Islands, Spain), from October 2011 to February 2012. The Instituto Geografico Nacional (IGN) seismic stations network evidenced seismic unrest since July 2011 and was a reference also to follow the evolution of the seismic activity associated with the volcanic eruption. Right after the eruption onset, in October 2011 a geophone string was deployed by the CSIC-IGN to monitor seismic activity. Monitoring with the seismic array continued till May 2012. The array was installed less than 2 km away from the new vol¬cano, next to La Restinga village shore in the harbor from 6 to 12m deep into the water. Our purpose was to record seismic activity related to the volcanic activity, continuously and with special interest on high frequency events. The seismic array was endowed with 8, high frequency, 3 component, 250 Hz, geophone cable string with a separation of 6 m between them. Each geophone consists on a 3-component module based on 3 orthogonal independent sensors that measures ground velocity. Some of the geophones were placed directly on the seabed, some were buried. Due to different factors, as the irregular characteristics of the seafloor. The data was recorded on the surface with a seismometer and stored on a laptop computer. We show how acoustic data collected underwater show a great correlation with the seismic data recorded on land. Finally we compare our data analysis results with the observed sea surface activity (ash and lava emission and degassing). This evidence is disclosing new and innovative tecniques on monitoring submarine volcanic activity. Reference Instituto Geográfico Nacional (IGN), "Serie El Hierro." Internet: http://www.ign.es/ign/resources /volcanologia/HIERRO.html [May, 17. 2013

  15. Seismic and acoustic recordings of an unusually large rockfall at Mount St. Helens, Washington

    USGS Publications Warehouse

    Moran, Seth C.; Matoza, R.S.; Garces, M.A.; Hedlin, M.A.H.; Bowers, D.; Scott, William E.; Sherrod, David R.; Vallance, James W.

    2008-01-01

    On 29 May 2006 a large rockfall off the Mount St. Helens lava dome produced an atmospheric plume that was reported by airplane pilots to have risen to 6,000 m above sea level and interpreted to be a result of an explosive event. However, subsequent field reconnaissance found no evidence of a ballistic field, indicating that there was no explosive component. The rockfall produced complex seismic and infrasonic signals, with the latter recorded at sites 0.6 and 13.4 km from the source. An unusual, very long-period (50 s) infrasonic signal was recorded, a signal we model as the result of air displacement. Two high-frequency infrasonic signals are inferred to result from the initial contact of a rock slab with the ground and from interaction of displaced air with a depression at the base of the active lava dome.

  16. Exploring methods of cGPS transient detections for the Chilean cGPS network in conjunction with displacement predictions from seismic catalogues: To what extent can we detect seismic and aseismic motion in the cGPS network?

    NASA Astrophysics Data System (ADS)

    Bedford, J. R.; Moreno, M.; Oncken, O.; Li, S.; Schurr, B.; Metzger, S.; Baez, J. C.; Deng, Z.; Melnick, D.

    2016-12-01

    Various algorithms for the detection of transient deformation in cGPS networks are under currently being developed to relieve us of by-eye detection, which is an error prone and time-expensive activity. Such algorithms aim to separate the time series into secular, seasonal, and transient components. Additional white and coloured noise, as well as common-mode (network correlated) noise, may remain in the separated transient component of the signal, depending on the processing flow before the separation step. The a-priori knowledge of regional seismicity can assist in the recognition of steps in the data, which are generally corrected for if they are above the noise-floor. Sometimes, the cumulative displacement caused by small earthquakes can create a seemingly continuous transient signal in the cGPS leading to confusion as to whether to attribute this transient motion as seismic or aseismic. Here we demonstrate the efficacy of various transient detection algorithms for subsets of the Chilean cGPS network and present the optimal processing flow for teasing out the transients. We present a step-detection and removal algorithm and estimate the seismic efficiency of any detected transient signals by forward modelling the surface displacements of the earthquakes and comparing to the recovered transient signals. A major challenge in separating signals in the Chilean cGPS network is the overlapping of postseismic effects at adjacent segments: For example, a Mw 9 earthquake will produce a postseismic viscoelastic relaxation that is sustained over decades and several hundreds of kilometres. Additionally, it has been observed in Chile and Japan that following moderately large earthquakes (e.g. Mw > 8) the secular velocities of adjacent segments in the subduction margin suddenly change and remain changed: this effect may be related to a change in speed of slab subduction rather than viscoelastic relaxation, and therefore the signal separation algorithms that assume a time

  17. Multifractal investigation of continuous seismic signal recorded at El Hierro volcano (Canary Islands) during the 2011-2012 pre- and eruptive phases

    NASA Astrophysics Data System (ADS)

    Telesca, Luciano; Lovallo, Michele; Martì Molist, Joan; López Moreno, Carmen; Abella Meléndez, Rafael

    2015-02-01

    The Multifractal Detrended Fluctuation Analysis (MF-DFA) is an effective method that allows detecting multifractality in non-stationary signals. We applied the MF-DFA to the continuous seismic signal recorded at El Hierro volcano (Canary Islands), which was affected by a submarine monogenetic eruption in October 2011. We investigated the multifractal properties of the continuous seismic signal before the onset of the eruption and after. We analysed three frames of the signal, one measured before the onset of eruption that occurred on October 10, 2011; and two after, but corresponding to two distinct eruptive episodes, the second one started on November 22, 2011 and lasting until late February 2012. The results obtained show a striking difference in the width of the multifractal spectrum, which is generally used to quantify the multifractal degree of a signal: the multifractal spectra of the signal frames recorded during the eruptive episodes are almost identical and much narrower than that of the signal frame measured before the onset of the eruption. Such difference indicates that the seismic signal recorded during the unrest reflects mostly the fracturing of the host rock under the overpressure exerted by the intruding magma, while that corresponding to the eruptive phases was mostly influenced by the flow of magma through the plumbing system, even some fracturing remains, not being possible to distinguish among the two eruptive episodes in terms of rock fracture mechanics.

  18. The planning of a passive seismic experiment: the Ketzin case

    NASA Astrophysics Data System (ADS)

    Rossi, G.; Petronio, L.

    2009-04-01

    In the last years, it has been recognized the importance of using microseismic activity data to gain information on the state and dynamics of a reservoir, notwithstanding the difficulties of recording, localizing the events, interpret them correctly, in terms of developing fractures, or thermal effects. The increasing number of CO2 storage experiments, with the necessity of providing efficient, economic, and long-term monitoring methods, both in the injection and post-injection phases, further encourage the development and improvement of recording and processing techniques. Microseismic signals are typically recorded with downhole sensors. Monitoring with surface sensors is problematic due to increased noise levels and signal attenuation particularly in the near surface. The actual detection distance depends on background noise conditions, seismic attenuation and the microseismic source strength. In the frame of the European project Co2ReMoVe and of the European Network of Excellence Co2GeoNet, a passive seismic experiment was planned in the Ketzin site for geological storage of CO2, a former gas store near Potsdam, object of the CO2SINK European project and inserted also in the European project Co2ReMoVe. Aim of the survey is to complement the CO2-SINK active seismic downhole experiments, adding precious information on the microseismicity induced by stress field changes at the reservoir level and in the overburden, due to the CO2 injection. The baseline survey was done in May 2008 by the Istituto Nazionale di Oceanografia e di Geofisica Sperimentale-OGS (Italy), with the support of the Deutsches GeoForschungsZentrum-GFZ (Germany) and the collaboration of the Institut für Geowissenschaftliche Gemeinschaftsaufgaben-GGA (Germany), shortly before the starting of the CO2 injection (June 30th 2008). A continuous monitoring (about 5 days) was performed by 2 downhole 3C geophones, and 3 surface 3C geophones located around the wells. This paper, based on the analysis of

  19. Dynamics of the Wulong landslide revealed by broadband seismic records

    NASA Astrophysics Data System (ADS)

    Li, Zhengyuan; Huang, Xinghui; Xu, Qiang; Yu, Dan; Fan, Junyi; Qiao, Xuejun

    2017-02-01

    The catastrophic Wulong landslide occurred at 14:51 (Beijing time, UTC+8) on 5 June 2009, in Wulong Prefecture, Southwest China. This rockslide occurred in a complex topographic environment. Seismic signals generated by this event were recorded by the seismic network deployed in the surrounding area, and long-period signals were extracted from 8 broadband seismic stations within 250 km to obtain source time functions by inversion. The location of this event was simultaneously acquired using a stepwise refined grid search approach, with an error of 2.2 km. The estimated source time functions reveal that, according to the movement parameters, this landslide could be divided into three stages with different movement directions, velocities, and increasing inertial forces. The sliding mass moved northward, northeastward and northward in the three stages, with average velocities of 6.5, 20.3, and 13.8 m/s, respectively. The maximum movement velocity of the mass reached 35 m/s before the end of the second stage. The basal friction coefficients were relatively small in the first stage and gradually increasing; large in the second stage, accompanied by the largest variability; and oscillating and gradually decreasing to a stable value, in the third stage. Analysis shows that the movement characteristics of these three stages are consistent with the topography of the sliding zone, corresponding to the northward initiation, eastward sliding after being stopped by the west wall, and northward debris flowing after collision with the east slope of the Tiejianggou valley. The maximum movement velocity of the sliding mass results from the largest height difference of the west slope of the Tiejianggou valley. The basal friction coefficients of the three stages represent the thin weak layer in the source zone, the dramatically varying topography of the west slope of the Tiejianggou valley, and characteristics of the debris flow along the Tiejianggou valley. Based on the above

  20. A permanent seismic station beneath the Ocean Bottom

    NASA Astrophysics Data System (ADS)

    Harris, David; Cessaro, Robert K.; Duennebier, Fred K.; Byrne, David A.

    1987-03-01

    The Hawaii Institute of Geophysics began development of the Ocean Subbottom Seisometer (OSS) system in 1978, and OSS systems were installed in four locations between 1979 and 1982. The OSS system is a permanent, deep ocean borehole seismic recording system composed of a borehole sensor package (tool), an electromechanical cable, recorder package, and recovery system. Installed near the bottom of a borehole (drilled by the D/V Glomar Challenger), the tool contains three orthogonal, 4.5-Hz geophones, two orthogonal tilt meters; and a temperature sensor. Signals from these sensors are multiplexed, digitized (with a floating point technique), and telemetered through approximately 10 km of electromechanical cable to a recorder package located near the ocean bottom. Electrical power for the tool is supplied from the recorder package. The digital seismic signals are demultiplexed, converted back to analog form, processed through an automatic gain control (AGC) circuit, and recorded along with a time code on magnetic tape cassettes in the recorder package. Data may be recorded continuously for up to two months in the self-contained recorder package. Data may also be recorded in real time (digital formal) during the installation and subsequent recorder package servicing. The recorder package is connected to a submerged recovery buoy by a length of bouyant polypropylene rope. The anchor on the recovery buoy is released by activating either of the acoustical command releases. The polypropylene rope may also be seized with a grappling hook to effect recovery. The recorder package may be repeatedly serviced as long as the tool remains functional A wide range of data has been recovered from the OSS system. Recovered analog records include signals from natural seismic sources such as earthquakes (teleseismic and local), man-made seismic sources such as refraction seismic shooting (explosives and air cannons), and nuclear tests. Lengthy continuous recording has permitted analysis

  1. Reevaluation of the Seismicity and seismic hazards of Northeastern Libya

    NASA Astrophysics Data System (ADS)

    Ben Suleman, abdunnur; Aousetta, Fawzi

    2014-05-01

    Libya, located at the northern margin of the African continent, underwent many episodes of orogenic activities. These episodes of orogenic activities affected and shaped the geological setting of the country. This study represents a detailed investigation that aims to focus on the seismicity and its implications on earthquake hazards of Northeastern Libya. At the end of year 2005 the Libyan National Seismological Network starts functioning with 15 stations. The Seismicity of the area under investigation was reevaluated using data recorded by the recently established network. The Al-Maraj earthquake occurred in May 22nd 2005was analyzed. This earthquake was located in a known seismically active area. This area was the sight of the well known 1963 earthquake that kills over 200 people. Earthquakes were plotted and resulting maps were interpreted and discussed. The level of seismic activity is higher in some areas, such as the city of Al-Maraj. The offshore areas north of Al-Maraj seem to have higher seismic activity. It is highly recommended that the recent earthquake activity is considered in the seismic hazard assessments for the northeastern part of Libya.

  2. Tools for educational access to seismic data

    NASA Astrophysics Data System (ADS)

    Taber, J. J.; Welti, R.; Bravo, T. K.; Hubenthal, M.; Frechette, K.

    2017-12-01

    Student engagement can be increased both by providing easy access to real data, and by addressing newsworthy events such as recent large earthquakes. IRIS EPO has a suite of access and visualization tools that can be used for such engagement, including a set of three tools that allow students to explore global seismicity, use seismic data to determine Earth structure, and view and analyze near-real-time ground motion data in the classroom. These tools are linked to online lessons that are designed for use in middle school through introductory undergraduate classes. The IRIS Earthquake Browser allows discovery of key aspects of plate tectonics, earthquake locations (in pseudo 3D) and seismicity rates and patterns. IEB quickly displays up to 20,000 seismic events over up to 30 years, making it one of the most responsive, practical ways to visualize historical seismicity in a browser. Maps are bookmarkable and preserve state, meaning IEB map links can be shared or worked into a lesson plan. The Global Seismogram Plotter automatically creates visually clear seismic record sections from selected large earthquakes that are tablet-friendly and can also to be printed for use in a classroom without computers. The plots are designed to be appropriate for use with no parameters to set, but users can also modify the plots, such as including a recording station near a chosen location. A guided exercise is provided where students use the record section to discover the diameter of Earth's outer core. Students can pick and compare phase arrival times onscreen which is key to performing the exercise. A companion station map shows station locations and further information and is linked to the record section. jAmaSeis displays seismic data in real-time from either a local instrument and/or from remote seismic stations that stream data using standard seismic data protocols, and can be used in the classroom or as a public display. Users can filter data, fit a seismogram to travel time

  3. Bed load transport and boundary roughness changes as competing causes of hysteresis in the relationship between river discharge and seismic amplitude recorded near a steep mountain stream

    NASA Astrophysics Data System (ADS)

    Roth, Danica L.; Finnegan, Noah J.; Brodsky, Emily E.; Rickenmann, Dieter; Turowski, Jens M.; Badoux, Alexandre; Gimbert, Florent

    2017-05-01

    Hysteresis in the relationship between bed load transport and river stage is a well-documented phenomenon with multiple known causes. Consequently, numerous studies have interpreted hysteresis in the relationship between seismic ground motion near rivers and some measure of flow strength (i.e., discharge or stage) as the signature of bed load transport. Here we test this hypothesis in the Erlenbach stream (Swiss Prealps) using a metric to quantitatively compare hysteresis in seismic data with hysteresis recorded by geophones attached beneath steel plates within the streambed, a well-calibrated proxy for direct sediment transport measurements. We find that while both the geophones and seismometers demonstrate hysteresis, the magnitude and direction of hysteresis are not significantly correlated between these data, indicating that the seismic signal at this site is primarily reflecting hysteresis in processes other than sediment transport. Seismic hysteresis also does not correlate significantly with the magnitude of sediment transport recorded by the geophones, contrary to previous studies' assumptions. We suggest that hydrologic sources and changes in water turbulence, for instance due to evolving boundary conditions at the bed, rather than changes in sediment transport rates, may sometimes contribute to or even dominate the hysteresis observed in seismic amplitudes near steep mountain rivers.Plain Language SummaryAn increasing number of studies have recently observed changes in the amount of <span class="hlt">seismic</span> shaking (hysteresis) <span class="hlt">recorded</span> near a river at a given discharge during floods. Most studies have assumed that this hysteresis was caused by changes in the amount of sediment being transported in the river and have therefore used the hysteresis to assess sediment transport rates and patterns. We examine concurrent <span class="hlt">seismic</span> and sediment transport data from a steep mountain stream in the Swiss Prealps and find that changes in</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70017326','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70017326"><span><span class="hlt">Seismic</span> excitation by space shuttles</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Kanamori, H.; Mori, J.; Sturtevant, B.; Anderson, D.L.; Heaton, T.</p> <p>1992-01-01</p> <p>Shock waves generated by the space shuttles Columbia (August 13, 1989), Atlantis (April 11, 1991) and Discovery (September 18, 1991) on their return to Edwards Air Force Base, California, were <span class="hlt">recorded</span> by TERRAscope (Caltech's broadband <span class="hlt">seismic</span> network), the Caltech-U.S.G.S Southern California <span class="hlt">Seismic</span> Network (SCSN), and the University of Southern California (USC) Los Angeles Basin <span class="hlt">Seismic</span> Network. The spatial pattern of the arrival times exhibits hyperbolic shock fronts from which the path, velocity and altitude of the space shuttle could be determined. The shock wave was acoustically coupled to the ground, converted to a <span class="hlt">seismic</span> wave, and <span class="hlt">recorded</span> clearly at the broadband TERRAscope stations. The acoustic coupling occurred very differently depending on the conditions of the Earth's surface surrounding the station. For a <span class="hlt">seismic</span> station located on hard bedrock, the shock wave (N wave) was clearly <span class="hlt">recorded</span> with little distortion. Aside from the N wave, very little acoustic coupling of the shock wave energy to the ground occurred at these sites. The observed N wave <span class="hlt">record</span> was used to estimate the overpressure of the shock wave accurately; a pressure change of 0.5 to 2.2 mbars was obtained. For a <span class="hlt">seismic</span> station located close to the ocean or soft sedimentary basins, a significant amount of shock wave energy was transferred to the ground through acoustic coupling of the shock wave and the oceanic Rayleigh wave. A distinct topography such as a mountain range was found effective to couple the shock wave energy to the ground. Shock wave energy was also coupled to the ground very effectively through large man made structures such as high rise buildings and offshore oil drilling platforms. For the space shuttle Columbia, in particular, a distinct pulse having a period of about 2 to 3 seconds was observed, 12.5 s before the shock wave, with a broadband seismograph in Pasadena. This pulse was probably excited by the high rise buildings in downtown Los Angeles which were</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFM.S31A4371T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFM.S31A4371T"><span>Induced <span class="hlt">Seismicity</span> Monitoring System</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Taylor, S. R.; Jarpe, S.; Harben, P.</p> <p>2014-12-01</p> <p>There are many seismological aspects associated with monitoring of permanent storage of carbon dioxide (CO2) in geologic formations. Many of these include monitoring underground gas migration through detailed tomographic studies of rock properties, integrity of the cap rock and micro <span class="hlt">seismicity</span> with time. These types of studies require expensive deployments of surface and borehole sensors in the vicinity of the CO2 injection wells. Another problem that may exist in CO2 sequestration fields is the potential for damaging induced <span class="hlt">seismicity</span> associated with fluid injection into the geologic reservoir. <span class="hlt">Seismic</span> hazard monitoring in CO2 sequestration fields requires a <span class="hlt">seismic</span> network over a spatially larger region possibly having stations in remote settings. Expensive observatory-grade <span class="hlt">seismic</span> systems are not necessary for <span class="hlt">seismic</span> hazard deployments or small-scale tomographic studies. Hazard monitoring requires accurate location of induced <span class="hlt">seismicity</span> to magnitude levels only slightly less than that which can be felt at the surface (e.g. magnitude 1), and the frequencies of interest for tomographic analysis are ~1 Hz and greater. We have developed a seismo/acoustic smart sensor system that can achieve the goals necessary for induced <span class="hlt">seismicity</span> monitoring in CO2 sequestration fields. The unit is inexpensive, lightweight, easy to deploy, can operate remotely under harsh conditions and features 9 channels of <span class="hlt">recording</span> (currently 3<span class="hlt">C</span> 4.5 Hz geophone, MEMS accelerometer and microphone). An on-board processor allows for satellite transmission of parameter data to a processing center. Continuous or event-detected data is kept on two removable flash SD cards of up to 64+ Gbytes each. If available, data can be transmitted via cell phone modem or picked up via site visits. Low-power consumption allows for autonomous operation using only a 10 watt solar panel and a gel-cell battery. The system has been successfully tested for long-term (> 6 months) remote operations over a wide range</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..19.8678C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..19.8678C"><span>Ambient <span class="hlt">seismic</span> noise monitoring of the Super-Sauze landslide from a very dense temporary <span class="hlt">seismic</span> array</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chtouki, Toufik; Vergne, Jerome; Provost, Floriane; Malet, Jean-Philippe; Burtin, Arnaud; Hibert, Clément</p> <p>2017-04-01</p> <p>The Super-Sauze landslide is located on the southern part of the Barcelonnette Basin (French Alps) and has developed in a soft clay-shale environment. It is one of the four sites continuously monitored through a wide variety of geophysical and hydro-geological techniques in the framework of the OMIV French national landslide observatory. From early June to mid-July 2016, a temporary dense <span class="hlt">seismic</span> array has been installed in the most active part of the landslide and at its surroundings. 50 different sites with an average inter-station distance of 50m have been instrumented with 150 miniaturized and autonomous <span class="hlt">seismic</span> stations (Zland nodes), allowing a continuous <span class="hlt">record</span> of the <span class="hlt">seismic</span> signal at frequencies higher than 0.2Hz over an almost regular grid. Concurrently, a Ground-Based InSAR device allowed for a precise and continuous monitoring of the surface deformation. Overall, this experiment is intended to better characterize the spatio-temporal evolution of the deformation processes related to various type of forcing. We analyze the continuous <span class="hlt">records</span> of ambient <span class="hlt">seismic</span> noise <span class="hlt">recorded</span> by the dense array. Using power spectral densities, we characterize the various types of natural and anthropogenic <span class="hlt">seismic</span> sources, including the effect of water turbulence and bedload transport in the small nearby torrents. We also compute the correlation of the ambient diffuse <span class="hlt">seismic</span> noise in various frequency bands for the 2448 station pairs to recover the empirical Green functions between them. The temporal evolution of the coda part of these noise correlation functions allows monitoring and localizing shear wave velocity variations in the sliding mass. Here we present some preliminary results of this analysis and compare the <span class="hlt">seismic</span> variations to meteorological data and surface deformation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.usgs.gov/of/2009/1002/index.html','USGSPUBS'); return false;" href="https://pubs.usgs.gov/of/2009/1002/index.html"><span>Digital <span class="hlt">seismic</span>-reflection data from western Rhode Island Sound, 1980</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>McMullen, K.Y.; Poppe, L.J.; Soderberg, N.K.</p> <p>2009-01-01</p> <p>During 1980, the U.S. Geological Survey (USGS) conducted a <span class="hlt">seismic</span>-reflection survey in western Rhode Island Sound aboard the Research Vessel Neecho. Data from this survey were <span class="hlt">recorded</span> in analog form and archived at the USGS Woods Hole Science Center's Data Library. Due to recent interest in the geology of Rhode Island Sound and in an effort to make the data more readily accessible while preserving the original paper <span class="hlt">records</span>, the <span class="hlt">seismic</span> data from this cruise were scanned and converted to Tagged Image File Format (TIFF) images and SEG-Y data files. Navigation data were converted from U.S. Coast Guard Long Range Aids to Navigation (LORAN-<span class="hlt">C</span>) time delays to latitudes and longitudes, which are available in Environmental Systems Research Institute, Inc. (ESRI) shapefile format and as eastings and northings in space-delimited text format.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2006AGUFM.S23B0159A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006AGUFM.S23B0159A"><span>Finite-Difference Numerical Simulation of <span class="hlt">Seismic</span> Gradiometry</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Aldridge, D. F.; Symons, N. P.; Haney, M. M.</p> <p>2006-12-01</p> <p>We use the phrase <span class="hlt">seismic</span> gradiometry to refer to the developing research area involving measurement, modeling, analysis, and interpretation of spatial derivatives (or differences) of a <span class="hlt">seismic</span> wavefield. In analogy with gradiometric methods used in gravity and magnetic exploration, <span class="hlt">seismic</span> gradiometry offers the potential for enhancing resolution, and revealing new (or hitherto obscure) information about the subsurface. For example, measurement of pressure and rotation enables the decomposition of <span class="hlt">recorded</span> <span class="hlt">seismic</span> data into compressional (P) and shear (S) components. Additionally, a complete observation of the total <span class="hlt">seismic</span> wavefield at a single receiver (including both rectilinear and rotational motions) offers the possibility of inferring the type, speed, and direction of an incident <span class="hlt">seismic</span> wave. Spatially extended receiver arrays, conventionally used for such directional and phase speed determinations, may be dispensed with. <span class="hlt">Seismic</span> wave propagation algorithms based on the explicit, time-domain, finite-difference (FD) numerical method are well-suited for investigating gradiometric effects. We have implemented in our acoustic, elastic, and poroelastic algorithms a point receiver that <span class="hlt">records</span> the 9 components of the particle velocity gradient tensor. Pressure and particle rotation are obtained by forming particular linear combinations of these tensor components, and integrating with respect to time. All algorithms entail 3D O(2,4) FD solutions of coupled, first- order systems of partial differential equations on uniformly-spaced staggered spatial and temporal grids. Numerical tests with a 1D model composed of homogeneous and isotropic elastic layers show isolation of P, SV, and SH phases <span class="hlt">recorded</span> in a multiple borehole configuration, even in the case of interfering events. Synthetic traces <span class="hlt">recorded</span> by geophones and rotation receivers in a shallow crosswell geometry with randomly heterogeneous poroelastic models also illustrate clear P (fast and slow) and S</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015EGUGA..17.2383B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015EGUGA..17.2383B"><span>MASW on the standard <span class="hlt">seismic</span> prospective scale using full spread <span class="hlt">recording</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Białas, Sebastian; Majdański, Mariusz; Trzeciak, Maciej; Gałczyński, Edward; Maksym, Andrzej</p> <p>2015-04-01</p> <p>The Multichannel Analysis of Surface Waves (MASW) is one of <span class="hlt">seismic</span> survey methods that use the dispersion curve of surface waves in order to describe the stiffness of the surface. Is is used mainly for geotechnical engineering scale with total length of spread between 5 - 450 m and spread offset between 1 - 100 m, the hummer is the <span class="hlt">seismic</span> source on this surveys. The standard procedure of MASW survey is: data acquisition, dispersion analysis and inversion of extracting dispersion curve to obtain the closest theoretical curve. The final result includes share-wave velocity (Vs) values at different depth along the surveyed lines. The main goal of this work is to expand this engineering method to the bigger scale with the length of standard prospecting spread of 20 km using 4.5 Hz version of vertical component geophones. The standard vibroseis and explosive method are used as the <span class="hlt">seismic</span> source. The acquisition were conducted on the full spread all the time during each single shoot. The <span class="hlt">seismic</span> data acquisition used for this analysis were carried out on the Braniewo 2014 project in north of Poland. The results achieved during standard MASW procedure says that this method can be used on much bigger scale as well. The different methodology of this analysis requires only much stronger <span class="hlt">seismic</span> source.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2013-title7-vol1/pdf/CFR-2013-title7-vol1-sec1c-115.pdf','CFR2013'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2013-title7-vol1/pdf/CFR-2013-title7-vol1-sec1c-115.pdf"><span>7 CFR 1<span class="hlt">c</span>.115 - IRB <span class="hlt">records</span>.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2013&page.go=Go">Code of Federal Regulations, 2013 CFR</a></p> <p></p> <p>2013-01-01</p> <p>... 7 Agriculture 1 2013-01-01 2013-01-01 false IRB <span class="hlt">records</span>. 1<span class="hlt">c</span>.115 Section 1<span class="hlt">c</span>.115 Agriculture Office of the Secretary of Agriculture PROTECTION OF HUMAN SUBJECTS § 1<span class="hlt">c</span>.115 IRB <span class="hlt">records</span>. (a) An institution..., including the following: (1) Copies of all research proposals reviewed, scientific evaluations, if any, that...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMMR43D0499O','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMMR43D0499O"><span>The Rock <span class="hlt">Record</span> of <span class="hlt">Seismic</span> Nucleation: examples from pseudotachylites beneath the Whipple Detachment Fault, eastern California</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ortega-Arroyo, D.; Behr, W. M.; Gentry, E.</p> <p>2017-12-01</p> <p>The mechanisms that lead to nucleation and dynamic weakening in the middle crust are not well understood. Proposed mechanisms include flash heating of asperities, thermal pressurization of pore fluids, dynamic instabilities, and fracture interactions. We investigate this issue in the rock <span class="hlt">record</span> using exhumed mid-crustal rocks exposed beneath the Whipple Detachment fault (WDF) in eastern CA. Analysis of pseudotachylites (PS) beneath the WDF, representing paleo-earthquakes, reveal two types: Type 1 PS exhibit little to no precursory cataclasis and are concentrated along shear bands at the margins of feldspar-rich lenses embedded in more quartz-rich domains. These appear synkinematic with S-<span class="hlt">C</span> fabrics in the surrounding mylonites and they exhibit finely dynamically recrystallized grains in quartz at their margins, suggesting coeval ductile deformation. By contrast, Type 2 PS occur along the principal slip surface of a brittle shear zone and show evidence for precursory cataclasis, brecciation, and fracturing. Some cataclasites inject into the host rock, forming eddies along the boundary with the PS. Slip appears to localize progressively into a 2 cm thick fault core, with PS concentrated primarily in the interior- the presence of solidified melt and fluidized cataclasite as clasts within the fault core suggests multiple slip events are preserved. We interpret the two types of pseudotachylites to represent different conditions and mechanisms of earthquake nucleation near the brittle-ductile transition (BDT). Type 1 PS are interpreted to represent nucleation in deeper sections of the BDT by failure along mineralogically-controlled stress concentrations hosted within an otherwise viscously deforming mylonite. Our data suggest that these do not develop into large-magnitude EQ's because <span class="hlt">seismic</span> slip is dampened into the surrounding quartz-rich viscous matrix; instead they may represent deep microseismicity and/or <span class="hlt">seismic</span> tremor. By contrast, Type 2 PS are interpreted to</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/21148981-probabilistic-simulation-territorial-seismic-scenarios','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/21148981-probabilistic-simulation-territorial-seismic-scenarios"><span>Probabilistic Simulation of Territorial <span class="hlt">Seismic</span> Scenarios</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Baratta, Alessandro; Corbi, Ileana</p> <p>2008-07-08</p> <p>The paper is focused on a stochastic process for the prevision of <span class="hlt">seismic</span> scenarios on the territory and developed by means of some basic assumptions in the procedure and by elaborating the fundamental parameters <span class="hlt">recorded</span> during some ground motions occurred in a <span class="hlt">seismic</span> area.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012AGUFM.S42C..03W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012AGUFM.S42C..03W"><span>Continuous, Large-Scale Processing of <span class="hlt">Seismic</span> Archives for High-Resolution Monitoring of <span class="hlt">Seismic</span> Activity and Seismogenic Properties</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Waldhauser, F.; Schaff, D. P.</p> <p>2012-12-01</p> <p>Archives of digital <span class="hlt">seismic</span> data <span class="hlt">recorded</span> by seismometer networks around the world have grown tremendously over the last several decades helped by the deployment of <span class="hlt">seismic</span> stations and their continued operation within the framework of monitoring earthquake activity and verification of the Nuclear Test-Ban Treaty. We show results from our continuing effort in developing efficient waveform cross-correlation and double-difference analysis methods for the large-scale processing of regional and global <span class="hlt">seismic</span> archives to improve existing earthquake parameter estimates, detect <span class="hlt">seismic</span> events with magnitudes below current detection thresholds, and improve real-time monitoring procedures. We demonstrate the performance of these algorithms as applied to the 28-year long <span class="hlt">seismic</span> archive of the Northern California <span class="hlt">Seismic</span> Network. The tools enable the computation of periodic updates of a high-resolution earthquake catalog of currently over 500,000 earthquakes using simultaneous double-difference inversions, achieving up to three orders of magnitude resolution improvement over existing hypocenter locations. This catalog, together with associated metadata, form the underlying relational database for a real-time double-difference scheme, DDRT, which rapidly computes high-precision correlation times and hypocenter locations of new events with respect to the background archive (http://ddrt.ldeo.columbia.edu). The DDRT system facilitates near-real-time <span class="hlt">seismicity</span> analysis, including the ability to search at an unprecedented resolution for spatio-temporal changes in seismogenic properties. In areas with continuously <span class="hlt">recording</span> stations, we show that a detector built around a scaled cross-correlation function can lower the detection threshold by one magnitude unit compared to the STA/LTA based detector employed at the network. This leads to increased event density, which in turn pushes the resolution capability of our location algorithms. On a global scale, we are currently building</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/21973353','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/21973353"><span>Two applications of time reversal mirrors: <span class="hlt">seismic</span> radio and <span class="hlt">seismic</span> radar.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Hanafy, Sherif M; Schuster, Gerard T</p> <p>2011-10-01</p> <p>Two <span class="hlt">seismic</span> applications of time reversal mirrors (TRMs) are introduced and tested with field experiments. The first one is sending, receiving, and decoding coded messages similar to a radio except <span class="hlt">seismic</span> waves are used. The second one is, similar to radar surveillance, detecting and tracking a moving object(s) in a remote area, including the determination of the objects speed of movement. Both applications require the prior <span class="hlt">recording</span> of calibration Green's functions in the area of interest. This reference Green's function will be used as a codebook to decrypt the coded message in the first application and as a moving sensor for the second application. Field tests show that <span class="hlt">seismic</span> radar can detect the moving coordinates (x(t), y(t), z(t)) of a person running through a calibration site. This information also allows for a calculation of his velocity as a function of location. Results with the <span class="hlt">seismic</span> radio are successful in <span class="hlt">seismically</span> detecting and decoding coded pulses produced by a hammer. Both <span class="hlt">seismic</span> radio and radar are highly robust to signals in high noise environments due to the super-stacking property of TRMs. © 2011 Acoustical Society of America</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018TCry...12.1715K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018TCry...12.1715K"><span>Deriving micro- to macro-scale <span class="hlt">seismic</span> velocities from ice-core <span class="hlt">c</span> axis orientations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kerch, Johanna; Diez, Anja; Weikusat, Ilka; Eisen, Olaf</p> <p>2018-05-01</p> <p>One of the great challenges in glaciology is the ability to estimate the bulk ice anisotropy in ice sheets and glaciers, which is needed to improve our understanding of ice-sheet dynamics. We investigate the effect of crystal anisotropy on <span class="hlt">seismic</span> velocities in glacier ice and revisit the framework which is based on fabric eigenvalues to derive approximate <span class="hlt">seismic</span> velocities by exploiting the assumed symmetry. In contrast to previous studies, we calculate the <span class="hlt">seismic</span> velocities using the exact <span class="hlt">c</span> axis angles describing the orientations of the crystal ensemble in an ice-core sample. We apply this approach to fabric data sets from an alpine and a polar ice core. Our results provide a quantitative evaluation of the earlier approximative eigenvalue framework. For near-vertical incidence our results differ by up to 135 m s-1 for P-wave and 200 m s-1 for S-wave velocity compared to the earlier framework (estimated 1 % difference in average P-wave velocity at the bedrock for the short alpine ice core). We quantify the influence of shear-wave splitting at the bedrock as 45 m s-1 for the alpine ice core and 59 m s-1 for the polar ice core. At non-vertical incidence we obtain differences of up to 185 m s-1 for P-wave and 280 m s-1 for S-wave velocities. Additionally, our findings highlight the variation in <span class="hlt">seismic</span> velocity at non-vertical incidence as a function of the horizontal azimuth of the <span class="hlt">seismic</span> plane, which can be significant for non-symmetric orientation distributions and results in a strong azimuth-dependent shear-wave splitting of max. 281 m s-1 at some depths. For a given incidence angle and depth we estimated changes in phase velocity of almost 200 m s-1 for P wave and more than 200 m s-1 for S wave and shear-wave splitting under a rotating <span class="hlt">seismic</span> plane. We assess for the first time the change in <span class="hlt">seismic</span> anisotropy that can be expected on a short spatial (vertical) scale in a glacier due to strong variability in crystal-orientation fabric (±50 m s-1 per 10 cm</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011AGUFM.S41C2194C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011AGUFM.S41C2194C"><span><span class="hlt">Seismic</span> Hazard Analysis as a Controlling Technique of Induced <span class="hlt">Seismicity</span> in Geothermal Systems</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Convertito, V.; Sharma, N.; Maercklin, N.; Emolo, A.; Zollo, A.</p> <p>2011-12-01</p> <p>The effect of induced <span class="hlt">seismicity</span> of geothermal systems during stimulation and fluid circulation can cover a wide range of values from light and unfelt to severe and damaging. If the design of a modern geothermal system requires the largest efficiency to be obtained from the social point of view it is required that the system could be managed in order to reduce possible impact in advance. In this framework, automatic control of the <span class="hlt">seismic</span> response of the stimulated reservoir is nowadays mandatory, particularly in proximity of densely populated areas. Recently, techniques have been proposed for this purpose mainly based on the concept of the traffic light. This system provides a tool to decide the level of stimulation rate based on the real-time analysis of the induced <span class="hlt">seismicity</span> and the ongoing ground motion values. However, in some cases the induced effect can be delayed with respect to the time when the reservoir is stimulated. Thus, a controlling system technique able to estimate the ground motion levels for different time scales can help to better control the geothermal system. Here we present an adaptation of the classical probabilistic <span class="hlt">seismic</span> hazard analysis to the case where the <span class="hlt">seismicity</span> rate as well as the propagation medium properties are not constant with time. We use a non-homogeneous <span class="hlt">seismicity</span> model for modeling purposes, in which the <span class="hlt">seismicity</span> rate and b-value of the recurrence relationship change with time. Additionally, as a further controlling procedure, we propose a moving time window analysis of the <span class="hlt">recorded</span> peak ground-motion values aimed at monitoring the changes in the propagation medium. In fact, for the same set of magnitude values <span class="hlt">recorded</span> at the same stations, we expect that on average peak ground motion values attenuate in same way. As a consequence, the residual differences can be reasonably ascribed to changes in medium properties. These changes can be modeled and directly introduced in the hazard integral. We applied the proposed</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.C41D1266C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.C41D1266C"><span><span class="hlt">Seismic</span> Signatures of Brine Release at Blood Falls, Taylor Glacier, Antarctica</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Carr, C. G.; Pettit, E. C.; Carmichael, J.</p> <p>2017-12-01</p> <p>Blood Falls is created by the release of subglacially-sourced, iron-rich brine at the surface of Taylor Glacier, McMurdo Dry Valleys, Antarctica. The supraglacial portion of this hydrological feature is episodically active. Englacial liquid brine flow occurs despite ice temperatures of -17°<span class="hlt">C</span> and we document supraglacial liquid brine release despite ambient air temperatures average -20°<span class="hlt">C</span>. In this study, we use data from a <span class="hlt">seismic</span> network, time-lapse cameras, and publicly available weather station data to address the questions: what are the characteristics of <span class="hlt">seismic</span> events that occur during Blood Falls brine release and how do these compare with <span class="hlt">seismic</span> events that occur during times of Blood Falls quiescence? How are different processes observable in the time-lapse imagery represented in the <span class="hlt">seismic</span> <span class="hlt">record</span>? Time-lapse photography constrains the timing of brine release events during the austral winter of 2014. We use a noise-adaptive digital power detector to identify <span class="hlt">seismic</span> events and cluster analysis to identify repeating events based on waveform similarity across the network. During the 2014 wintertime brine release, high-energy repeated <span class="hlt">seismic</span> events occurred proximal to Blood Falls. We investigate the ground motions associated with these clustered events, as well as their spatial distribution. We see evidence of possible tremor during the brine release periods, an indicator of fluid movement. If distinctive <span class="hlt">seismic</span> signatures are associated with Blood Falls brine release they could be identified based solely on <span class="hlt">seismic</span> data without any aid from time-lapse cameras. Passive seismologic monitoring has the benefit of continuity during the polar night and other poor visibility conditions, which make time-lapse imagery unusable.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015EGUGA..17.5611J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015EGUGA..17.5611J"><span><span class="hlt">Seismic</span> source models for very-long period <span class="hlt">seismic</span> signals on White Island, New Zealand</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jiwani-Brown, Elliot; Neuberg, Jurgen; Jolly, Art</p> <p>2015-04-01</p> <p>Very-long-period <span class="hlt">seismic</span> signals (VLP) from White Island have a duration of only a few tens of seconds and a waveform that indicates an elastic (or viscoelastic) interaction of a source region with the surrounding medium; unlike VLP signals on some other volcanoes that indicate a step function <span class="hlt">recorded</span> in the near field of the <span class="hlt">seismic</span> source, White Island VLPs exhibit a Ricker waveform. We explore a set of isotropic, <span class="hlt">seismic</span> source models based on the interaction between magma and water/brine in direct contact. <span class="hlt">Seismic</span> amplitude measurements are taken into account to estimate the volume changes at depth that can produce the observed displacement at the surface. Furthermore, the influence of different fluid types are explored.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1981STIN...8231576B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1981STIN...8231576B"><span>Studies on effects of infills in <span class="hlt">seismic</span> resistant R/<span class="hlt">C</span> construction</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Brokken, S. T.; Bertero, V. V.</p> <p>1981-10-01</p> <p>Experimental and analytical studies of the quantitative effects of infills in the <span class="hlt">seismic</span> performance of buildings (particularly in buildings whose structural systems are based on the use of moment resisting frames alone are summarized); and the implications of these effects regarding the design of new buildings and retrofitting of existing R/<span class="hlt">C</span> frame structures were evaluated. The first part is concerned with the infill problem and the experimental investigation conducted to study the effects of infill panels on <span class="hlt">seismic</span> response of reinforced concrete frames. This investigation consisted of a series of quasi-static cyclic and monotonic load tests on 1/3-scale models of the lower 3-1/2 stories of an 11 story-three bay reinforced concrete frame infilled in the outer two bays. The reinforced concrete moment frame was designed for high rotational ductility and resistance to degradation under reversed cyclic shear loads.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011AGUFM.P33A1742I','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011AGUFM.P33A1742I"><span>Infrasound and <span class="hlt">Seismic</span> Observation of Hayabusa Reentry as An Artificial Meteorite Fall</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ishihara, Y.; Hiramatsu, Y.; Yamamoto, M.; Furumoto, M.; Fujita, K.</p> <p>2011-12-01</p> <p>The Hayabusa, the world first sample-return minor body explorer, came back to the Earth, and reentered into the Earth's atmosphere on June 13, 2010. Following the reentries of the Genesis in 2004 and the Stardust in 2006, the return of the Hayabusa Sample Return Capsule (H-SRC) was the third direct reentry event from the interplanetary transfer orbit to the Earth at a velocity of over 11.2 km/s. In addition, it was the world first case of the direct reentry of the spacecraft (H-S/<span class="hlt">C</span>) itself from the interplanetary transfer orbit. The H-SRC and the H-S/<span class="hlt">C</span> reentries are very good analogue for studying bolide size meteors and meteorite falls. We, therefore, conducted a ground observation campaign for aspects of meteor sciences. We carried out multi-site ground observations of the Hayabusa reentry in the Woomera Prohibited Area (WPA), Australia. The observations were configured with optical imaging with still and video <span class="hlt">recordings</span>, spectroscopies, and shockwave detection with infrasound and <span class="hlt">seismic</span> sensors. In this study, we report details of the infrasound/<span class="hlt">seismic</span> observations and those results. To detect shockwaves from the H-SRC and the H-S/<span class="hlt">C</span>, we installed three small aperture infrasound/<span class="hlt">seismic</span> arrays as the main stations. In addition, we also installed three single component <span class="hlt">seismic</span> sub stations and an audible sound <span class="hlt">recorder</span>. The infrasound and <span class="hlt">seismic</span> sensors clearly <span class="hlt">recorded</span> sonic boom type shockwaves from the H-SRC and disrupted fragments of the H-S/<span class="hlt">C</span> itself. The audible <span class="hlt">recording</span> also detected those shockwave sounds in the human audible band. Positive overpressure values of shockwaves (corresponding to the H-SRC) <span class="hlt">recorded</span> at three main stations are 1.3 Pa, 1.0 Pa, and 0.7 Pa with the slant distance of 36.9 km, 54.9 km, and 67.8 km (i.e., the source altitude of 36.5 km, 38.9km, and 40.6 km), respectively. These amplitudes of shockwave overpressures are systematically smaller than those of theoretical predictions. We tried to identify the sources of shockwaves</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_5");'>5</a></li> <li><a href="#" onclick='return showDiv("page_6");'>6</a></li> <li class="active"><span>7</span></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_7 --> <div id="page_8" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_6");'>6</a></li> <li><a href="#" onclick='return showDiv("page_7");'>7</a></li> <li class="active"><span>8</span></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="141"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUFM.S41A2417M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUFM.S41A2417M"><span>Investigation on the real-time prediction of ground motions using <span class="hlt">seismic</span> <span class="hlt">records</span> observed in deep boreholes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Miyakoshi, H.; Tsuno, S.</p> <p>2013-12-01</p> <p>The present method of the EEW system installed in the railway field of Japan predicts <span class="hlt">seismic</span> ground motions based on the estimated earthquake information about epicentral distances and magnitudes using initial P-waves observed on the surface. In the case of local earthquakes beneath the Tokyo Metropolitan Area, however, a method to directly predict <span class="hlt">seismic</span> ground motions using P-waves observed in deep boreholes could issue EEWs more simply and surely. Besides, a method to predict <span class="hlt">seismic</span> ground motions, using S-waves observed in deep boreholes and S-wave velocity structures beneath <span class="hlt">seismic</span> stations, could show planar distributions of ground motions for train operation control areas in the aftermath of earthquakes. This information is available to decide areas in which the emergency inspection of railway structures should be performed. To develop those two methods, we investigated relationships between peak amplitudes on the surface and those in deep boreholes, using <span class="hlt">seismic</span> <span class="hlt">records</span> of KiK-net stations in the Kanto Basin. In this study, we used earthquake accelerograms observed in boreholes whose depths are deeper than the top face of Pre-Neogene basement and those on the surface at 12 <span class="hlt">seismic</span> stations of KiK-net. We selected 243 local earthquakes whose epicenters are located around the Kanto Region. Those JMA magnitudes are in the range from 4.5 to 7.0. We picked the on-set of P-waves and S-waves using a vertical component and two horizontal components, respectively. Peak amplitudes of P-waves and S-waves were obtained using vertical components and vector sums of two horizontal components, respectively. We estimated parameters which represent site amplification factors beneath <span class="hlt">seismic</span> stations, using peak amplitudes of S-waves observed in the deep borehole and those on the surface, to minimize the residuals between calculations by the theoretical equation and observations. Correlation coefficients between calculations and observations are high values in the range</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009AGUFM.S23A1730W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009AGUFM.S23A1730W"><span><span class="hlt">Seismic</span> Noise Characterization in the Northern Mississippi Embayment</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wiley, S.; Deshon, H. R.; Boyd, O. S.</p> <p>2009-12-01</p> <p>We present a study of <span class="hlt">seismic</span> noise sources present within the northern Mississippi embayment near the New Madrid <span class="hlt">Seismic</span> Zone (NMSZ). The northern embayment contains up to 1 km of unconsolidated coastal plain sediments overlying bedrock, making it an inherently noisy environment for <span class="hlt">seismic</span> stations. The area is known to display high levels of cultural noise caused by agricultural activity, passing cars, trains, etc. We characterize continuous broadband <span class="hlt">seismic</span> noise data <span class="hlt">recorded</span> for the months of March through June 2009 at six stations operated by the Cooperative New Madrid <span class="hlt">Seismic</span> Network. We looked at a single horizontal component of data during nighttime hours, defined as 6:15PM to 5:45AM Central Standard Time, which we determined to be the lowest amplitude period of noise for the region. Hourly median amplitudes were compared to daily average wind speeds downloaded from the National Oceanic and Atmospheric Administration. We find a correlation between time periods of increased noise and days with high wind speeds, suggesting that wind is likely a prevalent source of <span class="hlt">seismic</span> noise in the area. The effects of wind on <span class="hlt">seismic</span> <span class="hlt">recordings</span> may result from wind induced tree root movement which causes ground motion to be <span class="hlt">recorded</span> at the vaults located ~3m below ground. Automated studies utilizing the local network or the EarthScope Transportable Array, scheduled to arrive in the area in 2010-11, should expect to encounter wind induced noise fluctuations and must account for this in their analysis.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..19.4605D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..19.4605D"><span>5 years of continuous <span class="hlt">seismic</span> monitoring of a mountain river in the Pyrenees</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Diaz, Jordi; Sanchez-Pastor, Pilar S.; Gallart, Josep</p> <p>2017-04-01</p> <p>The analysis of background <span class="hlt">seismic</span> noise variations in the proximity of river channels has revealed as a useful tool to monitor river flow, even for modest discharges. Nevertheless, this monitoring is usually carried on using temporal deployments of <span class="hlt">seismic</span> stations. The CANF <span class="hlt">seismic</span> broad-band station, acquiring data continuously since 2010 and located inside an old railway tunnel in the Central Pyrenees, at about 400 m of the Aragón River channel, provides an excellent opportunity to enlarge this view and present a long term monitoring of a mountain river. <span class="hlt">Seismic</span> signals in the 2-10 Hz band clearly related to river discharges have been identified in the <span class="hlt">seismic</span> <span class="hlt">records</span>. Discharge increases due to rainfall, large storms resulting in floods and snowmelt periods can be discriminated from the analysis of the <span class="hlt">seismic</span> data. Up to now, two large rainfall events resulting in large discharge and damaging floods have been <span class="hlt">recorded</span>, both sharing similar properties which can be used to implement automatic procedures to identify <span class="hlt">seismically</span> potentially damaging floods. Another natural process that can be characterized using continuouly acquired <span class="hlt">seismic</span> data is mountain snowmelt, as this process results in characteristic discharge patterns which can be identified in the <span class="hlt">seismic</span> data. The time occurrence and intensity of the snowmelt stages for each season can be identified and the 5 seasons available so far compared to detect possible trends The so-called fluvial seismology can also provide important clues to evaluate the beadload transport in rivers, an important parameter to evaluate erosion rates in mountain environments. Analyzing both the amplitude and frequency variations of the <span class="hlt">seismic</span> data and its hysteresis cycles, it seems possible to estimate the relative contribution of water flow and bedload transport to the <span class="hlt">seismic</span> signal. The available results suggest that most of the river-generated <span class="hlt">seismic</span> signal seems related to bed load transportation, while water</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1047774','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1047774"><span>Newberry <span class="hlt">Seismic</span> Deployment Fieldwork Report</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Wang, J; Templeton, D C</p> <p>2012-03-21</p> <p>This report summarizes the <span class="hlt">seismic</span> deployment of Lawrence Livermore National Laboratory (LLNL) Geotech GS-13 short-period seismometers at the Newberry Enhanced Geothermal System (EGS) Demonstration site located in Central Oregon. This Department of Energy (DOE) demonstration project is managed by AltaRock Energy Inc. AltaRock Energy had previously deployed Geospace GS-11D geophones at the Newberry EGS Demonstration site, however the quality of the <span class="hlt">seismic</span> data was somewhat low. The purpose of the LLNL deployment was to install more sensitive sensors which would <span class="hlt">record</span> higher quality <span class="hlt">seismic</span> data for use in future <span class="hlt">seismic</span> studies, such as ambient noise correlation, matched field processing earthquakemore » detection studies, and general EGS microearthquake studies. For the LLNL deployment, seven three-component <span class="hlt">seismic</span> stations were installed around the proposed AltaRock Energy stimulation well. The LLNL <span class="hlt">seismic</span> sensors were connected to AltaRock Energy Gueralp CMG-DM24 digitizers, which are powered by AltaRock Energy solar panels and batteries. The deployment took four days in two phases. In phase I, the sites were identified, a cavity approximately 3 feet deep was dug and a flat concrete pad oriented to true North was made for each site. In phase II, we installed three single component GS-13 seismometers at each site, quality controlled the data to ensure that each station was <span class="hlt">recording</span> data properly, and filled in each cavity with native soil.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.S31D..06C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.S31D..06C"><span><span class="hlt">Seismic</span> Imaging of the Source Physics Experiment Site with the Large-N <span class="hlt">Seismic</span> Array</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chen, T.; Snelson, C. M.; Mellors, R. J.</p> <p>2017-12-01</p> <p>The Source Physics Experiment (SPE) consists of a series of chemical explosions at the Nevada National Security Site. The goal of SPE is to understand <span class="hlt">seismic</span> wave generation and propagation from these explosions. To achieve this goal, we need an accurate geophysical model of the SPE site. A Large-N <span class="hlt">seismic</span> array that was deployed at the SPE site during one of the chemical explosions (SPE-5) helps us construct high-resolution local geophysical model. The Large-N <span class="hlt">seismic</span> array consists of 996 geophones, and covers an area of approximately 2 × 2.5 km. The array is located in the northern end of the Yucca Flat basin, at a transition from Climax Stock (granite) to Yucca Flat (alluvium). In addition to the SPE-5 explosion, the Large-N array also <span class="hlt">recorded</span> 53 weight drops. Using the Large-N <span class="hlt">seismic</span> array <span class="hlt">recordings</span>, we perform body wave and surface wave velocity analysis, and obtain 3D <span class="hlt">seismic</span> imaging of the SPE site for the top crust of approximately 1 km. The imaging results show clear variation of geophysical parameter with local geological structures, including heterogeneous weathering layer and various rock types. The results of this work are being incorporated in the larger 3D modeling effort of the SPE program to validate the predictive models developed for the site.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010EGUGA..12.2574J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010EGUGA..12.2574J"><span>Background noise model development for <span class="hlt">seismic</span> stations of KMA</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jeon, Youngsoo</p> <p>2010-05-01</p> <p>The background noise <span class="hlt">recorded</span> at seismometer is exist at any <span class="hlt">seismic</span> signal due to the natural phenomena of the medium which the signal passed through. Reducing the <span class="hlt">seismic</span> noise is very important to improve the data quality in <span class="hlt">seismic</span> studies. But, the most important aspect of reducing <span class="hlt">seismic</span> noise is to find the appropriate place before installing the seismometer. For this reason, NIMR(National Institution of Meteorological Researches) starts to develop a model of standard background noise for the broadband <span class="hlt">seismic</span> stations of the KMA(Korea Meteorological Administration) using a continuous data set obtained from 13 broadband stations during the period of 2007 and 2008. We also developed the model using short period <span class="hlt">seismic</span> data from 10 stations at the year of 2009. The method of Mcmara and Buland(2004) is applied to analyse background noise of Korean Peninsula. The fact that borehole seismometer <span class="hlt">records</span> show low noise level at frequency range greater than 1 Hz compared with that of <span class="hlt">records</span> at the surface indicate that the cultural noise of inland Korean Peninsula should be considered to process the <span class="hlt">seismic</span> data set. Reducing Double Frequency peak also should be regarded because the Korean Peninsula surrounded by the seas from eastern, western and southern part. The development of KMA background model shows that the Peterson model(1993) is not applicable to fit the background noise signal generated from Korean Peninsula.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.usgs.gov/of/1995/0228/of95-228.txt','USGSPUBS'); return false;" href="https://pubs.usgs.gov/of/1995/0228/of95-228.txt"><span>Multichannel <span class="hlt">seismic</span>-reflection profiling on the R/V Maurice Ewing during the Los Angeles Region <span class="hlt">Seismic</span> Experiment (LARSE), California</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Brocher, Thomas M.; Clayton, Robert W.; Klitgord, Kim D.; Bohannon, Robert G.; Sliter, Ray; McRaney, John K.; Gardner, James V.; Keene, J.B.</p> <p>1995-01-01</p> <p>This report describes the acquisition of deep-crustal multichannel <span class="hlt">seismic</span>-reflection data in the Inner California Borderland aboard the R/V Maurice Ewing, conducted in October 1994 as part of the Los Angeles Regional <span class="hlt">Seismic</span> Experiment (LARSE). LARSE is a cooperative study of the crustal structure of southern California involving earth scientists from the U.S. Geological Survey, Caltech, the University of Southern California, the University of California Los Angeles, and the Southern California Earthquake Center (SCEC). During LARSE, the R/V Ewing's 20- element air gun array, totaling 137.7 liters (8470 cu. in.), was used as the primary <span class="hlt">seismic</span> source for wide-angle <span class="hlt">recording</span> along three main onshore-offshore lines centered on the Los Angeles basin and the epicenters of the 1933 Long Beach and 1994 Northridge earthquakes. The LARSE onshore-offshore lines were each 200-250 km long, with the offshore portions being between 90 and 150 km long. The nearly 24,000 air gun signals generated by the Ewing were <span class="hlt">recorded</span> by an array of 170 PASSCAL REFTEK <span class="hlt">recorders</span> deployed at 2 km intervals along all three of the onshore lines and 9 ocean bottom seismometers (OBSs) deployed along two of the lines. Separate passes over the OBS-deployment lines were performed with a long air gun repetition rate (60 and 90 seconds) to minimize acoustic-wave interference from previous shots in the OBS data. The Ewing's 4.2-km, 160-channel, digital streamer was also used to <span class="hlt">record</span> approximately 1250 km of 40-fold multichannel <span class="hlt">seismic</span>-reflection data. To enhance the fold of the wide-angle data <span class="hlt">recorded</span> onshore, mitigating against cultural and wind noise in the Los Angeles basin, the entire ship track was repeated at least once resulting in fewer than about 660 km of unique trackline coverage in the Inner Borderland. Portions of the <span class="hlt">seismic</span>-reflection lines were repeated up to 6 times. A variety of other geophysical data were also continuously <span class="hlt">recorded</span>, including 3.5 kHz bathymetry, multi</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/549187-overview-seismic-potential-central-eastern-united-states','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/549187-overview-seismic-potential-central-eastern-united-states"><span>Overview of <span class="hlt">seismic</span> potential in the central and eastern United States</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Schweig, E.S.</p> <p>1995-12-31</p> <p>The <span class="hlt">seismic</span> potential of any region can be framed in terms the locations of source zones, the frequency of earthquake occurrence for each source, and the maximum size earthquake that can be expect from each source. As delineated by modern and historical <span class="hlt">seismicity</span>, the most important <span class="hlt">seismic</span> source zones affecting the eastern United States include the New Madrid and Wabash Valley <span class="hlt">seismic</span> zones of the central U.S., the southern Appalachians and Charleston, South Carolina, areas in the southeast, and the northern Appalachians and Adirondacks in the northeast. The most prominant of these in terms of current <span class="hlt">seismicity</span> and historical seismicmore » moment release in the New Madrid <span class="hlt">seismic</span> zone, which produced three earthquakes of moment magnitude {ge} 8 in 1811 and 1812. The frequency of earthquake recurrence can be examined using the instrumental <span class="hlt">record</span>, the historical <span class="hlt">record</span>, and the geological <span class="hlt">record</span>. Each <span class="hlt">record</span> covers a unique time period and has a different scale of temporal resolution and completeness of the data set. The Wabash Valley is an example where the long-term geological <span class="hlt">record</span> indicates a greater potential than the instrumental and historical <span class="hlt">records</span>. This points to the need to examine all of the evidence in any region in order to obtain a credible estimates of earthquake hazards. Although earthquake hazards may be dominated by mid-magnitude 6 earthquakes within the mapped <span class="hlt">seismic</span> source zones, the 1994 Northridge, California, earthquake is just the most recent example of the danger of assuming future events will occur on faults known to have had past events and how destructive such an earthquake can be.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015EGUGA..17.6684J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015EGUGA..17.6684J"><span>Could the IMS Infrasound Stations Support a Global Network of Small Aperture <span class="hlt">Seismic</span> Arrays?</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>J, Gibbons, Steven; Kværna, Tormod; Mykkeltveit, Svein</p> <p>2015-04-01</p> <p>The infrasound stations of the International Monitoring System are arrays consisting of up to 15 sites and with apertures of up to 3 km. The arrays are distributed remarkably uniformly over the globe and provide excellent coverage of South America, Africa, and Antarctica. This is to say that there are many infrasound arrays in regions many thousands of kilometers from the closest <span class="hlt">seismic</span> array. Several infrasound arrays are in the immediate vicinity of existing 3-component <span class="hlt">seismic</span> stations and these provide us with examples of how typical <span class="hlt">seismic</span> signals look at these locations. We can make idealized estimates of the predicted performance of <span class="hlt">seismic</span> arrays, consisting of seismometers at each site of the infrasound arrays, by duplicating the signals from the 3-<span class="hlt">C</span> stations at all sites of the array. However, the true performance of <span class="hlt">seismic</span> arrays at these sites will depend both upon Signal-to-Noise Ratios of <span class="hlt">seismic</span> signals and the coherence of both signal and noise between sensors. These properties can only be determined experimentally. <span class="hlt">Recording</span> <span class="hlt">seismic</span> data of sufficient quality at many of these arrays may require borehole deployments since the microbarometers in the infrasound arrays are often situated in vaults placed in soft sediments. The geometries of all the current IMS infrasound arrays are examined and compared and we demonstrate that, from a purely geometrical perspective, essentially all the array configurations would provide <span class="hlt">seismic</span> arrays with acceptable slowness resolution for both regional and teleseismic phase arrivals. <span class="hlt">Seismic</span> arrays co-located with the infrasound arrays in many regions would likely enhance significantly the <span class="hlt">seismic</span> monitoring capability in parts of the world where only 3-component stations are currently available. Co-locating <span class="hlt">seismic</span> and infrasound sensors would facilitate the development of <span class="hlt">seismic</span> arrays that share the infrastructure of the infrasound arrays, reducing the development and operational costs. Hosting countries might</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018GeoJI.212.1588V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018GeoJI.212.1588V"><span>Spatial wavefield gradient-based <span class="hlt">seismic</span> wavefield separation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Van Renterghem, C.; Schmelzbach, C.; Sollberger, D.; Robertsson, J. OA</p> <p>2018-03-01</p> <p>Measurements of the horizontal and vertical components of particle motion combined with estimates of the spatial gradients of the <span class="hlt">seismic</span> wavefield enable <span class="hlt">seismic</span> data to be acquired and processed using single dedicated multicomponent stations (e.g. rotational sensors) and/or small receiver groups instead of large receiver arrays. Here, we present <span class="hlt">seismic</span> wavefield decomposition techniques that use spatial wavefield gradient data to separate land and ocean bottom data into their upgoing/downgoing and P/S constituents. Our method is based on the elastodynamic representation theorem with the derived filters requiring local measurements of the wavefield and its spatial gradients only. We demonstrate with synthetic data and a land <span class="hlt">seismic</span> field data example that combining translational measurements with spatial wavefield gradient estimates allows separating <span class="hlt">seismic</span> data <span class="hlt">recorded</span> either at the Earth's free-surface or at the sea bottom into upgoing/downgoing and P/S wavefield constituents for typical incidence angle ranges of body waves. A key finding is that the filter application only requires knowledge of the elastic properties exactly at the <span class="hlt">recording</span> locations and is valid for a wide elastic property range.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA473124','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA473124"><span>Obtaining Unique, Comprehensive Deep <span class="hlt">Seismic</span> Sounding Data Sets for CTBT Monitoring and Broad Seismological Studies</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2007-07-02</p> <p>TYPE Final Report 3. DATES COVERED (From - To) 26-Sep-01 to 26-Jun-07 4. TITLE AND SUBTITLE OBTAINING UNIQUE, COMPREHENSIVE DEEP <span class="hlt">SEISMIC</span> ... <span class="hlt">seismic</span> <span class="hlt">records</span> from 12 major Deep <span class="hlt">Seismic</span> Sounding (DSS) projects acquired in 1970-1980’s in the former Soviet Union. The data include 3-component...<span class="hlt">records</span> from 22 Peaceful Nuclear Explosions (PNEs) and over 500 chemical explosions <span class="hlt">recorded</span> by a grid of linear, reversed <span class="hlt">seismic</span> profiles covering a</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017GeoRL..44.2237Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017GeoRL..44.2237Z"><span>Noise-based <span class="hlt">seismic</span> monitoring of the Campi Flegrei caldera</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zaccarelli, Lucia; Bianco, Francesca</p> <p>2017-03-01</p> <p>The Campi Flegrei caldera is one of the highest risk volcanic fields worldwide, because of its eruptive history and the large population hosted within the caldera. It experiences bradiseismic crises: sudden uplift with low energetic <span class="hlt">seismic</span> swarm occurrences. No <span class="hlt">seismicity</span> is <span class="hlt">recorded</span> out of these deformation rate changes. Therefore, a continuous <span class="hlt">seismic</span> monitoring of the caldera is possible only by means of the ambient <span class="hlt">seismic</span> noise. We apply a noise-based <span class="hlt">seismic</span> monitoring technique to the cross correlations of 5 year <span class="hlt">recordings</span> at the mobile <span class="hlt">seismic</span> network. The resulting relative velocity variations are compared to the temporal behavior of the geophysical and geochemical observations routinely sampled at Campi Flegrei. We discriminate between two kinds of crustal stress field variations acting at different timescales. They are related to a possible magmatic intrusion and to the gradual heating of the hydrothermal system, respectively. This study sets up the basis for future volcano monitoring strategies.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.usgs.gov/of/1967/of67-024/of67-024.pdf','USGSPUBS'); return false;" href="https://pubs.usgs.gov/of/1967/of67-024/of67-024.pdf"><span><span class="hlt">Seismic</span> measurements of explosions in the Tatum Salt Dome, Mississippi</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Borcherdt, Roger D.; Healy, J.H.; Jackson, W.H.; Warren, D.R.</p> <p>1967-01-01</p> <p>Project Sterling provided for the detonation of a nuclear device in the cavity resulting from the Salmon nuclear explosion in the Tatum salt dome in southern Mississippi. It also provided for a high explosive (HE) comparison shot in a nearby drill hole. The purpose of the experiment was to gather information on the <span class="hlt">seismic</span> decoupling of a nuclear explosion in a cavity by comparing <span class="hlt">seismic</span> signals from a nuclear shot in the Salmon cavity with <span class="hlt">seismic</span> signals <span class="hlt">recorded</span> from Salmon and with <span class="hlt">seismic</span> signals <span class="hlt">recorded</span> from a muall (about 2 tons) HE shot in the salt dome. Surface <span class="hlt">seismic</span> measurements were made by the U.S. Geological Survey, the U.S. Coast and Geodetic Survey, and the Air Force Technical Applications Center with coordination and overall direction by the Lawrence Radiation Laboratory. This report covers only the <span class="hlt">seismic</span> measurements made by the U. S. Geological Survey. The first objective of this report is to describe the field <span class="hlt">recording</span> procedures and the data obtained by the U. S. Geological Survey from these events. The second objective is to describe the spectral analyses which have been made on the data and the relative <span class="hlt">seismic</span> amplitudes which have been determined from these analyses.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/983425','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/983425"><span>Second Quarter Hanford <span class="hlt">Seismic</span> Report for Fiscal Year 2010</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Rohay, Alan C.; Sweeney, Mark D.; Hartshorn, Donald C.</p> <p>2010-06-30</p> <p>The Hanford <span class="hlt">Seismic</span> Assessment Program (HSAP) provides an uninterrupted collection of high-quality raw and processed <span class="hlt">seismic</span> data from the Hanford <span class="hlt">Seismic</span> Network for the U.S. Department of Energy and its contractors. The HSAP is responsible for locating and identifying sources of <span class="hlt">seismic</span> activity and monitoring changes in the historical pattern of <span class="hlt">seismic</span> activity at the Hanford Site. The data are compiled, archived, and published for use by the Hanford Site for waste management, natural phenomena hazards assessments, and engineering design and construction. In addition, the HSAP works with the Hanford Site Emergency Services Organization to provide assistance in the eventmore » of a significant earthquake on the Hanford Site. The Hanford <span class="hlt">Seismic</span> Network and the Eastern Washington Regional Network consist of 44 individual sensor sites and 15 radio relay sites maintained by the Hanford <span class="hlt">Seismic</span> Assessment Team. The Hanford <span class="hlt">Seismic</span> Network <span class="hlt">recorded</span> 90 local earthquakes during the second quarter of FY 2010. Eighty-one of these earthquakes were detected in the vicinity of Wooded Island, located about eight miles north of Richland just west of the Columbia River. The Wooded Island events <span class="hlt">recorded</span> this quarter were a continuation of the swarm events observed during the 2009 and 2010 fiscal years and reported in previous quarterly and annual reports (Rohay et al; 2009a, 2009b, 2009<span class="hlt">c</span>, and 2010). Most of the events were considered minor (coda-length magnitude [Mc] less than 1.0) with only 1 event in the 2.0-3.0 range; the maximum magnitude event (3.0 Mc) occurred February 4, 2010 at depth 2.4 km. The average depth of the Wooded Island events during the quarter was 1.6 km with a maximum depth estimated at 3.5 km. This placed the Wooded Island events within the Columbia River Basalt Group (CRBG). The low magnitude of the Wooded Island events has made them undetectable to all but local area residents. The Hanford Strong Motion Accelerometer (SMA) network was triggered</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFM.C43B0802K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFM.C43B0802K"><span>Towards Quantification of Glacier Dynamic Ice Loss through Passive <span class="hlt">Seismic</span> Monitoring</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Köhler, A.; Nuth, C.; Weidle, C.; Schweitzer, J.; Kohler, J.; Buscaino, G.</p> <p>2015-12-01</p> <p>Global glaciers and ice caps loose mass through calving, while existing models are currently not equipped to realistically predict dynamic ice loss. This is mainly because long-term continuous calving <span class="hlt">records</span>, that would help to better understand fine scale processes and key climatic-dynamic feedbacks between calving, climate, terminus evolution and marine conditions, do not exist. Combined passive <span class="hlt">seismic</span>/acoustic strategies are the only technique able to capture rapid calving events continuously, independent of daylight or meteorological conditions. We have produced such a continuous calving <span class="hlt">record</span> for Kronebreen, a tidewater glacier in Svalbard, using data from permanent <span class="hlt">seismic</span> stations between 2001 and 2014. However, currently no method has been established in cryo-seismology to quantify the calving ice loss directly from <span class="hlt">seismic</span> data. Independent calibration data is required to derive 1) a realistic estimation of the dynamic ice loss unobserved due to <span class="hlt">seismic</span> noise and 2) a robust scaling of <span class="hlt">seismic</span> calving signals to ice volumes. Here, we analyze the <span class="hlt">seismic</span> calving <span class="hlt">record</span> at Kronebreen and independent calving data in a first attempt to quantify ice loss directly from <span class="hlt">seismic</span> <span class="hlt">records</span>. We make use of a) calving flux data with weekly to monthly resolution obtained from satellite remote sensing and GPS data between 2007 and 2013, and b) direct, visual calving observations in two weeks in 2009 and 2010. Furthermore, the magnitude-scaling property of <span class="hlt">seismic</span> calving events is analyzed. We derive and discuss an empirical relation between <span class="hlt">seismic</span> calving events and calving flux which for the first time allows to estimate a time series of calving volumes more than one decade back in time. Improving our model requires to incorporate more precise, high-resolution calibration data. A new field campaign will combine innovative, multi-disciplinary monitoring techniques to measure calving ice volumes and dynamic ice-ocean interactions simultaneously with terrestrial laser</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70026922','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70026922"><span>Paleogeodetic <span class="hlt">records</span> of <span class="hlt">seismic</span> and aseismic subduction from central Sumatran microatolls, Indonesia</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Natawidjaja, D.H.; Sieh, K.; Ward, S.N.; Cheng, H.; Edwards, R. Lawrence; Galetzka, J.; Suwargadi, B.W.</p> <p>2004-01-01</p> <p>We utilize coral microatolls in western Sumatra to document vertical deformation associated with subduction. Microatolls are very sensitive to fluctuations in sea level and thus act as natural tide gauges. They <span class="hlt">record</span> not only the magnitude of vertical deformation associated with earthquakes (paleoseismic data), but also continuously track the long-term aseismic deformation that occurs during the intervals between earthquakes (paleogeodetic data). This paper focuses on the twentieth century paleogeodetic history of the equatorial region. Our coral paleogeodetic <span class="hlt">record</span> of the 1935 event reveals a classical example of deformations produced by <span class="hlt">seismic</span> rupture of a shallow subduction interface. The site closest to the trench rose 90 cm, whereas sites further east sank by as much as 35 cm. Our model reproduces these paleogeodetic data with a 2.3 m slip event on the interface 88 to 125 km from the trench axis. Our coral paleogeodetic data reveal slow submergence during the decades before and after the event in the areas of coseismic emergence. Likewise, interseismic emergence occurred before and after the 1935 event in areas of coseismic submergence. Among the interesting phenomenon we have discovered in the coral <span class="hlt">record</span> is evidence of a large aseismic slip or "silent even" in 1962, 27 years after the 1935 event. Paleogeodetic deformation rates in the decades before, after, and between the 1935 and 1962 events have varied both temporally and spatially. During the 25 years following the 1935 event, submergence rates were dramatically greater than in prior decades. During the past four decades, however, rates have been lower than in the preceding decades, but are still higher than they were prior to 1935. These paleogeodetic <span class="hlt">records</span> enable us to model the kinematics of the subduction interface throughout the twentieth century. Copyright 2004 by the American Geophysical Union.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..19.8048R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..19.8048R"><span>First approximations in avalanche model validations using <span class="hlt">seismic</span> information</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Roig Lafon, Pere; Suriñach, Emma; Bartelt, Perry; Pérez-Guillén, Cristina; Tapia, Mar; Sovilla, Betty</p> <p>2017-04-01</p> <p>Avalanche dynamics modelling is an essential tool for snow hazard management. Scenario based numerical modelling provides quantitative arguments for decision-making. The software tool RAMMS (WSL Institute for Snow and Avalanche Research SLF) is one such tool, often used by government authorities and geotechnical offices. As avalanche models improve, the quality of the numerical results will depend increasingly on user experience on the specification of input (e.g. release and entrainment volumes, secondary releases, snow temperature and quality). New model developments must continue to be validated using real phenomena data, for improving performance and reliability. The avalanches group form University of Barcelona (RISKNAT - UB), has studied the <span class="hlt">seismic</span> signals generated from avalanches since 1994. Presently, the group manages the <span class="hlt">seismic</span> installation at SLF's Vallée de la Sionne experimental site (VDLS). At VDLS the <span class="hlt">recorded</span> <span class="hlt">seismic</span> signals can be correlated to other avalanche measurement techniques, including both advanced remote sensing methods (radars, videogrammetry) and obstacle based sensors (pressure, capacitance, optical sender-reflector barriers). This comparison between different measurement techniques allows the group to address the question if <span class="hlt">seismic</span> analysis can be used alone, on more additional avalanche tracks, to gain insight and validate numerical avalanche dynamics models in different terrain conditions. In this study, we aim to add the <span class="hlt">seismic</span> data as an external <span class="hlt">record</span> of the phenomena, able to validate RAMMS models. The <span class="hlt">seismic</span> sensors are considerable easy and cheaper to install than other physical measuring tools, and are able to <span class="hlt">record</span> data from the phenomena in every atmospheric conditions (e.g. bad weather, low light, freezing make photography, and other kind of sensors not usable). With <span class="hlt">seismic</span> signals, we <span class="hlt">record</span> the temporal evolution of the inner and denser parts of the avalanche. We are able to recognize the approximate position</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2003EAEJA.....8677S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2003EAEJA.....8677S"><span>The underground <span class="hlt">seismic</span> array of Gran Sasso (UNDERSEIS), central Italy</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Scarpa, R.; Muscente, R.; Tronca, F.; Fischione, C.; Rotella, P.; Abril, M.; Alguacil, G.; Martini, M.; de Cesare, W.</p> <p>2003-04-01</p> <p>Since early May, 2002, a small aperture <span class="hlt">seismic</span> array has been installed in the underground Physics Laboratories of Gran Sasso, located near <span class="hlt">seismic</span> active faults of central Apennines, Italy. This array is presently composed by 21 three-component short period <span class="hlt">seismic</span> stations (Mark L4<span class="hlt">C</span>-3D), with average distance 90 m and semi-circular aperture of 400 m x 600 m. It is intersecting a main seismogenic fault where the presence of slow earthquakes has been recently detected through two wide band geodetic laser interferometers. The underground Laboratories are shielded by a limestone rock layer having 1400 m thickness. Each seismometer is linked, through a 24 bits A/D board, to a set of 6 industrial PC via a serial RS-485 standard. The six PC transmit data to a server through an ethernet network. Time syncronization is provided by a Master Oscillator controlled by an atomic clock. Earthworm package is used for data selection and transmission. High quality data have been <span class="hlt">recorded</span> since May 2002, including local and regional earthquakes. In particular the 31 October, 2002, Molise (Mw=5.8 earthquake) and its aftershocks have been <span class="hlt">recorded</span> at this array. Array techniques such as polarisation and frequency-slowness analyses with the MUSIC noise algorithm indicate the high performance of this array, as compared to the national <span class="hlt">seismic</span> network, for identifying the basic source parameters for earthquakes located at distance of few hundreds of km.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.S22B..06H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.S22B..06H"><span>Combined GPS and <span class="hlt">seismic</span> monitoring of a 12-story structure in a region of induced <span class="hlt">seismicity</span> in Oklahoma</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Haase, J. S.; Soliman, M.; Kim, H.; Jaiswal, P.; Saunders, J. K.; Vernon, F.; Zhang, W.</p> <p>2017-12-01</p> <p>This work focuses on quantifying ground motions and their effects in Oklahoma near the location of the 2016 Mw 5.8 Pawnee earthquake, where <span class="hlt">seismicity</span> has been increasing due to wastewater injection related to oil and natural gas production. Much of the building inventory in Oklahoma was constructed before the increase in <span class="hlt">seismicity</span> and before the implementation of earthquake design and detailing provisions for reinforced concrete (RC) structures. We will use combined GPS/<span class="hlt">seismic</span> monitoring techniques to measure ground motion in the field and the response of structures to this ground motion. Several Oklahoma State University buildings experienced damage due to the Pawnee earthquake. The USGS Shake Map product estimated peak ground acceleration (PGA) ranging from 0.12g to 0.15g at campus locations. We are deploying a high-rate GPS sensor and accelerometer on the roof and another accelerometer at ground level of a 12-story RC structure and at selected field sites in order to collect ambient noise data and nearby <span class="hlt">seismicity</span>. The longer period <span class="hlt">recording</span> characteristics of the GPS/<span class="hlt">seismic</span> system are particularly well adapted to monitoring these large structures in the event of a significant earthquake. Gross characteristics of the structural system are described, which consists of RC columns and RC slabs in all stories. We conducted a preliminary structural analysis including modal analysis and response spectrum analysis based on a finite element (FE) simulation, which indicated that the period associated with the first X-axis bending, first torsional, and first Y-axis bending modes are 2.2 s, 2.1 s, and 1.8 s, respectively. Next, a preliminary analysis was conducted to estimate the range of expected deformation at the roof level for various earthquake excitations. The earthquake analysis shows a maximum roof displacement of 5 and 7 cm in the horizontal directions resulting from earthquake loads with PGA of 0.2g, well above the noise level of the combined GPS/<span class="hlt">seismic</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19750030304&hterms=infrasound&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dinfrasound','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19750030304&hterms=infrasound&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dinfrasound"><span>Investigations of acoustic-<span class="hlt">seismic</span> effects at long range - Early-arriving <span class="hlt">seismic</span> waves from Apollo 16</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Dalins, I.; Mccarty, V. M.; Kaschak, G.; Donn, W. L.</p> <p>1974-01-01</p> <p>A reasonably comprehensive technical effort is described dealing with the investigations of acoustically generated <span class="hlt">seismic</span> waves of Apollo 16 and Apollo 17 origin along the eastern seabord of the United States. This expanded effort is a continuation of earlier, rather successful detections of rocket-generated <span class="hlt">seismic</span> disturbances on Skidaway Island, Georgia. The more recent effort has yielded few positive results other than a <span class="hlt">recording</span> of an early-arriving <span class="hlt">seismic</span> wave from Apollo 16 that was detected in Jacksonville. Evaluation of the negative results obtained in the Fort Monmouth area, with earlier studies of infrasound, local weather conditions, and geology, could be advantageous in the process of trying to gain a better insight into the acoustic-<span class="hlt">seismic</span> resonance mechanism requiring phase-velocity matching at the atmosphere-ground interface.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_6");'>6</a></li> <li><a href="#" onclick='return showDiv("page_7");'>7</a></li> <li class="active"><span>8</span></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_8 --> <div id="page_9" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_7");'>7</a></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li class="active"><span>9</span></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="161"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017GeoJI.211.1494O','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017GeoJI.211.1494O"><span>Spectral element modelling of <span class="hlt">seismic</span> wave propagation in visco-elastoplastic media including excess-pore pressure development</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Oral, Elif; Gélis, Céline; Bonilla, Luis Fabián; Delavaud, Elise</p> <p>2017-12-01</p> <p>Numerical modelling of <span class="hlt">seismic</span> wave propagation, considering soil nonlinearity, has become a major topic in <span class="hlt">seismic</span> hazard studies when strong shaking is involved under particular soil conditions. Indeed, when strong ground motion propagates in saturated soils, pore pressure is another important parameter to take into account when successive phases of contractive and dilatant soil behaviour are expected. Here, we model 1-D <span class="hlt">seismic</span> wave propagation in linear and nonlinear media using the spectral element numerical method. The study uses a three-component (3<span class="hlt">C</span>) nonlinear rheology and includes pore-pressure excess. The 1-D-3<span class="hlt">C</span> model is used to study the 1987 Superstition Hills earthquake (ML 6.6), which was <span class="hlt">recorded</span> at the Wildlife Refuge Liquefaction Array, USA. The data of this event present strong soil nonlinearity involving pore-pressure effects. The ground motion is numerically modelled for different assumptions on soil rheology and input motion (1<span class="hlt">C</span> versus 3<span class="hlt">C</span>), using the <span class="hlt">recorded</span> borehole signals as input motion. The computed acceleration-time histories show low-frequency amplification and strong high-frequency damping due to the development of pore pressure in one of the soil layers. Furthermore, the soil is found to be more nonlinear and more dilatant under triaxial loading compared to the classical 1<span class="hlt">C</span> analysis, and significant differences in surface displacements are observed between the 1<span class="hlt">C</span> and 3<span class="hlt">C</span> approaches. This study contributes to identify and understand the dominant phenomena occurring in superficial layers, depending on local soil properties and input motions, conditions relevant for site-specific studies.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFM.S13B2821T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFM.S13B2821T"><span>The Southern Kansas <span class="hlt">Seismic</span> Network</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Terra, F. M.</p> <p>2015-12-01</p> <p>Historically aseismic Harper and Sumner counties in Southern Kansas experienced a dramatic increase in <span class="hlt">seismicity</span> beginning in early 2014, coincident with the development of new oil production in the Mississippi Lime Play. In order to better understand the potential relationships between <span class="hlt">seismicity</span> and oil development, the USGS installed a real-time telemetered <span class="hlt">seismic</span> network in cooperation with the Kansas Geological Survey, the Kansas Corporation Commission, the Kansas Department of Health and Environment, Harper County, and the Oklahoma Geological Survey. The network began operation in March 2014 with an initial deployment of 5 NetQuakes accelerometers and by July 2014 had expanded to include 10 broadband sites. The network currently has 14 stations, all with accelerometers and 12 with broadband seismometers. The network has interstation spacing of 15 - 25 km and typical azimuthal gap of 80 for well-located events. Data are continuously streamed to IRIS at 200 samples per second from most sites. Earthquake locations are augmented with additional stations from the USGS National Network, Oklahoma Geological Survey <span class="hlt">Seismic</span> Network, Kansas <span class="hlt">Seismic</span> Monitoring Network and the Enid Oklahoma Network. Since the spring of 2014 over 7500 earthquakes have been identified with data from this network, 1400 of which have been manually timed and cataloged. Focal depths for earthquakes typically range between 2 and 7 km. The catalog is available at earthquake.usgs.gov/earthquakes/search/ under network code 'Ismpkansas'. The network <span class="hlt">recorded</span> the largest known earthquake in Harper County, Mw 4.3, on October 2, 2014 and in Sumner County, Mw 4.9, on November 12, 2014. <span class="hlt">Recorded</span> ground motions at the epicenter of the October earthquake were 0.70 g (PGA) and 12 cm/s (PGV). These high ground motion values agree with near-source <span class="hlt">recordings</span> made by other USGS temporary deployments in the U. S. midcontinent, indicating a significant shaking hazard from such shallow, moderate</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.S23C0826D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.S23C0826D"><span><span class="hlt">Seismicity</span> in Oklahoma Before Prague</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Delorey, A. A.; Johnson, P. A.</p> <p>2017-12-01</p> <p>The 2011 M5.7 Prague earthquake was the first large anthropogenically induced earthquake in Oklahoma. Since then, three more M5+ earthquakes followed it near Fairview, Pawnee, and Cushing. Oklahoma induced <span class="hlt">seismicity</span> has garnered a lot of attention from both the media and the scientific community. But, little is known about <span class="hlt">seismicity</span> in Oklahoma prior to the Prague earthquake due to a lack of instrumentation. We ask the question, "Was there any indication in the geophysical <span class="hlt">record</span> prior to the Prague earthquake that bigger earthquakes were becoming more likely?" Fortunately, stations from Earthscope's Transportable Array were in Oklahoma during 2010 and 2011 providing a sparse, but still useful data set. Using our microseismicity detector called Interstation <span class="hlt">Seismic</span> Coherence, we were able to catalog over 3000 earthquakes with a magnitude of completeness around 2.0 in northeastern Oklahoma over 17 months between June 2010 and the Prague earthquake in November 2011. During this period of time there are less than 200 earthquakes in the ANSS Comprehensive Catalog and 900 in the catalog produced by the Array Network Facility at the UCSD using Transportable Array stations. The M>5 earthquakes occurred in a region where stress conditions and <span class="hlt">seismicity</span> rates were evolving much faster than they do in many natural systems presenting an opportunity to study the time dependence of upper crustal behavior. A clustering analysis shows that earthquakes occurring in northeastern Oklahoma during 2010-2011 are highly correlated with the magnitude of solid earth tides. Although some aftershocks and clusters were <span class="hlt">recorded</span> following the Prague earthquake using temporary arrays, regional <span class="hlt">seismicity</span> is not well <span class="hlt">recorded</span> again until later in 2013. Of note, after 2013, we no longer observe tidal correlation suggesting the ensemble of fault criticality has evolved. One explanation for this change in earthquake behavior is a change in poroelastic conditions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70016945','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70016945"><span><span class="hlt">Seismic</span> excitation by the space shuttle Columbia</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Kanamori, H.; Mori, J.; Anderson, D.L.; Heaton, T.H.</p> <p>1991-01-01</p> <p><span class="hlt">SEISMIC</span> stations in southern California <span class="hlt">recorded</span> the atmospheric shock waves generated by the space shuttle Columbia on its return to the Edwards Air Force base on 13 August 1989 (Fig. 1). In addition to the shock wave, the broad-band IRIS-TERRAscope station at Pasadena <span class="hlt">recorded</span> a distinct pulse with a period of ???2-3 seconds, which arrived 12.5 seconds before the shock wave (Fig. 2). This pulse was also <span class="hlt">recorded</span> at the University of Southern California, near downtown Los Angeles, where it arrived 3 seconds after the shock wave. The origin of this pulse could not be readily identified. We show here that it was a <span class="hlt">seismic</span> P wave excited by the motion of high-rise buildings in downtown Los Angeles, which were hit by the shock wave. The proximity of the natural period of the high-rise buildings to that of the Los Angeles basin enabled efficient energy transfer from shock wave to <span class="hlt">seismic</span> wave.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008AGUFM.S41C1865C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008AGUFM.S41C1865C"><span><span class="hlt">Seismic</span> moment tensor for anisotropic media: implication for Non-double-couple earthquakes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Cai, X.; Chen, X.; Chen, Y.; Cai, M.</p> <p>2008-12-01</p> <p>It is often found that the inversion results of <span class="hlt">seismic</span> moment tensor from real <span class="hlt">seismic</span> <span class="hlt">recorded</span> data show the trace of <span class="hlt">seismic</span> moment tensor M is not zero, a phenomenon called non-double-couple earthquake sources mechanism. Recently we have derived the analytical expressions of M in transversely isotropic media with the titled axis of symmetry and the results shows even only pure shear-motion of fault can lead to the implosive components determined by several combined anisotropic elastic constants. Many non-double-couple earthquakes from observations often appear in volcanic and geothermal areas (Julian, 1998), where there exist a mount of stress-aligned fluid-saturated parallel vertical micro-cracks identical to transversely isotropic media (Crampin, 2008), this stress-aligned crack will modify the <span class="hlt">seismic</span> moment tensor. In another word, non-double-couple earthquakes don't mean to have a <span class="hlt">seismic</span> failure movement perpendicular to the fault plane, while traditional research of <span class="hlt">seismic</span> moment tensor focus on the case of isotropy, which cannot provide correct interpretation of <span class="hlt">seismic</span> source mechanism. Reference: Julian, B.R., Miller, A.D. and Foulger, G.R., 1998. Non-double-couple earthquakes,1. Theory, Rev. Geophys., 36, 525¨<span class="hlt">C</span>549. Crampin,S., Peacock,S., 2008, A review of the current understanding of <span class="hlt">seismic</span> shear-wave splitting in the Earth's crust and common fallacies in interpretation, wave motion, 45,675-722</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70010139','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70010139"><span>Missile impacts as sources of <span class="hlt">seismic</span> energy on the moon</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Latham, G.V.; McDonald, W.G.; Moore, H.J.</p> <p>1970-01-01</p> <p><span class="hlt">Seismic</span> signals <span class="hlt">recorded</span> from impacts of missiles at the White Sands Missile Range are radically different from the signal <span class="hlt">recorded</span> from the Apollo 12 lunar module impact. This implies that lunar structure to depths of at least 10 to 20 kilometers is quite different from the typical structure of the earth's crust. Results obtained from this study can be used to predict <span class="hlt">seismic</span> wave amplitudes from future man-made lunar impacts. <span class="hlt">Seismic</span> energy and crater dimensions from impacts are compared with measurements from chemical explosions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.S42B..06H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.S42B..06H"><span>Investigating subduction reversal in Papua New Guinea from automatic analysis of <span class="hlt">seismicity</span> <span class="hlt">recorded</span> on a temporary local network</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hicks, S. P.; Harmon, N.; Rychert, C.; Tharimena, S.; Bogiatzis, P.; Savage, B.; Shen, Y.; Baillard, C.</p> <p>2017-12-01</p> <p>The area of Papua New Guinea is one of the most <span class="hlt">seismically</span> active regions on the planet. <span class="hlt">Seismicity</span> in the region results from oblique convergence between the Pacific and India-Australia plates, with deformation occurring across a broad region involving several microplates. The region gives an excellent natural laboratory to test geodynamic models of subduction polarity reversal, microplate interaction, and to delineate the structure of subducting plates and relic structures at depth. However, a lack of permanent <span class="hlt">seismic</span> stations means that routine earthquake locations for small to intermediate sized earthquakes have significant location errors. In 2014, we deployed a temporary network of eight broadband stations on islands in eastern Papua New Guinea to <span class="hlt">record</span> ongoing <span class="hlt">seismic</span> deformation. The network straddles a complex region where subduction of the Solomon plate occurs to the south and possible subduction of the Ontong-Java plateau occurs to the north. The stations were installed for 27 months. During the deployment period, there were 13 M>6.5 earthquakes in the area, including M7.5 doublet events in 2015, giving a rich <span class="hlt">seismic</span> dataset. A high-quality catalogue of local events was formed by a multi-step process. Using the scanloc module of SeisComp3, we first detect P-onsets using a STA/LTA detection. Once clusters of P onsets are found, S-wave picks are incorporated based on a pre-defined window length of maximum S-P time. Groups of onsets are then associated to events, giving us a starting catalogue of 269 events (1765 P-onsets) with minimum magnitude of M 3.5. In a second step, we refine onset times using a Kurtosis picker to improve location accuracy. To form robust hypocentral locations using an appropriate structural model for the area and to constrain crust and mantle structure in the region, we derive a minimum 1-D velocity model using the VELEST program. We use a starting model from Abers et al. (1991) and we restrict our catalogue to events with an</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.S42B..06H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.S42B..06H"><span>Investigating subduction reversal in Papua New Guinea from automatic analysis of <span class="hlt">seismicity</span> <span class="hlt">recorded</span> on a temporary local network</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hicks, S. P.; Harmon, N.; Rychert, C.; Tharimena, S.; Bogiatzis, P.; Savage, B.; Shen, Y.; Baillard, C.</p> <p>2016-12-01</p> <p>The area of Papua New Guinea is one of the most <span class="hlt">seismically</span> active regions on the planet. <span class="hlt">Seismicity</span> in the region results from oblique convergence between the Pacific and India-Australia plates, with deformation occurring across a broad region involving several microplates. The region gives an excellent natural laboratory to test geodynamic models of subduction polarity reversal, microplate interaction, and to delineate the structure of subducting plates and relic structures at depth. However, a lack of permanent <span class="hlt">seismic</span> stations means that routine earthquake locations for small to intermediate sized earthquakes have significant location errors. In 2014, we deployed a temporary network of eight broadband stations on islands in eastern Papua New Guinea to <span class="hlt">record</span> ongoing <span class="hlt">seismic</span> deformation. The network straddles a complex region where subduction of the Solomon plate occurs to the south and possible subduction of the Ontong-Java plateau occurs to the north. The stations were installed for 27 months. During the deployment period, there were 13 M>6.5 earthquakes in the area, including M7.5 doublet events in 2015, giving a rich <span class="hlt">seismic</span> dataset. A high-quality catalogue of local events was formed by a multi-step process. Using the scanloc module of SeisComp3, we first detect P-onsets using a STA/LTA detection. Once clusters of P onsets are found, S-wave picks are incorporated based on a pre-defined window length of maximum S-P time. Groups of onsets are then associated to events, giving us a starting catalogue of 269 events (1765 P-onsets) with minimum magnitude of M 3.5. In a second step, we refine onset times using a Kurtosis picker to improve location accuracy. To form robust hypocentral locations using an appropriate structural model for the area and to constrain crust and mantle structure in the region, we derive a minimum 1-D velocity model using the VELEST program. We use a starting model from Abers et al. (1991) and we restrict our catalogue to events with an</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/940860','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/940860"><span>Berkeley Seismological Laboratory <span class="hlt">Seismic</span> Moment Tensor Report for the August 6, 2007 M3.9 <span class="hlt">Seismic</span> event in central Utah</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Ford, S; Dreger, D; Hellweg, P</p> <p>2007-08-08</p> <p>We have performed a complete moment tensor analysis of the <span class="hlt">seismic</span> event, which occurred on Monday August 6, 2007 at 08:48:40 UTC 21 km from Mt.Pleasant, Utah. In our analysis we utilized complete three-component <span class="hlt">seismic</span> <span class="hlt">records</span> <span class="hlt">recorded</span> by the USArray, University of Utah, and EarthScope <span class="hlt">seismic</span> arrays. The <span class="hlt">seismic</span> waveform data was integrated to displacement and filtered between 0.02 to 0.10 Hz following instrument removal. We used the Song et al. (1996) velocity model to compute Green's functions used in the moment tensor inversion. A map of the stations we used and the location of the event is shown inmore » Figure 1. In our moment tensor analysis we assumed a shallow source depth of 1 km consistent with the shallow depth reported for this event. As shown in Figure 2 the results point to a source mechanism with negligible double-couple radiation and is composed of dominant CLVD and implosive isotropic components. The total scalar <span class="hlt">seismic</span> moment is 2.12e22 dyne cm corresponding to a moment magnitude (Mw) of 4.2. The long-period <span class="hlt">records</span> are very well matched by the model (Figure 2) with a variance reduction of 73.4%. An all dilational (down) first motion radiation pattern is predicted by the moment tensor solution, and observations of first motions are in agreement.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017E%26ES...62a2048T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017E%26ES...62a2048T"><span>Full Waveform Modelling for Subsurface Characterization with Converted-Wave <span class="hlt">Seismic</span> Reflection</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Triyoso, Wahyu; Oktariena, Madaniya; Sinaga, Edycakra; Syaifuddin, Firman</p> <p>2017-04-01</p> <p>While a large number of reservoirs have been explored using P-waves <span class="hlt">seismic</span> data, P-wave <span class="hlt">seismic</span> survey ceases to provide adequate result in <span class="hlt">seismically</span> and geologically challenging areas, like gas cloud, shallow drilling hazards, strong multiples, highly fractured, anisotropy. Most of these reservoir problems can be addressed using P and PS <span class="hlt">seismic</span> data combination. Multicomponent <span class="hlt">seismic</span> survey <span class="hlt">records</span> both P-wave and S-wave unlike conventional survey that only <span class="hlt">records</span> compressional P-wave. Under certain conditions, conventional energy source can be used to <span class="hlt">record</span> P and PS data using the fact that compressional wave energy partly converts into shear waves at the reflector. Shear component can be <span class="hlt">recorded</span> using down going P-wave and upcoming S-wave by placing a horizontal component geophone on the ocean floor. A synthetic model is created based on real data to analyze the effect of gas cloud existence to PP and PS wave reflections which has a similar characteristic to Sub-Volcanic imaging. The challenge within the multicomponent <span class="hlt">seismic</span> is the different travel time between P-wave and S-wave, therefore the converted-wave <span class="hlt">seismic</span> data should be processed with different approach. This research will provide a method to determine an optimum converted point known as Common Conversion Point (CCP) that can solve the Asymmetrical Conversion Point of PS data. The value of γ (Vp/Vs) is essential to estimate the right CCP that will be used in converted-wave <span class="hlt">seismic</span> processing. This research will also continue to the advanced processing method of converted-wave <span class="hlt">seismic</span> by applying Joint Inversion to PP&PS <span class="hlt">seismic</span>. Joint Inversion is a simultaneous model-based inversion that estimates the P&S-wave impedance which are consistent with the PP&PS amplitude data. The result reveals a more complex structure mirrored in PS data below the gas cloud area. Through estimated γ section resulted from Joint Inversion, we receive a better imaging improvement below gas cloud area tribute to</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/4783796-site-cavity-location-seismic-profiling-nevada-test-site','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/4783796-site-cavity-location-seismic-profiling-nevada-test-site"><span>ON-SITE CAVITY LOCATION-<span class="hlt">SEISMIC</span> PROFILING AT NEVADA TEST SITE</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Forbes, C.B.; Peterson, R.A.; Heald, C.L.</p> <p>1961-10-25</p> <p>Experimental <span class="hlt">seismic</span> studies were conducted at the Nevada Test Site for the purpose of designing and evaluating the most promising <span class="hlt">seismic</span> techniques for on-site inspection. Post-explosion <span class="hlt">seismic</span> profiling was done in volcanic tuff in the vicinity of the Rainier and Blanca underground explosions. Pre-explosion <span class="hlt">seismic</span> profiling was done over granitic rock outcrops in the Climax Stock area, and over tuff at proposed location for Linen and Orchid. Near surface velocity profiling techniques based on measurements of <span class="hlt">seismic</span> time-distance curves gave evidence of disturbances in near surface rock velocities over the Rainier and Refer als0 to abstract 30187. Blanca sites. Thesemore » disturbances appear to be related to near surface fracturing and spallation effects resulting from the reflection of the original intense compression wave pulse at the near surface as a tension pulse. Large tuned seismometer arrays were used for horizontal <span class="hlt">seismic</span> ranging in an attempt to <span class="hlt">record</span> back-scattered'' or reflected <span class="hlt">seismic</span> waves from subsurface cavities or zones of rock fracturing around the underground explosions. Some possible <span class="hlt">seismic</span> events were <span class="hlt">recorded</span> from the near vicinities of the Rainier and Blanca sites. However, many more similar events were <span class="hlt">recorded</span> from numerous other locations, presumably originating from naturally occurring underground geological features. No means was found for discriminating between artificial and natural events <span class="hlt">recorded</span> by horizontal <span class="hlt">seismic</span> ranging, and the results were, therefore, not immediately useful for inspection purposes. It is concluded that in some instances near surface velocity profiling methods may provide a useful tool in verifying the presence of spalled zones above underground nuclear explosion sites. In the case of horizontal <span class="hlt">seismic</span> ranging it appears that successful application would require development of satisfactory means for recognition of and discrimination against <span class="hlt">seismic</span> responses to naturally occurring geological</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014GeoJI.197.1608J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014GeoJI.197.1608J"><span>Microearthquake mechanism from wave amplitudes <span class="hlt">recorded</span> by a close-to-surface <span class="hlt">seismic</span> array at Ocnele Mari, Romania</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jechumtálová, Z.; Šílený, J.; Trifu, C.-I.</p> <p>2014-06-01</p> <p>The resolution of event mechanism is investigated in terms of the unconstrained moment tensor (MT) source model and the shear-tensile crack (STC) source model representing a slip along the fault with an off-plane component. Data are simulated as <span class="hlt">recorded</span> by the actual <span class="hlt">seismic</span> array installed at Ocnele Mari (Romania), where sensors are placed in shallow boreholes. Noise is included as superimposed on synthetic data, and the analysis explores how the results are influenced (i) by data <span class="hlt">recorded</span> by the complete <span class="hlt">seismic</span> array compared to that provided by the subarray of surface sensors, (ii) by using three- or one-component sensors and (iii) by inverting P- and S-wave amplitudes versus P-wave amplitudes only. The orientation of the pure shear fracture component is resolved almost always well. On the other hand, the noise increase distorts the non-double-couple components (non-DC) of the MT unless a high-quality data set is available. The STC source model yields considerably less spurious non-shear fracture components. Incorporating <span class="hlt">recordings</span> at deeper sensors in addition to those obtained from the surface ones allows for the processing of noisier data. Performance of the network equipped with three-component sensors is only slightly better than that with uniaxial sensors. Inverting both P- and S-wave amplitudes compared to the inversion of P-wave amplitudes only markedly improves the resolution of the orientation of the source mechanism. Comparison of the inversion results for the two alternative source models permits the assessment of the reliability of non-shear components retrieved. As example, the approach is investigated on three microseismic events occurred at Ocnele Mari, where both large and small non-DC components were found. The analysis confirms a tensile fracturing for two of these events, and a shear slip for the third.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014GeoRL..41.8775P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014GeoRL..41.8775P"><span><span class="hlt">Seismic</span> anisotropy and slab dynamics from SKS splitting <span class="hlt">recorded</span> in Colombia</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Porritt, Robert W.; Becker, Thorsten W.; Monsalve, Gaspar</p> <p>2014-12-01</p> <p>The Nazca, Caribbean, and South America plates meet in northwestern South America where the northern end of the Andean volcanic arc and Wadati-Benioff zone <span class="hlt">seismicity</span> indicate ongoing subduction. However, the termination of Quaternary volcanism at ~5.5°N and eastward offset in <span class="hlt">seismicity</span> underneath Colombia suggest the presence of complex slab geometry. To help link geometry to dynamics, we analyze SKS splitting for 38 broadband stations of the Colombian national network. Measurements of fast polarization axes in western Colombia close to the trench show dominantly trench-perpendicular orientations. Orientations measured at stations in the back arc, farther to the east, however, abruptly change to roughly trench parallel anisotropy. This may indicate along-arc mantle flow, possibly related to the suggested "Caldas" slab tear, or a lithospheric signature, but smaller-scale variations in anisotropy remain to be explained. Our observations are atypical globally and challenge our understanding of the complexities of subduction zone <span class="hlt">seismic</span> anisotropy.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMNH41B1795H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMNH41B1795H"><span>Dynamics of the Wulong Landslide Revealed by Broadband <span class="hlt">Seismic</span> <span class="hlt">Records</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Huang, X.; Dan, Y.</p> <p>2016-12-01</p> <p>Long-period <span class="hlt">seismic</span> signals are frequently used to trace the dynamic process of large scale landslides. The catastrophic WuLong landslide occurred at 14:51 on 5 June 2009 (Beijing time, UTC+8) in Wulong Prefecture, Southwest China. The topography in landslide area varies dramatically, enhancing the complexity in its movement characteristics. The mass started sliding northward on the upper part of the cliff located upon the west slope of the Tiejianggou gully, and shifted its movement direction to northeastward after being blocked by stable bedrock in front, leaving a scratch zone. The sliding mass then moved downward along the west slope of the gully until it collided with the east slope, and broke up into small pieces after the collision, forming a debris flow along the gully. We use long-period <span class="hlt">seismic</span> signals extracted from eight broadband <span class="hlt">seismic</span> stations within 250 km of the landslide to estimate its source time functions. Combining with topographic surveys done before and after the event, we can also resolve kinematic parameters of sliding mass, i.e. velocities, displacements and trajectories, perfectly characterizing its movement features. The runout trajectory deduced from source time functions is consistent with the sliding path, including two direction changing processes, corresponding to scratching the western bedrock and collision with the east slope respectively. Topographic variations can be reflected from estimated velocities. The maximum velocity of the sliding mass reaches 35 m/s before the collision with the east slope of the Tiejianggou gully, resulting from the height difference between the source zone and the deposition zone. What is important is that dynamics of scratching and collision can be characterized by source time functions. Our results confirm that long-period <span class="hlt">seismic</span> signals are sufficient to characterize dynamics and kinematics of large scale landslides which occur in a region with complex topography.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EGUGA..18.4020S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EGUGA..18.4020S"><span>First <span class="hlt">seismic</span> shear wave velocity profile of the lunar crust as extracted from the Apollo 17 active <span class="hlt">seismic</span> data by wavefield gradient analysis</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sollberger, David; Schmelzbach, Cedric; Robertsson, Johan O. A.; Greenhalgh, Stewart A.; Nakamura, Yosio; Khan, Amir</p> <p>2016-04-01</p> <p>We present a new <span class="hlt">seismic</span> velocity model of the shallow lunar crust, including, for the first time, shear wave velocity information. So far, the shear wave velocity structure of the lunar near-surface was effectively unconstrained due to the complexity of lunar seismograms. Intense scattering and low attenuation in the lunar crust lead to characteristic long-duration reverberations on the seismograms. The reverberations obscure later arriving shear waves and mode conversions, rendering them impossible to identify and analyze. Additionally, only vertical component data were <span class="hlt">recorded</span> during the Apollo active <span class="hlt">seismic</span> experiments, which further compromises the identification of shear waves. We applied a novel processing and analysis technique to the data of the Apollo 17 lunar <span class="hlt">seismic</span> profiling experiment (LSPE), which involved <span class="hlt">recording</span> <span class="hlt">seismic</span> energy generated by several explosive packages on a small areal array of four vertical component geophones. Our approach is based on the analysis of the spatial gradients of the <span class="hlt">seismic</span> wavefield and yields key parameters such as apparent phase velocity and rotational ground motion as a function of time (depth), which cannot be obtained through conventional <span class="hlt">seismic</span> data analysis. These new observables significantly enhance the data for interpretation of the <span class="hlt">recorded</span> <span class="hlt">seismic</span> wavefield and allow, for example, for the identification of S wave arrivals based on their lower apparent phase velocities and distinct higher amount of generated rotational motion relative to compressional (P-) waves. Using our methodology, we successfully identified pure-mode and mode-converted refracted shear wave arrivals in the complex LSPE data and derived a P- and S-wave velocity model of the shallow lunar crust at the Apollo 17 landing site. The extracted elastic-parameter model supports the current understanding of the lunar near-surface structure, suggesting a thin layer of low-velocity lunar regolith overlying a heavily fractured crust of basaltic</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.S51A2741H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.S51A2741H"><span><span class="hlt">Seismic</span> Yield Estimates of UTTR Surface Explosions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hayward, C.; Park, J.; Stump, B. W.</p> <p>2016-12-01</p> <p>Since 2007 the Utah Test and Training Range (UTTR) has used explosive demolition as a method to destroy excess solid rocket motors ranging in size from 19 tons to less than 2 tons. From 2007 to 2014, 20 high quality <span class="hlt">seismic</span> stations within 180 km <span class="hlt">recorded</span> most of the more than 200 demolitions. This provides an interesting dataset to examine <span class="hlt">seismic</span> source scaling for surface explosions. Based upon observer <span class="hlt">records</span>, shots were of 4 sizes, corresponding to the size of the rocket motors. Instrument corrections for the stations were quality controlled by examining the P-wave amplitudes of all magnitude 6.5-8 earthquakes from 30 to 90 degrees away. For each station <span class="hlt">recording</span>, the instrument corrected RMS <span class="hlt">seismic</span> amplitude in the first 10 seconds after the P-onset was calculated. Waveforms at any given station for all the observed explosions are nearly identical. The observed RMS amplitudes were fit to a model including a term for combined distance and station correction, a term for observed RMS amplitude, and an error term for the actual demolition size. The observed <span class="hlt">seismic</span> yield relationship is RMS=k*Weight2/3 . Estimated yields for the largest shots vary by about 50% from the stated weights, with a nearly normal distribution.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://archives.datapages.com/data/circ_pac/6/17_b.htm','USGSPUBS'); return false;" href="http://archives.datapages.com/data/circ_pac/6/17_b.htm"><span><span class="hlt">Recording</span> and processing procedures for multi-channel <span class="hlt">seismic</span>-reflection data collected in the western Ross Sea, Antarctica</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Dadisman, Shawn V.; Ryan, Holly F.; Mann, Dennis M.</p> <p>1987-01-01</p> <p>During 1984, over 2300 km of multichannel <span class="hlt">seismic</span>-reflection data were <span class="hlt">recorded</span> by the U.S. Geological Survey in the western Ross Sea and Iselin Bank regions.  A temporary loss and sinking of the streamer led to increasing the streamer tow depth to 20 m, which resulted in some attenuation of frequencies in the 30-50 Hz range but no significant difference in resolution of the stacked data.  Severe water bottom multiples were encountered and removed by dip-filtering, weighted stacking, and severe post-NMO muting.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015E%26PSL.429..122L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015E%26PSL.429..122L"><span>Landslide <span class="hlt">seismic</span> magnitude</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lin, C. H.; Jan, J. C.; Pu, H. C.; Tu, Y.; Chen, C. C.; Wu, Y. M.</p> <p>2015-11-01</p> <p>Landslides have become one of the most deadly natural disasters on earth, not only due to a significant increase in extreme climate change caused by global warming, but also rapid economic development in topographic relief areas. How to detect landslides using a real-time system has become an important question for reducing possible landslide impacts on human society. However, traditional detection of landslides, either through direct surveys in the field or remote sensing images obtained via aircraft or satellites, is highly time consuming. Here we analyze very long period <span class="hlt">seismic</span> signals (20-50 s) generated by large landslides such as Typhoon Morakot, which passed though Taiwan in August 2009. In addition to successfully locating 109 large landslides, we define landslide <span class="hlt">seismic</span> magnitude based on an empirical formula: Lm = log ⁡ (A) + 0.55 log ⁡ (Δ) + 2.44, where A is the maximum displacement (μm) <span class="hlt">recorded</span> at one <span class="hlt">seismic</span> station and Δ is its distance (km) from the landslide. We conclude that both the location and <span class="hlt">seismic</span> magnitude of large landslides can be rapidly estimated from broadband <span class="hlt">seismic</span> networks for both academic and applied purposes, similar to earthquake monitoring. We suggest a real-time algorithm be set up for routine monitoring of landslides in places where they pose a frequent threat.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010AGUFM.S51D..01H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010AGUFM.S51D..01H"><span>Studies of infrasound propagation using the USArray <span class="hlt">seismic</span> network (Invited)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hedlin, M. A.; Degroot-Hedlin, C. D.; Walker, K. T.</p> <p>2010-12-01</p> <p>Although there are currently ~ 100 infrasound arrays worldwide, more than ever before, the station density is still insufficient to provide validation for detailed propagation modeling. Much structure in the atmosphere is short-lived and occurs at spatial scales much smaller than the average distance between infrasound stations. Relatively large infrasound signals can be observed on <span class="hlt">seismic</span> channels due to coupling at the Earth's surface. Recent research, using data from the 70-km spaced 400-station USArray and other <span class="hlt">seismic</span> network deployments, has shown the value of dense <span class="hlt">seismic</span> network data for filling in the gaps between infrasound arrays. The dense sampling of the infrasound wavefield has allowed us to observe complete travel-time branches of infrasound signals and shed more light on the nature of infrasound propagation. We present early results from our studies of impulsive atmospheric sources, such as series of UTTR rocket motor detonations in Utah. The Utah blasts have been well <span class="hlt">recorded</span> by USArray <span class="hlt">seismic</span> stations and infrasound arrays in Nevada and Washington State. <span class="hlt">Recordings</span> of <span class="hlt">seismic</span> signals from a series of six events in 2007 are used to pinpoint the shot times to < 1 second. Variations in the acoustic branches and signal arrival times at the arrays are used to probe variations in atmospheric structure. Although we currently use coupled signals we anticipate studying dense acoustic network <span class="hlt">recordings</span> as the USArray is currently being upgraded with infrasound microphones. These new sensors will allow us to make semi-continental scale network <span class="hlt">recordings</span> of infrasound signals free of concerns about how the signals observed on <span class="hlt">seismic</span> channels were modified when being coupled to <span class="hlt">seismic</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1431874-depth-discrimination-using-rg-sg-spectral-amplitude-ratios-seismic-events-utah-recorded-local-distances','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1431874-depth-discrimination-using-rg-sg-spectral-amplitude-ratios-seismic-events-utah-recorded-local-distances"><span>Depth Discrimination Using Rg-to-Sg Spectral Amplitude Ratios for <span class="hlt">Seismic</span> Events in Utah <span class="hlt">Recorded</span> at Local Distances</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Tibi, Rigobert; Koper, Keith D.; Pankow, Kristine L.; ...</p> <p>2018-03-20</p> <p>Most of the commonly used <span class="hlt">seismic</span> discrimination approaches are designed for regional data. Relatively little attention has focused on discriminants for local distances (< 200 km), the range at which the smallest events are <span class="hlt">recorded</span>. We take advantage of the variety of <span class="hlt">seismic</span> sources and the existence of a dense regional <span class="hlt">seismic</span> network in the Utah region to evaluate amplitude ratio <span class="hlt">seismic</span> discrimination at local distances. First, we explored phase-amplitude Pg-to-Sg ratios for multiple frequency bands to classify events in a dataset that comprises populations of single-shot surface explosions, shallow and deep ripple-fired mining blasts, mining-induced events, and tectonic earthquakes.more » We achieved a limited success. Then, for the same dataset, we combined the Pg-to-Sg phase-amplitude ratios with Sg-to-Rg spectral amplitude ratios in a multivariate quadratic discriminant function (QDF) approach. For two-category, pairwise classification, seven out of ten population pairs show misclassification rates of about 20% or less, with five pairs showing rates of about 10% or less. The approach performs best for the pair involving the populations of single-shot explosions and mining-induced events. By combining both Pg-to-Sg and Rg-to-Sg ratios in the multivariate QDFs, we are able to achieve an average improvement of about 4–14% in misclassification rates compared to Pg-to-Sg ratios alone. When all five event populations are considered simultaneously, as expected, the potential for misclassification increases and our QDF approach using both Pg-to-Sg and Rg-to-Sg ratios achieves an average success rate of about 74%, compared to the rate of about 86% for two-category, pairwise classification.« less</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_7");'>7</a></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li class="active"><span>9</span></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_9 --> <div id="page_10" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li class="active"><span>10</span></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="181"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1431874-depth-discrimination-using-rg-sg-spectral-amplitude-ratios-seismic-events-utah-recorded-local-distances','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1431874-depth-discrimination-using-rg-sg-spectral-amplitude-ratios-seismic-events-utah-recorded-local-distances"><span>Depth Discrimination Using Rg-to-Sg Spectral Amplitude Ratios for <span class="hlt">Seismic</span> Events in Utah <span class="hlt">Recorded</span> at Local Distances</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Tibi, Rigobert; Koper, Keith D.; Pankow, Kristine L.</p> <p></p> <p>Most of the commonly used <span class="hlt">seismic</span> discrimination approaches are designed for regional data. Relatively little attention has focused on discriminants for local distances (< 200 km), the range at which the smallest events are <span class="hlt">recorded</span>. We take advantage of the variety of <span class="hlt">seismic</span> sources and the existence of a dense regional <span class="hlt">seismic</span> network in the Utah region to evaluate amplitude ratio <span class="hlt">seismic</span> discrimination at local distances. First, we explored phase-amplitude Pg-to-Sg ratios for multiple frequency bands to classify events in a dataset that comprises populations of single-shot surface explosions, shallow and deep ripple-fired mining blasts, mining-induced events, and tectonic earthquakes.more » We achieved a limited success. Then, for the same dataset, we combined the Pg-to-Sg phase-amplitude ratios with Sg-to-Rg spectral amplitude ratios in a multivariate quadratic discriminant function (QDF) approach. For two-category, pairwise classification, seven out of ten population pairs show misclassification rates of about 20% or less, with five pairs showing rates of about 10% or less. The approach performs best for the pair involving the populations of single-shot explosions and mining-induced events. By combining both Pg-to-Sg and Rg-to-Sg ratios in the multivariate QDFs, we are able to achieve an average improvement of about 4–14% in misclassification rates compared to Pg-to-Sg ratios alone. When all five event populations are considered simultaneously, as expected, the potential for misclassification increases and our QDF approach using both Pg-to-Sg and Rg-to-Sg ratios achieves an average success rate of about 74%, compared to the rate of about 86% for two-category, pairwise classification.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017ExG....48..272E','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017ExG....48..272E"><span>New comprehensive standard <span class="hlt">seismic</span> noise models and 3D <span class="hlt">seismic</span> noise variation for Morocco territory, North Africa, obtained using <span class="hlt">seismic</span> broadband stations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>El Fellah, Younes; El-Aal, Abd El-Aziz Khairy Abd; Harnafi, Mimoun; Villaseñor, Antonio</p> <p>2017-05-01</p> <p>In the current work, we constructed new comprehensive standard <span class="hlt">seismic</span> noise models and 3D temporal-spatial <span class="hlt">seismic</span> noise level cubes for Morocco in north-west Africa to be used for seismological and engineering purposes. Indeed, the original global standard <span class="hlt">seismic</span> noise models published by Peterson (1993) and their following updates by Astiz and Creager (1995), Ekström (2001) and Berger et al. (2003) had no contributing <span class="hlt">seismic</span> stations deployed in North Africa. Consequently, this preliminary study was conducted to shed light on <span class="hlt">seismic</span> noise levels specific to north-west Africa. For this purpose, 23 broadband <span class="hlt">seismic</span> stations recently installed in different structural domains throughout Morocco are used to study the nature and characteristics of <span class="hlt">seismic</span> noise and to create <span class="hlt">seismic</span> noise models for Morocco. Continuous data <span class="hlt">recorded</span> during 2009, 2010 and 2011 were processed and analysed to construct these new noise models and 3D noise levels from all stations. We compared the Peterson new high-noise model (NHNM) and low-noise model (NLNM) with the Moroccan high-noise model (MHNM) and low-noise model (MLNM). These new noise models are comparable to the United States Geological Survey (USGS) models in the short period band; however, in the period range 1.2 s to 1000 s for MLNM and 10 s to 1000 s for MHNM display significant variations. This variation is attributed to differences in the nature of <span class="hlt">seismic</span> noise sources that dominate Morocco in these period bands. The results of this study have a new perception about permanent <span class="hlt">seismic</span> noise models for this spectacular region and can be considered a significant contribution because it supplements the Peterson models and can also be used to site future permanent <span class="hlt">seismic</span> stations in Morocco.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007AGUFM.U23C1447W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007AGUFM.U23C1447W"><span>Back to the Future: Long-Term <span class="hlt">Seismic</span> Archives Revisited</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Waldhauser, F.; Schaff, D. P.</p> <p>2007-12-01</p> <p>Archives of digital <span class="hlt">seismic</span> data <span class="hlt">recorded</span> by seismometer networks around the world have grown tremendously over the last several decades helped by the deployment of <span class="hlt">seismic</span> stations and their continued operation within the framework of monitoring <span class="hlt">seismic</span> activity. These archives typically consist of waveforms of <span class="hlt">seismic</span> events and associated parametric data such as phase arrival time picks and the location of hypocenters. Catalogs of earthquake locations are fundamental data in seismology, and even in the Earth sciences in general. Yet, these locations have notoriously low spatial resolution because of errors in both the picks and the models commonly used to locate events one at a time. This limits their potential to address fundamental questions concerning the physics of earthquakes, the structure and composition of the Earth's interior, and the <span class="hlt">seismic</span> hazards associated with active faults. We report on the comprehensive use of modern waveform cross-correlation based methodologies for high- resolution earthquake location - as applied to regional and global long-term <span class="hlt">seismic</span> databases. By simultaneous re-analysis of two decades of the digital <span class="hlt">seismic</span> archive of Northern California, reducing pick errors via cross-correlation and model errors via double-differencing, we achieve up to three orders of magnitude resolution improvement over existing hypocenter locations. The relocated events image networks of discrete faults at seismogenic depths across various tectonic settings that until now have been hidden in location uncertainties. Similar location improvements are obtained for earthquakes <span class="hlt">recorded</span> at global networks by re- processing 40 years of parametric data from the ISC and corresponding waveforms archived at IRIS. Since our methods are scaleable and run on inexpensive Beowulf clusters, periodic re-analysis of entire archives may thus become a routine procedure to continuously improve resolution in existing catalogs. We demonstrate the role of <span class="hlt">seismic</span> archives</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017GI......6..505V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017GI......6..505V"><span>Data quality control and tools in passive <span class="hlt">seismic</span> experiments exemplified on the Czech broadband <span class="hlt">seismic</span> pool MOBNET in the AlpArray collaborative project</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Vecsey, Luděk; Plomerová, Jaroslava; Jedlička, Petr; Munzarová, Helena; Babuška, Vladislav; AlpArray Working Group</p> <p>2017-12-01</p> <p>This paper focuses on major issues related to the data reliability and network performance of 20 broadband (BB) stations of the Czech (CZ) MOBNET (MOBile NETwork) <span class="hlt">seismic</span> pool within the AlpArray <span class="hlt">seismic</span> experiments. Currently used high-resolution seismological applications require high-quality data <span class="hlt">recorded</span> for a sufficiently long time interval at seismological observatories and during the entire time of operation of the temporary stations. In this paper we present new hardware and software tools we have been developing during the last two decades while analysing data from several international passive experiments. The new tools help to assure the high-quality standard of broadband <span class="hlt">seismic</span> data and eliminate potential errors before supplying data to seismological centres. Special attention is paid to crucial issues like the detection of sensor misorientation, timing problems, interchange of <span class="hlt">record</span> components and/or their polarity reversal, sensor mass centring, or anomalous channel amplitudes due to, for example, imperfect gain. Thorough data quality control should represent an integral constituent of <span class="hlt">seismic</span> data <span class="hlt">recording</span>, preprocessing, and archiving, especially for data from temporary stations in passive <span class="hlt">seismic</span> experiments. Large international <span class="hlt">seismic</span> experiments require enormous efforts from scientists from different countries and institutions to gather hundreds of stations to be deployed in the field during a limited time period. In this paper, we demonstrate the beneficial effects of the procedures we have developed for acquiring a reliable large set of high-quality data from each group participating in field experiments. The presented tools can be applied manually or automatically on data from any <span class="hlt">seismic</span> network.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUFM.V13G2695D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUFM.V13G2695D"><span>Mammoth Mountain, California broadband <span class="hlt">seismic</span> experiment</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Dawson, P. B.; Pitt, A. M.; Wilkinson, S. K.; Chouet, B. A.; Hill, D. P.; Mangan, M.; Prejean, S. G.; Read, C.; Shelly, D. R.</p> <p>2013-12-01</p> <p>Mammoth Mountain is a young cumulo-volcano located on the southwest rim of Long Valley caldera, California. Current volcanic processes beneath Mammoth Mountain are manifested in a wide range of <span class="hlt">seismic</span> signals, including swarms of shallow volcano-tectonic earthquakes, upper and mid-crustal long-period earthquakes, swarms of brittle-failure earthquakes in the lower crust, and shallow (3-km depth) very-long-period earthquakes. Diffuse emissions of <span class="hlt">C</span>02 began after a magmatic dike injection beneath the volcano in 1989, and continue to present time. These indications of volcanic unrest drive an extensive monitoring effort of the volcano by the USGS Volcano Hazards Program. As part of this effort, eleven broadband seismometers were deployed on Mammoth Mountain in November 2011. This temporary deployment is expected to run through the fall of 2013. These stations supplement the local short-period and broadband <span class="hlt">seismic</span> stations of the Northern California <span class="hlt">Seismic</span> Network (NCSN) and provide a combined network of eighteen broadband stations operating within 4 km of the summit of Mammoth Mountain. Data from the temporary stations are not available in real-time, requiring the merging of the data from the temporary and permanent networks, timing of phases, and relocation of <span class="hlt">seismic</span> events to be accomplished outside of the standard NCSN processing scheme. The timing of phases is accomplished through an interactive Java-based phase-picking routine, and the relocation of <span class="hlt">seismicity</span> is achieved using the probabilistic non-linear software package NonLinLoc, distributed under the GNU General Public License by Alomax Scientific. Several swarms of shallow volcano-tectonic earthquakes, spasmodic bursts of high-frequency earthquakes, a few long-period events located within or below the edifice of Mammoth Mountain and numerous mid-crustal long-period events have been <span class="hlt">recorded</span> by the network. To date, about 900 of the ~2400 events occurring beneath Mammoth Mountain since November 2011 have</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013Tectp.603...68R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013Tectp.603...68R"><span><span class="hlt">Seismic</span> activity offshore Martinique and Dominica islands (Central Lesser Antilles subduction zone) from temporary onshore and offshore <span class="hlt">seismic</span> networks</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ruiz, M.; Galve, A.; Monfret, T.; Sapin, M.; Charvis, P.; Laigle, M.; Evain, M.; Hirn, A.; Flueh, E.; Gallart, J.; Diaz, J.; Lebrun, J. F.</p> <p>2013-09-01</p> <p>This work focuses on the analysis of a unique set of seismological data <span class="hlt">recorded</span> by two temporary networks of seismometers deployed onshore and offshore in the Central Lesser Antilles Island Arc from Martinique to Guadeloupe islands. During the whole <span class="hlt">recording</span> period, extending from January to the end of August 2007, more than 1300 local <span class="hlt">seismic</span> events were detected in this area. A subset of 769 earthquakes was located precisely by using HypoEllipse. We also computed focal mechanisms using P-wave polarities of the best azimuthally constrained earthquakes. We detected earthquakes beneath the Caribbean forearc and in the Atlantic oceanic plate as well. At depth <span class="hlt">seismicity</span> delineates the Wadati-Benioff Zone down to 170 km depth. The main <span class="hlt">seismic</span> activity is concentrated in the lower crust and in the mantle wedge, close to the island arc beneath an inner forearc domain in comparison to an outer forearc domain where little <span class="hlt">seismicity</span> is observed. We propose that the difference of the <span class="hlt">seismicity</span> beneath the inner and the outer forearc is related to a difference of crustal structure between the inner forearc interpreted as a dense, thick and rigid crustal block and the lighter and more flexible outer forearc. <span class="hlt">Seismicity</span> is enhanced beneath the inner forearc because it likely increases the vertical stress applied to the subducting plate.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009AGUFM.S44B..08Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009AGUFM.S44B..08Z"><span>Signal Quality and the Reliability of <span class="hlt">Seismic</span> Observations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zeiler, C. P.; Velasco, A. A.; Pingitore, N. E.</p> <p>2009-12-01</p> <p>The ability to detect, time and measure <span class="hlt">seismic</span> phases depends on the location, size, and quality of the <span class="hlt">recorded</span> signals. Additional constraints are an analyst’s familiarity with a seismogenic zone and with the <span class="hlt">seismic</span> stations that <span class="hlt">record</span> the energy. Quantification and qualification of an analyst’s ability to detect, time and measure <span class="hlt">seismic</span> signals has not been calculated or fully assessed. The fundamental measurement for computing the accuracy of a <span class="hlt">seismic</span> measurement is the signal quality. Several methods have been proposed to measure signal quality; however, the signal-to-noise ratio (SNR) has been adopted as a short-term average over the long-term average. While the standard SNR is an easy and computationally inexpensive term, the overall statistical significance has not been computed for <span class="hlt">seismic</span> measurement analysis. The prospect of canonizing the process of cataloging <span class="hlt">seismic</span> arrivals hinges on the ability to repeat measurements made by different methods and analysts. The first step in canonizing phase measurements has been done by the IASPEI, which established a reference for accepted practices in naming <span class="hlt">seismic</span> phases. The New Manual for Seismological Observatory Practices (NMSOP, 2002) outlines key observations for <span class="hlt">seismic</span> phases <span class="hlt">recorded</span> at different distances and proposes to quantify timing uncertainty with a user-specified windowing technique. However, this added measurement would not completely remove bias introduced by different techniques used by analysts to time <span class="hlt">seismic</span> arrivals. The general guideline to time a <span class="hlt">seismic</span> arrival is to <span class="hlt">record</span> the time where a noted change in frequency and/or amplitude begins. This is generally achieved by enhancing the arrivals through filtering or beam forming. However, these enhancements can alter the characteristics of the arrival and how the arrival will be measured. Furthermore, each enhancement has user-specified parameters that can vary between analysts and this results in reduced ability to repeat</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..19.4213A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..19.4213A"><span>Development of Deep-tow Autonomous Cable <span class="hlt">Seismic</span> (ACS) for Seafloor Massive Sulfides (SMSs) Exploration.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Asakawa, Eiichi; Murakami, Fumitoshi; Tsukahara, Hitoshi; Saito, Shutaro; Lee, Sangkyun; Tara, Kenji; Kato, Masafumi; Jamali Hondori, Ehsan; Sumi, Tomonori; Kadoshima, Kazuyuki; Kose, Masami</p> <p>2017-04-01</p> <p>Within the EEZ of Japan, numerous surveys exploring ocean floor resources have been conducted. The exploration targets are gas hydrates, mineral resources (manganese, cobalt or rare earth) and especially seafloor massive sulphide (SMS) deposits. These resources exist in shallow subsurface areas in deep waters (>1500m). For <span class="hlt">seismic</span> explorations very high resolution images are required. These cannot be effectively obtained with conventional marine <span class="hlt">seismic</span> techniques. Therefore we have been developing autonomous <span class="hlt">seismic</span> survey systems which <span class="hlt">record</span> the data close to the seafloor to preserve high frequency <span class="hlt">seismic</span> energy. Very high sampling rate (10kHz) and high accurate synchronization between <span class="hlt">recording</span> systems and shot time are necessary. We adopted Cs-base atomic clock considering its power consumption. At first, we developed a Vertical Cable <span class="hlt">Seismic</span> (VCS) system that uses hydrophone arrays moored vertically from the ocean bottom to <span class="hlt">record</span> close to the target area. This system has been successfully applied to SMS exploration. Specifically it fixed over known sites to assess the amount of reserves with the resultant 3D volume. Based on the success of VCS, we modified the VCS system to use as a more efficient deep-tow <span class="hlt">seismic</span> survey system. Although there are other examples of deep-tow <span class="hlt">seismic</span> systems, signal transmission cables present challenges in deep waters. We use our autonomous <span class="hlt">recording</span> system to avoid these problems. Combining a high frequency piezoelectric source (Sub Bottom Profiler:SBP) that automatically shots with a constant interval, we achieve the high resolution deep-tow <span class="hlt">seismic</span> without data transmission/power cable to the board. Although the data cannot be monitored in real-time, the towing system becomes very simple. We have carried out survey trial, which showed the systems utility as a high-resolution deep-tow <span class="hlt">seismic</span> survey system. Furthermore, the frequency ranges of deep-towed source (SBP) and surface towed sparker are 700-2300Hz and 10-200Hz</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/9566337','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/9566337"><span>Broadband spectra of <span class="hlt">seismic</span> survey air-gun emissions, with reference to dolphin auditory thresholds.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Goold, J C; Fish, P J</p> <p>1998-04-01</p> <p>Acoustic emissions from a 2120 cubic in air-gun array were <span class="hlt">recorded</span> through a towed hydrophone assembly during an oil industry 2-D <span class="hlt">seismic</span> survey off the West Wales Coast of the British Isles. <span class="hlt">Recorded</span> <span class="hlt">seismic</span> pulses were sampled, calibrated, and analyzed post-survey to investigate power levels of the pulses in the band 200 Hz-22 kHz at 750-m, 1-km, 2.2-km, and 8-km range from source. At 750-m range from source, <span class="hlt">seismic</span> pulse power at the 200-Hz end of the spectrum was 140 dB re: 1 microPa2/Hz, and at the 20-kHz end of the spectrum <span class="hlt">seismic</span> pulse power was 90 dB re: 1 microPa2/Hz. Although the background noise levels of the <span class="hlt">seismic</span> <span class="hlt">recordings</span> were far in excess of ambient, due to the proximity of engine, propeller, and flow sources of the ship towing the hydrophone, <span class="hlt">seismic</span> power dominated the entire <span class="hlt">recorded</span> bandwidth of 200 Hz-22 kHz at ranges of up to 2 km from the air-gun source. Even at 8-km range <span class="hlt">seismic</span> power was still clearly in excess of the high background noise levels up to 8 kHz. Acoustic observations of common dolphins during preceding <span class="hlt">seismic</span> surveys suggest that these animals avoided the immediate vicinity of the air-gun array while firing was in progress, i.e., localized disturbance occurred during <span class="hlt">seismic</span> surveying. Although a general pattern of localized disturbance is suggested, one specific observation revealed that common dolphins were able to tolerate the <span class="hlt">seismic</span> pulses at 1-km range from the air-gun array. Given the high broadband <span class="hlt">seismic</span> pulse power levels across the entire <span class="hlt">recorded</span> bandwidth, and known auditory thresholds for several dolphin species, we consider such <span class="hlt">seismic</span> emissions to be clearly audible to dolphins across a bandwidth of tens on kilohertz, and at least out to 8-km range.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.usgs.gov/of/1980/0177/ofr1980177.pdf','USGSPUBS'); return false;" href="https://pubs.usgs.gov/of/1980/0177/ofr1980177.pdf"><span>Single-channel <span class="hlt">seismic</span>-reflection profiles and sidescan sonar <span class="hlt">records</span> collected during May 15-20, 1978, on the southern New England continental shelf</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Twichell, David C.</p> <p>1980-01-01</p> <p>The U.S. Geological Survey completed a cruise aboard the R/V CAPE HENLOPEN during May 15-20, 1978, to map the surface character, thickness and extent of the fine-grained.sediment deposit that covers an area 100 x 200 km on the southern New England Continental Shelf. The study area lies between Great South Channel to the east and Black Channel to the west, and extends from the 50-m isobath to the shelf edge.Single-channel high-resolution <span class="hlt">seismic</span>-reflection profiles and echo-sounding profiles were collected along 941 km of trackline, sidescan sonar <span class="hlt">records</span> were collected along 673 km of trackline. The subbottom profiles were collected by using a Huntec*system that was towed at midwater depths. Filters were set at 1 to 7 kHz. Echo-sounding <span class="hlt">records</span> were collected by using a 60 kHz EDO Western system. A Klein stdescan sonar, set to scan 100 m to either side of the towed fish, was used to collect the sonographs.Navigation during the survey was done by the scientific staff using Loran-<span class="hlt">C</span> equipment. Fixes were <span class="hlt">recorded</span> and logged at least every 15 minutes; after the cruise, they were digitized and stored on magnetic tape.The original <span class="hlt">records</span> can be seen and studied at the U.S. Geological Survey Data Library at Woods Hole, MA 02543. Microfilm copies of the subbottom, echo­sounding, and sidescan sonar <span class="hlt">records</span> collected during the cruise can be purchased from the National Geophysical and Solar-Terrestrial Data Center, NOAA (National Oceanic ancl Atmosphere Administration), Boulder, CO 80302.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.S43F..08M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.S43F..08M"><span>Using <span class="hlt">Seismic</span> Interferometry to Investigate <span class="hlt">Seismic</span> Swarms</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Matzel, E.; Morency, C.; Templeton, D. C.</p> <p>2017-12-01</p> <p><span class="hlt">Seismicity</span> provides a direct means of measuring the physical characteristics of active tectonic features such as fault zones. Hundreds of small earthquakes often occur along a fault during a <span class="hlt">seismic</span> swarm. This <span class="hlt">seismicity</span> helps define the tectonically active region. When processed using novel geophysical techniques, we can isolate the energy sensitive to the fault, itself. Here we focus on two methods of <span class="hlt">seismic</span> interferometry, ambient noise correlation (ANC) and the virtual seismometer method (VSM). ANC is based on the observation that the Earth's background noise includes coherent energy, which can be recovered by observing over long time periods and allowing the incoherent energy to cancel out. The cross correlation of ambient noise between a pair of stations results in a waveform that is identical to the seismogram that would result if an impulsive source located at one of the stations was <span class="hlt">recorded</span> at the other, the Green function (GF). The calculation of the GF is often stable after a few weeks of continuous data correlation, any perturbations to the GF after that point are directly related to changes in the subsurface and can be used for 4D monitoring.VSM is a style of <span class="hlt">seismic</span> interferometry that provides fast, precise, high frequency estimates of the Green's function (GF) between earthquakes. VSM illuminates the subsurface precisely where the pressures are changing and has the potential to image the evolution of <span class="hlt">seismicity</span> over time, including changes in the style of faulting. With hundreds of earthquakes, we can calculate thousands of waveforms. At the same time, VSM collapses the computational domain, often by 2-3 orders of magnitude. This allows us to do high frequency 3D modeling in the fault region. Using data from a swarm of earthquakes near the Salton Sea, we demonstrate the power of these techniques, illustrating our ability to scale from the far field, where sources are well separated, to the near field where their locations fall within each other</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1071904','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1071904"><span>Bighorns Arch <span class="hlt">Seismic</span> Experiment (BASE): Amplitude Response to Different <span class="hlt">Seismic</span> Charge Configurations</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Harder, S. H., Killer, K. C., Worthington, L. L., Snelson, C. M.</p> <p>2010-09-02</p> <p>Contrary to popular belief, charge weight is not the most important engineering parameter determining the <span class="hlt">seismic</span> amplitudes generated by a shot. The scientific literature has long claimed that the relationship, A ~R2L1/2, where A is the <span class="hlt">seismic</span> amplitude generated by a shot, R is the radius of the <span class="hlt">seismic</span> charge and L is the length of that charge, holds. Assuming the coupling to the formation and the pressure generated by the explosive are constants, this relationship implies that the one should be able to increase the charge radius while decreasing the charge length and obtain more <span class="hlt">seismic</span> amplitude with lessmore » charge weight. This has significant implications for the economics of lithospheric <span class="hlt">seismic</span> shots, because shallower holes and small charge sizes decrease cost. During the Bighorns Array <span class="hlt">Seismic</span> Experiment (BASE) conducted in the summer of 2010, 24 shots with charge sizes ranging from 110 to 900 kg and drill hole diameters of 300 and 450 mm were detonated and <span class="hlt">recorded</span> by an array of up to 2000 single-channel Texan seismographs. Maximum source-receiver offset of 300 km. Five of these shots were located within a one-acre square in an effort to eliminate coupling effects due to differing geological formations. We present a quantitative comparison of the data from these five shots to experimentally test the equation above.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUSM.S52A..07B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUSM.S52A..07B"><span><span class="hlt">Seismic</span> Catalogue and <span class="hlt">Seismic</span> Network in Haiti</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Belizaire, D.; Benito, B.; Carreño, E.; Meneses, C.; Huerfano, V.; Polanco, E.; McCormack, D.</p> <p>2013-05-01</p> <p>The destructive earthquake occurred on January 10, 2010 in Haiti, highlighted the lack of preparedness of the country to address <span class="hlt">seismic</span> phenomena. At the moment of the earthquake, there was no <span class="hlt">seismic</span> network operating in the country, and only a partial control of the past <span class="hlt">seismicity</span> was possible, due to the absence of a national catalogue. After the 2010 earthquake, some advances began towards the installation of a national network and the elaboration of a <span class="hlt">seismic</span> catalogue providing the necessary input for <span class="hlt">seismic</span> Hazard Studies. This paper presents the state of the works carried out covering both aspects. First, a <span class="hlt">seismic</span> catalogue has been built, compiling data of historical and instrumental events occurred in the Hispaniola Island and surroundings, in the frame of the SISMO-HAITI project, supported by the Technical University of Madrid (UPM) and Developed in cooperation with the Observatoire National de l'Environnement et de la Vulnérabilité of Haiti (ONEV). Data from different agencies all over the world were gathered, being relevant the role of the Dominican Republic and Puerto Rico seismological services which provides local data of their national networks. Almost 30000 events <span class="hlt">recorded</span> in the area from 1551 till 2011 were compiled in a first catalogue, among them 7700 events with Mw ranges between 4.0 and 8.3. Since different magnitude scale were given by the different agencies (Ms, mb, MD, ML), this first catalogue was affected by important heterogeneity in the size parameter. Then it was homogenized to moment magnitude Mw using the empirical equations developed by Bonzoni et al (2011) for the eastern Caribbean. At present, this is the most exhaustive catalogue of the country, although it is difficult to assess its degree of completeness. Regarding the <span class="hlt">seismic</span> network, 3 stations were installed just after the 2010 earthquake by the Canadian Government. The data were sent by telemetry thought the Canadian System CARINA. In 2012, the Spanish IGN together</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/17799298','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/17799298"><span><span class="hlt">Seismic</span> data from man-made impacts on the moon.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Latham, G; Ewing, M; Dorman, J; Press, F; Toksoz, N; Sutton, G; Meissner, R; Duennebier, F; Nakamura, Y; Kovach, R; Yates, M</p> <p>1970-11-06</p> <p>Unusually long reverberations were <span class="hlt">recorded</span> from two lunar impacts by a <span class="hlt">seismic</span> station installed on the lunar surface by the Apollo 12 astronauts. <span class="hlt">Seismic</span> data from these impacts suggest that the lunar mare in the region of the Apollo 12 landing site consists of material with very low <span class="hlt">seismic</span> velocities near the surface, with velocity increasing with depth to 5 to 6 kilometers per second (for compressional waves) at a depth of 20 kilometers. Absorption of <span class="hlt">seismic</span> waves in this structure is extremely low relative to typical continental crustal materials on earth. It is unlikely that a major boundary similar to the crustmantle interface on earth exists in the outer 20 kilometers of the moon. A combination of dispersion and scattering of surface waves probably explains the lunar <span class="hlt">seismic</span> reverberation. Scattering of these waves implies the presence of heterogeneity within the outer zone of the mare on a scale of from several hundred meters (or less) to several kilometers. <span class="hlt">Seismic</span> signals from 160 events of natural origin have been <span class="hlt">recorded</span> during the first 7 months of operation of the Apollo 12 <span class="hlt">seismic</span> station. At least 26 of the natural events are small moonquakes. Many of the natural events are thought to be meteoroid impacts.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.S41A2764I','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.S41A2764I"><span><span class="hlt">Seismic</span> Structure of Perth Basin (Australia) and surroundings from Passive <span class="hlt">Seismic</span> Deployments</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Issa, N.; Saygin, E.; Lumley, D. E.; Hoskin, T. E.</p> <p>2016-12-01</p> <p>We image the subsurface structure of Perth Basin, Western Australia and surroundings by using ambient <span class="hlt">seismic</span> noise data from 14 <span class="hlt">seismic</span> stations recently deployed by University of Western Australia (UWA) and other available permanent stations from Geoscience Australia <span class="hlt">seismic</span> network and the Australian Seismometers in Schools program. Each of these 14 UWA <span class="hlt">seismic</span> stations comprises a broadband sensor and a high fidelity 3-component 10 Hz geophone, <span class="hlt">recording</span> in tandem at 250 Hz and 1000 Hz. The other stations used in this study are equipped with short period and broadband sensors. In addition, one shallow borehole station is operated with eight 3 component geophones at depths of between 2 and 44 m. The network is deployed to characterize natural <span class="hlt">seismicity</span> in the basin and to try and identify any microseismic activity across Darling Fault Zone (DFZ), bounding the basin to the east. The DFZ stretches to approximately 1000 km north-south in Western Australia, and is one of the longest fault zones on the earth with a limited number of detected earthquakes. We use <span class="hlt">seismic</span> noise cross- and auto-correlation methods to map <span class="hlt">seismic</span> velocity perturbations across the basin and the transition from DFZ to the basin. Retrieved Green's functions are stable and show clear dispersed waveforms. Travel times of the surface wave Green's functions from noise cross-correlations are inverted with a two-step probabilistic framework to map the absolute shear wave velocities as a function of depth. The single station auto-correlations from the <span class="hlt">seismic</span> noise yields P wave reflectivity under each station, marking the major discontinuities. Resulting images show the shear velocity perturbations across the region. We also quantify the variation of ambient <span class="hlt">seismic</span> noise at different depths in the near surface using the geophones in the shallow borehole array.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70034754','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70034754"><span><span class="hlt">Seismically</span> observed seiching in the Panama Canal</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>McNamara, D.E.; Ringler, A.T.; Hutt, C.R.; Gee, L.S.</p> <p>2011-01-01</p> <p>A large portion of the <span class="hlt">seismic</span> noise spectrum is dominated by water wave energy coupled into the solid Earth. Distinct mechanisms of water wave induced ground motions are distinguished by their spectral content. For example, cultural noise is generally <1 s period, microseisms dominate the <span class="hlt">seismic</span> spectrum from periods of 2 to 20 s, and the Earth's "hum" is in the range of 50 to 600 s. We show that in a large lake in the Panama Canal there is an additional source of long-period noise generated by standing water waves, seiches, induced by disturbances such as passing ships and wind pressure. We compare <span class="hlt">seismic</span> waveforms to water level <span class="hlt">records</span> and relate these observations to changes in local tilt and gravity due to an oscillating seiche. The methods and observations discussed in this paper provide a first step toward quantifying the impact of water inundation as <span class="hlt">recorded</span> by seismometers. This type of quantified understanding of water inundation will help in future estimates of similar phenomena such as the <span class="hlt">seismic</span> observations of tsunami impact. Copyright 2011 by the American Geophysical Union.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011AGUFM.S51A2186A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011AGUFM.S51A2186A"><span>Development of Vertical Cable <span class="hlt">Seismic</span> System</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Asakawa, E.; Murakami, F.; Sekino, Y.; Okamoto, T.; Ishikawa, K.; Tsukahara, H.; Shimura, T.</p> <p>2011-12-01</p> <p>In 2009, Ministry of Education, Culture, Sports, Science and Technology(MEXT) started the survey system development for Hydrothermal deposit. We proposed the Vertical Cable <span class="hlt">Seismic</span> (VCS), the reflection <span class="hlt">seismic</span> survey with vertical cable above seabottom. VCS has the following advantages for hydrothermal deposit survey. (1) VCS is an efficient high-resolution 3D <span class="hlt">seismic</span> survey in limited area. (2) It achieves high-resolution image because the sensors are closely located to the target. (3) It avoids the coupling problems between sensor and seabottom that cause serious damage of <span class="hlt">seismic</span> data quality. (4) Because of autonomous <span class="hlt">recording</span> system on sea floor, various types of marine source are applicable with VCS such as sea-surface source (GI gun etc.) , deep-towed or ocean bottom source. Our first experiment of 2D/3D VCS surveys has been carried out in Lake Biwa, JAPAN, in November 2009. The 2D VCS data processing follows the walk-away VSP, including wave field separation and depth migration. <span class="hlt">Seismic</span> Interferometry technique is also applied. The results give much clearer image than the conventional surface <span class="hlt">seismic</span>. Prestack depth migration is applied to 3D data to obtain good quality 3D depth volume. <span class="hlt">Seismic</span> Interferometry technique is applied to obtain the high resolution image in the very shallow zone. Based on the feasibility study, we have developed the autonomous <span class="hlt">recording</span> VCS system and carried out the trial experiment in actual ocean at the water depth of about 400m to establish the procedures of deployment/recovery and to examine the VC position or fluctuation at seabottom. The result shows that the VC position is estimated with sufficient accuracy and very little fluctuation is observed. Institute of Industrial Science, the University of Tokyo took the research cruise NT11-02 on JAMSTEC R/V Natsushima in February, 2011. In the cruise NT11-02, JGI carried out the second VCS survey using the autonomous VCS <span class="hlt">recording</span> system with the deep towed source provided by</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EGUGA..18.5372V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EGUGA..18.5372V"><span><span class="hlt">Seismic</span> Investigations of Europa and Other Ocean Worlds</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Vance, Steve; Tsai, Victor; Kedar, Sharon; Bills, Bruce; Castillo-Rogez, Julie; Jackson, Jennifer</p> <p>2016-04-01</p> <p><span class="hlt">Seismic</span> investigations offer the most comprehensive view into the deep interiors of planetary bodies. Developing missions (InSight, Europa Lander, Lunar Geophysical Network) identify seismology as a critical measurement to constrain interior structure and thermal state. In oceanic icy worlds, pinpointing the radial depths of compositional interfaces using seismology in a broad frequency range can address uncertainty in interior structures inferred from gravity and magnetometry studies, such as those planned for NASA's Europa and ESA's JUICE missions. Seismology also offers information about fluid motions within or beneath ice, which complement magnetic studies; and can <span class="hlt">record</span> the dynamics of ice layers, which would reveal mechanisms and spatiotemporal occurrence of crack formation and propagation. Investigating these with future missions will require detailed modeling of <span class="hlt">seismic</span> sources and signatures in order to develop the most suitable instrumentation. We evaluate <span class="hlt">seismic</span> sources and their propagation in Europa, with extension to other oceanic icy worlds, building on prior studies (Kovach and Chyba 2001, Lee et al. 2003, Cammarano et al. 2006, Panning et al. 2006, Leighton et al. 2008). We also consider additional sources: gravitationally forced librations, which will create volume-filling turbulent flow (le Bars et al. 2015), a possible <span class="hlt">seismic</span> source similar to that seen from turbulent flow in terrestrial rivers (Tsai et al., 2012; Gimbert et al., 2014; Chao et al., 2015); downflow of dense brines from chaos regions on Europa into its underlying ocean (Sotin et al. 2002), possibly resembling riverine flows and flows through glacial channels (Tsai and Rice 2012); ocean acoustic signals that couple with the overlying ice to produce <span class="hlt">seismic</span> waves, by analogy with Earth's ocean-generated <span class="hlt">seismic</span> hum (Kedar 2011, Ardhuin 2015). Ardhuin, F., Gualtieri, L., and Stutzmann, E. (2015). GRL., 42. Cammarano, F., Lekic, V., Manga, M., Panning, M., and Romanowicz, B. (2006</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EGUGA..1815962F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EGUGA..1815962F"><span><span class="hlt">Seismicity</span> and seismogenic structures of Central Apennines (Italy): constraints on the present-day stress field from focal mechanisms - The SLAM (<span class="hlt">Seismicity</span> of Lazio-Abruzzo and Molise) project</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Frepoli, Alberto; Battista Cimini, Giovanni; De Gori, Pasquale; De Luca, Gaetano; Marchetti, Alessandro; Montuori, Caterina; Pagliuca, Nicola</p> <p>2016-04-01</p> <p>We present new results for the microseismic activity in the Central Apennines <span class="hlt">recorded</span> from a total of 81<span class="hlt">seismic</span> stations. The large number of <span class="hlt">recording</span> sites derives from the combination of temporary and permanent <span class="hlt">seismic</span> networks operating in the study region. Between January 2009 and October 2013 we <span class="hlt">recorded</span> 6923 earthquakes with local magnitudes ML ranging from 0.1 to 4.8. We located hypocentres by using a refined 1D crustal velocity model. The majority of the hypocenters are located beneath the axes of the Apenninic chain, while the <span class="hlt">seismic</span> activity observed along the peri-Tyrrhenian margin is lower. The <span class="hlt">seismicity</span> extends to a depth of 32 km; the hypocentral depth distribution exhibits a pronounced peak of <span class="hlt">seismic</span> energy release in the depth range between 8 and 20 km. During the observation period we <span class="hlt">recorded</span> two major <span class="hlt">seismic</span> swarms and one <span class="hlt">seismic</span> sequence in the Marsica-Sorano area in which we have had the largest detected magnitude (ML = 4.8). Fault plane solutions for a total of 600 earthquakes were derived from P-polarities. This new data set consists of a number of focal plane solutions that is about four times the data so far available for regional stress field study. The majority of the focal mechanisms show predominantly normal fault solutions. T-axis trends are oriented NE-SW confirming that the area is in extension. We also derived the azimuths of the principal stress axes by inverting the fault plane solutions and calculated the direction of the maximum horizontal stress, which is mainly sub-vertical oriented. The study region has been historically affected by many strong earthquakes, some of them very destructive. This work can give an important contribution to the <span class="hlt">seismic</span> hazard assessment in an area densely populated as the city of Rome which is distant around 60 km from the main seismogenic structures of Central Apennine.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMNH21A0156T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMNH21A0156T"><span>Probabilistic <span class="hlt">Seismic</span> Hazard Analysis for Georgia</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tsereteli, N. S.; Varazanashvili, O.; Sharia, T.; Arabidze, V.; Tibaldi, A.; Bonali, F. L. L.; Russo, E.; Pasquaré Mariotto, F.</p> <p>2017-12-01</p> <p>Nowadays, <span class="hlt">seismic</span> hazard studies are developed in terms of the calculation of Peak Ground Acceleration (PGA), Spectral Acceleration (SA), Peak Ground Velocity (PGV) and other <span class="hlt">recorded</span> parameters. In the frame of EMME project PSH were calculated for Georgia using GMPE based on selection criteria. In the frame of Project N 216758 (supported by Shota Rustaveli National Science Foundation (SRNF)) PSH maps were estimated using hybrid- empirical ground motion prediction equation developed for Georgia. Due to the paucity of <span class="hlt">seismically</span> <span class="hlt">recorded</span> information, in this work we focused our research on a more robust dataset related to macroseismic data,and attempted to calculate the probabilistic <span class="hlt">seismic</span> hazard directly in terms of macroseismicintensity. For this reason, we started calculating new intensity prediction equations (IPEs)for Georgia taking into account different sets, belonging to the same new database, as well as distances from the <span class="hlt">seismic</span> source.With respect to the <span class="hlt">seismic</span> source, in order to improve the quality of the results, we have also hypothesized the size of faults from empirical relations, and calculated new IPEs also by considering Joyner-Boore and rupture distances in addition to epicentral and hypocentral distances. Finally, site conditions have been included as variables for IPEs calculation Regarding the database, we used a brand new revised set of macroseismic data and instrumental <span class="hlt">records</span> for the significant earthquakes that struck Georgia between 1900 and 2002.Particularly, a large amount of research and documents related to macroseismic effects of individual earthquakes, stored in the archives of the Institute of Geophysics, were used as sources for the new macroseismic data. The latter are reported in the Medvedev-Sponheuer-Karnikmacroseismic scale (MSK64). For each earthquake the magnitude, the focal depth and the epicenter location are also reported. An online version of the database, with therelated metadata,has been produced for the 69</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li class="active"><span>10</span></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_10 --> <div id="page_11" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li class="active"><span>11</span></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="201"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EGUGA..18.1943A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EGUGA..18.1943A"><span>New data of the Gakkel Ridge <span class="hlt">seismicity</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Antonovskaya, Galina; Basakina, Irina; Kremenetskaya, Elena</p> <p>2016-04-01</p> <p>250 earthquakes were <span class="hlt">recorded</span> in the Gakkel Ridge during the period 2012-2014 by Arkhangelsk <span class="hlt">seismic</span> network. The magnitude Ml of these earthquakes is 1.5 - 5.7, 70% of them have Ml up to 3.0. <span class="hlt">Seismic</span> events are arranged along to a narrow center line of the Mid-Arctic Ridge, most of the earthquakes are confined to the southern board of the Ridge. Presumably it's connected with the reflection of spreading processes. The high <span class="hlt">seismic</span> activity zones, which we associate with the volcano-tectonic processes, have been identified. Have been <span class="hlt">recorded</span> 13 events per day in the Western Volcanic Zone. The largest number of events (75%) is confined to the Sparsely Magmatic Zone. About 30% of all <span class="hlt">recorded</span> earthquakes with magnitudes above 2.9 have a T-phase. We divided the Gakkel Ridge's earthquakes into two groups by using spectral-time analysis. The first group: maximum energy of the earthquake is observed from 1.5 to 10 Hz, values of magnitudes Ml 2.50-5.29. Earthquakes are distributed along the Gakkel Ridge. The second group: maximum energy of the earthquake is observed from 1.5 to 20 Hz, clearly expressed a high-frequency component, values of magnitudes Ml 2.3-3.4. Earthquakes 2 groups focused only in the Sparsely Magmatic Zone. The new <span class="hlt">seismic</span> data shows an unique information about geodynamic processes of the Gakkel Ridge.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..1910923E','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..1910923E"><span>Characteristics of Helicopter-Generated and Volcano-Related <span class="hlt">Seismic</span> Tremor Signals</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Eibl, Eva P. S.; Lokmer, Ivan; Bean, Christopher J.; Akerlie, Eggert; Vogfjörd, Kristin S.</p> <p>2017-04-01</p> <p>In volcanic environments it is crucial to distinguish between man-made <span class="hlt">seismic</span> signals and signals created by the volcano. We compare volcanic, <span class="hlt">seismic</span> signals with helicopter generated, <span class="hlt">seismic</span> signals <span class="hlt">recorded</span> in the last 2.5 years in Iceland. In both cases a long-lasting, emergent <span class="hlt">seismic</span> signal, that can be referred to as <span class="hlt">seismic</span> tremor, was generated. In the case of a helicopter, the rotating blades generate pressure pulses that travel through the air and excite Rayleigh waves at up to 40 km distance depending on wind speed, wind direction and topographic features. The longest helicopter related <span class="hlt">seismic</span> signal we <span class="hlt">recorded</span> was at the order of 40 minutes long. The tremor usually has a fundamental frequency of more than 10 Hz and overtones at integers of the fundamental frequency. Changes in distance lead to either increases or decreases of the frequency due to the Doppler Effect and are strongest for small source-receiver distances. The volcanic tremor signal was <span class="hlt">recorded</span> during the Bardarbunga eruption at Holuhraun in 2014/15. For volcano-related <span class="hlt">seismic</span> signals it is usually more difficult to determine the source process that generated the tremor. The pre-eruptive tremor persists for 2 weeks, while the co-eruptive tremor lasted for 6 months. We observed no frequency changes, most energy between 1 and 2 Hz and no or very little energy above 5 Hz. We compare the different characteristics of helicopter-related and volcano-related <span class="hlt">seismic</span> signals and discuss how they can be distinguished. In addition we discuss how we can determine if a frequency change is related to a moving source or change in repeat time or a change in the geometry of the resonating body.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1429839-depth-discrimination-using-rg-sg-spectral-amplitude-ratios-seismic-events-utah-recorded-local-distances','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1429839-depth-discrimination-using-rg-sg-spectral-amplitude-ratios-seismic-events-utah-recorded-local-distances"><span>Depth Discrimination Using Rg-to-Sg Spectral Amplitude Ratios for <span class="hlt">Seismic</span> Events in Utah <span class="hlt">Recorded</span> at Local Distances</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Tibi, Rigobert; Koper, Keith D.; Pankow, Kristine L.</p> <p></p> <p>Short-period fundamental-mode Rayleigh waves (Rg) are commonly observed on seismograms of anthropogenic <span class="hlt">seismic</span> events and shallow, naturally occurring tectonic earthquakes (TEs) <span class="hlt">recorded</span> at local distances. In the Utah region, strong Rg waves traveling with an average group velocity of about 1.8 km/s are observed at ~1 Hz on waveforms from shallow events ( depth<10 km ) <span class="hlt">recorded</span> at distances up to about 150 km. At these distances, Sg waves, which are direct shear waves traveling in the upper crust, are generally the dominant signals for TEs. Here in this study, we leverage the well-known notion that Rg amplitude decreases dramaticallymore » with increasing event depth to propose a new depth discriminant based on Rg-to-Sg spectral amplitude ratios. The approach is successfully used to discriminate shallow events (both earthquakes and anthropogenic events) from deeper TEs in the Utah region <span class="hlt">recorded</span> at local distances ( <150 km ) by the University of Utah Seismographic Stations (UUSS) regional <span class="hlt">seismic</span> network. Using Mood’s median test, we obtained probabilities of nearly zero that the median Rg-to-Sg spectral amplitude ratios are the same between shallow events on the one hand (including both shallow TEs and anthropogenic events), and deeper earthquakes on the other, suggesting that there is a statistically significant difference in the estimated Rg-to-Sg ratios between the two populations. We also observed consistent disparities between the different types of shallow events (e.g., mining blasts vs. mining-induced earthquakes), implying that it may be possible to separate the subpopulations that make up this group. Lastly, this suggests that using local distance Rg-to-Sg spectral amplitude ratios one can not only discriminate shallow events from deeper events but may also be able to discriminate among different populations of shallow events.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.usgs.gov/pp/1313/report.pdf','USGSPUBS'); return false;" href="https://pubs.usgs.gov/pp/1313/report.pdf"><span>Studies related to the Charleston, South Carolina, earthquake of 1886; tectonics and <span class="hlt">seismicity</span></span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Gottfried, David; Annell, C.S.; Byerly, G.R.; Lanphere, Marvin A.; Phillips, Jeffrey D.; Gohn, Gregory S.; Houser, Brenda B.; Schneider, Ray R.; Ackermann, Hans D.; Yantis, B.R.; Costain, John K.; Schilt, F. Steve; Brown, Larry; Oliver, Jack E.; Kaufman, Sidney; Hamilton, Robert Morrison; Behrendt, John C.; Henry, V. James; Bayer, Kenneth C.; Daniels, David L.; Zietz, Isidore; Popenoe, Peter; Chowns, T.M.; Williams, C.T.; Dooley, Robert E.; Wampler, J.; Dillon, William P.; Klitgord, Kim D.; Paull, Charles K.; McGinnis, Lyle D.; Dewey, James W.; Tarr, Arthur C.; Rhea, Susan; Wentworth, Carl M.; Mergner-Keefer, Marcia; Bollinger, G.A.; Gohn, Gregory S.</p> <p>1983-01-01</p> <p>Since 1973, the U.S. Geological Survey (USGS), with support from the Nuclear Regulatory Commission, has conducted extensive investigations of the tectonic and <span class="hlt">seismic</span> history of the Charleston, S.<span class="hlt">C</span>., earthquake zone and surrounding areas. The goal of these investigations has been to discover the cause of the large intraplate Charleston earthquake of 1886, which dominates the <span class="hlt">record</span> of <span class="hlt">seismicity</span> in the Southeastern United States, through an understanding of the historic and modern <span class="hlt">seismicity</span> at Charleston and of the tectonic setting of the <span class="hlt">seismicity</span>. This goal is being pursued to evaluate the potential for additional large earthquakes in the Charleston area and surrounding regions and to determine whether the Charleston area differs tectonically in any significant fashion from other parts of the Southeastern United States. An understanding of the specific cause for the 1886 event and of the regional distribution of any structures that are generically related to or geometrically and mechanically similar to the source structure is essential for evaluation of <span class="hlt">seismic</span> hazards throughout the Southeast.The results given herein represent significant progress toward understanding the tectonic setting of the Charleston-area <span class="hlt">seismicity</span>. Several chapters in the volume address the distribution and origin of pre-Cretaceous rocks and structures beneath Coastal Plain sediments in the Charleston area and regionally beneath the southern Atlantic Coastal Plain and adjacent Continental Shelf. The modern <span class="hlt">seismicity</span> at Charleston is occurring at depths equal to or greater than the known extent of these older structures, and rejuvenation of an older fault in the modern stress field is a possible cause of the <span class="hlt">seismicity</span>. Accordingly, several chapters discuss the possible relationships of the various pre-Cretaceous structures to faults identified near Charleston that have a known Cretaceous and Cenozoic movement history and to the historic and instrumentally <span class="hlt">recorded</span> <span class="hlt">seismicity</span>. However</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.T51A0444B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.T51A0444B"><span><span class="hlt">Seismic</span> Attenuation Structure and Intraplate Deformation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bezada, M.; Kowalke, S.; Smale, J.</p> <p>2017-12-01</p> <p>It has been suggested that intraplate deformation and <span class="hlt">seismicity</span> is localized at weak zones in the lithosphere and at rheological boundaries. Comparisons of intraplate deformation regions with mantle <span class="hlt">seismic</span> velocity structure suggest a correlation, but are not universally accepted as compelling evidence. We present P-wave attenuation models built from <span class="hlt">records</span> of teleseismic deep-focus earthquakes in three different regions that show significant correlation between attenuation structure and intraplate <span class="hlt">seismicity</span> and deformation. In the eastern United States, the New Madrid, Wabash Valley, Eastern Tennessee, Central Virginia, and Carolina <span class="hlt">seismic</span> zones all occur at or near the edges of high-Q (low attenuation) regions. In Spain, intraplate <span class="hlt">seismicity</span> is absent from high-Q regions but relatively abundant in surrounding low-Q regions where intraplate orogeny is also observed. In Australia, where our model resolution is relatively poor owing to sparse and uneven station coverage, the Petermann and Alice Springs intraplate orogens occur near the edge of a high-Q feature roughly coinciding with the undeformed Amadeus basin. Our results suggest that lithospheric structure exerts important controls on the localization of intraplate deformation and <span class="hlt">seismicity</span> and that <span class="hlt">seismic</span> attenuation is a useful proxy for lithospheric strength.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010AGUFM.T43B2212N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010AGUFM.T43B2212N"><span>Velocity and Attenuation Structure of the Tibetan Lithosphere using <span class="hlt">Seismic</span> Attributes of P-waves from Regional Earthquakes <span class="hlt">Recorded</span> by the Hi-CLIMB Array</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Nowack, R. L.; Bakir, A. C.; Griffin, J.; Chen, W.; Tseng, T.</p> <p>2010-12-01</p> <p>Using data from regional earthquakes <span class="hlt">recorded</span> by the Hi-CLIMB array in Tibet, we utilize <span class="hlt">seismic</span> attributes from crustal and Pn arrivals to constrain the velocity and attenuation structure in the crust and the upper mantle in central and western Tibet. The <span class="hlt">seismic</span> attributes considered include arrival times, Hilbert envelope amplitudes, and instantaneous as well as spectral frequencies. We have constructed more than 30 high-quality regional <span class="hlt">seismic</span> profiles, and of these, 10 events have been selected with excellent crustal and Pn arrivals for further analysis. Travel-times <span class="hlt">recorded</span> by the Hi-CLIMB array are used to estimate the large-scale velocity structure in the region, with four near regional events to the array used to constrain the crustal structure. The travel times from the far regional events indicate that the Moho beneath the southern Lhasa terrane is up to 75 km thick, with Pn velocities greater than 8 km/s. In contrast, the data sampling the Qiangtang terrane north of the Bangong-Nujiang (BNS) suture shows thinner crust with Pn velocities less than 8 km/s. <span class="hlt">Seismic</span> amplitude and frequency attributes have been extracted from the crustal and Pn wave trains, and these data are compared with numerical results for models with upper-mantle velocity gradients and attenuation, which can strongly affect Pn amplitudes and pulse frequencies. The numerical modeling is performed using the complete spectral element method (SEM), where the results from the SEM method are in good agreement with analytical and reflectivity results for different models with upper-mantle velocity gradients. The results for the attenuation modeling in Tibet imply lower upper mantle Q values in the Qiangtang terrane to the north of the BNS compared to the less attenuative upper mantle beneath the Lhasa terrane to the south of the BNS.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFM.S41B2748S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFM.S41B2748S"><span>Using Ambient <span class="hlt">Seismic</span> Noise to Monitor Post-<span class="hlt">Seismic</span> Relaxation After the 2010 Mw 7.1 Darfield Earthquake, New Zealand</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Savage, M. K.; Heckels, R.; Townend, J.</p> <p>2015-12-01</p> <p>Quantifying <span class="hlt">seismic</span> velocity changes following large earthquakes can provide insights into the crustal response of the earth. The use of ambient <span class="hlt">seismic</span> noise to monitor these changes is becoming increasingly widespread. Cross-correlations of long-duration ambient noise <span class="hlt">records</span> can be used to give stable impulse response functions without the need for repeated <span class="hlt">seismic</span> events. Temporal velocity changes were detected in the four months following the September 2010 Mw 7.1 Darfield event in South Island, New Zealand, using temporary <span class="hlt">seismic</span> networks originally deployed to <span class="hlt">record</span> aftershocks in the region. The arrays consisted of stations lying on and surrounding the fault, with a maximum inter-station distance of 156km. The 2010-2011 Canterbury earthquake sequence occurred largely on previously unknown and buried faults. The Darfield earthquake was the first and largest in a sequence of events that hit the region, rupturing the Greendale Fault. A surface rupture of nearly 30km was observed. The sequence also included the Mw 6.3 February 2011 Christchurch event, which caused widespread damage throughout the city and resulted in almost 200 deaths. Nine-component, day-long Green's functions were computed for frequencies between 0.1 - 1.0 Hz for full waveform <span class="hlt">seismic</span> data from immediately after the 4th September 2010 earthquake until mid-January 2011. Using the moving window cross-spectral method, stacks of daily functions covering the study period (reference functions), were compared to consecutive 10 day stacks of cross-correlations to measure time delays between them. These were then inverted for <span class="hlt">seismic</span> velocity changes with respect to the reference functions. Over the study period an increase in <span class="hlt">seismic</span> velocity of 0.25% ± 0.02% was determined proximal to the Greendale fault. These results are similar to studies in other regions, and we attribute the changes to post-<span class="hlt">seismic</span> relaxation through crack-healing of the Greendale Fault and throughout the region.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..19.6058Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..19.6058Y"><span>Building rainfall thresholds for large-scales landslides by extracting occurrence time of landslides from <span class="hlt">seismic</span> <span class="hlt">records</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yen, Hsin-Yi; Lin, Guan-Wei</p> <p>2017-04-01</p> <p>Understanding the rainfall condition which triggers mass moment on hillslope is the key to forecast rainfall-induced slope hazards, and the exact time of landslide occurrence is one of the basic information for rainfall statistics. In the study, we focused on large-scale landslides (LSLs) with disturbed area larger than 10 ha and conducted a string of studies including the recognition of landslide-induced ground motions and the analyses of different terms of rainfall thresholds. More than 10 heavy typhoons during the periods of 2005-2014 in Taiwan induced more than hundreds of LSLs and provided the opportunity to characterize the rainfall conditions which trigger LSLs. A total of 101 landslide-induced <span class="hlt">seismic</span> signals were identified from the <span class="hlt">records</span> of Taiwan <span class="hlt">seismic</span> network. These signals exposed the occurrence time of landslide to assess rainfall conditions. Rainfall analyses showed that LSLs occurred when cumulative rainfall exceeded 500 mm. The results of rainfall-threshold analyses revealed that it is difficult to distinct LSLs from small-scale landslides (SSLs) by the I-D and R-D methods, but the I-R method can achieve the discrimination. Besides, an enhanced three-factor threshold considering deep water content was proposed as the rainfall threshold for LSLs.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012EGUGA..1412788M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012EGUGA..1412788M"><span><span class="hlt">Seismic</span> monitoring at Deception Island volcano (Antarctica): the 2010-2011 survey</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Martín, R.; Carmona, E.; Almendros, J.; Serrano, I.; Villaseñor, A.; Galeano, J.</p> <p>2012-04-01</p> <p>As an example of the recent advances introduced in <span class="hlt">seismic</span> monitoring of Deception Island volcano (Antarctica) during recent years, we describe the instrumental network deployed during the 2010-2011 survey by the Instituto Andaluz de Geofísica of University of Granada, Spain (IAG-UGR). The period of operation extended from December 19, 2010 to March 5, 2011. We deployed a wireless <span class="hlt">seismic</span> network composed by four three-component <span class="hlt">seismic</span> stations. These stations are based on 24-bit SL04 SARA dataloggers sampling at 100 sps. They use a PC with embedded linux and SEISLOG data acquisition software. We use two types of three-component seismometers: short-period Mark L4<span class="hlt">C</span> with natural frequency of 1 Hz and medium-period Lennartz3D/5s with natural frequency of 0.2 Hz. The network was designed for an optimum spatial coverage of the northern half of Deception, where a magma chamber has been reported. Station locations include the vicinity of the Spanish base "Gabriel de Castilla" (Gd<span class="hlt">C</span>), Obsidianas Beach, a zone near the craters from the 1970 eruptions, and the Chilean Shelter located south of Pendulum Cove. Continuous data from the local <span class="hlt">seismic</span> network are received in real-time in the base by wifi transmission. We used Ubiquiti Networks Nanostation2 antennas with 2.4 GHz, dual-polarity, 10 dBi gain, and 54 Mbps transmission rate. They have shown a great robustness and speed for real-time applications. To prioritize data acquisition when the battery level is low, we have designed a circuit that allows independent power management for the <span class="hlt">seismic</span> station and wireless transmission system. The reception antenna located at Gd<span class="hlt">C</span> is connected to a computer running SEISCOMP. This software supports several transmission protocols and manages the visualization and <span class="hlt">recording</span> of <span class="hlt">seismic</span> data, including the generation of summary plots to show the <span class="hlt">seismic</span> activity. These twelve data channels are stored in miniseed format and displayed in real time, which allows for a rapid evaluation of</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70014338','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70014338"><span><span class="hlt">Seismicity</span> in South Carolina</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Shedlock, K.M.</p> <p>1988-01-01</p> <p>The largest historical earthquake in South Carolina, and in the southeastern US, occurred in the Coastal Plain province, probably northwest of Charleston, in 1886. Locations for aftershocks associated with this earthquake, estimated using intensities based on newspaper accounts, defined a northwest trending zone about 250 km long that was at least 100 km wide in the Coastal Plain but widened to a northeast trending zone in the Piedmont. The subsequent historical and instrumentally <span class="hlt">recorded</span> <span class="hlt">seismicity</span> in South Carolina images the 1886 aftershock zone. Instrumentally <span class="hlt">recorded</span> <span class="hlt">seismicity</span> in the Coastal Plain province occurs in 3 <span class="hlt">seismic</span> zones or clusters: Middleton Place-Summervile (MPSSZ), Adams Run (ARC), and Bowman (BSZ). Approximately 68% of the Coastal Plain earthquakes occur in the MPSSZ, a north trending zone about 22 km long and 12 km wide, lying about 20 km northwest of Charleston. The hypocenters of MPSSZ earthquakes range in depth from near the surface to almost 12 km. Thrust, strike-slip, and some normal faulting are indicated by the fault plane solutions for Coastal Plain earthquakes. The maximum horizontal compressive stress, inferred from the P-axes of the fault plane solutions, is oriented NE-SW in the shallow crust (<9 km deep) but appears to be diffusely E-W between 9 to 12 km deep. -from Author</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.V53C3106T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.V53C3106T"><span><span class="hlt">Seismicity</span> of Cascade Volcanoes: Characterization and Comparison</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Thelen, W. A.</p> <p>2016-12-01</p> <p>Here we summarize and compare the <span class="hlt">seismicity</span> around each of the Very High Threat Volcanoes of the Cascade Range of Washington, Oregon and California as defined by the National Volcanic Early Warning System (NVEWS) threat assessment (Ewert et al., 2005). Understanding the background <span class="hlt">seismic</span> activity and processes controlling it is critical for assessing changes in <span class="hlt">seismicity</span> and their implications for volcanic hazards. Comparing <span class="hlt">seismicity</span> at different volcanic centers can help determine what critical factors or processes affect the observed <span class="hlt">seismic</span> behavior. Of the ten Very High Threat Volcanoes in the Cascade Range, five volcanoes are consistently seismogenic when considering earthquakes within 10 km of the volcanic center or caldera edge (Mount Rainier, Mount St. Helens, Mount Hood, Newberry Caldera, Lassen Volcanic Center). Other Very High Threat volcanoes (South Sister, Mount Baker, Glacier Peak, Crater Lake and Mount Shasta) have comparatively low rates of <span class="hlt">seismicity</span> and not enough <span class="hlt">recorded</span> earthquakes to calculate catalog statistics. Using a swarm definition of 3 or more earthquakes occurring in a day with magnitudes above the largest of the network's magnitude of completenesses (M 0.9), we find that Lassen Volcanic Center is the "swarmiest" in terms of percent of <span class="hlt">seismicity</span> occurring in swarms, followed by Mount Hood, Mount St. Helens and Rainier. The predominance of swarms at Mount Hood may be overstated, as much of the <span class="hlt">seismicity</span> is occurring on surrounding crustal faults (Jones and Malone, 2005). Newberry Caldera has a relatively short <span class="hlt">record</span> of <span class="hlt">seismicity</span> since the permanent network was installed in 2011, however there have been no swarms detected as defined here. Future work will include developing discriminates for volcanic versus tectonic <span class="hlt">seismicity</span> to better filter the <span class="hlt">seismic</span> catalog and more precise binning of depths at some volcanoes so that we may better consider different processes. Ewert J. W., Guffanti, M. and Murray, T. L. (2005). An</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013EGUGA..1512426J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013EGUGA..1512426J"><span>Monitoring El Hierro submarine volcanic eruption events with a submarine <span class="hlt">seismic</span> array</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jurado, Maria Jose; Molino, Erik; Lopez, Carmen</p> <p>2013-04-01</p> <p>A submarine volcanic eruption took place near the southernmost emerged land of the El Hierro Island (Canary Islands, Spain), from October 2011 to February 2012. The Instituto Geografico Nacional (IGN) <span class="hlt">seismic</span> stations network evidenced <span class="hlt">seismic</span> unrest since July 2012 and was a reference also to follow the evolution of the <span class="hlt">seismic</span> activity associated with the volcanic eruption. From the beginning of the eruption a geophone string was installed less than 2 km away from the new volcano, next to La Restinga village shore, to <span class="hlt">record</span> <span class="hlt">seismic</span> activity related to the volcanic activity, continuously and with special interest on high frequency events. The <span class="hlt">seismic</span> array was endowed with 8, high frequency, 3 component, 250 Hz, geophone cable string with a separation of 6 m between them. The analysis of the dataset using spectral techniques allows the characterization of the different phases of the eruption and the study of its dynamics. The correlation of the data analysis results with the observed sea surface activity (ash and lava emission and degassing) and also with the <span class="hlt">seismic</span> activity <span class="hlt">recorded</span> by the IGN field <span class="hlt">seismic</span> monitoring system, allows the identification of different stages suggesting the existence of different signal sources during the volcanic eruption and also the posteruptive <span class="hlt">record</span> of the degassing activity. The study shows that the high frequency capability of the geophone array allow the study of important features that cannot be registered by the standard <span class="hlt">seismic</span> stations. The accumulative spectral amplitude show features related to eruptive changes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70164355','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70164355"><span>New <span class="hlt">seismic</span> study begins in Puerto Rico</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Tarr, A.C.</p> <p>1974-01-01</p> <p>A new seismological project is now underway in Puerto Rico to provide information needed for accurate assessment of the island's <span class="hlt">seismic</span> hazard. The project should also help to increase understanding of the tectonics and geologic evolution of the Caribbean region. The Puerto Rico <span class="hlt">Seismic</span> Program is being conducted by the Geological Survey with support provided by the Puerto Rico Water Resources Authority, an agency responsible for generation and distribution of electric power throughout the Commonwealth. The Program will include the installation of a network of high quality seismograph stations to monitor <span class="hlt">seismic</span> activity on and around Puerto Rico. These stations will be distributed across the island to <span class="hlt">record</span> the <span class="hlt">seismicity</span> as uniformly as possible. The detection and accurate location of small earthquakes, as well as moderate magnitude shocks, will aid in mapping active <span class="hlt">seismic</span> zones and in compiling frequency of occurrence statistics which ultimately wil be useful in <span class="hlt">seismic</span> risk-zoning of hte island. </p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017E%26ES...84a2042M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017E%26ES...84a2042M"><span><span class="hlt">Seismic</span> safety in conducting large-scale blasts</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mashukov, I. V.; Chaplygin, V. V.; Domanov, V. P.; Semin, A. A.; Klimkin, M. A.</p> <p>2017-09-01</p> <p>In mining enterprises to prepare hard rocks for excavation a drilling and blasting method is used. With the approach of mining operations to settlements the negative effect of large-scale blasts increases. To assess the level of <span class="hlt">seismic</span> impact of large-scale blasts the scientific staff of Siberian State Industrial University carried out expertise for coal mines and iron ore enterprises. Determination of the magnitude of surface <span class="hlt">seismic</span> vibrations caused by mass explosions was performed using <span class="hlt">seismic</span> receivers, an analog-digital converter with <span class="hlt">recording</span> on a laptop. The registration results of surface <span class="hlt">seismic</span> vibrations during production of more than 280 large-scale blasts at 17 mining enterprises in 22 settlements are presented. The maximum velocity values of the Earth’s surface vibrations are determined. The safety evaluation of <span class="hlt">seismic</span> effect was carried out according to the permissible value of vibration velocity. For cases with exceedance of permissible values recommendations were developed to reduce the level of <span class="hlt">seismic</span> impact.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EGUGA..18.4174L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EGUGA..18.4174L"><span>Impact of wind on ambient noise <span class="hlt">recorded</span> by the "13 BB star" <span class="hlt">seismic</span> array in northern Poland</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lepore, Simone; Markowicz, Krzysztof; Grad, Marek</p> <p>2016-04-01</p> <p><span class="hlt">Seismic</span> interferometry and beam forming techniques were applied to ambient noise <span class="hlt">recorded</span> during January 2014 at the "13 BB star" array, composed of thirteen <span class="hlt">seismic</span> stations located in northern Poland, with the aim of evaluating the azimuth of noise sources and the velocities of surface waves. After normalizing the raw <span class="hlt">recordings</span> in time and frequency domain, the spectral characteristics of the ambient noise were studied to choose a frequency band suitable for the waves' retrieval. To get the velocity of surface waves by <span class="hlt">seismic</span> interferometry, the crosscorrelation between all station pairs was analysed for the vertical and horizontal components in the 0.05-0.1 Hz, 0.1-1 Hz and 1 10 Hz frequency bands. For each pair, the crosscorrelation was applied to one hour <span class="hlt">recordings</span> extracted from the ambient noise. The obtained traces were calculated for a complete day, and then summed together: the daily results were stacked for the whole January 2014. In the lowest frequency range, most of the energy is located around the 3.0 km/s line, meaning that the surface waves coming from the uppermost mantle will be retrieved. The intermediate frequency range shows most of the energy between the 2.0 km/s and 1.5 km/s lines: consequently, surface waves originating from the crust will be retrieved. In the highest frequency range, the surface waves are barely visible on the crosscorrelation traces, implying that the associated energy is strongly attenuated. The azimuth variation associated to the noise field was evaluated by means of the beam forming method, using the data from the whole array for all the three components. To that, the beam power was estimated in a small range of frequencies every day for the whole month. For each day, one hour long results of beam forming applications were stacked together. To avoid aliasing and near field effects, the minimum frequency was set at 0.05 Hz and the maximum to 0.1 Hz. In this frequency band, the amplitude maximum was sought</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/30560','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/30560"><span>Continuous <span class="hlt">seismic</span>-reflection survey defining shallow sedimentary layers in the Charlotte Harbor and Venice areas, southwest Florida</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Wolansky, R.M.; Haeni, F.P.; Sylvester, R.E.</p> <p>1983-01-01</p> <p>A continuous marine <span class="hlt">seismic</span>-reflection survey system was used to define the configuration of shallow sedimentary layers underlying the Charlotte Harbor and Venice areas, southwest Florida. <span class="hlt">Seismic</span> profiling was conducted over a distance of about 57 miles of Charlotte Harbor, the Peace and Myakka Rivers, and the Intracoastal Waterway near Venice using a high resolution energy source capable of penetrating 200 feet of sediments with a resolution of 1 to 3 feet. Five stratigraphic units defined from the <span class="hlt">seismic</span> <span class="hlt">records</span> includes sediments to Holocene to early Miocene age. All <span class="hlt">seismic</span>-profile <span class="hlt">records</span> are presented, along with geologic sections constructed from the <span class="hlt">records</span>. <span class="hlt">Seismic</span> reflection amplitude, frequency, continuity, configuration, external form, and areal association were utilized to interpret facies and depositional environments of the stratigraphic units. The despositional framework of the units ranges from shallow shelf to prograded slope. The stratigraphic units are correlated with the surficial aquifer and intermediate artesian aquifers, and permeable zones of the aquifers are related to the <span class="hlt">seismic</span> <span class="hlt">records</span>. (USGS)</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.T11D2650D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.T11D2650D"><span>Surface Deformation and Source Model at Semisopochnoi Volcano from InSAR and <span class="hlt">Seismic</span> Analysis During the 2014 and 2015 <span class="hlt">Seismic</span> Swarms</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>DeGrandpre, K.; Pesicek, J. D.; Lu, Z.</p> <p>2016-12-01</p> <p>During the summer of 2014 and the early spring of 2015 two notable increases in <span class="hlt">seismic</span> activity at Semisopochnoi volcano in the western Aleutian islands were <span class="hlt">recorded</span> on AVO seismometers on Semisopochnoi and neighboring islands. These <span class="hlt">seismic</span> swarms did not lead to an eruption. This study employs differential SAR techniques using TerraSAR-X images in conjunction with more accurately relocating the <span class="hlt">recorded</span> <span class="hlt">seismic</span> events through simultaneous inversion of event travel times and a three-dimensional velocity model using tomoDD. The interferograms created from the SAR images exhibit surprising coherence and an island wide spatial distribution of inflation that is then used in a Mogi model in order to define the three-dimensional location and volume change required for a source at Semisopochnoi to produce the observed surface deformation. The tomoDD relocations provide a more accurate and realistic three-dimensional velocity model as well as a tighter clustering of events for both swarms that clearly outline a linear <span class="hlt">seismic</span> void within the larger group of shallow (<10 km) <span class="hlt">seismicity</span>. While no direct conclusions as to the relationship of these <span class="hlt">seismic</span> events and the observed surface deformation can be made at this time, these techniques are both complimentary and efficient forms of remotely monitoring volcanic activity that provide much deeper insights into the processes involved without having to risk hazardous or costly field work.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012EGUGA..14.1077K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012EGUGA..14.1077K"><span><span class="hlt">Seismic</span> noise study for a new <span class="hlt">seismic</span> station at King Fahd University of Petroleum and Minerals in Saudi Arabia</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kaka, S. I.</p> <p>2012-04-01</p> <p>We have carried out a <span class="hlt">seismic</span> noise study in order to understand the noise level at three selected locations at King Fahd University of Petroleum and Minerals (KFUPM), Dhahran, Saudi Arabia. The main purpose is to select a suitable site with low <span class="hlt">seismic</span> noise and good signal-to-noise ratio for our new broadband <span class="hlt">seismic</span> station. There are several factors involved in the selection of a site location for a new station. Most importantly, we need to strike a balance between a logistically convenient site versus a technically suitable site. As a starting point, we selected six potential sites due to accessibility and proximity to the <span class="hlt">seismic</span> processing center laboratory in the Department of Earth Sciences (ESD) at KFUPM. We then eliminated two sites that are relatively close to possible low-frequency noise sources. We have considered many possible noise sources which include: vehicle traffic / heavy machinery, the direct path of air flowing from air conditioning vent, tall trees / power poles and metal doorways. One more site was eliminated because the site was located in the open where it experiences maximum wind speed which is considered a major source of noise. All three potential sites are situated within the Dammam Dome where both lower middle and upper Rus Formations are exposed. The upper Rus is mainly made up of fine grained chalky limestone and the lower Rus is made up of alternation of marls and thin dolomitic limestone. The area is not known for any major faults and considered very low <span class="hlt">seismicity</span> and hence the identification of seismoteconic features is not required. Before conducting the noise study, we calibrated and tested the <span class="hlt">seismic</span> <span class="hlt">recording</span> system, which was recently acquired by the ESD at KFUPM. The system includes a <span class="hlt">seismic</span> <span class="hlt">recorder</span> and a sensor with a GPS device. We deployed the system in order to measure the low-frequency background noise. Knowing the low frequency noise will help in predicting the high-frequency noise. The <span class="hlt">recording</span> systems were</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFM.S53A2769S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFM.S53A2769S"><span>ASDF: An Adaptable <span class="hlt">Seismic</span> Data Format with Full Provenance</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Smith, J. A.; Krischer, L.; Tromp, J.; Lefebvre, M. P.</p> <p>2015-12-01</p> <p>In order for seismologists to maximize their knowledge of how the Earth works, they must extract the maximum amount of useful information from all <span class="hlt">recorded</span> <span class="hlt">seismic</span> data available for their research. This requires assimilating large sets of waveform data, keeping track of vast amounts of metadata, using validated standards for quality control, and automating the workflow in a careful and efficient manner. In addition, there is a growing gap between CPU/GPU speeds and disk access speeds that leads to an I/O bottleneck in <span class="hlt">seismic</span> workflows. This is made even worse by existing <span class="hlt">seismic</span> data formats that were not designed for performance and are limited to a few fixed headers for storing metadata.The Adaptable <span class="hlt">Seismic</span> Data Format (ASDF) is a new data format for seismology that solves the problems with existing <span class="hlt">seismic</span> data formats and integrates full provenance into the definition. ASDF is a self-describing format that features parallel I/O using the parallel HDF5 library. This makes it a great choice for use on HPC clusters. The format integrates the standards QuakeML for <span class="hlt">seismic</span> sources and StationXML for receivers. ASDF is suitable for storing earthquake data sets, where all waveforms for a single earthquake are stored in a one file, ambient noise cross-correlations, and adjoint sources. The format comes with a user-friendly Python reader and writer that gives seismologists access to a full set of Python tools for seismology. There is also a faster <span class="hlt">C</span>/Fortran library for integrating ASDF into performance-focused numerical wave solvers, such as SPECFEM3D_GLOBE. Finally, a GUI tool designed for visually exploring the format exists that provides a flexible interface for both research and educational applications. ASDF is a new <span class="hlt">seismic</span> data format that offers seismologists high-performance parallel processing, organized and validated contents, and full provenance tracking for automated seismological workflows.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70018377','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70018377"><span><span class="hlt">Seismicity</span> of the Adriatic microplate</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Console, R.; Di, Giovambattista R.; Favali, P.; Presgrave, B.W.; Smriglio, G.</p> <p>1993-01-01</p> <p>The Adriatic microplate was previously considered to be a unique block, tectonically active only along its margins. The <span class="hlt">seismic</span> sequences that took place in the basin from 1986 to 1990 give new information about the geodynamics of this area. Three subsets of well <span class="hlt">recorded</span> events were relocated by the joint hypocentre determination technique. On the whole, this <span class="hlt">seismic</span> activity was concentrated in a belt crossing the southern Adriatic sea around latitude 42??, in connection with regional E-W fault systems. Some features of this <span class="hlt">seismicity</span>, similar to those observed in other well known active margins of the Adriatic plate, support a model of a southern Adriatic lithospheric block, detached from the Northern one. Other geophysical information provides evidence of a transitional zone at the same latitude. ?? 1993.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li class="active"><span>11</span></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_11 --> <div id="page_12" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li class="active"><span>12</span></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="221"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1372241-faulting-natural-serpentinite-implications-intermediate-depth-seismicity','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1372241-faulting-natural-serpentinite-implications-intermediate-depth-seismicity"><span>Faulting of natural serpentinite: Implications for intermediate-depth <span class="hlt">seismicity</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Gasc, Julien; Hilairet, Nadège; Yu, Tony</p> <p></p> <p>The <span class="hlt">seismic</span> potential of serpentinites at high pressure was investigated via deformation experiments on cored natural serpentinite samples, during which micro-<span class="hlt">seismicity</span> was monitored by <span class="hlt">recording</span> Acoustic Emissions (AEs). Deformation was performed at pressures of 3–5 GPa, using a Deformation-DIA device, and over a wide range of temperatures, both within and outside antigorite's stability field. Below 400 °<span class="hlt">C</span>, serpentinite deformation involves “silent” semi-brittle mechanisms, even in cases where strain localization is observed. At high temperature (i.e., above 600 °<span class="hlt">C</span>), despite conditions propitious to dehydration embrittlement (i.e., fast strain rates and reaction kinetics), joint deformation and dehydration lead to ductile shear, withoutmore » generation of AEs. Brittle behavior was observed in a narrow temperature window ca. 500 °<span class="hlt">C</span>. In this latter case, AEs are consistently observed upon faulting and extremely sharp strain localization is observed in recovered samples. The resulting microstructures are consistent with the inverse ductile-to-brittle transition proposed by Proctor and Hirth (2016) in antigorite. This may therefore be a source of <span class="hlt">seismicity</span> in subducting slabs at mantle pressures and temperatures from 500 to 600 °<span class="hlt">C</span>. However, the acoustic signal observed here is orders of magnitude weaker than what is obtained at low PT conditions with brittle failure, consistently with low radiation efficiency of serpentinite faulting (Prieto et al., 2013) and suggests that other mechanisms are responsible for large intermediate-depth earthquakes. In fact, the present results are in line with a recent study (Ferrand et al., 2017), that suggests that intermediate earthquakes are likely induced by mechanical instabilities due to dehydration in partly hydrated peridotites.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017E%26PSL.474..138G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017E%26PSL.474..138G"><span>Faulting of natural serpentinite: Implications for intermediate-depth <span class="hlt">seismicity</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gasc, Julien; Hilairet, Nadège; Yu, Tony; Ferrand, Thomas; Schubnel, Alexandre; Wang, Yanbin</p> <p>2017-09-01</p> <p>The <span class="hlt">seismic</span> potential of serpentinites at high pressure was investigated via deformation experiments on cored natural serpentinite samples, during which micro-<span class="hlt">seismicity</span> was monitored by <span class="hlt">recording</span> Acoustic Emissions (AEs). Deformation was performed at pressures of 3-5 GPa, using a Deformation-DIA device, and over a wide range of temperatures, both within and outside antigorite's stability field. Below 400 °<span class="hlt">C</span>, serpentinite deformation involves ;silent; semi-brittle mechanisms, even in cases where strain localization is observed. At high temperature (i.e., above 600 °<span class="hlt">C</span>), despite conditions propitious to dehydration embrittlement (i.e., fast strain rates and reaction kinetics), joint deformation and dehydration lead to ductile shear, without generation of AEs. Brittle behavior was observed in a narrow temperature window ca. 500 °<span class="hlt">C</span>. In this latter case, AEs are consistently observed upon faulting and extremely sharp strain localization is observed in recovered samples. The resulting microstructures are consistent with the inverse ductile-to-brittle transition proposed by Proctor and Hirth (2016) in antigorite. This may therefore be a source of <span class="hlt">seismicity</span> in subducting slabs at mantle pressures and temperatures from 500 to 600 °<span class="hlt">C</span>. However, the acoustic signal observed here is orders of magnitude weaker than what is obtained at low PT conditions with brittle failure, consistently with low radiation efficiency of serpentinite faulting (Prieto et al., 2013) and suggests that other mechanisms are responsible for large intermediate-depth earthquakes. In fact, the present results are in line with a recent study (Ferrand et al., 2017), that suggests that intermediate earthquakes are likely induced by mechanical instabilities due to dehydration in partly hydrated peridotites.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70019445','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70019445"><span>Lithofacies and <span class="hlt">seismic</span>-reflection interpretation of temperate glacimarine sedimentation in Tarr Inlet, Glacier Bay, Alaska</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Cai, J.; Powell, R.D.; Cowan, E.A.; Carlson, P.R.</p> <p>1997-01-01</p> <p>High-resolution <span class="hlt">seismic</span>-reflection profiles of sediment fill within Tart Inlet of Glacier Bay, Alaska, show <span class="hlt">seismic</span> facies changes with increasing distance from the glacial termini. Five types of <span class="hlt">seismic</span> facies are recognized from analysis of Huntec and minisparker <span class="hlt">records</span>, and seven lithofacies are determined from detailed sedimentologic study of gravity-, vibro- and box-cores, and bottom grab samples. Lithofacies and <span class="hlt">seismic</span> facies associations, and fjord-floor morphology allow us to divide the fjord into three sedimentary environments: ice-proximal, iceberg-zone and ice-distal. The ice-proximal environment, characterized by a morainal-bank depositional system, can be subdivided into bank-back, bank-core and bank-front subenvironments, each of which is characterized by a different depositional subsystem. A bank-back subsystem shows chaotic <span class="hlt">seismic</span> facies with a mounded surface, which we infer consists mainly of unsorted diamicton and poorly sorted coarse-grained sediments. A bank-core depositional subsystem is a mixture of diamicton, rubble, gravel, sand and mud. <span class="hlt">Seismic</span>-reflection <span class="hlt">records</span> of this subsystem are characterized by chaotic <span class="hlt">seismic</span> facies with abundant hyperbolic diffractions and a hummocky surface. A bank-front depositional subsystem consists of mainly stratified and massive sand, and is characterized by internal hummocky facies on <span class="hlt">seismic</span>-reflection <span class="hlt">records</span> with significant surface relief and sediment gravity flow channels. The depositional system formed in the iceberg-zone environment consists of rhythmically laminated mud interbedded with thin beds of weakly stratified diamicton and stratified or massive sand and silt. On <span class="hlt">seismic</span>-reflection profiles, this depositional system is characterized by discontinuously stratified facies with multiple channels on the surface in the proximal zone and a single channel on the largely flat sediment surface in the distal zone. The depositional system formed in the ice-distal environment consists of interbedded</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.S43F3199S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.S43F3199S"><span>The INGV <span class="hlt">seismic</span> monitoring system: activities during the first month of the 2016 Amatrice <span class="hlt">seismic</span> sequence.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Scognamiglio, L.; Margheriti, L.; Moretti, M.; Pintore, S.</p> <p>2016-12-01</p> <p>At 01:36:32 UTC on August 24, 2016 an earthquake of ML=6.0 occurred in Central Italy, near Amatrice village; 21 s after the origin time, the first automatic location became available while the first magnitude estimate followed 47s after. The INGV seismologists on duty provided the alert to the Italian Civil Protection Department and thereby triggered the <span class="hlt">seismic</span> emergency protocol In the hours after the earthquake, hundreds of events were <span class="hlt">recorded</span> by the Italian <span class="hlt">Seismic</span> Network of the INGV. SISMIKO, the coordinating body of the emergency <span class="hlt">seismic</span> network, was activated few minutes after the mainshock. The main goal of this emergency group is to install temporary dense <span class="hlt">seismic</span> network integrated with the existing permanent networks in the epicentral area to better constrain the aftershock hypocenters. From August the 24th to the 30th, SISMIKO deployed 18 <span class="hlt">seismic</span> stations, generally six components (equipped with both seismometer and accelerometer), 13 of which were transmitting in real-time to the INGV <span class="hlt">seismic</span> surveillance room in Rome. All data acquired are available at the European Integrated Data Archive (EIDA). The <span class="hlt">seismic</span> sequence in the first month generated thousands of earthquakes which were processed and detected by the INGV automated localization system. We analyzed the performance of this system. Hundreds of those events were located by seismologists on shifts, the others were left to be analyzed by the Bollettino Sismico Italiano (BSI). The procedures of the BSI revise and integrate all available data. This allows for a better constrained location and for a more realistic hypocentral depth estimation. The first eight hours of August 24th were the most critical for the INGV surveillance room. Data <span class="hlt">recorded</span> in these hours were carefully re-analyzed by BSI operators and the number of located events increased from 133 to 408, while the magnitude of completeness dropped significantly from about 3.5 to 2.7.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011AGUFM.V33C2656R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011AGUFM.V33C2656R"><span>Properties of Repetitive Long-Period <span class="hlt">Seismicity</span> at Villarrica Volcano, Chile</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Richardson, J.; Waite, G. P.; Palma, J.; Johnson, J. B.</p> <p>2011-12-01</p> <p>Villarrica Volcano, Chile hosts a persistent lava lake and is characterized by degassing and long-period <span class="hlt">seismicity</span>. In order to better understand the relationship between outgassing and <span class="hlt">seismicity</span>, we <span class="hlt">recorded</span> broadband <span class="hlt">seismic</span> and acoustic data along with high-rate SO2 emission data. We used both a densely-spaced linear array deployed on the northern flank of Villarrica, during the austral summer of 2011, and a wider aperture array of stations distributed around the volcano that was active in the austral summer of 2010. Both deployments consisted of three-component broadband stations and were augmented with broadband infrasound sensors. Of particular interests are repetitive, ~1 Hz <span class="hlt">seismic</span> and coincident infrasound signals that occurred approximately every 2 minutes. Because these events are typically very low amplitude, we used a matched filter approach to identify them. We windowed several high-amplitude <span class="hlt">records</span> of these events from broadband <span class="hlt">seismic</span> stations near the vent. The <span class="hlt">record</span> section of each event served as a template to compare with the entire dataset by cross-correlation. This approach identified ~20,000 nearly identical events during the ~7 day deployment of the linear array, which were otherwise difficult to identify in the raw <span class="hlt">records</span>. Assuming that all of the events that we identified have identical source mechanisms and depths, we stack the large suite of events to produce low-noise <span class="hlt">records</span> and particle motions at receivers farther than 5 km from the vent. We find that the <span class="hlt">records</span> from stations near the edifice are dominated by tangential particle motion, suggesting the influence of near-field components. Correlation of these data with broadband acoustic data collected at the summit suggest that these repeatable <span class="hlt">seismic</span> processes are linked to acoustic emissions, probably due to gas bubbles bursting at the magma free surface, as no eruptive products besides gas were being emitted by the volcano during the instrument deployment. The acoustic</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.usgs.gov/of/1984/0657/','USGSPUBS'); return false;" href="https://pubs.usgs.gov/of/1984/0657/"><span>Noise analysis of the <span class="hlt">seismic</span> system employed in the northern and southern California <span class="hlt">seismic</span> nets</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Eaton, J.P.</p> <p>1984-01-01</p> <p>The <span class="hlt">seismic</span> networks have been designed and operated to support <span class="hlt">recording</span> on Develocorders (less than 40db dynamic range) and analog magnetic tape (about 50 db dynamic range). The principal analysis of the <span class="hlt">records</span> has been based on Develocorder films; and background earth noise levels have been adjusted to be about 1 to 2 mm p-p on the film readers. Since the traces are separated by only 10 to 12 mm on the reader screen, they become hopelessly tangled when signal amplitudes on several adjacent traces exceed 10 to 20 mm p-p. Thus, the background noise level is hardly more than 20 db below the level of largest readable signals. The situation is somewhat better on tape playbacks, but the high level of background noise set to accomodate processing from film <span class="hlt">records</span> effectively limits the range of maximum-signal to background-earth-noise on high gain channels to a little more than 30 db. Introduction of the PDP 11/44 <span class="hlt">seismic</span> data acquisition system has increased the potential dynamic range of <span class="hlt">recorded</span> network signals to more than 60 db. To make use of this increased dynamic range we must evaluate the characteristics and performance of the <span class="hlt">seismic</span> system. In particular, we must determine whether the electronic noise in the system is or can be made sufficiently low so that background earth noise levels can be lowered significantly to take advantage of the increased dynamic range of the digital <span class="hlt">recording</span> system. To come to grips with the complex problem of system noise, we have carried out a number of measurements and experiments to evaluate critical components of the system as well as to determine the noise characteristics of the system as a whole.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUFM.S21B2415M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUFM.S21B2415M"><span>SIG-VISA: Signal-based Vertically Integrated <span class="hlt">Seismic</span> Monitoring</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Moore, D.; Mayeda, K. M.; Myers, S. C.; Russell, S.</p> <p>2013-12-01</p> <p>Traditional <span class="hlt">seismic</span> monitoring systems rely on discrete detections produced by station processing software; however, while such detections may constitute a useful summary of station activity, they discard large amounts of information present in the original <span class="hlt">recorded</span> signal. We present SIG-VISA (Signal-based Vertically Integrated <span class="hlt">Seismic</span> Analysis), a system for <span class="hlt">seismic</span> monitoring through Bayesian inference on <span class="hlt">seismic</span> signals. By directly modeling the <span class="hlt">recorded</span> signal, our approach incorporates additional information unavailable to detection-based methods, enabling higher sensitivity and more accurate localization using techniques such as waveform matching. SIG-VISA's Bayesian forward model of <span class="hlt">seismic</span> signal envelopes includes physically-derived models of travel times and source characteristics as well as Gaussian process (kriging) statistical models of signal properties that combine interpolation of historical data with extrapolation of learned physical trends. Applying Bayesian inference, we evaluate the model on earthquakes as well as the 2009 DPRK test event, demonstrating a waveform matching effect as part of the probabilistic inference, along with results on event localization and sensitivity. In particular, we demonstrate increased sensitivity from signal-based modeling, in which the SIGVISA signal model finds statistical evidence for arrivals even at stations for which the IMS station processing failed to register any detection.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19910005047','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19910005047"><span>Specification goals for a Mars <span class="hlt">seismic</span> network</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Davis, Paul M.</p> <p>1990-01-01</p> <p>A <span class="hlt">seismic</span> network on Mars should have enough stations (e.g., 24) to characterize the <span class="hlt">seismicity</span> of the planet for comparison with a diversity of structural features; be comprised of low noise stations, preferably underground, 3 to 4 orders of magnitude more sensitive than those used on Viking; <span class="hlt">record</span> over a sufficient band-width (DC-30 Hz) to detect micro-earthquakes to normal modes; and <span class="hlt">record</span> for a sufficient duration (10 years) and data rate (10(exp 8) Mb/day/station) to obtain a data set comparable to that from the Apollo mission to the Moon so that locations of major internal boundaries can be inferred, such as those in the Earth, i.e., crust - lithosphere - asthenosphere - upper - lower phase transitions - outer - inner core. The proposed Mars Global Network Mission provides an opportunity to sense the dynamics and probe the interior of the planet. The <span class="hlt">seismic</span> objectives, the availability of the instrumentation and trade-offs to meet them are discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUFM.V21B2707C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUFM.V21B2707C"><span>Sub-crustal <span class="hlt">seismic</span> activity beneath Klyuchevskoy Volcano</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Carr, M. J.; Droznina, S.; Levin, V. L.; Senyukov, S.</p> <p>2013-12-01</p> <p><span class="hlt">Seismic</span> activity is extremely vigorous beneath the Klyuchevskoy Volcanic Group (KVG). The unique aspect is the distribution in depth. In addition to upper-crustal <span class="hlt">seismicity</span>, earthquakes take place at depths in excess of 20 km. Similar observations are known in other volcanic regions, however the KVG is unique in both the number of earthquakes and that they occur continuously. Most other instances of deep <span class="hlt">seismicity</span> beneath volcanoes appear to be episodic or transient. Digital <span class="hlt">recording</span> of <span class="hlt">seismic</span> signals started at the KVG in early 2000s.The dense local network reliably locates earthquakes as small as ML~1. We selected <span class="hlt">records</span> of 20 earthquakes located at depths over 20 km. Selection was based on the quality of the routine locations and the visual clarity of the <span class="hlt">records</span>. Arrivals of P and S waves were re-picked, and hypocentral parameters re-established. Newl locations fell within the ranges outlined by historical <span class="hlt">seismicity</span>, confirming the existence of two distinct <span class="hlt">seismically</span> active regions. A shallower zone is at ~20 km depth, and all hypocenters are to the northeast of KVG, in a region between KVG and Shiveluch volcano. A deeper zone is at ~30 km, and all hypocenters cluster directly beneath the edifice of the Kyuchevskoy volcano. Examination of individual <span class="hlt">records</span> shows that earthquakes in both zones are tectonic, with well-defined P and S waves - another distinction of the deep <span class="hlt">seismicity</span> beneath KVG. While the upper <span class="hlt">seismic</span> zone is unquestionably within the crust, the provenance of the deeper earthquakes is enigmatic. The crustal structure beneath KVG is highly complex, with no agreed-upon definition of the crust-mantle boundary. Rather, a range of values, from under 30 to over 40 km, exists in the literature. Similarly, a range of velocity structures has been reported. Teleseismic receiver functions (RFs) provide a way to position the earthquakes with respect to the crust-mantle boundary. We compare the differential travel times of S and P waves from deep</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.S54A..03W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.S54A..03W"><span>The sequentially discounting autoregressive (SDAR) method for on-line automatic <span class="hlt">seismic</span> event detecting on long term observation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wang, L.; Toshioka, T.; Nakajima, T.; Narita, A.; Xue, Z.</p> <p>2017-12-01</p> <p>In recent years, more and more Carbon Capture and Storage (CCS) studies focus on <span class="hlt">seismicity</span> monitoring. For the safety management of geological CO2 storage at Tomakomai, Hokkaido, Japan, an Advanced Traffic Light System (ATLS) combined different <span class="hlt">seismic</span> messages (magnitudes, phases, distributions et al.) is proposed for injection controlling. The primary task for ATLS is the <span class="hlt">seismic</span> events detection in a long-term sustained time series <span class="hlt">record</span>. Considering the time-varying characteristics of Signal to Noise Ratio (SNR) of a long-term <span class="hlt">record</span> and the uneven energy distributions of <span class="hlt">seismic</span> event waveforms will increase the difficulty in automatic <span class="hlt">seismic</span> detecting, in this work, an improved probability autoregressive (AR) method for automatic <span class="hlt">seismic</span> event detecting is applied. This algorithm, called sequentially discounting AR learning (SDAR), can identify the effective <span class="hlt">seismic</span> event in the time series through the Change Point detection (CPD) of the <span class="hlt">seismic</span> <span class="hlt">record</span>. In this method, an anomaly signal (<span class="hlt">seismic</span> event) can be designed as a change point on the time series (<span class="hlt">seismic</span> <span class="hlt">record</span>). The statistical model of the signal in the neighborhood of event point will change, because of the <span class="hlt">seismic</span> event occurrence. This means the SDAR aims to find the statistical irregularities of the <span class="hlt">record</span> thought CPD. There are 3 advantages of SDAR. 1. Anti-noise ability. The SDAR does not use waveform messages (such as amplitude, energy, polarization) for signal detecting. Therefore, it is an appropriate technique for low SNR data. 2. Real-time estimation. When new data appears in the <span class="hlt">record</span>, the probability distribution models can be automatic updated by SDAR for on-line processing. 3. Discounting property. the SDAR introduces a discounting parameter to decrease the influence of present statistic value on future data. It makes SDAR as a robust algorithm for non-stationary signal processing. Within these 3 advantages, the SDAR method can handle the non-stationary time-varying long</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EGUGA..1810035C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EGUGA..1810035C"><span>Long period <span class="hlt">seismic</span> noise modulated by atmospheric tides</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Custódio, Susana; Helffrich, George</p> <p>2016-04-01</p> <p>The amplitudes of long-period (LP) <span class="hlt">seismic</span> noise often exhibit a daily modulation, which is particularly visible on data <span class="hlt">recorded</span> by temporary stations and horizontal components. These daily variations of the LP noise have been associated with temperature fluctuations. Temperature has been suggested to affect the noise <span class="hlt">recorded</span> by seismometers by means of thermal convection around the sensor or by causing thermally induced tilts. Recently, we observed a semi-diurnal (12.0 hr) modulation of LP <span class="hlt">seismic</span> noise amplitudes in seismometers in Portugal, SW Europe. This modulation was associated with the variation of atmospheric pressure, the only environmental signal to display a dominant 12-hr periodicity (at some locations). In this presentation we will present an analysis of this semi-diurnal modulation of long-period <span class="hlt">seismic</span> noise. We show that the modulation: 1) is not instrument dependent, being <span class="hlt">recorded</span> in a variety of sensors; 2) is observed in stations in mainland Portugal, Madeira island (N Atlantic), Florida (USA) and Mozambique, where it is strongest; 3) is seen only at a minority of sites without a clear geographical association, thus appearing to be strongly site-dependent; 5) is stronger during the Summer than during the Winter; and 6) is more clearly seen on vertical components. We will use data from the Transportable Array (EarthScope, USA) to investigate the admittance between LP <span class="hlt">seismic</span> noise variations and co-located atmospheric pressure measurements.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..19.5254P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..19.5254P"><span><span class="hlt">Seismic</span> source parameters of the induced <span class="hlt">seismicity</span> at The Geysers geothermal area, California, by a generalized inversion approach</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Picozzi, Matteo; Oth, Adrien; Parolai, Stefano; Bindi, Dino; De Landro, Grazia; Amoroso, Ortensia</p> <p>2017-04-01</p> <p>The accurate determination of stress drop, <span class="hlt">seismic</span> efficiency and how source parameters scale with earthquake size is an important for <span class="hlt">seismic</span> hazard assessment of induced <span class="hlt">seismicity</span>. We propose an improved non-parametric, data-driven strategy suitable for monitoring induced <span class="hlt">seismicity</span>, which combines the generalized inversion technique together with genetic algorithms. In the first step of the analysis the generalized inversion technique allows for an effective correction of waveforms for the attenuation and site contributions. Then, the retrieved source spectra are inverted by a non-linear sensitivity-driven inversion scheme that allows accurate estimation of source parameters. We therefore investigate the earthquake source characteristics of 633 induced earthquakes (ML 2-4.5) <span class="hlt">recorded</span> at The Geysers geothermal field (California) by a dense <span class="hlt">seismic</span> network (i.e., 32 stations of the Lawrence Berkeley National Laboratory Geysers/Calpine surface <span class="hlt">seismic</span> network, more than 17.000 velocity <span class="hlt">records</span>). We find for most of the events a non-selfsimilar behavior, empirical source spectra that requires ωγ source model with γ > 2 to be well fitted and small radiation efficiency ηSW. All these findings suggest different dynamic rupture processes for smaller and larger earthquakes, and that the proportion of high frequency energy radiation and the amount of energy required to overcome the friction or for the creation of new fractures surface changes with the earthquake size. Furthermore, we observe also two distinct families of events with peculiar source parameters that, in one case suggests the reactivation of deep structures linked to the regional tectonics, while in the other supports the idea of an important role of steeply dipping fault in the fluid pressure diffusion.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMNS14A..05W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMNS14A..05W"><span>Reprocessing <span class="hlt">Seismic</span> Data - Using Wits <span class="hlt">Seismic</span> Exploration Data to Image the Karoo Basin</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Webb, S. J.; Scheiber-Enslin, S. E.; Manzi, M. S.</p> <p>2016-12-01</p> <p>During the heyday of <span class="hlt">seismic</span> exploration of the Witwatersrand Basin, Anglo American's Gold Division acquired several thousand kilometres of Vibroseis reflection <span class="hlt">seismic</span> data. These data, acquired from 1983-1994, were collected with the goal of finding extensions to the Witwatersrand Basin. In a prescient move, over 500 line kilometres were collected at 16 s two way travel time (TWT), extending to depths of 50 -70 km and have provided critical insight into the formation of the Kaapvaal Craton. In addition to these deep <span class="hlt">seismic</span> lines, Anglo American acquired an extensive network of heretofore unpublished <span class="hlt">seismic</span> lines that were collected at 6 sec TWT extending well beyond the known limits of the Witwatersrand Basin. The South African government as part of the national geophysical program in the late 1980s acquired six research reflection <span class="hlt">seismic</span> lines in varied geological settings accruing another 700 km of data. Many of these data are now hosted at the University of the Witwatersrand's newly established <span class="hlt">Seismic</span> Research Centre and represent unprecedented coverage and research opportunities. With recent global interest in shale gas, attention focused on the Karoo Basin in South Africa. Early exploration <span class="hlt">seismic</span> data acquired by Soekor in the 1970s has been lost; however, digitized paper <span class="hlt">records</span> indicate clear reflection targets. Here we examine one of the AngloGold <span class="hlt">seismic</span> lines that was acquired in the middle of the Karoo Basin just south of Trompsburg extending to the southeast towards Molteno. This 150 km long line crosses the edge of the Kaapvaal Craton and shows clear reflectors throughout the Karoo Basin. These include the well-defined base of the Karoo and a number of dolerite sills within it. Nearby gas escape structures have been identified on surface and it is likely that several disruptions along this line are related to these or to dykes associated with the sills.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010EGUGA..1211958R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010EGUGA..1211958R"><span><span class="hlt">Seismic</span> Activity offshore Martinique and Dominique islands (Lesser Antilles subduction zone)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ruiz Fernandez, Mario; Galve, Audrey; Monfret, Tony; Charvis, Philippe; Laigle, Mireille; Flueh, Ernst; Gallart, Josep; Hello, Yann</p> <p>2010-05-01</p> <p>In the framework of the European project Thales was Right, two <span class="hlt">seismic</span> surveys (Sismantilles II and Obsantilles) were carried out to better constrain the lithospheric structure of the Lesser Antilles subduction zone, its <span class="hlt">seismic</span> activity and to evaluate the associated <span class="hlt">seismic</span> hazards. Sismantilles II experiment was conducted in January, 2007 onboard R/V Atalante (IFREMER). A total of 90 OBS belonging to Géoazur, INSU-CNRS and IFM-Geomar were deployed on a regular grid, offshore Antigua, Guadeloupe, Dominique and Martinique islands. During the active part of the survey, more than 2500 km of multichannel <span class="hlt">seismic</span> profiles were shot along the grid lines. Then the OBS remained on the seafloor continuously <span class="hlt">recording</span> for the <span class="hlt">seismic</span> activity for approximately 4 months. On April 2007 Obsantilles experiment, carried out onboard R/V Antea (IRD), was focused on the recovery of those OBS and the redeployment of 28 instruments (Géoazur OBS) off Martinique and Dominica Islands for 4 additional months of continuous <span class="hlt">recording</span> of the <span class="hlt">seismicity</span>. This work focuses on the analysis of the seismological data <span class="hlt">recorded</span> in the southern sector of the study area, offshore Martinique and Dominique. During the two <span class="hlt">recording</span> periods, extending from January to the end of August 2007, more than 3300 <span class="hlt">seismic</span> events were detected in this area. Approximately 1100 earthquakes had enough quality to be correctly located. Station corrections, obtained from multichannel <span class="hlt">seismic</span> profiles, were introduced to each OBS to take in to account the sedimentary cover and better constrain the hypocentral determinations. Results show events located at shallower depths in the northern sector of the array, close to the Tiburon Ridge, where the <span class="hlt">seismic</span> activity is mainly located between 20 to 40 km depth. In the southern sector, offshore Martinique, hypocenters become deeper, ranging to 60 km depth and dipping to the west. Focal solutions have also been obtained using the P wave polarities of the best azimuthally</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.S43D0884G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.S43D0884G"><span>Spatial Distribution of <span class="hlt">Seismic</span> Anisotropy in the Crust in the Northeast Front Zone of Tibetan Plateau</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gao, Y.; Wang, Q.; SHI, Y.</p> <p>2017-12-01</p> <p>There are orogenic belts and strong deformation in northeastern zone of Tibetan Plateau. The media in crust and in the upper mantle are <span class="hlt">seismic</span> anisotropic there. This study uses <span class="hlt">seismic</span> <span class="hlt">records</span> by permanent <span class="hlt">seismic</span> stations and portable <span class="hlt">seismic</span> arrays, and adopts analysis techniques on body waves to obtain spatial anisotropic distribution in northeastern front zone of Tibetan Plateau. With <span class="hlt">seismic</span> <span class="hlt">records</span> of small local earthquakes, we study shear-wave splitting in the upper crust. The polarization of fast shear wave (PFS) can be obtained, and PFS is considered parallel to the strike of the cracks, as well as the direction of maximum horizontal compressive stress. However, the result shows the strong influence from tectonics, such as faults. It suggests multiple-influence including stress and fault. Spatial distribution of <span class="hlt">seismic</span> anisotropy in study zone presents the effect in short range. PFS at the station on the strike-slip fault is quite different to PFS at station just hundreds of meters away from the fault. With <span class="hlt">seismic</span> <span class="hlt">records</span> of teleseismic waveforms, we obtained <span class="hlt">seismic</span> anisotropy in the whole crust by receiver functions. The PFS directions from Pms receiver functions show consistency, generally in WNW. The time-delay of slow S phases is significant. With <span class="hlt">seismic</span> <span class="hlt">records</span> of SKS, PKS and SKKS phases, we can detect <span class="hlt">seismic</span> anisotropy in the upper mantle by splitting analysis. The fast directions of these phases also show consistency, generally in WNW, similar to those of receiver functions, but larger time-delays. It suggests significant <span class="hlt">seismic</span> anisotropy in the crust and crustal deformation is coherent to that in the upper mantle.<span class="hlt">Seismic</span> anisotropy in the upper crust, in the whole crust and in the upper mantle are discussed both in difference and tectonic implications [Grateful to the support by NSFC Project 41474032].</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.usgs.gov/pp/1750/chapters/pp2008-1750_chapter07.pdf','USGSPUBS'); return false;" href="https://pubs.usgs.gov/pp/1750/chapters/pp2008-1750_chapter07.pdf"><span><span class="hlt">Seismic</span>-monitoring changes and the remote deployment of <span class="hlt">seismic</span> stations (<span class="hlt">seismic</span> spider) at Mount St. Helens, 2004-2005: Chapter 7 in A volcano rekindled: the renewed eruption of Mount St. Helens, 2004-2006</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>McChesney, Patrick J.; Couchman, Marvin R.; Moran, Seth C.; Lockhart, Andrew B.; Swinford, Kelly J.; LaHusen, Richard G.; Sherrod, David R.; Scott, William E.; Stauffer, Peter H.</p> <p>2008-01-01</p> <p>The instruments in place at the start of volcanic unrest at Mount St. Helens in 2004 were inadequate to <span class="hlt">record</span> the large earthquakes and monitor the explosions that occurred as the eruption developed. To remedy this, new instruments were deployed and the short-period <span class="hlt">seismic</span> network was modified. A new method of establishing near-field <span class="hlt">seismic</span> monitoring was developed, using remote deployment by helicopter. The remotely deployed <span class="hlt">seismic</span> sensor was a piezoelectric accelerometer mounted on a surface-coupled platform. Remote deployment enabled placement of stations within 250 m of the active vent.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018GeoJI.213..931H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018GeoJI.213..931H"><span>Post-<span class="hlt">seismic</span> velocity changes following the 2010 Mw 7.1 Darfield earthquake, New Zealand, revealed by ambient <span class="hlt">seismic</span> field analysis</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Heckels, R. EG; Savage, M. K.; Townend, J.</p> <p>2018-05-01</p> <p>Quantifying <span class="hlt">seismic</span> velocity changes following large earthquakes can provide insights into fault healing and reloading processes. This study presents temporal velocity changes detected following the 2010 September Mw 7.1 Darfield event in Canterbury, New Zealand. We use continuous waveform data from several temporary <span class="hlt">seismic</span> networks lying on and surrounding the Greendale Fault, with a maximum interstation distance of 156 km. Nine-component, day-long Green's functions were computed for frequencies between 0.1 and 1.0 Hz for continuous <span class="hlt">seismic</span> <span class="hlt">records</span> from immediately after the 2010 September 04 earthquake until 2011 January 10. Using the moving-window cross-spectral method, <span class="hlt">seismic</span> velocity changes were calculated. Over the study period, an increase in <span class="hlt">seismic</span> velocity of 0.14 ± 0.04 per cent was determined near the Greendale Fault, providing a new constraint on post-<span class="hlt">seismic</span> relaxation rates in the region. A depth analysis further showed that velocity changes were confined to the uppermost 5 km of the subsurface. We attribute the observed changes to post-<span class="hlt">seismic</span> relaxation via crack healing of the Greendale Fault and throughout the surrounding region.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.S13B0656W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.S13B0656W"><span>Precision <span class="hlt">Seismic</span> Monitoring of Volcanic Eruptions at Axial Seamount</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Waldhauser, F.; Wilcock, W. S. D.; Tolstoy, M.; Baillard, C.; Tan, Y. J.; Schaff, D. P.</p> <p>2017-12-01</p> <p>Seven permanent ocean bottom seismometers of the Ocean Observatories Initiative's real time cabled observatory at Axial Seamount off the coast of the western United States <span class="hlt">record</span> <span class="hlt">seismic</span> activity since 2014. The array captured the April 2015 eruption, shedding light on the detailed structure and dynamics of the volcano and the Juan de Fuca midocean ridge system (Wilcock et al., 2016). After a period of continuously increasing <span class="hlt">seismic</span> activity primarily associated with the reactivation of caldera ring faults, and the subsequent <span class="hlt">seismic</span> crisis on April 24, 2015 with 7000 <span class="hlt">recorded</span> events that day, <span class="hlt">seismicity</span> rates steadily declined and the array currently <span class="hlt">records</span> an average of 5 events per day. Here we present results from ongoing efforts to automatically detect and precisely locate <span class="hlt">seismic</span> events at Axial in real-time, providing the computational framework and fundamental data that will allow rapid characterization and analysis of spatio-temporal changes in seismogenic properties. We combine a kurtosis-based P- and S-phase onset picker and time domain cross-correlation detection and phase delay timing algorithms together with single-event and double-difference location methods to rapidly and precisely (tens of meters) compute the location and magnitudes of new events with respect to a 2-year long, high-resolution background catalog that includes nearly 100,000 events within a 5×5 km region. We extend the real-time double-difference location software DD-RT to efficiently handle the anticipated high-rate and high-density earthquake activity during future eruptions. The modular monitoring framework will allow real-time tracking of other <span class="hlt">seismic</span> events such as tremors and sea-floor lava explosions that enable the timing and location of lava flows and thus guide response research cruises to the most interesting sites. Finally, rapid detection of eruption precursors and initiation will allow for adaptive sampling by the OOI instruments for optimal <span class="hlt">recording</span> of future</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1252131','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1252131"><span><span class="hlt">Seismic</span> Fracture Characterization Methodologies for Enhanced Geothermal Systems</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Queen, John H.</p> <p>2016-05-09</p> <p>Executive Summary The overall objective of this work was the development of surface and borehole <span class="hlt">seismic</span> methodologies using both compressional and shear waves for characterizing faults and fractures in Enhanced Geothermal Systems. We used both surface <span class="hlt">seismic</span> and vertical <span class="hlt">seismic</span> profile (VSP) methods. We adapted these methods to the unique conditions encountered in Enhanced Geothermal Systems (EGS) creation. These conditions include geological environments with volcanic cover, highly altered rocks, severe structure, extreme near surface velocity contrasts and lack of distinct velocity contrasts at depth. One of the objectives was the development of methods for identifying more appropriate <span class="hlt">seismic</span> acquisition parametersmore » for overcoming problems associated with these geological factors. Because temperatures up to 300º <span class="hlt">C</span> are often encountered in these systems, another objective was the testing of VSP borehole tools capable of operating at depths in excess of 1,000 m and at temperatures in excess of 200º <span class="hlt">C</span>. A final objective was the development of new processing and interpretation techniques based on scattering and time-frequency analysis, as well as the application of modern <span class="hlt">seismic</span> migration imaging algorithms to <span class="hlt">seismic</span> data acquired over geothermal areas. The use of surface <span class="hlt">seismic</span> reflection data at Brady's Hot Springs was found useful in building a geological model, but only when combined with other extensive geological and geophysical data. The use of fine source and geophone spacing was critical in producing useful images. The surface <span class="hlt">seismic</span> reflection data gave no information about the internal structure (extent, thickness and filling) of faults and fractures, and modeling suggests that they are unlikely to do so. Time-frequency analysis was applied to these data, but was not found to be significantly useful in their interpretation. Modeling does indicate that VSP and other <span class="hlt">seismic</span> methods with sensors located at depth in wells will be the most</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..1910571S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..1910571S"><span>Design and implementation of a low-cost multichannel <span class="hlt">seismic</span> noise <span class="hlt">recorder</span> for array measurements</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Soler-Llorens, Juan Luis; Juan Giner-Caturla, Jose; Molina-Palacios, Sergio; Galiana-Merino, Juan Jose; Rosa-Herranz, Julio; Agea-Medina, Noelia</p> <p>2017-04-01</p> <p>Soil characterization is the starting point for <span class="hlt">seismic</span> hazard studies. Currently, the methods based on ambient noise measurements are very used because they are non-invasive methods and relatively easy to implement in urban areas. Among these methods, the analysis of array measurements provides the dispersion curve and subsequently the shear-wave velocity profile associated to the site under study. In this case, we need several sensors <span class="hlt">recording</span> simultaneously and a data acquisition system with one channel by sensor, what can become the complete equipment unaffordable for small research groups. In this work, we have designed and implemented a low-cost multichannel ambient noise <span class="hlt">recorder</span> for array measurements. The complete system is based on Arduino, an open source electronic development platform, which allows <span class="hlt">recording</span> 12 differential input channels simultaneously. Besides, it is complemented with a conditioning circuit that includes an anti-aliasing filter and a selectable gain between 0 and 40dB. The data acquisition is set up through a user-friendly graphical user interface. It is important to note that the electronic scheme as well as the programming code are open hardware and software, respectively, so it allows other researchers to suite the system to their particular requirements. The developed equipment has been tested at several sites around the province of Alicante (southeast of Spain), where the soil characteristics are well-known from previous studies. Array measurements have been taken and after that, the <span class="hlt">recorded</span> data have been analysed using the frequency-wavenumber (f-k) and the extended spatial autocorrelation (ESAC) methods. The comparison of the obtained dispersion curves with the ones obtained in previous studies shows the suitability of the implemented low-cost system for array measurements.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li class="active"><span>12</span></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_12 --> <div id="page_13" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li class="active"><span>13</span></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="241"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.S31A0801L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.S31A0801L"><span>Investigating the ocean generated acoustic/<span class="hlt">seismic</span> wavefields in NE Atlantic</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Le Pape, F.; Bean, C. J.; Craig, D.; Jousset, P.; Donne, S. E.; Möllhoff, M.</p> <p>2017-12-01</p> <p>In this study, we look at the comparison of 3D simulations of acoustic and <span class="hlt">seismic</span> waves propagation with OBS data <span class="hlt">recorded</span> across the shelf offshore Ireland and out into the Rockall Trough. Real and synthetic observations are combined to characterize both acoustic and <span class="hlt">seismic</span> wavefields in the marine environment and particularly study secondary microseisms propagation from deep to shallow water to the land. Whereas the <span class="hlt">recorded</span> OBS data show a strong change in the energy of "noise events" in the primary microseism band from the shelf to the land, the secondary microseism band is associated with stronger signal in the deep water compared to the shelf area. Furthermore, the data also highlight seasonal variations in the <span class="hlt">seismic</span> and acoustic wavefields likely related to changes in noise source locations. The 3D simulations of acoustic and <span class="hlt">seismic</span> waves propagation in the Rockall Trough look promising to reconcile deep ocean, shelf and land <span class="hlt">seismic</span> observations as well as the effect of the water column and sediments thickness on "<span class="hlt">seismic</span> ambient noise" generation and propagation. For instance, the simulations reveal interesting results on the acoustic/<span class="hlt">seismic</span> coupling and its implication on the secondary microseisms source origin. This project is part of the Irish Centre for Research in Applied Geoscience (ICRAG), funded under the SFI Research Centres Programme and is co-funded under the European Regional Development Fund.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EGUGA..18.2131G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EGUGA..18.2131G"><span><span class="hlt">Seismic</span> Techniques for Subsurface Voids Detection</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gritto, Roland; Korneev, Valeri; Elobaid Elnaiem, Ali; Mohamed, Fathelrahman; Sadooni, Fadhil</p> <p>2016-04-01</p> <p> orthogonal transmission surveys to detect and locate the object. Furthermore, we showed that ambient noise <span class="hlt">recordings</span> may generate data with sufficient signal-to-noise ratio to successfully detect and locate subsurface voids. Being able to use ambient noise <span class="hlt">recordings</span> would eliminate the need to employ active <span class="hlt">seismic</span> sources that are time consuming and more expensive to operate.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015EGUGA..17.1666C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015EGUGA..17.1666C"><span><span class="hlt">Seismic</span> anisotropy in the lower crust: The link between rock composition, microstructure, texture and <span class="hlt">seismic</span> properties.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Czaplinska, Daria; Piazolo, Sandra; Almqvist, Bjarne</p> <p>2015-04-01</p> <p><span class="hlt">Seismic</span> anisotropy observed in Earth's interior is caused by the presence of aligned anisotropic minerals (crystallographic and shape preferred orientation; CPO and SPO respectively), and fluid and/or melt inclusions related to deformation. Therefore, the variations in <span class="hlt">seismic</span> anisotropy carry valuable information about the structure of the mantle and crust. For example, anisotropy observed in the upper mantle is mainly attributed to the CPO of olivine, and provides strong evidence for the flow within the upper mantle. <span class="hlt">Seismic</span> anisotropy in the crust is still poorly constrained, mostly due to the much larger heterogeneity of the crustal rocks in comparison with the more homogenous mantle. Anisotropy in the crust will be affected by the variations in rock composition, microstructure, texture (presence or lack of CPO), brittle structures (e.g. fracture systems) and chemical composition of the minerals. However, once the relationships between those variables and <span class="hlt">seismic</span> properties of the crustal rocks are established, <span class="hlt">seismic</span> anisotropy can be used to derive characteristics of rocks otherwise out of reach. Our study focuses on two sets of samples of middle to lower crustal rocks collected in Fiordland (New Zealand) and in Sweden. Samples from Fiordland represent a root of a thick (ca. 80 km) magmatic arc and comprise igneous rocks, which crystallized at high P and T conditions and were subsequently metamorphosed and deformed. Samples from Sweden are derived from a metasedimentary nappe in the Caledonian orogenic belt, which is mostly composed of gneisses, amphibolites and calc-silicates that have experienced different amounts of strain. We use large area EBSD mapping to measure the CPO of the constituent phases and <span class="hlt">record</span> the geometric relationships of the rock microstructure. Data is then used to calculate the elastic properties of the rock from single-crystal stiffnesses. Here, we utilize the EBSD GUI software (Cook et al., 2013), which offers varied homogenization</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/15016015','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/15016015"><span><span class="hlt">Seismic</span> Monitoring for the United Arab Emirates</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Rodgers, A; Nakanishi, K</p> <p>2005-04-11</p> <p>There is potential for earthquakes in the United Arab Emirates and in the Zagros mountains to cause structural damage and pose a threat to safety of people. Damaging effects from earthquakes can be mitigated by knowledge of the location and size of earthquakes, effects on construction, and monitoring these effects over time. Although a general idea of <span class="hlt">seismicity</span> in the UAE may be determined with data from global <span class="hlt">seismic</span> networks, these global networks do not have the sensitivity to <span class="hlt">record</span> smaller <span class="hlt">seismic</span> events and do not have the necessary accuracy to locate the events. A National <span class="hlt">Seismic</span> Monitoring Observatory ismore » needed for the UAE that consists of a modern <span class="hlt">seismic</span> network and a multidisciplinary staff that can analyze and interpret the data from the network. A <span class="hlt">seismic</span> network is essential to locate earthquakes, determine event magnitudes, identify active faults and measure ground motions from earthquakes. Such a network can provide the data necessary for a reliable <span class="hlt">seismic</span> hazard assessment in the UAE. The National <span class="hlt">Seismic</span> Monitoring Observatory would ideally be situated at a university that would provide access to the wide range of disciplines needed in operating the network and providing expertise in analysis and interpretation.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.T31C0641G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.T31C0641G"><span>Porosity, Fracturing and Alteration of Young Oceanic Crust: New <span class="hlt">Seismic</span> Analyses at Borehole 504B</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gregory, E. P. M.; Hobbs, R. W.; Peirce, C.; Wilson, D. J.</p> <p>2017-12-01</p> <p>DSDP/ODP borehole 504B, drilled 2111 m into 6.9 Ma oceanic crust, provides in-situ core and logging measurements of the lithology, fracturing and porosity of crust originally formed at the Costa Rica Rift and its subsequent alteration by hydrothermal fluids. A recent active <span class="hlt">seismic</span> survey over the borehole and surrounding area reveals wider spatial variations in velocity that can be related to this porosity and fracturing. Over 10,000 airgun shots were fired in a 30 x 30 km grid over the borehole region, using both high-frequency and low-frequency airgun arrays. The shots were <span class="hlt">recorded</span> on a 4.5 km-long streamer and 24 ocean-bottom seismographs, each equipped with a three-component geophone and an hydrophone. A vertical hydrophone array <span class="hlt">recorded</span> the downgoing source wavelet, and underway gravity, magnetic field and multibeam bathymetry data were also <span class="hlt">recorded</span>. This combined dataset enables the most comprehensive geophysical analysis of this area of crust to date, while the ground-truthing provided by 504B enables us to address the questions of what do the <span class="hlt">seismic</span> oceanic crustal layers represent and what controls their characteristics as the crust ages? Wide-angle <span class="hlt">seismic</span> modelling with a Monte Carlo based uncertainty analysis reveals new 2D and 3D Vp and Vs models of the area, which show relatively homogeneous crust around borehole 504B, and place the <span class="hlt">seismic</span> layer 2B/2<span class="hlt">C</span>, and <span class="hlt">seismic</span> layer 2/3 boundaries coincident with fracturing and alteration fronts rather than the lithological boundaries between lavas and dykes, and dykes and gabbros, respectively. Analysis of Poisson's ratio, <span class="hlt">seismic</span> anisotropy and particle motions reveal patterns in fracturing and porosity across the survey area, and locate possible fossilised hydrothermal circulation cells. These cells appear to have influenced the porosity of the crust through alteration and mineralisation processes, with faults inherited from initial crustal accretion influencing basement topographic highs and providing</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008AGUFM.H51F0897Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008AGUFM.H51F0897Z"><span><span class="hlt">Seismic</span> Monitoring of Rock Falls in Yosemite National Park</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zimmer, V. L.; Stock, G. M.; Sitar, N.</p> <p>2008-12-01</p> <p>Between 1857 and 2007, more than 600 landslide events have been documented in Yosemite National Park, with the vast majority of events occurring as rock falls in Yosemite Valley. The conditions leading to and triggering rock fall are understood in approximately 50 percent of cases, but in the other 50 percent, there were no apparent triggers. Occasionally, large rock falls have been preceded by smaller events that, in retrospect, may have been precursors. Close range <span class="hlt">seismic</span> monitoring presents an opportunity to study the conditions leading up to rock fall, as well as the mechanics of the actual rock fall as <span class="hlt">recorded</span> <span class="hlt">seismically</span>. During the winter of 2007-08, we conducted a rock fall <span class="hlt">seismic</span> monitoring feasibility study in Yosemite Valley. A station consisting of an 8 Hz geophone and an accelerometer was placed on a ledge 1000 feet above the valley floor, in a historically active rock fall area known as the Three Brothers. At least two rock falls in this area were <span class="hlt">recorded</span> by the instrumentation and witnessed by visitors, representing the first time rock falls have been <span class="hlt">recorded</span> with <span class="hlt">seismic</span> instrumentation in Yosemite Valley. Significant energy was <span class="hlt">recorded</span> in a wide frequency range, from a few Hz to approximately 150 Hz, limited by the geophone response and attenuation of the signal due to distance to the source (400 m). Furthermore, there exists a weak signal approximately 5-10 seconds before the obvious rock fall signature. We hypothesize that the weak signal represents rock fall initiation manifesting as the first blocks sliding down the cliff face, while the stronger impulses represent these blocks impacting ledges and the bottom talus field. This study demonstrated that rock fall monitoring is feasible with <span class="hlt">seismic</span> instrumentation, and serves as the catalyst for future studies using a network of sensors for more advanced analysis.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70023654','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70023654"><span><span class="hlt">Seismic</span> reflection images of shallow faulting, northernmost Mississippi embayment, north of the New Madrid <span class="hlt">seismic</span> zone</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>McBride, J.H.; Nelson, W.J.</p> <p>2001-01-01</p> <p>High-resolution <span class="hlt">seismic</span> reflection surveys document tectonic faults that displace Pleistocene and older strata just beyond the northeast termination of the New Madrid <span class="hlt">seismic</span> zone, at the northernmost extent of the Mississippi embayment. These faults, which are part of the Fluorspar Area fault complex in southeastern Illinois, are directly in line with the northeast-trending <span class="hlt">seismic</span> zone. The reflection data were acquired using an elastic weight-drop source <span class="hlt">recorded</span> to 500 msec by a 48-geophone array (24-fold) with a 10-ft (??3.0m) station interval. Recognizable reflections were <span class="hlt">recorded</span> to about 200 msec (100-150 m). The effects of multiple reflections, numerous diffractions, low apparent velocity (i.e., steeply dipping) noise, and the relatively low-frequency content of the <span class="hlt">recorded</span> signal provided challenges for data processing and interpreting subtle fault offsets. Data processing steps that were critical to the detection of faults included residual statics, post-stack migration, deconvolution, and noise-reduction filtering. <span class="hlt">Seismic</span> migration was crucial for detecting and mitigating complex fault-related diffraction patterns, which produced an apparent 'folding' of reflectors on unmigrated sections. Detected individual offsets of shallow reflectors range from 5 to 10 m for the top of Paleozoic bedrock and younger strata. The migrated sections generally indicate vertical to steeply dipping normal and reverse faults, which in places outline small horsts and/or grabens. Tilting or folding of stratal reflectors associated with faulting is also locally observed. At one site, the observed faulting is superimposed over a prominent antiformal structure, which may itself be a product of the Quaternary deformation that produced the steep normal and reverse faults. Our results suggest that faulting of the Paleozoic bedrock and younger sediments of the northern Mississippi embayment is more pervasive and less localized than previously thought.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.S31E..01V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.S31E..01V"><span>Global <span class="hlt">Seismic</span> Cross-Correlation Results: Characterizing Repeating <span class="hlt">Seismic</span> Events</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Vieceli, R.; Dodge, D. A.; Walter, W. R.</p> <p>2016-12-01</p> <p>Increases in <span class="hlt">seismic</span> instrument quality and coverage have led to increased knowledge of earthquakes, but have also revealed the complex and diverse nature of earthquake ruptures. Nonetheless, some earthquakes are sufficiently similar to each other that they produce correlated waveforms. Such repeating events have been used to investigate interplate coupling of subduction zones [e.g. Igarashi, 2010; Yu, 2013], study spatio-temporal changes in slip rate at plate boundaries [e.g. Igarashi et al., 2003], observe variations in <span class="hlt">seismic</span> wave propagation velocities in the crust [e.g. Schaff and Beroza, 2004; Sawazaki et al., 2015], and assess inner core rotation [e.g. Yu, 2016]. The characterization of repeating events on a global scale remains a very challenging problem. An initial global <span class="hlt">seismic</span> cross-correlation study used over 310 million waveforms from nearly 3.8 million events <span class="hlt">recorded</span> between 1970 and 2013 to determine an initial look at global correlated <span class="hlt">seismicity</span> [Dodge and Walter, 2015]. In this work, we analyze the spatial and temporal distribution of the most highly correlated event clusters or "multiplets" from the Dodge and Walter [2015] study. We examine how the distributions and characteristics of multiplets are effected by tectonic environment, source-station separation, and frequency band. Preliminary results suggest that the distribution of multiplets does not correspond to the tectonic environment in any obvious way, nor do they always coincide with the occurrence of large earthquakes. Future work will focus on clustering correlated pairs and working to reduce the bias introduced by non-uniform <span class="hlt">seismic</span> station coverage and data availability. This work performed under the auspices of the U.S. Department of Energy by Lawrence Livermore National Laboratory under Contract DE-AC52-07NA27344.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.U23B..01K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.U23B..01K"><span>Back-Projection Imaging of extended, diffuse <span class="hlt">seismic</span> sources in volcanic and hydrothermal systems</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kelly, C. L.; Lawrence, J. F.; Beroza, G. C.</p> <p>2017-12-01</p> <p>Volcanic and hydrothermal systems exhibit a wide range of <span class="hlt">seismicity</span> that is directly linked to fluid and volatile activity in the subsurface and that can be indicative of imminent hazardous activity. Seismograms <span class="hlt">recorded</span> near volcanic and hydrothermal systems typically contain "noisy" <span class="hlt">records</span>, but in fact, these complex signals are generated by many overlapping low-magnitude displacements and pressure changes at depth. Unfortunately, excluding times of high-magnitude eruptive activity that typically occur infrequently relative to the length of a system's entire eruption cycle, these signals often have very low signal-to-noise ratios and are difficult to identify and study using established <span class="hlt">seismic</span> analysis techniques (i.e. phase-picking, template matching). Arrays of short-period and broadband <span class="hlt">seismic</span> sensors are proven tools for monitoring short- and long-term changes in volcanic and hydrothermal systems. Time-reversal techniques (i.e. back-projection) that are improved by additional <span class="hlt">seismic</span> observations have been successfully applied to locating volcano-<span class="hlt">seismic</span> sources <span class="hlt">recorded</span> by dense sensor arrays. We present results from a new computationally efficient back-projection method that allows us to image the evolution of extended, diffuse sources of volcanic and hydrothermal <span class="hlt">seismicity</span>. We correlate short time-window seismograms from receiver-pairs to find coherent signals and propagate them back in time to potential source locations in a 3D subsurface model. The strength of coherent <span class="hlt">seismic</span> signal associated with any potential source-receiver-receiver geometry is equal to the correlation of the short time-windows of <span class="hlt">seismic</span> <span class="hlt">records</span> at appropriate time lags as determined by the velocity structure and ray paths. We stack (sum) all short time-window correlations from all receiver-pairs to determine the cumulative coherence of signals at each potential source location. Through stacking, coherent signals from extended and/or repeating sources of short-period energy</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.usgs.gov/of/2000/ofr-00-0286/','USGSPUBS'); return false;" href="https://pubs.usgs.gov/of/2000/ofr-00-0286/"><span>Regional <span class="hlt">seismic</span> lines reprocessed using post-stack processing techniques; National Petroleum Reserve, Alaska</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Miller, John J.; Agena, W.F.; Lee, M.W.; Zihlman, F.N.; Grow, J.A.; Taylor, D.J.; Killgore, Michele; Oliver, H.L.</p> <p>2000-01-01</p> <p>This CD-ROM contains stacked, migrated, 2-Dimensional <span class="hlt">seismic</span> reflection data and associated support information for 22 regional <span class="hlt">seismic</span> lines (3,470 line-miles) <span class="hlt">recorded</span> in the National Petroleum Reserve ? Alaska (NPRA) from 1974 through 1981. Together, these lines constitute about one-quarter of the <span class="hlt">seismic</span> data collected as part of the Federal Government?s program to evaluate the petroleum potential of the Reserve. The regional lines, which form a grid covering the entire NPRA, were created by combining various individual lines <span class="hlt">recorded</span> in different years using different <span class="hlt">recording</span> parameters. These data were reprocessed by the USGS using modern, post-stack processing techniques, to create a data set suitable for interpretation on interactive <span class="hlt">seismic</span> interpretation computer workstations. Reprocessing was done in support of ongoing petroleum resource studies by the USGS Energy Program. The CD-ROM contains the following files: 1) 22 files containing the digital <span class="hlt">seismic</span> data in standard, SEG-Y format; 2) 1 file containing navigation data for the 22 lines in standard SEG-P1 format; 3) 22 small scale graphic images of each <span class="hlt">seismic</span> line in Adobe Acrobat? PDF format; 4) a graphic image of the location map, generated from the navigation file, with hyperlinks to the graphic images of the <span class="hlt">seismic</span> lines; 5) an ASCII text file with cross-reference information for relating the sequential trace numbers on each regional line to the line number and shotpoint number of the original component lines; and 6) an explanation of the processing used to create the final <span class="hlt">seismic</span> sections (this document). The SEG-Y format <span class="hlt">seismic</span> files and SEG-P1 format navigation file contain all the information necessary for loading the data onto a <span class="hlt">seismic</span> interpretation workstation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFM.S33F..02G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFM.S33F..02G"><span>The Utility of the Extended Images in Ambient <span class="hlt">Seismic</span> Wavefield Migration</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Girard, A. J.; Shragge, J. C.</p> <p>2015-12-01</p> <p>Active-source 3D <span class="hlt">seismic</span> migration and migration velocity analysis (MVA) are robust and highly used methods for imaging Earth structure. One class of migration methods uses extended images constructed by incorporating spatial and/or temporal wavefield correlation lags to the imaging conditions. These extended images allow users to directly assess whether images focus better with different parameters, which leads to MVA techniques that are based on the tenets of adjoint-state theory. Under certain conditions (e.g., geographical, cultural or financial), however, active-source methods can prove impractical. Utilizing ambient <span class="hlt">seismic</span> energy that naturally propagates through the Earth is an alternate method currently used in the scientific community. Thus, an open question is whether extended images are similarly useful for ambient <span class="hlt">seismic</span> migration processing and verifying subsurface velocity models, and whether one can similarly apply adjoint-state methods to perform ambient migration velocity analysis (AMVA). Herein, we conduct a number of numerical experiments that construct extended images from ambient <span class="hlt">seismic</span> <span class="hlt">recordings</span>. We demonstrate that, similar to active-source methods, there is a sensitivity to velocity in ambient <span class="hlt">seismic</span> <span class="hlt">recordings</span> in the migrated extended image domain. In synthetic ambient imaging tests with varying degrees of error introduced to the velocity model, the extended images are sensitive to velocity model errors. To determine the extent of this sensitivity, we utilize acoustic wave-equation propagation and cross-correlation-based migration methods to image weak body-wave signals present in the <span class="hlt">recordings</span>. Importantly, we have also observed scenarios where non-zero correlation lags show signal while zero-lags show none. This may be a valuable missing piece for ambient migration techniques that have yielded largely inconclusive results, and might be an important piece of information for performing AMVA from ambient <span class="hlt">seismic</span> <span class="hlt">recordings</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..19.4942F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..19.4942F"><span>Broadband <span class="hlt">seismic</span> effects from train vibrations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Fuchs, Florian; Bokelmann, Götz</p> <p>2017-04-01</p> <p>Seismologists rarely study train induced vibrations which are mainly regarded an unwanted source of noise for classical seismological applications such as earthquake monitoring. A few seismological studies try to utilize train vibrations however as active sources, e.g. for subsurface imaging, but they do not focus on the characteristics of the train signal itself. Most available studies on train induced vibrations take an engineering approach and aim at better understanding the generation and short-distance propagation of train induced vibrations, mainly for mitigation and construction purposes. They mostly rely on numerical simulations and/or short-period or accelerometer <span class="hlt">recordings</span> obtained directly on the train track or up to few hundred meters away and almost no studies exist with <span class="hlt">seismic</span> <span class="hlt">recordings</span> further away from the track. In some of these previous studies sharp and equidistant peaks are present in the vibration spectrum of heavy freight trains, but they do not attempt to explain them. Here we show and analyze various train vibration signals obtained from a set of <span class="hlt">seismic</span> broadband stations installed in the context of the temporary, large-scale regional <span class="hlt">seismic</span> network AlpArray. The geometrical restrictions of this <span class="hlt">seismic</span> network combined with budget and safety considerations resulted in a number of broad-band instruments deployed in the vicinity of busy railway lines. On these stations we observe very characteristic <span class="hlt">seismic</span> signals associated with different types of trains, typically showing pronounced equidistant spectral lines over a wide frequency range. In this study we analyze the nature of such signals and discuss if they are generated by a source effect or by wave propagation effects in near-surface soil layers.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70147411','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70147411"><span>Ground motions <span class="hlt">recorded</span> in Rome during the April 2009 L’Aquila <span class="hlt">seismic</span> sequence: site response and comparison with ground‐motion predictions based on a global dataset</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Caserta, Arrigo; Boore, David; Rovelli, Antonio; Govoni, Aladino; Marra, Fabrizio; Monica, Gieseppe Della; Boschi, Enzo</p> <p>2013-01-01</p> <p>The mainshock and moderate‐magnitude aftershocks of the 6 April 2009 M 6.3 L’Aquila <span class="hlt">seismic</span> sequence, about 90 km northeast of Rome, provided the first earthquake ground‐motion <span class="hlt">recordings</span> in the urban area of Rome. Before those <span class="hlt">recordings</span> were obtained, the assessments of the <span class="hlt">seismic</span> hazard in Rome were based on intensity observations and theoretical considerations. The L’Aquila <span class="hlt">recordings</span> offer an unprecedented opportunity to calibrate the city response to central Apennine earthquakes—earthquakes that have been responsible for the largest damage to Rome in historical times. Using the data <span class="hlt">recorded</span> in Rome in April 2009, we show that (1) published theoretical predictions of a 1 s resonance in the Tiber valley are confirmed by observations showing a significant amplitude increase in response spectra at that period, (2) the empirical soil‐transfer functions inferred from spectral ratios are satisfactorily fit through 1D models using the available geological, geophysical, and laboratory data, but local variability can be large for individual events, (3) response spectra for the motions <span class="hlt">recorded</span> in Rome from the L’Aquila earthquakes are significantly amplified in the radial component at periods near 1 s, even at a firm site on volcanic rocks, and (4) short‐period response spectra are smaller than expected when compared to ground‐motion predictions from equations based on a global dataset, whereas the observed response spectra are higher than expected for periods near 1 s.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012AGUFMNH11A1538K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012AGUFMNH11A1538K"><span>Frequency Distribution of <span class="hlt">Seismic</span> Intensity in Japan between 1950 and 2009</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kato, M.; Kohayakawa, Y.</p> <p>2012-12-01</p> <p>JMA <span class="hlt">Seismic</span> Intensity is an index of <span class="hlt">seismic</span> ground motion which is frequently used and reported in the media. While it is always difficult to represent complex ground motion with one index, the fact that it is widely accepted in the society makes the use of JMA <span class="hlt">Seismic</span> Intensity preferable when seismologists communicate with the public and discuss hazard assessment and risk management. With the introduction on JMA Instrumental Intensity in 1996, the number of <span class="hlt">seismic</span> intensity observation sites has substantially increased and the spatial coverage has improved vastly. Together with a long history of non-instrumental intensity <span class="hlt">records</span>, the intensity data represent some aspects of the <span class="hlt">seismic</span> ground motion in Japan. We investigate characteristics of <span class="hlt">seismic</span> ground motion between 1950 and 2009 utilizing JMA <span class="hlt">Seismic</span> Intensity Database. Specifically we are interested in the frequency distribution of intensity <span class="hlt">recordings</span>. Observations of large intensity is rare compared to those of small intensity, and previous studies such as Ikegami [1961] demonstrated that frequency distribution of observed intensity obeys an exponential law, which is equivalent to the Ishimoto-Iida law [Ishimoto & Iida, 1939]. Such behavior could be used to empirically construct probabilistic <span class="hlt">seismic</span> hazard maps [e.g., Kawasumi, 1951]. For the recent instrumental intensity data as well as pre-instrumental data, we are able to confirm that Ishimoto-Iida law explains the observation. Exponents of the Ishimoto-Iida law, or slope of the exponential law in the semi-log plot, is approximately 0.5. At stations with long <span class="hlt">recordings</span>, there is no apparent difference between pre-instrumental and instrumental intensities when Ishimoto-Iida law is used as a measure. Numbers of average intensity reports per year and exponents of the frequency distribution curve vary regionally and local <span class="hlt">seismicity</span> is apparently the controlling factor. The observed numbers of large intensity is slightly less than extrapolated and</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014EGUGA..1613375C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014EGUGA..1613375C"><span><span class="hlt">Seismic</span> local site effects characterization in the Andarax River Valley (SE Spain) from ambient <span class="hlt">seismic</span> noise</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Carmona, Enrique; García-Jerez, Antonio; Luzón, Francisco; Sánchez-Martos, Francisco; Sánchez-Sesma, Francisco J.; Piña, José</p> <p>2014-05-01</p> <p>This work is focused on the characterization of <span class="hlt">seismic</span> local effects in the Low Andarax River Valley (SE Spain). The Low Andarax River valley is located in an active <span class="hlt">seismic</span> region, with the higher <span class="hlt">seismic</span> hazard values in Spain. The landform is composed mainly by sedimentary materials which increase its <span class="hlt">seismic</span> hazard due to the amplification of the <span class="hlt">seismic</span> inputs and spectral resonances. We study <span class="hlt">seismic</span> local effects in the Low Andarax River by analyzing the Horizontal-to-Vertical Spectral Ratio (HVSR) of ambient noise <span class="hlt">records</span>. The noise data were <span class="hlt">recorded</span> during two field campaigns in 2012 and 2013. There have been a total of 374 noise measurements with 15 and 30 minutes duration. The acquisition was performed with a Digital Broadband Seismometer Guralp CMG-6TD. The distance between measurements was about 200 meters, covering an area around 40 km2. There have been 6 significant peak frequencies between 0.3 Hz and 5 Hz. It was possible to find interesting areas with similar spectral peaks that coincide with zones with similar microgravimetric anomalies at the alluvial valley. It is also observed a decrease in the frequency peaks from West to East suggesting increased sediment layer. We also compute the soil models at those sites where geotechnical information is available, assuming that the <span class="hlt">seismic</span> noise is diffuse. We invert the HVSR for these places using horizontally layered models and in the imaginary part the Green functions at the source. It is observed that the S wave velocity inverted models are consistent with the known geotechnical information obtained from drilled boreholes. We identify the elastodynamic properties of the limestone-dolomite materials with a formation of phyllites and quartzite that form the basement of the depression, and those properties of the Miocene and Pliocene detrital deposits (marls, sandy silts, sands and conglomerates) that fill the valley. These results together with the observed resonant frequencies along the Andarax</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..19.5206P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..19.5206P"><span>Passive <span class="hlt">seismic</span> experiment in the Olduvai Gorge and Laetoli region (Ngorongoro Conservation Area), Northern Tanzania.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Parisi, Laura; Lombardo, Luigi; Tang, Zheng; Mai, P. Martin</p> <p>2017-04-01</p> <p>The Olduvai Gorge and Laetoli basins, located within the Ngorogoro Conservation Area (NCA), are a cornerstone for understanding the evolution of early humans and are two paleo-antropological excavation sites of global importance. NCA is located at the boundary between the Tanzanian Craton and East African Rift (EAR), in the vicinity of Ngorongoro Crater and other major volcanic edifices. Thus, understanding the geology and tectonics of the NCA may shed light onto the question why early Hominins settled in this region. Environmental and geological conditions in the Olduvai and Laetoli region that promoted human settlement and development are still debated by geologists and paleo-anthropologists. Paleo-geographical reconstructions of the study area of the last 2 million years may take advantage of modern passive seismology. Therefore, we installed a dense <span class="hlt">seismic</span> network covering a surface of approximately 30 x 40 km within the NCA to map the depth extent of known faults, and to identify <span class="hlt">seismically</span> active faults that have no surface expression. Our ten <span class="hlt">seismic</span> stations, equipped with Trillium Compact 120 s sensors, started to operate in June 2016 and will continue for a total of 2 years. At the end of the first year, other 5 stations will densify our network. Here we analyse data quality of the first four months of continuous <span class="hlt">recordings</span>. Our network provides good quality 3-<span class="hlt">C</span> waveforms in the frequency range of 0.7-50 Hz. Vertical component seismograms <span class="hlt">record</span> frequencies reliably down to 8 mHz. Preliminary results of the <span class="hlt">seismicity</span> obtained with standard location procedures show that NCA is characterised by frequent tectonic <span class="hlt">seismicity</span> (not volcano-related) with Ml between 0.5 and 2.0. <span class="hlt">Seismic</span> activity is more frequent in the South (Laetoli region) where major fault systems have not been recognised at the surface yet.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2014-title14-vol3/pdf/CFR-2014-title14-vol3-part135-appC.pdf','CFR2014'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2014-title14-vol3/pdf/CFR-2014-title14-vol3-part135-appC.pdf"><span>14 CFR Appendix <span class="hlt">C</span> to Part 135 - Helicopter Flight <span class="hlt">Recorder</span> Specifications</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2014&page.go=Go">Code of Federal Regulations, 2014 CFR</a></p> <p></p> <p>2014-01-01</p> <p>... 14 Aeronautics and Space 3 2014-01-01 2014-01-01 false Helicopter Flight <span class="hlt">Recorder</span> Specifications <span class="hlt">C</span> Appendix <span class="hlt">C</span> to Part 135 Aeronautics and Space FEDERAL AVIATION ADMINISTRATION, DEPARTMENT OF TRANSPORTATION.... <span class="hlt">C</span> Appendix <span class="hlt">C</span> to Part 135—Helicopter Flight <span class="hlt">Recorder</span> Specifications Parameters Range Installed system...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFM.S41B2740S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFM.S41B2740S"><span>Enhanced Rayleigh waves tomography of Mexico using ambient noise cross-correlations (<span class="hlt">C</span>1) and correlations of coda of correlations (<span class="hlt">C</span>3)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Spica, Z. J.; Perton, M.; Calo, M.; Cordoba-Montiel, F.; Legrand, D.; Iglesias, A.</p> <p>2015-12-01</p> <p>Standard application of the <span class="hlt">seismic</span> ambient noise tomography considers the existence of synchronous <span class="hlt">records</span> at stations for green's functions retrieval. More recent theoretical and experimental observations showed the possibility to apply correlation of coda of noise correlation (<span class="hlt">C</span>3) to obtain green's functions between stations of asynchronous <span class="hlt">seismic</span> networks making possible to dramatically increase databases for imagining the Earth's interior. However, this possibility has not been fully exploited yet, and right now the data <span class="hlt">C</span>3 are not included into tomographic inversions to refine <span class="hlt">seismic</span> structures. Here we show for the first time how to incorporate the data of <span class="hlt">C</span>1 and <span class="hlt">C</span>3 to calculate dispersion maps of Rayleigh waves in the range period of 10-120s, and how the merging of these datasets improves the resolution of the structures imaged. Tomographic images are obtained for an area covering Mexico, the Gulf of Mexico and the southern U.S. We show dispersion maps calculated using both data of <span class="hlt">C</span>1 and the complete dataset (<span class="hlt">C</span>1+<span class="hlt">C</span>3). The latter provide new details of the <span class="hlt">seismic</span> structure of the region allowing a better understanding of their role on the geodynamics of the study area. The resolving power obtained in our study is several times higher than in previous studies based on ambient noise. This demonstrates the new possibilities for imaging the Earth's crust and upper mantle using this enlarged database.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70024379','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70024379"><span>Mapping the sources of the <span class="hlt">seismic</span> wave field at Kilauea volcano, Hawaii, using data <span class="hlt">recorded</span> on multiple <span class="hlt">seismic</span> Antennas</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Almendros, J.; Chouet, B.; Dawson, P.; Huber, Caleb G.</p> <p>2002-01-01</p> <p><span class="hlt">Seismic</span> antennas constitute a powerful tool for the analysis of complex wave fields. Well-designed antennas can identify and separate components of a complex wave field based on their distinct propagation properties. The combination of several antennas provides the basis for a more complete understanding of volcanic wave fields, including an estimate of the location of each individual wave-field component identified simultaneously by at least two antennas. We used frequency-slowness analyses of data from three antennas to identify and locate the different components contributing to the wave fields <span class="hlt">recorded</span> at Kilauea volcano, Hawaii, in February 1997. The wave-field components identified are (1) a sustained background volcanic tremor in the form of body waves generated in a shallow hydrothermal system located below the northeastern edge of the Halemaumau pit crater; (2) surface waves generated along the path between this hydrothermal source and the antennas; (3) back-scattered surface wave energy from a shallow reflector located near the southeastern rim of Kilauea caldera; (4) evidence for diffracted wave components originating at the southeastern edge of Halemaumau; and (5) body waves reflecting the activation of a deeper tremor source between 02 hr 00 min and 16 hr 00 min Hawaii Standard Time on 11 February.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.V41B..08E','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.V41B..08E"><span>Hazard Monitoring of Growing Lava Flow Fields Using <span class="hlt">Seismic</span> Tremor</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Eibl, E. P. S.; Bean, C. J.; Jónsdottir, I.; Hoskuldsson, A.; Thordarson, T.; Coppola, D.; Witt, T.; Walter, T. R.</p> <p>2017-12-01</p> <p>An effusive eruption in 2014/15 created a 85 km2 large lava flow field in a remote location in the Icelandic highlands. The lava flows did not threaten any settlements or paved roads but they were nevertheless interdisciplinarily monitored in detail. Images from satellites and aircraft, ground based video monitoring, GPS and <span class="hlt">seismic</span> <span class="hlt">recordings</span> allowed the monitoring and reconstruction of a detailed time series of the growing lava flow field. While the use of satellite images and probabilistic modelling of lava flows are quite common tools to monitor the current and forecast the future growth direction, here we show that <span class="hlt">seismic</span> <span class="hlt">recordings</span> can be of use too. We installed a cluster of seismometers at 15 km from the vents and <span class="hlt">recorded</span> the ground vibrations associated with the eruption. This <span class="hlt">seismic</span> tremor was not only generated below the vents, but also at the edges of the growing lava flow field and indicated the parts of the lava flow field that were most actively growing. Whilst the time resolution is in the range of days for satellites, <span class="hlt">seismic</span> stations easily sample continuously at 100 Hz and could therefore provide a much better resolution and estimate of the lava flow hazard in real-time.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li class="active"><span>13</span></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_13 --> <div id="page_14" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li class="active"><span>14</span></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="261"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFM.S11F4410A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFM.S11F4410A"><span>Neural Models: An Option to Estimate <span class="hlt">Seismic</span> Parameters of Accelerograms</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Alcántara, L.; García, S.; Ovando-Shelley, E.; Macías, M. A.</p> <p>2014-12-01</p> <p><span class="hlt">Seismic</span> instrumentation for <span class="hlt">recording</span> strong earthquakes, in Mexico, goes back to the 60´s due the activities carried out by the Institute of Engineering at Universidad Nacional Autónoma de México. However, it was after the big earthquake of September 19, 1985 (M=8.1) when the project of <span class="hlt">seismic</span> instrumentation assumes a great importance. Currently, strong ground motion networks have been installed for monitoring <span class="hlt">seismic</span> activity mainly along the Mexican subduction zone and in Mexico City. Nevertheless, there are other major regions and cities that can be affected by strong earthquakes and have not yet begun their <span class="hlt">seismic</span> instrumentation program or this is still in development.Because of described situation some relevant earthquakes (e.g. Huajuapan de León Oct 24, 1980 M=7.1, Tehuacán Jun 15, 1999 M=7 and Puerto Escondido Sep 30, 1999 M= 7.5) have not been registered properly in some cities, like Puebla and Oaxaca, and that were damaged during those earthquakes. Fortunately, the good maintenance work carried out in the <span class="hlt">seismic</span> network has permitted the <span class="hlt">recording</span> of an important number of small events in those cities. So in this research we present a methodology based on the use of neural networks to estimate significant duration and in some cases the response spectra for those <span class="hlt">seismic</span> events. The neural model developed predicts significant duration in terms of magnitude, epicenter distance, focal depth and soil characterization. Additionally, for response spectra we used a vector of spectral accelerations. For training the model we selected a set of accelerogram <span class="hlt">records</span> obtained from the small events <span class="hlt">recorded</span> in the strong motion instruments installed in the cities of Puebla and Oaxaca. The final results show that neural networks as a soft computing tool that use a multi-layer feed-forward architecture provide good estimations of the target parameters and they also have a good predictive capacity to estimate strong ground motion duration and response spectra.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.usgs.gov/of/1986/0405/report.pdf','USGSPUBS'); return false;" href="https://pubs.usgs.gov/of/1986/0405/report.pdf"><span>Multichannel <span class="hlt">seismic</span>-reflection data collected in 1980 in the eastern Chukchi Sea</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Grantz, Arthur; Mann, Dennis M.; May, Steven D.</p> <p>1986-01-01</p> <p>The U.S. Geological Survey (USGS) collected approximately 2,652 km of 24-channel <span class="hlt">seismic</span>-reflection data in early September, 1980, over the continental shelf in the eastern Chukchi Sea (Fig. 1). The profiles were collected on the USGS Research Vessel S.P. Lee. The <span class="hlt">seismic</span> energy source consisted of a tuned array of five airguns with a total volume of 1213 cubic inches of air compressed to approximately 1900 psi. The <span class="hlt">recording</span> system consisted of a 24-channel, 2400 meter long streamer with a group interval of 100 m, and a GUS (Global Universal Science) model 4200 digital <span class="hlt">recording</span> instrument. Shots were fired every 50 meters. Navigational control for the survey was provided by a Magnavox integrated navigation system using transit satellites and doppler-sonar augmented by Loran <span class="hlt">C</span> (Rho-Rho). A 2-millisecond sampling rate was used in the field; the data were later desampled to 4-milliseconds during the demultiplexing process. 8 seconds data length was <span class="hlt">recorded</span>. Processing was done at the USGS Pacific Marine Geology Multichannel Processing Center in Menlo Park, California, in the sequence: editing-demultiplexing, velocity analysis, CDP stacking, deconvolution-filtering, and plotting on an electrostatic plotter. Plate 1 is a trackline chart showing shotpoint navigation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMNH43A0174M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMNH43A0174M"><span>High frequency <span class="hlt">seismic</span> signal generated by landslides on complex topographies: from point source to spatially distributed sources</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mangeney, A.; Kuehnert, J.; Capdeville, Y.; Durand, V.; Stutzmann, E.; Kone, E. H.; Sethi, S.</p> <p>2017-12-01</p> <p>During their flow along the topography, landslides generate <span class="hlt">seismic</span> waves in a wide frequency range. These so called landquakes can be <span class="hlt">recorded</span> at very large distances (a few hundreds of km for large landslides). The <span class="hlt">recorded</span> signals depend on the landslide <span class="hlt">seismic</span> source and the <span class="hlt">seismic</span> wave propagation. If the wave propagation is well understood, the <span class="hlt">seismic</span> signals can be inverted for the <span class="hlt">seismic</span> source and thus can be used to get information on the landslide properties and dynamics. Analysis and modeling of long period <span class="hlt">seismic</span> signals (10-150s) have helped in this way to discriminate between different landslide scenarios and to constrain rheological parameters (e.g. Favreau et al., 2010). This was possible as topography poorly affects wave propagation at these long periods and the landslide <span class="hlt">seismic</span> source can be approximated as a point source. In the near-field and at higher frequencies (> 1 Hz) the spatial extent of the source has to be taken into account and the influence of the topography on the <span class="hlt">recorded</span> <span class="hlt">seismic</span> signal should be quantified in order to extract information on the landslide properties and dynamics. The characteristic signature of distributed sources and varying topographies is studied as a function of frequency and <span class="hlt">recording</span> distance.The time dependent spatial distribution of the forces applied to the ground by the landslide are obtained using granular flow numerical modeling on 3D topography. The generated <span class="hlt">seismic</span> waves are simulated using the spectral element method. The simulated <span class="hlt">seismic</span> signal is compared to observed <span class="hlt">seismic</span> data from rockfalls at the Dolomieu Crater of Piton de la Fournaise (La Réunion).Favreau, P., Mangeney, A., Lucas, A., Crosta, G., and Bouchut, F. (2010). Numerical modeling of landquakes. Geophysical Research Letters, 37(15):1-5.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70195676','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70195676"><span>1986 Great Lakes <span class="hlt">Seismic</span> refraction survey (GLIMPCE): Line A - refraction mode</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Morel-a-l'Huissier, Patrick; Karl, John H.; Tréhu, Anne M.; Hajnal, Zoltan; Mereu, Robert F.; Meyer, Robert P.; Sexton, John L.; Ervin, C. Patrick; Green, Alan G.; Hutchinson, Deborah</p> <p>1990-01-01</p> <p>In the fall of 1986, the Geological Survey of Canada (GSC), the United States Geological Survey (USGS), two Canadian universities -- University of Western Ontario and University of Saskatchewan, and four American universities -- Northern Illinois University, Southern Illinois University, University of Wisconsin-Madison and University of Wisconsin-Oshkosh participated in a major deep <span class="hlt">seismic</span> experiment in Lake Superior under the GLIMPCE (Great Lakes International Multidisciplinary Program on Crustal Evolution) umbrella. This Open-File Report presents the <span class="hlt">seismic</span> sections for line A, which was shot specifically for refraction <span class="hlt">recording</span>. The main target for study by this line was the Mid-Continent Rift System. All <span class="hlt">recording</span> stations, 31 in total (26 land stations and 5 OBSs), <span class="hlt">recorded</span> energy from shots fired every two minutes (333 m spacing) by a tuned airgun array towed by a contracted ship along line A in Lake Superior. These data are the densest such data ever <span class="hlt">recorded</span> in the continental North America over such distances. It is also unique since coincident <span class="hlt">seismic</span> reflection and refraction are available.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018GeoJI.tmp..128S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018GeoJI.tmp..128S"><span>Automated <span class="hlt">seismic</span> waveform location using Multichannel Coherency Migration (MCM)-I. Theory</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Shi, Peidong; Angus, Doug; Rost, Sebastian; Nowacki, Andy; Yuan, Sanyi</p> <p>2018-03-01</p> <p>With the proliferation of dense <span class="hlt">seismic</span> networks sampling the full <span class="hlt">seismic</span> wavefield, <span class="hlt">recorded</span> <span class="hlt">seismic</span> data volumes are getting bigger and automated analysis tools to locate <span class="hlt">seismic</span> events are essential. Here, we propose a novel Multichannel Coherency Migration (MCM) method to locate earthquakes in continuous <span class="hlt">seismic</span> data and reveal the location and origin time of <span class="hlt">seismic</span> events directly from <span class="hlt">recorded</span> waveforms. By continuously calculating the coherency between waveforms from different receiver pairs, MCM greatly expands the available information which can be used for event location. MCM does not require phase picking or phase identification, which allows fully automated waveform analysis. By migrating the coherency between waveforms, MCM leads to improved source energy focusing. We have tested and compared MCM to other migration-based methods in noise-free and noisy synthetic data. The tests and analysis show that MCM is noise resistant and can achieve more accurate results compared with other migration-based methods. MCM is able to suppress strong interference from other <span class="hlt">seismic</span> sources occurring at a similar time and location. It can be used with arbitrary 3D velocity models and is able to obtain reasonable location results with smooth but inaccurate velocity models. MCM exhibits excellent location performance and can be easily parallelized giving it large potential to be developed as a real-time location method for very large datasets.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUOSHE44B1508G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUOSHE44B1508G"><span><span class="hlt">Seismic</span> Imaging of Circumpolar Deep Water Exchange across the Shelf Break of the Antarctic Peninsula</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gunn, K.; White, N.; Larter, R. D.; Falder, M.; Caulfield, C. C. P.</p> <p>2016-02-01</p> <p>The western Antarctic Peninsula is an area of recent extreme atmospheric warming. In the adjacent ocean, there is particular interest in on-shelf movement of Circumpolar Deep Water as a possible link to changing climate by affecting ice shelf processes. Here, we investigate on-shelf intrusions using two-dimensional <span class="hlt">seismic</span> imaging of the water column which has vertical and horizontal resolutions of 10 m. 8 <span class="hlt">seismic</span> profiles were acquired in February 2015 using the RRS James Clark Ross. These profiles traverse the shelf break and cross two bathymetric features, the Marguerite and Biscoe troughs, which may play a role in water exchange processes. <span class="hlt">Seismic</span> data were acquired using two Generator-Injector air guns fired every 10 s with a pressure of 2000 psi. Reflections were <span class="hlt">recorded</span> on a 2.4 km streamer of 192 receivers spaced every 12.5 m. Observed reflections in the processed <span class="hlt">records</span> are caused by rapid changes of temperature ( 80%) and salinity ( 20%), delineating water masses of different properties. 13 XCTDs and XBTs plus a 38 kHz echo-sounder profile were simultaneously acquired along <span class="hlt">seismic</span> profiles and used for calibration. Preliminary results show the top of the Winter Water layer as a bright reflection at 50-120 m depth across the entire survey, corresponding to temperatures ≤ -1°<span class="hlt">C</span>. Curved, discontinuous, eddy-like reflections, also seen on echo-sounder profiles, are attributed to modified Upper Circumpolar Deep Water with temperatures ≥ 1.34°<span class="hlt">C</span>. A warm core eddy, 11 km long and 220 m high, is visible 2 km inland of the shelf break. Pure Upper Circumpolar Deep Water of temperatures ≥ 1.80°<span class="hlt">C</span> is aligned with weak but discernible, lens-shaped reflections. Eddy-like structures and the overall reflective morphology yield useful insights into shelf exchange processes, suggestive of three potential mechanisms: (i) topography controlled flow; (ii) an 'ice-pump' mechanism; and (iii) mesoscale eddies.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011AGUFM.S53B2276B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011AGUFM.S53B2276B"><span>Unusual Signals <span class="hlt">Recorded</span> by Ocean Bottom Seismometers in the Caldera of Deception Island Volcano: Biological Activity or Hydrothermally Generated <span class="hlt">Seismicity</span>?</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bowman, D. C.; Wilcock, W. S.</p> <p>2011-12-01</p> <p>As part of an active source land-sea tomography experiment, ocean bottom seismometers (OBSs) were deployed at Deception Island Volcano, Antarctica, in January 2005. Following the tomography study, three OBSs were left for a month inside the flooded caldera and ten on the outer slopes of the volcano to <span class="hlt">record</span> seismo-volcanic signals. The OBS sensor package included three-orthogonal 1-Hz geophones but no hydrophone. The OBSs were deployed in water depths of 125 to 143 m inside the caldera and at depths of 119 to 475 m on the volcano's flanks. Only two volcano-tectonic earthquakes and three long period events were <span class="hlt">recorded</span> by the network. However, the OBSs inside the caldera <span class="hlt">recorded</span> over 4,500 unusual <span class="hlt">seismic</span> events. These were detected by only one station at a time and were completely absent from OBSs on the flank of the volcano and from land stations deployed on the island. The signals had a dominant frequency of 5 Hz and were one to ten seconds long. Event activity in the caldera was variable with the number of events per hour ranging from 0 up to 60 and the level of activity decreasing slightly over the study period. We categorize the signals into three types based on waveform characteristics. Type 1 events have an impulsive onset and last 1 to 2 s with characteristics that are consistent with the impulse response of a poorly coupled OBS. Type 2 events typically last 2 to 4 s and comprise a low amplitude initial arrival followed less than a second later by a more energetic second phase that looks a Type 1 event. Type 3 events last up to 10 s and have more complex waveforms that appear to comprise several arrivals of varying amplitudes. Type 1 events are similar to the 'fish-bump' signals reported from previous studies that attributed them to biological activity. The consistent timing and relative amplitudes of the two arrivals for Type 2 events are difficult to explain by animals randomly touching the OBSs. Type 3 events are quite similar in frequency, duration</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.T52B..06G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.T52B..06G"><span><span class="hlt">Seismicity</span> and <span class="hlt">seismic</span> hazard in Sabah, East Malaysia from earthquake and geodetic data</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gilligan, A.; Rawlinson, N.; Tongkul, F.; Stephenson, R.</p> <p>2017-12-01</p> <p>While the levels of <span class="hlt">seismicity</span> are low in most of Malaysia, the state of Sabah in northern Borneo has moderate levels of <span class="hlt">seismicity</span>. Notable earthquakes in the region include the 1976 M6.2 Lahad Datu earthquake and the 2015 M6 Ranau earthquake. The recent Ranau earthquake resulted in the deaths of 18 people on Mt Kinabalu, an estimated 100 million RM ( US$23 million) damage to buildings, roads, and infrastructure from shaking, and flooding, reduced water quality, and damage to farms from landslides. Over the last 40 years the population of Sabah has increased to over four times what it was in 1976, yet <span class="hlt">seismic</span> hazard in Sabah remains poorly understood. Using <span class="hlt">seismic</span> and geodetic data we hope to better quantify the hazards posed by earthquakes in Sabah, and thus help to minimize risk. In order to do this we need to know about the locations of earthquakes, types of earthquakes that occur, and faults that are generating them. We use data from 15 MetMalaysia <span class="hlt">seismic</span> stations currently operating in Sabah to develop a region-specific velocity model from receiver functions and a pre-existing surface wave model. We use this new velocity model to (re)locate earthquakes that occurred in Sabah from 2005-2016, including a large number of aftershocks from the 2015 Ranau earthquake. We use a probabilistic nonlinear earthquake location program to locate the earthquakes and then refine their relative locations using a double difference method. The <span class="hlt">recorded</span> waveforms are further used to obtain moment tensor solutions for these earthquakes. Earthquake locations and moment tensor solutions are then compared with the locations of faults throughout Sabah. Faults are identified from high-resolution IFSAR images and subsequent fieldwork, with a particular focus on the Lahad Datau and Ranau areas. Used together, these <span class="hlt">seismic</span> and geodetic data can help us to develop a new <span class="hlt">seismic</span> hazard model for Sabah, as well as aiding in the delivery of outreach activities regarding <span class="hlt">seismic</span> hazard</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFMOS33A1052L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFMOS33A1052L"><span><span class="hlt">Seismic</span> Site Effects from the Seafloor Motion <span class="hlt">Recorded</span> by the Short-period Ocean Bottom Seismometers</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lin, J. Y.; Cheng, W. B.; Chin, S. J.; Hsu, S. K.; Dong, J. J.</p> <p>2014-12-01</p> <p>For decades, it has been mentioned that submarine slope failures are spatially linked to the presence of gas hydrates/gas-charged sediments. When triggered by earthquakes, oversteepen and instable sediments may prompt breakouts of the slopes containing gas hydrates and cause submarine landslides and tsunamis. Widely distributed BSRs have been observed in the area offshore of southwestern Taiwan where the active accretionary complex meets with the passive China continental margin. In the region, large or small scale landslides were also reported based on <span class="hlt">seismic</span> interpretations. In order to clarify the link between earthquake, landslide and the presence of gas hydrate, we evaluate the response of seafloor sediments in regard to passive dynamic loads. Horizontal-to-vertical (H/V) spectral ratios are used to characterize the local sediment response. Ambient noise as well as distant earthquakes are used as generators of the passive dynamic loads. Based on this study, we aim to characterize the site in terms of its physical properties and the local site effect produced by shallow marine sediments. The results show that the maximum H/V ratios appeared in the range of 5-10 Hz, where the horizontal amplitudes increased by an order of magnitude relative to the vertical amplitude. The stations located in the northwestern part of study area were characterized by another relatively small peak at proximately 2 Hz, which may indicates the presence of a discontinuity of sediments. For most stations, the H/V ratios estimated based on the earthquake (i.e. strong input signal) and noise (background, micro-<span class="hlt">seismic</span> noise) <span class="hlt">records</span> were characterized by different pattern. No distinct peak is observed for the H/V pattern calculated during earthquakes. This phenomenon may suggest that no clear sedimentary boundary exist when a stronger motion applies. Estimating H/V spectral ratios of data <span class="hlt">recorded</span> by the seven short period OBSs (Ocean Bottom Seismometer) deployed in the southwest Taiwan</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016ExG....47..123C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016ExG....47..123C"><span>High lateral resolution exploration using surface waves from noise <span class="hlt">records</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chávez-García, Francisco José Yokoi, Toshiaki</p> <p>2016-04-01</p> <p>Determination of the shear-wave velocity structure at shallow depths is a constant necessity in engineering or environmental projects. Given the sensitivity of Rayleigh waves to shear-wave velocity, subsoil structure exploration using surface waves is frequently used. Methods such as the spectral analysis of surface waves (SASW) or multi-channel analysis of surface waves (MASW) determine phase velocity dispersion from surface waves generated by an active source <span class="hlt">recorded</span> on a line of geophones. Using MASW, it is important that the receiver array be as long as possible to increase the precision at low frequencies. However, this implies that possible lateral variations are discarded. Hayashi and Suzuki (2004) proposed a different way of stacking shot gathers to increase lateral resolution. They combined strategies used in MASW with the common mid-point (CMP) summation currently used in reflection seismology. In their common mid-point with cross-correlation method (CMPCC), they cross-correlate traces sharing CMP locations before determining phase velocity dispersion. Another recent approach to subsoil structure exploration is based on <span class="hlt">seismic</span> interferometry. It has been shown that cross-correlation of a diffuse field, such as <span class="hlt">seismic</span> noise, allows the estimation of the Green's Function between two receivers. Thus, a virtual-source <span class="hlt">seismic</span> section may be constructed from the cross-correlation of <span class="hlt">seismic</span> noise <span class="hlt">records</span> obtained in a line of receivers. In this paper, we use the <span class="hlt">seismic</span> interferometry method to process <span class="hlt">seismic</span> noise <span class="hlt">records</span> obtained in <span class="hlt">seismic</span> refraction lines of 24 geophones, and analyse the results using CMPCC to increase the lateral resolution of the results. Cross-correlation of the noise <span class="hlt">records</span> allows reconstructing <span class="hlt">seismic</span> sections with virtual sources at each receiver location. The Rayleigh wave component of the Green's Functions is obtained with a high signal-to-noise ratio. Using CMPCC analysis of the virtual-source <span class="hlt">seismic</span> lines, we are able to</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFM.S52B..03K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFM.S52B..03K"><span>Dense <span class="hlt">Seismic</span> <span class="hlt">Recordings</span> of Two Surface-Detonated Chemical Explosions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Koper, K. D.; Hale, J. M.; Burlacu, R.; Goddard, K. J.; Trow, A.; Linville, L. M.; Stein, J. R.; Drobeck, D.; Leidig, M.</p> <p>2015-12-01</p> <p>In the summer of 2015 two controlled chemical explosions were carried out near Dugway, Utah. The 2 June 2015 explosion consisted of 30,000 lbs of ammonium nitrate fuel oil (ANFO) and the 22 July 2015 explosion consisted of 60,000 lbs of ANFO. The explosion centroids were 1-2 m above the Earth's surface and both created significant craters in the soft desert alluvium. To better understand the <span class="hlt">seismic</span> source associated with surface explosions, we deployed an array of wireless, three-component, short-period (5 Hz corner frequency) seismometers for several days around each shot. For the first explosion, 46 receivers were deployed in a "lollipop" geometry that had a sparse ring at a radius of 1 km, and a dense stem with 100 m spacing for distances of 0.5-4.5 km. For the second explosion, 48 receivers were deployed similarly, but with a dense ring spaced in azimuthal increments of 10 degrees at a distance of 1 km, and a sparse stem (~500 m spacing) that extended to a distance of nearly 6 km. A rich variety of phases were <span class="hlt">recorded</span> including direct P waves, refracted and reflected P waves, nearly monochromatic air-coupled Rayleigh waves, normally dispersed fundamental mode Rayleigh waves (Rg), primary airblast arrivals, some secondary airblast arrivals, and possibly tertiary airblast arrivals. There is also evidence of converted S waves on the radial components and possibly direct S energy on the radial and transverse components, although the transverse energy does not always possess a simple, coherent move-out with distance, implying that it might have a scattering origin. To aid in the phase identification, especially of the apparent SH and Love energy, we are currently performing tau-p, f-k, and particle motion analysis.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015IzPSE..51..268N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015IzPSE..51..268N"><span><span class="hlt">Seismic</span> hazard and <span class="hlt">seismic</span> risk assessment based on the unified scaling law for earthquakes: Himalayas and adjacent regions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Nekrasova, A. K.; Kossobokov, V. G.; Parvez, I. A.</p> <p>2015-03-01</p> <p>For the Himalayas and neighboring regions, the maps of <span class="hlt">seismic</span> hazard and <span class="hlt">seismic</span> risk are constructed with the use of the estimates for the parameters of the unified scaling law for earthquakes (USLE), in which the Gutenberg-Richter law for magnitude distribution of <span class="hlt">seismic</span> events within a given area is applied in the modified version with allowance for linear dimensions of the area, namely, log N( M, L) = A + B (5 - M) + <span class="hlt">C</span> log L, where N( M, L) is the expected annual number of the earthquakes with magnitude M in the area with linear dimension L. The spatial variations in the parameters A, B, and <span class="hlt">C</span> for the Himalayas and adjacent regions are studied on two time intervals from 1965 to 2011 and from 1980 to 2011. The difference in A, B, and <span class="hlt">C</span> between these two time intervals indicates that <span class="hlt">seismic</span> activity experiences significant variations on a scale of a few decades. With a global consideration of the <span class="hlt">seismic</span> belts of the Earth overall, the estimates of coefficient A, which determines the logarithm of the annual average frequency of the earthquakes with a magnitude of 5.0 and higher in the zone with a linear dimension of 1 degree of the Earth's meridian, differ by a factor of 30 and more and mainly fall in the interval from -1.1 to 0.5. The values of coefficient B, which describes the balance between the number of earthquakes with different magnitudes, gravitate to 0.9 and range from less than 0.6 to 1.1 and higher. The values of coefficient <span class="hlt">C</span>, which estimates the fractal dimension of the local distribution of epicenters, vary from 0.5 to 1.4 and higher. In the Himalayas and neighboring regions, the USLE coefficients mainly fall in the intervals of -1.1 to 0.3 for A, 0.8 to 1.3 for B, and 1.0 to 1.4 for <span class="hlt">C</span>. The calculations of the local value of the expected peak ground acceleration (PGA) from the maximal expected magnitude provided the necessary basis for mapping the <span class="hlt">seismic</span> hazards in the studied region. When doing this, we used the local estimates of the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/966299','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/966299"><span>Third Quarter Hanford <span class="hlt">Seismic</span> Report for Fiscal Year 2009</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Rohay, Alan C.; Sweeney, Mark D.; Hartshorn, Donald C.</p> <p>2009-09-30</p> <p>The Hanford <span class="hlt">Seismic</span> Assessment Program (HSAP) provides an uninterrupted collection of high-quality raw and processed <span class="hlt">seismic</span> data from the Hanford <span class="hlt">Seismic</span> Network for the U.S. Department of Energy and its contractors. The HSAP is responsible for locating and identifying sources of <span class="hlt">seismic</span> activity and monitoring changes in the historical pattern of <span class="hlt">seismic</span> activity at the Hanford Site. The data are compiled, archived, and published for use by the Hanford Site for waste management, natural phenomena hazards assessments, and engineering design and construction. In addition, the HSAP works with the Hanford Site Emergency Services Organization to provide assistance in the eventmore » of a significant earthquake on the Hanford Site. The Hanford <span class="hlt">Seismic</span> Network and the Eastern Washington Regional Network consist of 44 individual sensor sites and 15 radio relay sites maintained by the Hanford <span class="hlt">Seismic</span> Assessment Team. The Hanford <span class="hlt">Seismic</span> Network <span class="hlt">recorded</span> 771 local earthquakes during the third quarter of FY 2009. Nearly all of these earthquakes were detected in the vicinity of Wooded Island, located about eight miles north of Richland just west of the Columbia River. The Wooded Island events <span class="hlt">recorded</span> this quarter is a continuation of the swarm events observed during the January – March 2009 time period and reported in the previous quarterly report (Rohay et al, 2009). The frequency of Wooded Island events has subsided with 16 events <span class="hlt">recorded</span> during June 2009. Most of the events were considered minor (magnitude (Mc) less than 1.0) with 25 events in the 2.0-3.0 range. The estimated depths of the Wooded Island events are shallow (averaging less than 1.0 km deep) with a maximum depth estimated at 2.2 km. This places the Wooded Island events within the Columbia River Basalt Group (CRBG). The low magnitude of the Wooded Island events has made them undetectable to all but local area residents. However, some Hanford employees working within a few miles of the area of highest</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/5117738-vertical-seismic-profile-processing','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/5117738-vertical-seismic-profile-processing"><span>On vertical <span class="hlt">seismic</span> profile processing</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Tariel, P.; Michon, D.</p> <p>1984-10-01</p> <p>From the wealth of information which can be deduced from VSP, the information most directly comparable to well logs is considered: P-wave and S-wave interval velocity, acoustic impedance, and the velocity ratio ..gamma.. = V /SUB s/ /V /SUB p/ . This information not only allows better interpretation of surface <span class="hlt">seismic</span> sections but also improves processing. For these results to be usable a number of precautions must be taken during acquisition and processing; the sampling in depth should be chosen in such a way that aliasing phenomena do not unnecessarily limit the spectra during the separation of upwards and downwardsmore » travelling waves. True amplitudes should be respected and checked by <span class="hlt">recording</span> of signatures, and the interference of upwards and downwards travelling waves should be taken into account for the picking of first arrivals. The different steps in processing and the combination of results in the interpretation of surface <span class="hlt">seismic</span> results are described with actual <span class="hlt">records</span>.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.usgs.gov/sir/2004/5211/','USGSPUBS'); return false;" href="https://pubs.usgs.gov/sir/2004/5211/"><span><span class="hlt">Seismic</span> monitoring at Cascade Volcanic Centers, 2004?status and recommendations</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Moran, Seth C.</p> <p>2004-01-01</p> <p>The purpose of this report is to assess the current (May, 2004) status of <span class="hlt">seismic</span> monitoring networks at the 13 major Cascade volcanic centers. Included in this assessment are descriptions of each network, analyses of the ability of each network to detect and to locate <span class="hlt">seismic</span> activity, identification of specific weaknesses in each network, and a prioritized list of those networks that are most in need of additional <span class="hlt">seismic</span> stations. At the outset it should be recognized that no Cascade volcanic center currently has an adequate <span class="hlt">seismic</span> network relative to modern-day networks at Usu Volcano (Japan) or Etna and Stromboli volcanoes (Italy). For a system the size of Three Sisters, for example, a modern-day, cutting-edge <span class="hlt">seismic</span> network would ideally consist of a minimum of 10 to 12 short-period three-component seismometers (for determining particle motions, reliable S-wave picks, moment tensor inversions, fault-plane solutions, and other important <span class="hlt">seismic</span> parameters) and 7 to 10 broadband sensors (which, amongst other considerations, enable detection and location of very long period (VLP) and other low-frequency events, moment tensor inversions, and, because of their wide dynamic range, on-scale <span class="hlt">recording</span> of large-amplitude events). Such a dense, multi component <span class="hlt">seismic</span> network would give the ability to, for example, detect in near-real-time earthquake migrations over a distance of ~0.5km or less, locate tremor sources, determine the nature of a <span class="hlt">seismic</span> source (that is, pure shear, implosive, explosive), provide on-scale <span class="hlt">recordings</span> of very small and very large-amplitude <span class="hlt">seismic</span> signals, and detect localized changes in <span class="hlt">seismic</span> stress tensor orientations caused by movement of magma bodies. However, given that programmatic resources are currently limited, installation of such networks at this time is unrealistic. Instead, this report focuses on identifying what additional stations are needed to guarantee that anomalous <span class="hlt">seismicity</span> associated with volcanic unrest will be</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.S13B2545M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.S13B2545M"><span>An Application of Reassigned Time-Frequency Representations for <span class="hlt">Seismic</span> Noise/Signal Decomposition</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mousavi, S. M.; Langston, C. A.</p> <p>2016-12-01</p> <p><span class="hlt">Seismic</span> data <span class="hlt">recorded</span> by surface arrays are often strongly contaminated by unwanted noise. This background noise makes the detection of small magnitude events difficult. An automatic method for <span class="hlt">seismic</span> noise/signal decomposition is presented based upon an enhanced time-frequency representation. Synchrosqueezing is a time-frequency reassignment method aimed at sharpening a time-frequency picture. Noise can be distinguished from the signal and suppressed more easily in this reassigned domain. The threshold level is estimated using a general cross validation approach that does not rely on any prior knowledge about the noise level. Efficiency of thresholding has been improved by adding a pre-processing step based on higher order statistics and a post-processing step based on adaptive hard-thresholding. In doing so, both accuracy and speed of the denoising have been improved compared to our previous algorithms (Mousavi and Langston, 2016a, 2016b; Mousavi et al., 2016). The proposed algorithm can either kill the noise (either white or colored) and keep the signal or kill the signal and keep the noise. Hence, It can be used in either normal denoising applications or in ambient noise studies. Application of the proposed method on synthetic and real <span class="hlt">seismic</span> data shows the effectiveness of the method for denoising/designaling of local microseismic, and ocean bottom <span class="hlt">seismic</span> data. References: Mousavi, S.M., <span class="hlt">C</span>. A. Langston., and S. P. Horton (2016), Automatic Microseismic Denoising and Onset Detection Using the Synchrosqueezed-Continuous Wavelet Transform. Geophysics. 81, V341-V355, doi: 10.1190/GEO2015-0598.1. Mousavi, S.M., and <span class="hlt">C</span>. A. Langston (2016a), Hybrid <span class="hlt">Seismic</span> Denoising Using Higher-Order Statistics and Improved Wavelet Block Thresholding. Bull. Seismol. Soc. Am., 106, doi: 10.1785/0120150345. Mousavi, S.M., and <span class="hlt">C</span>.A. Langston (2016b), Adaptive noise estimation and suppression for improving microseismic event detection, Journal of Applied Geophysics., doi: http</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JOUC...16..223L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JOUC...16..223L"><span>Numerical simulation of bubble plumes and an analysis of their <span class="hlt">seismic</span> attributes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Li, Canping; Gou, Limin; You, Jiachun</p> <p>2017-04-01</p> <p>To study the bubble plume's <span class="hlt">seismic</span> response characteristics, the model of a plume water body has been built in this article using the bubble-contained medium acoustic velocity model and the stochastic medium theory based on an analysis of both the acoustic characteristics of a bubble-contained water body and the actual features of a plume. The finite difference method is used for forward modelling, and the single-shot <span class="hlt">seismic</span> <span class="hlt">record</span> exhibits the characteristics of a scattered wave field generated by a plume. A meaningful conclusion is obtained by extracting <span class="hlt">seismic</span> attributes from the pre-stack shot gather <span class="hlt">record</span> of a plume. The values of the amplitude-related <span class="hlt">seismic</span> attributes increase greatly as the bubble content goes up, and changes in bubble radius will not cause <span class="hlt">seismic</span> attributes to change, which is primarily observed because the bubble content has a strong impact on the plume's acoustic velocity, while the bubble radius has a weak impact on the acoustic velocity. The above conclusion provides a theoretical reference for identifying hydrate plumes using <span class="hlt">seismic</span> methods and contributes to further study on hydrate decomposition and migration, as well as on distribution of the methane bubble in seawater.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PhDT.........1Q','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PhDT.........1Q"><span><span class="hlt">Seismic</span> reflection imaging with conventional and unconventional sources</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Quiros Ugalde, Diego Alonso</p> <p></p> <p>This manuscript reports the results of research using both conventional and unconventional energy sources as well as conventional and unconventional analysis to image crustal structure using reflected <span class="hlt">seismic</span> waves. The work presented here includes the use of explosions to investigate the Taiwanese lithosphere, the use of 'noise' from railroads to investigate the shallow subsurface of the Rio Grande rift, and the use of microearthquakes to image subsurface structure near an active fault zone within the Appalachian mountains. Chapter 1 uses <span class="hlt">recordings</span> from the land refraction and wide-angle reflection component of the Taiwan Integrated Geodynamic Research (TAIGER) project. The most prominent reflection feature imaged by these surveys is an anomalously strong reflector found in northeastern Taiwan. The goal of this chapter is to analyze the TAIGER <span class="hlt">recordings</span> and to place the reflector into a geologic framework that fits with the modern tectonic kinematics of the region. Chapter 2 uses railroad traffic as a source for reflection profiling within the Rio Grande rift. Here the railroad <span class="hlt">recordings</span> are treated in an analogous way to Vibroseis <span class="hlt">recordings</span>. These results suggest that railroad noise in general can be a valuable new tool in imaging and characterizing the shallow subsurface in environmental and geotechnical studies. In chapters 3 and 4, earthquakes serve as the <span class="hlt">seismic</span> imaging source. In these studies the methodology of Vertical <span class="hlt">Seismic</span> Profiling (VSP) is borrowed from the oil and gas industry to develop reflection images. In chapter 3, a single earthquake is used to probe a small area beneath Waterboro, Maine. In chapter 4, the same method is applied to multiple earthquakes to take advantage of the increased redundancy that results from multiple events illuminating the same structure. The latter study demonstrates how dense arrays can be a powerful new tool for delineating, and monitoring temporal changes of deep structure in areas characterized by significant</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015EGUGA..1710159D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015EGUGA..1710159D"><span>The ISC <span class="hlt">Seismic</span> Event Bibliography</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Di Giacomo, Domenico; Storchak, Dmitry</p> <p>2015-04-01</p> <p>The International Seismological Centre (ISC) is a not-for-profit organization operating in the UK for the last 50 years and producing the ISC Bulletin - the definitive worldwide summary of <span class="hlt">seismic</span> events, both natural and anthropogenic - starting from the beginning of 20th century. Often researchers need to gather information related to specific <span class="hlt">seismic</span> events for various reasons. To facilitate such task, in 2012 we set up a new database linking earthquakes and other <span class="hlt">seismic</span> events in the ISC Bulletin to bibliographic <span class="hlt">records</span> of scientific articles (mostly peer-reviewed journals) that describe those events. Such association allows users of the ISC Event Bibliography (www.isc.ac.uk/event_bibliography/index.php) to run searches for publications via a map-based web interface and, optionally, selecting scientific publications related to either specific events or events in the area of interest. Some of the greatest earthquakes were described in several hundreds of articles published over a period of few years. The journals included in our database are not limited to seismology but bring together a variety of fields in geosciences (e.g., engineering seismology, geodesy and remote sensing, tectonophysics, monitoring research, tsunami, geology, geochemistry, hydrogeology, atmospheric sciences, etc.) making this service useful in multidisciplinary studies. Usually papers dealing with large data set are not included (e.g., papers describing a <span class="hlt">seismic</span> catalogue). Currently the ISC Event Bibliography includes over 17,000 individual publications from about 500 titles related to over 14,000 events that occurred in last 100+ years. The bibliographic <span class="hlt">records</span> in the Event Bibliography start in the 1950s, and it is updated as new publications become available.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008AGUFM.T33E..05W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008AGUFM.T33E..05W"><span>Diverse <span class="hlt">Seismic</span> Imaging Created by the <span class="hlt">Seismic</span> Explosion Experiment of the TAIGER Project</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wang, C.; Okaya, D.; Wu, F.; Yen, H.; Huang, B.; Liang, W.</p> <p>2008-12-01</p> <p>The TAIGER (TAiwan Integrated GEodynamics Research) project which examines the Taiwan orogeny includes five experiments: natural earthquake <span class="hlt">recording</span>, man-made explosion <span class="hlt">recording</span>, Magnetotelluic imaging, marine MCS and sea-land shooting, and deformation evolution modeling. During Feb-Mar 2008, the explosion experiment was carried out. Ten sources with 500~3000kg dynamite were detonated along two transects across northern and southern Taiwan. Over 600 PASSCAL Texans and 40 R-130 instruments <span class="hlt">record</span> the signals over 100~300 km range. Additional arrays with 100 seismometers were deployed to collect north-south line and fan shoot data for 3D imaging. Furthermore, there are 9 ocean bottom seismometers (OBS) in the Taiwan Strait and two lines with 20 seismometers deployed on the mainland China side. A large volume of qualified data has been created. Except explosion signals, numerous local and regional earthquakes were also <span class="hlt">recorded</span> even by the Texan instruments. The rich earthquake-explosion dataset now exists at the Institute of Earth Sciences, Academia Sinica operated by the Taiwan Earthquake Center (TEC). Preliminary examination of the data reveal crustal Pg, PmP, Pn and intermediate crustal reflection phases within the transect profiles and in the 3D cross-arrays. These data provide direct <span class="hlt">seismic</span> imaging of the continental Moho under Taiwan and the sharp Moho root configuration associated with mountain building. <span class="hlt">Seismic</span> tomography and raytrace methods reveal velocity structure consistent with convergence and vertical exhumation of the Central Ranges.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li class="active"><span>14</span></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_14 --> <div id="page_15" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li class="active"><span>15</span></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="281"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011PhDT.......107Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011PhDT.......107Z"><span><span class="hlt">Seismic</span> performance of geosynthetic-soil retaining wall structures</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zarnani, Saman</p> <p></p> <p>Vertical inclusions of expanded polystyrene (EPS) placed behind rigid retaining walls were investigated as geofoam <span class="hlt">seismic</span> buffers to reduce earthquake-induced loads. A numerical model was developed using the program FLAC and the model validated against 1-g shaking table test results of EPS geofoam <span class="hlt">seismic</span> buffer models. Two constitutive models for the component materials were examined: elastic-perfectly plastic with Mohr-Coulomb (M-<span class="hlt">C</span>) failure criterion and non-linear hysteresis damping model with equivalent linear method (ELM) approach. It was judged that the M-<span class="hlt">C</span> model was sufficiently accurate for practical purposes. The mechanical property of interest to attenuate dynamic loads using a <span class="hlt">seismic</span> buffer was the buffer stiffness defined as K = E/t (E = buffer elastic modulus, t = buffer thickness). For the range of parameters investigated in this study, K ≤50 MN/m3 was observed to be the practical range for the optimal design of these systems. Parametric numerical analyses were performed to generate design charts that can be used for the preliminary design of these systems. A new high capacity shaking table facility was constructed at RMC that can be used to study the <span class="hlt">seismic</span> performance of earth structures. Reduced-scale models of geosynthetic reinforced soil (GRS) walls were built on this shaking table and then subjected to simulated earthquake loading conditions. In some shaking table tests, combined use of EPS geofoam and horizontal geosynthetic reinforcement layers was investigated. Numerical models were developed using program FLAC together with ELM and M-<span class="hlt">C</span> constitutive models. Physical and numerical results were compared against predicted values using analysis methods found in the journal literature and in current North American design guidelines. The comparison shows that current Mononobe-Okabe (M-O) based analysis methods could not consistently satisfactorily predict measured reinforcement connection load distributions at all elevations under both static</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFM.S33D2810S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFM.S33D2810S"><span>Toward the Autonomous <span class="hlt">Recording</span> and Transmission of <span class="hlt">Seismic</span> Data from the Oceans: Testing the Son-O-Mermaid Float in the Sargasso Sea</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Simon, J. D.; Simons, F. J.; Vincent, H. T.; Nolet, G.</p> <p>2015-12-01</p> <p>We report on the deployment of two new Son-O-Mermaid floats into theSargasso Sea during a cruise aboard the R/V Atlantic Explorer, whichdeparted from Bermuda in May of 2015. Son-O-Mermaid is a freelyfloating and autonomous oceangoing system composed of a surface buoyconnected to a length of cable from which a three-hydrophone array issuspended. The main objective of the Son-O-Mermaid project is torecord signals suitable for global tomography in the deep ocean andprovide the <span class="hlt">seismic</span> community with an abundance of novel raypaths frompreviously unsampled regions of the Earth. The Son-O-Mermaid float,with its ability to continually <span class="hlt">record</span>, analyze, and transmit seismicdata from the oceans in near-real time has the potential torevolutionize the field of seismology. We analyze new data returnedfrom this deployment, a previous Son-O-Mermaid test, as well as theongoing MERMAID mission in the time, spectral, and wavelet domains. Afull description of the float and deployment report will be presented.A short-term goal of the project is determining realistic magnitude,distance, and pressure relationships for teleseismic earthquakes thatare <span class="hlt">recorded</span> in the water column. Our analysis of this question isaided by synthetics created using SPECFEM2D and guided by the data,especially noise <span class="hlt">records</span> <span class="hlt">recorded</span> by Son-O-Mermaid and MERMAID fromoceans throughout the world. Synthetics provide an idealized waveformuseful for understanding the often very messy and noisy arrivalscommon in midcolumn acoustic <span class="hlt">recordings</span>. Notably, synthetics allowthe confirmation or rejection of unlikely phases which are matched toearthquake databases after arrivals are detected by automatic pickingalgorithms. Additionally, marine-acoustic processing techniques willbe improved once the underwater acoustic field is better modeled usingrealistic signal-to-noise ratios and noise spectra returned fromSon-O-Mermaid and MERMAID missions. This analysis, particularly whenimplemented in the wavelet domain, is proving</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUSMNS21C..04E','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUSMNS21C..04E"><span>Coherent Waves in <span class="hlt">Seismic</span> Researches</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Emanov, A.; Seleznev, V. S.</p> <p>2013-05-01</p> <p>Development of digital processing algorithms of <span class="hlt">seismic</span> wave fields for the purpose of useful event picking to study environment and other objects is the basis for the establishment of new <span class="hlt">seismic</span> techniques. In the submitted paper a fundamental property of <span class="hlt">seismic</span> wave field coherence is used. The authors extended conception of coherence types of observed wave fields and devised a technique of coherent component selection from observed wave field. Time coherence and space coherence are widely known. In this paper conception "parameter coherence" has been added. The parameter by which wave field is coherent can be the most manifold. The reason is that the wave field is a multivariate process described by a set of parameters. Coherence in the first place means independence of linear connection in wave field of parameter. In <span class="hlt">seismic</span> wave fields, <span class="hlt">recorded</span> in confined space, in building-blocks and stratified mediums time coherent standing waves are formed. In prospecting seismology at observation systems with multiple overlapping head waves are coherent by parallel correlation course or, in other words, by one measurement on generalized plane of observation system. For detail prospecting seismology at observation systems with multiple overlapping on basis of coherence property by one measurement of area algorithms have been developed, permitting <span class="hlt">seismic</span> <span class="hlt">records</span> to be converted to head wave time sections which have neither reflected nor other types of waves. Conversion in time section is executed on any specified observation base. Energy storage of head waves relative to noise on basis of multiplicity of observation system is realized within area of head wave <span class="hlt">recording</span>. Conversion on base below the area of wave tracking is performed with lack of signal/noise ratio relative to maximum of this ratio, fit to observation system. Construction of head wave time section and dynamic plots a basis of automatic processing have been developed, similar to CDP procedure in method of</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1368358','SCIGOV-DOEDE'); return false;" href="https://www.osti.gov/servlets/purl/1368358"><span>Triggered MEQ Events on LBNL Permanent <span class="hlt">Seismic</span> Array, Brady's EGS, March 2016</span></a></p> <p><a target="_blank" href="http://www.osti.gov/dataexplorer">DOE Data Explorer</a></p> <p>Michelle Robertson</p> <p>2016-06-01</p> <p>List of triggered events <span class="hlt">recorded</span> on LBNL's permanent EGS <span class="hlt">seismic</span> array at Brady's geothermal field. This submission also includes links to the NCEDC EGS Earthquake Catalog Search page and to the metadata for the <span class="hlt">seismic</span> array installed at Brady's Geothermal Field.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70019856','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70019856"><span>Propagation of <span class="hlt">seismic</span> waves in tall buildings</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Safak, E.</p> <p>1998-01-01</p> <p>A discrete-time wave propagation formulation of the <span class="hlt">seismic</span> response of tall buildings is introduced. The building is modeled as a layered medium, similar to a layered soil medium, and is subjected to vertically propagating <span class="hlt">seismic</span> shear waves. Soil layers and the bedrock under the foundation are incorporated in the formulation as additional layers. <span class="hlt">Seismic</span> response is expressed in terms of the wave travel times between the layers, and the wave reflection and transmission coefficients at the layer interfaces. The equations account for the frequency-dependent filtering effects of the foundation and floor masses. The calculation of <span class="hlt">seismic</span> response is reduced to a pair of simple finite-difference equations for each layer, which can be solved recursively starting from the bedrock. Compared to the commonly used vibration formulation, the wave propagation formulation provides several advantages, including simplified calculations, better representation of damping, ability to account for the effects of the soil layers under the foundation, and better tools for identification and damage detection from <span class="hlt">seismic</span> <span class="hlt">records</span>. Examples presented show the versatility of the method. ?? 1998 John Wiley & Sons, Ltd.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EJPh...38b3001V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EJPh...38b3001V"><span>Teaching hands-on geophysics: examples from the Rū <span class="hlt">seismic</span> network in New Zealand</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>van Wijk, Kasper; Simpson, Jonathan; Adam, Ludmila</p> <p>2017-03-01</p> <p>Education in physics and geosciences can be effectively illustrated by the analysis of earthquakes and the subsequent propagation of <span class="hlt">seismic</span> waves in the Earth. Educational seismology has matured to a level where both the hard- and software are robust and user friendly. This has resulted in successful implementation of educational networks around the world. <span class="hlt">Seismic</span> data <span class="hlt">recorded</span> by students are of such quality that these can be used in classic earthquake location exercises, for example. But even ocean waves weakly coupled into the Earth’s crust can now be <span class="hlt">recorded</span> on educational seismometers. These signals are not just noise, but form the basis of more recent developments in seismology, such as <span class="hlt">seismic</span> interferometry, where <span class="hlt">seismic</span> waves generated by ocean waves—instead of earthquakes—can be used to infer information about the Earth’s interior. Here, we introduce an earthquake location exercise and an analysis of ambient <span class="hlt">seismic</span> noise, and present examples. Data are provided, and all needed software is freely available.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014EGUGA..16.2319M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014EGUGA..16.2319M"><span>The preglacial sediment <span class="hlt">record</span> of Lake Ladoga, Russia - first results from a <span class="hlt">seismic</span> survey and sediment coring in 2013</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Melles, Martin; Krastel, Sebastian; Fedorov, Grigory; Subetto, Dmitry A.; Savelieva, Larisa A.; Andreev, Andrej; Wagner, Bernd</p> <p>2014-05-01</p> <p>The new German-Russian project PLOT (Paleolimnological Transect) aims at investigating the Late Quaternary climatic and environmental history along a more than 6000 km long longitudinal transect crossing northern Eurasia. Special emphasis is put on the preglacial history. For this purpose shallow and deep <span class="hlt">seismic</span> surveys shall be carried out on five lakes, which potentially host preglacial sediment <span class="hlt">records</span>, followed by sediment coring based on the results of the <span class="hlt">seismic</span> campaigns. The well-studied Lake El'gygytgyn represents the eastern-most location of the transect and acts as reference site. Within the scope of a pilot phase for the PLOT project, funded by the German Federal Ministry of Education and Research, we were able to investigate Lake Ladoga, which is located close to St. Petersburg at the western end of the transect. Lake Ladoga is the largest lake in Europe, covering an area of almost 18.000 km2. The modern sedimentation as well as the late glacial and Holocene history of the lake were already studied in detail over the past decades. The older, preglacial lake history, however, is only rudimentary known from a core transect drilled in the southern lake in the 1930th. The cores of up to about 60 m length were only briefly described and are not existing any more. The results from these cores, known from unpublished reports only, suggest the existence of marine sediments of presumably Eemian age, representing a time when Lake Lagoga was part of a precursor of the Baltic Sea, which had a connection via Ladoga and Onega Lakes to the White Sea and further to the Arctic Ocean. In late August/early September 2013 we carried out a <span class="hlt">seismic</span> survey on Lake Ladoga using a Mini-GI-Gun and a 32-channel <span class="hlt">seismic</span> streamer. In total, 1500 km of <span class="hlt">seismic</span> profiles were measured, covering most parts of the lake. The <span class="hlt">seismic</span> lines typically show acoustically well stratified Holocene muds overlaying rather transparent postglacial varves. These sediment successions can reach</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70013239','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70013239"><span><span class="hlt">SEISMIC</span> STUDY OF THE AGUA DE PAU GEOTHERMAL PROSPECT, SAO MIGUEL, AZORES.</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Dawson, Phillip B.; Rodrigues da Silva, Antonio; Iyer, H.M.; Evans, John R.</p> <p>1985-01-01</p> <p>A 16 station array was operated over the 200 km**2 central portion of Sao Miguel utilizing 8 permanent Instituto Nacional de Meterologia e Geofisica stations and 8 USGS portable stations. Forty four local events with well constrained solutions and 15 regional events were located. In addition, hundreds of unlocatable <span class="hlt">seismic</span> events were <span class="hlt">recorded</span>. The most interesting <span class="hlt">seismic</span> activity occurred in a swarm on September 6 and 7, 1983 when over 200 events were <span class="hlt">recorded</span> in a 16 hour period. The <span class="hlt">seismic</span> activity around Agua de Pau was centered on the east and northeast slopes of the volcano. The data suggest a boiling hydrothermal system beneath the Agua de Pau volcano, consistent with a variety of other data.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PApGe.174.1711S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PApGe.174.1711S"><span>Crustal Structure, <span class="hlt">Seismic</span> Anisotropy and Deformations of the Ediacaran/Cambrian of the Małopolska Block in SE Poland Based on Data from Two <span class="hlt">Seismic</span> Wide-Angle Experiments</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Środa, Piotr</p> <p>2017-04-01</p> <p>The area of SE Poland represents a complex contact of tectonic units of different consolidation age—from the Precambrian East European Craton, through Palaeozoic West European Platform (including Małopolska Block) to Cenozoic Carpathians and Carpathian Foredeep. In order to investigate the anisotropic properties of the upper crust of the Małopolska Block and their relation to tectonic evolution of the area, two <span class="hlt">seismic</span> datasets were used: <span class="hlt">seismic</span> wide-angle off-line <span class="hlt">recordings</span> from POLCRUST-01 deep <span class="hlt">seismic</span> reflection profile and <span class="hlt">recordings</span> from active deep <span class="hlt">seismic</span> experiment CELEBRATION 2000. During acquisition of deep reflection <span class="hlt">seismic</span> profile POLCRUST-01 in 2010, a 35-km-long line of 14 <span class="hlt">recorders</span> (PA-14), oriented perpendicularly to the profile, was deployed to <span class="hlt">record</span> the refractions from the upper crust (Pg) at wide range of azimuths. These data were used for an analysis of the azimuthal anisotropy of the MB with the modified delay-time inversion method. The results of modelling of the off-line refractions from the MB suggest 6% HTI anisotropy of the Cambrian/Ediacaran basement, with 130º azimuth of the fast velocity axis and mean Vp of 4.9 km/s. To compare this result with previous, independent information about anisotropy at larger depth, a subset of previously modelled data from CELEBRATION 2000 experiment, <span class="hlt">recorded</span> in the MB area, was also analysed by inversion. The <span class="hlt">recordings</span> of Pg phase at up to 120 km offsets were analysed using anisotropic delay-time inversion, providing information down to 12 km depth. The CELEBRATION 2000 model shows 9% HTI anisotropy with 126º orientation of the fast axis. Thus, local-scale anisotropy of this part of MB confirms the large-scale anisotropy suggested by previous studies based on data from a broader area and larger depth interval. The azimuthal anisotropy (i.e. HTI symmetry of the medium) is interpreted as a result of strong compressional deformation during the accretion of terranes to the EEC margin, leading to</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUSM.S51A..04E','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUSM.S51A..04E"><span>Updated Colombian <span class="hlt">Seismic</span> Hazard Map</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Eraso, J.; Arcila, M.; Romero, J.; Dimate, C.; Bermúdez, M. L.; Alvarado, C.</p> <p>2013-05-01</p> <p>The Colombian <span class="hlt">seismic</span> hazard map used by the National Building Code (NSR-98) in effect until 2009 was developed in 1996. Since then, the National Seismological Network of Colombia has improved in both coverage and technology providing fifteen years of additional <span class="hlt">seismic</span> <span class="hlt">records</span>. These improvements have allowed a better understanding of the regional geology and tectonics which in addition to the <span class="hlt">seismic</span> activity in Colombia with destructive effects has motivated the interest and the need to develop a new <span class="hlt">seismic</span> hazard assessment in this country. Taking advantage of new instrumental information sources such as new broad band stations of the National Seismological Network, new historical <span class="hlt">seismicity</span> data, standardized global databases availability, and in general, of advances in models and techniques, a new Colombian <span class="hlt">seismic</span> hazard map was developed. A PSHA model was applied. The use of the PSHA model is because it incorporates the effects of all <span class="hlt">seismic</span> sources that may affect a particular site solving the uncertainties caused by the parameters and assumptions defined in this kind of studies. First, the <span class="hlt">seismic</span> sources geometry and a complete and homogeneous <span class="hlt">seismic</span> catalog were defined; the parameters of <span class="hlt">seismic</span> rate of each one of the <span class="hlt">seismic</span> sources occurrence were calculated establishing a national seismotectonic model. Several of attenuation-distance relationships were selected depending on the type of <span class="hlt">seismicity</span> considered. The <span class="hlt">seismic</span> hazard was estimated using the CRISIS2007 software created by the Engineering Institute of the Universidad Nacional Autónoma de México -UNAM (National Autonomous University of Mexico). A uniformly spaced grid each 0.1° was used to calculate the peak ground acceleration (PGA) and response spectral values at 0.1, 0.2, 0.3, 0.5, 0.75, 1, 1.5, 2, 2.5 and 3.0 seconds with return periods of 75, 225, 475, 975 and 2475 years. For each site, a uniform hazard spectrum and exceedance rate curves were calculated. With the results, it is</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.rintonpress.com/proceedings/0581.html','USGSPUBS'); return false;" href="http://www.rintonpress.com/proceedings/0581.html"><span>A deployment of broadband <span class="hlt">seismic</span> stations in two deep gold mines, South Africa</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>McGarr, Arthur F.; Boettcher, Margaret S.; Fletcher, Jon Peter B.; Johnston, Malcolm J.; Durrheim, R.; Spottiswoode, S.; Milev, A.</p> <p>2009-01-01</p> <p>In-mine <span class="hlt">seismic</span> networks throughout the TauTona and Mponeng gold mines provide precise locations and <span class="hlt">seismic</span> source parameters of earthquakes. They also support small-scale experimental projects, including NELSAM (Natural Earthquake Laboratory in South African Mines), which is intended to <span class="hlt">record</span>, at close hand, <span class="hlt">seismic</span> rupture of a geologic fault that traverses the project region near the deepest part of TauTona. To resolve some questions regarding the in-mine and NELSAM networks, we deployed four portable broadband <span class="hlt">seismic</span> stations at deep sites within TauTona and Mponeng for one week during September 2007 and <span class="hlt">recorded</span> ground acceleration. Moderately large earthquakes within our temporary network were <span class="hlt">recorded</span> with sufficiently high signal-to-noise that we were able to integrate the acceleration to ground velocity and displacement, from which moment tensors could be determined. We resolved the questions concerning the NELSAM and in-mine networks by using these moment tensors to calculate synthetic seismograms at various network <span class="hlt">recording</span> sites for comparison with the ground motion <span class="hlt">recorded</span> at the same locations. We also used the peak velocity of the S wave pulse, corrected for attenuation with distance, to estimate the maximum slip within the rupture zone of an earthquake. We then combined the maximum slip and <span class="hlt">seismic</span> moment with results from laboratory friction experiments to estimate maximum slip rates within the same high-slip patches of the rupture zone. For the four largest earthquakes <span class="hlt">recorded</span> within our network, all with magnitudes near 2, these inferred maximum slips range from 4 to 27 mm and the corresponding maximum slip rates range from 1 to 6 m/s. These results, in conjunction with information from previous ground motion studies, indicate that underground support should be capable of withstanding peak ground velocities of at least 5 m/s.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2010-title41-vol3/pdf/CFR-2010-title41-vol3-sec128-1-8006.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title41-vol3/pdf/CFR-2010-title41-vol3-sec128-1-8006.pdf"><span>41 CFR 128-1.8006 - <span class="hlt">Seismic</span> Safety Program requirements.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2010&page.go=Go">Code of Federal Regulations, 2010 CFR</a></p> <p></p> <p>2010-07-01</p> <p>... reviewer shall verify that the current level of <span class="hlt">seismic</span> resistance of the existing building at least equals the <span class="hlt">seismic</span> resistance level of the building before the addition. (<span class="hlt">c</span>) The Department <span class="hlt">Seismic</span> Safety... conduct the reviews required under this section, as appropriate. (a) New building projects. Construction...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFM.S53B2827C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFM.S53B2827C"><span>Large-N <span class="hlt">Seismic</span> Deployment at the Source Physics Experiment (SPE) Site</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chen, T.; Snelson, C. M.; Mellors, R. J.; Pitarka, A.</p> <p>2015-12-01</p> <p>The Source Physics Experiment (SPE) is multi-institutional and multi-disciplinary project that consists of a series of chemical explosion experiments at the Nevada National Security Site. The goal of SPE is to understand the complicated effect of earth structures on source energy partitioning and <span class="hlt">seismic</span> wave propagation, develop and validate physics-based monitoring, and ultimately better discriminate low-yield nuclear explosions from background <span class="hlt">seismicity</span>. Deployment of a large number of <span class="hlt">seismic</span> sensors is planned for SPE to image the full 3-D wavefield with about 500 three-component sensors and 500 vertical component sensors. This large-N <span class="hlt">seismic</span> deployment will operate near the site of SPE-5 shot for about one month, <span class="hlt">recording</span> the SPE-5 shot, ambient noise, and additional controlled-sources. This presentation focuses on the design of the large-N <span class="hlt">seismic</span> deployment. We show how we optimized the sensor layout based on the geological structure and experiment goals with a limited number of sensors. In addition, we will also show some preliminary <span class="hlt">record</span> sections from deployment. This work was conducted under Contract No. DE-AC52-06NA25946 with the U.S. Department of Energy.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2006AGUSM.S23A..01W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006AGUSM.S23A..01W"><span><span class="hlt">Seismic</span> Constraints on Geometry, <span class="hlt">Seismic</span> Velocity and Anisotropy of the "African Anomaly"</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wang, Y.; Wen, L.</p> <p>2006-05-01</p> <p><span class="hlt">Seismic</span> evidence shows that the "African Anomaly", a prominent low-velocity structure in the lower mantle beneath Africa, has a broad base near the core-mantle boundary (CMB) and extends at least 1000 km upward into the mid-lower mantle. Waveform modeling results indicate that its base is a very-low velocity province (VLVP) in the lowermost 200-300 km of the Earth's mantle with rapidly varying geometries and a strong Vs reduction gradient of -2% - -12% from top to bottom. These features unambiguously indicate the VLVP is compositionally distinct and can be best explained by partial melting driven by a compositional change produced in the early Earth's history [Wen, 2001; Wen et. al, 2001; Wang and Wen, 2004]. <span class="hlt">Seismic</span> structure for the mid-lower mantle portion of the "African Anomaly" and the anisotropic behavior related to the VLVP remain unclear. In this presentation, we will present <span class="hlt">seismic</span> data to constrain geometry and both P- and S- velocity perturbations for the "African Anomaly" along the great arc from the East Pacific Rise to the Japan Sea, and discuss <span class="hlt">seismic</span> anisotropic behavior inside the VLVP and in the surrounding areas. We collected direct S, ScS, SKS, and SKKS waveforms data sets for 9 earthquakes <span class="hlt">recorded</span> at the temporary broadband Kaapvaal, Tanzania, and Ethiopia/Kenya <span class="hlt">seismic</span> arrays in Africa. These <span class="hlt">seismic</span> data provide reasonably good coverage for the "African Anomaly" along a great circle path in opposite directions. We corrected for the effects of the earthquake mislocation and the <span class="hlt">seismic</span> heterogeneities outside the anomaly. <span class="hlt">Seismic</span> data suggest that the "African Anomaly" exhibits a "cusp-like" shape along the great arc and continuously extends from the CMB to about 1300 km above the CMB with both sides tilting toward its center beneath southern Africa. The magnitude of these travel time residuals can be best explained by a shear velocity structure with average Vs reductions of -5% for the basal layer and -2% - -3% for the portion in the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70196334','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70196334"><span>Integrate urban‐scale <span class="hlt">seismic</span> hazard analyses with the U.S. National <span class="hlt">Seismic</span> Hazard Model</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Moschetti, Morgan P.; Luco, Nicolas; Frankel, Arthur; Petersen, Mark D.; Aagaard, Brad T.; Baltay, Annemarie S.; Blanpied, Michael; Boyd, Oliver; Briggs, Richard; Gold, Ryan D.; Graves, Robert; Hartzell, Stephen; Rezaeian, Sanaz; Stephenson, William J.; Wald, David J.; Williams, Robert A.; Withers, Kyle</p> <p>2018-01-01</p> <p>For more than 20 yrs, damage patterns and instrumental <span class="hlt">recordings</span> have highlighted the influence of the local 3D geologic structure on earthquake ground motions (e.g., M">M 6.7 Northridge, California, Gao et al., 1996; M">M 6.9 Kobe, Japan, Kawase, 1996; M">M 6.8 Nisqually, Washington, Frankel, Carver, and Williams, 2002). Although this and other local‐scale features are critical to improving <span class="hlt">seismic</span> hazard forecasts, historically they have not been explicitly incorporated into the U.S. National <span class="hlt">Seismic</span> Hazard Model (NSHM, national model and maps), primarily because the necessary basin maps and methodologies were not available at the national scale. Instead,...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70028764','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70028764"><span><span class="hlt">Recorded</span> earthquake responses from the integrated <span class="hlt">seismic</span> monitoring network of the Atwood Building, Anchorage, Alaska</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Celebi, M.</p> <p>2006-01-01</p> <p>An integrated <span class="hlt">seismic</span> monitoring system with a total of 53 channels of accelerometers is now operating in and at the nearby free-field site of the 20-story steel-framed Atwood Building in highly <span class="hlt">seismic</span> Anchorage, Alaska. The building has a single-story basement and a reinforced concrete foundation without piles. The monitoring system comprises a 32-channel structural array and a 21-channel site array. Accelerometers are deployed on 10 levels of the building to assess translational, torsional, and rocking motions, interstory drift (displacement) between selected pairs of adjacent floors, and average drift between floors. The site array, located approximately a city block from the building, comprises seven triaxial accelerometers, one at the surface and six in boreholes ranging in depths from 15 to 200 feet (???5-60 meters). The arrays have already <span class="hlt">recorded</span> low-amplitude shaking responses of the building and the site caused by numerous earthquakes at distances ranging from tens to a couple of hundred kilometers. Data from an earthquake that occurred 186 km away traces the propagation of waves from the deepest borehole to the roof of the building in approximately 0.5 seconds. Fundamental structural frequencies [0.58 Hz (NS) and 0.47 Hz (EW)], low damping percentages (2-4%), mode coupling, and beating effects are identified. The fundamental site frequency at approximately 1.5 Hz is close to the second modal frequencies (1.83 Hz NS and 1.43 EW) of the building, which may cause resonance of the building. Additional earthquakes prove repeatability of these characteristics; however, stronger shaking may alter these conclusions. ?? 2006, Earthquake Engineering Research Institute.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017Tectp.717..226S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017Tectp.717..226S"><span>Micro-<span class="hlt">seismicity</span> in the Gulf of Cadiz: Is there a link between micro-<span class="hlt">seismicity</span>, high magnitude earthquakes and active faults?</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Silva, Sónia; Terrinha, Pedro; Matias, Luis; Duarte, João C.; Roque, Cristina; Ranero, César R.; Geissler, Wolfram H.; Zitellini, Nevio</p> <p>2017-10-01</p> <p>The Gulf of Cadiz <span class="hlt">seismicity</span> is characterized by persistent low to intermediate magnitude earthquakes, occasionally punctuated by high magnitude events such as the M 8.7 1755 Great Lisbon earthquake and the M = 7.9 event of February 28th, 1969. Micro-<span class="hlt">seismicity</span> was <span class="hlt">recorded</span> during 11 months by a temporary network of 25 ocean bottom seismometers (OBSs) in an area of high <span class="hlt">seismic</span> activity, encompassing the potential source areas of the mentioned large magnitude earthquakes. We combined micro-<span class="hlt">seismicity</span> analysis with processing and interpretation of deep crustal <span class="hlt">seismic</span> reflection profiles and available refraction data to investigate the possible tectonic control of the <span class="hlt">seismicity</span> in the Gulf of Cadiz area. Three controlling mechanisms are explored: i) active tectonic structures, ii) transitions between different lithospheric domains and inherited Mesozoic structures, and iii) fault weakening mechanisms. Our results show that micro-<span class="hlt">seismicity</span> is mostly located in the upper mantle and is associated with tectonic inversion of extensional rift structures and to the transition between different lithospheric/rheological domains. Even though the crustal structure is well imaged in the <span class="hlt">seismic</span> profiles and in the bathymetry, crustal faults show low to negligible <span class="hlt">seismic</span> activity. A possible explanation for this is that the crustal thrusts are thin-skinned structures rooting in relatively shallow sub-horizontal décollements associated with (aseismic) serpentinization levels at the top of the lithospheric mantle. Therefore, co-<span class="hlt">seismic</span> slip along crustal thrusts may only occur during large magnitude events, while for most of the inter-<span class="hlt">seismic</span> cycle these thrusts remain locked, or slip aseismically. We further speculate that high magnitude earthquake's ruptures may only nucleate in the lithospheric mantle and then propagate into the crust across the serpentinized layers.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1120','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1120"><span>Hanford Quarter <span class="hlt">Seismic</span> Report - 98<span class="hlt">C</span> <span class="hlt">Seismicity</span> On and Near the Hanford Site, Pasco Basin, Washington: April 1, 1998 Through June 30, 1998</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>DC Hartshorn, SP Reidel, AC Rohay</p> <p>1998-10-23</p> <p>Hanford <span class="hlt">Seismic</span> Monitoring provides an uninterrupted collection of high-quality raw and processed <span class="hlt">seismic</span> data from the Hanford <span class="hlt">Seismic</span> Network (HSN) for the U.S. Department of Energy and its contractors. The staff also locates aud identifies sources of <span class="hlt">seismic</span> activity and monitors changes in the hi~orical pattern of <span class="hlt">seismic</span> activity at the Hanford Site. The data are. compiled archived, and published for use by the Hanford Site for waste management Natural Phenomena Hazards assessments, and engineering design and construction. In addition, the <span class="hlt">seismic</span> monitoring organization works with the Hanford Site Emergency Services Organization to provide assistance in the event of zinmore » earthquake on the Hanford Site. The HSN and Ihe Eastern Washington Regional Network (EN/RN) consist-of 42 individual sensor sites and 15 radio relay sites maintained by the Hanford <span class="hlt">Seismic</span> Monitoring staff. The operational rate for the third quarter of FY 1998 for stations in the HSN was 99.99%. The operational rate for the third quarter of FY 1998 for stations of the EWRN was 99.95%. For the third quarter of FY 1998, the acquisition computer triggered 133 times. Of these triggers 11 were local earthquakes: 5 (45Yo) in the Columbia River Basalt Group, 2(1 8%) in the pre-basalt sediments, and 4 (36%) in the crystalline basement. The geologic and tectonic environments where these earthquakes occurred are discussed in this report.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/6223225-hanford-quarter-seismic-report-seismicity-near-hanford-site-pasco-basin-washington-april-through-june','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/6223225-hanford-quarter-seismic-report-seismicity-near-hanford-site-pasco-basin-washington-april-through-june"><span>Hanford Quarter <span class="hlt">Seismic</span> Report - 98<span class="hlt">C</span> <span class="hlt">Seismicity</span> On and Near the Hanford Site, Pasco Basin, Washington: April 1, 1998 Through June 30, 1998</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>DC Hartshorn, SP Reidel, AC Rohay.</p> <p>1998-10-23</p> <p>Hanford <span class="hlt">Seismic</span> Monitoring provides an uninterrupted collection of high-quality raw and processed <span class="hlt">seismic</span> data from the Hanford <span class="hlt">Seismic</span> Network (HSN) for the U.S. Department of Energy and its contractors. The staff also locates aud identifies sources of <span class="hlt">seismic</span> activity and monitors changes in the hi orical pattern of <span class="hlt">seismic</span> activity at the Hanford Site. The data are. compiled archived, and published for use by the Hanford Site for waste management Natural Phenomena Hazards assessments, and engineering design and construction. In addition, the <span class="hlt">seismic</span> monitoring organization works with the Hanford Site Emergency Services Organization to provide assistance in the event ofmore » zin earthquake on the Hanford Site. The HSN and Ihe Eastern Washington Regional Network (EN/RN) consist-of 42 individual sensor sites and 15 radio relay sites maintained by the Hanford <span class="hlt">Seismic</span> Monitoring staff. The operational rate for the third quarter of FY 1998 for stations in the HSN was 99.99%. The operational rate for the third quarter of FY 1998 for stations of the EWRN was 99.95%. For the third quarter of FY 1998, the acquisition computer triggered 133 times. Of these triggers 11 were local earthquakes: 5 (45Yo) in the Columbia River Basalt Group, 2(1 8%) in the pre-basalt sediments, and 4 (36%) in the crystalline basement. The geologic and tectonic environments where these earthquakes occurred are discussed in this report.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JGRB..122.2173N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JGRB..122.2173N"><span><span class="hlt">Seismicity</span> of the rocky mountains and Rio Grande Rift from the EarthScope Transportable Array and CREST temporary <span class="hlt">seismic</span> networks, 2008-2010</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Nakai, J. S.; Sheehan, A. F.; Bilek, S. L.</p> <p>2017-03-01</p> <p>We developed a catalog of small magnitude (ML -0.1 to 4.7) <span class="hlt">seismicity</span> across Colorado and New Mexico from the EarthScope USArray Transportable Array and CREST (Colorado Rocky Mountains Experiment and <span class="hlt">Seismic</span> Transects) <span class="hlt">seismic</span> networks from 2008 to 2010 to characterize active deformation in the Rio Grande Rift. We <span class="hlt">recorded</span> over 900 earthquakes in the Rio Grande Rift region, not including induced earthquakes and mine blasts, and find that the rift is actively deforming both broadly and in distinct regions. <span class="hlt">Seismic</span> events that are likely induced, mostly in the Raton Basin, make up 66% of the catalog (1837 earthquakes). Neogene faults in the northern rift in north central Colorado are <span class="hlt">seismically</span> active in the North Park Basin and northwestern Colorado. The central rift from the San Luis Basin (southern Colorado) to south of the Socorro Magma Body is the most <span class="hlt">seismically</span> active rift region, and <span class="hlt">seismicity</span> delineates the deformation in the Colorado Plateau transition zone, which is spatially correlated with volcanic vents, dikes, and faults within the western Jemez Lineament. The eastern Jemez Lineament is nearly aseismic and surrounded by a halo of <span class="hlt">seismicity</span> culminating in boundaries defined by recent moderate (Mw 3.9 and Mw 3.3) earthquakes. The southern rift is characterized by diffuse <span class="hlt">seismicity</span> in Texas and Mexico. This study provides an updated <span class="hlt">seismic</span> catalog built with uniformity in seismometer coverage and low epicentral uncertainties ( 2 km) that allows for regional evaluation of <span class="hlt">seismicity</span>. During this time period, clusters of <span class="hlt">seismicity</span> and moderate magnitude earthquakes characterize deformation in a low-strain rate extensional environment.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li class="active"><span>15</span></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_15 --> <div id="page_16" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li class="active"><span>16</span></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="301"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2002AGUFM.S72F1359P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2002AGUFM.S72F1359P"><span>Triggered <span class="hlt">Seismicity</span> in Utah from the November 3, 2002, Denali Fault Earthquake</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pankow, K. L.; Nava, S. J.; Pechmann, J. C.; Arabasz, W. J.</p> <p>2002-12-01</p> <p>Coincident with the arrival of the surface waves from the November 3, 2002, Mw 7.9 Denali Fault, Alaska earthquake (DFE), the University of Utah Seismograph Stations (UUSS) regional <span class="hlt">seismic</span> network detected a marked increase in <span class="hlt">seismicity</span> along the Intermountain <span class="hlt">Seismic</span> Belt (ISB) in central and north-central Utah. The number of earthquakes per day in Utah located automatically by the UUSS's Earthworm system in the week following the DFE was approximately double the long-term average during the preceding nine months. From these preliminary data, the increased <span class="hlt">seismicity</span> appears to be characterized by small magnitude events (M = 3.2) and concentrated in five distinct spatial clusters within the ISB between 38.75°and 42.0° N. The first of these earthquakes was an M 2.2 event located ~20 km east of Salt Lake City, Utah, which occurred during the arrival of the Love waves from the DFE. The increase in Utah earthquake activity at the time of the arrival of the surface waves from the DFE suggests that these surface waves triggered earthquakes in Utah at distances of more than 3,000 km from the source. We estimated the peak dynamic shear stress caused by these surface waves from measurements of their peak vector velocities at 43 <span class="hlt">recording</span> sites: 37 strong-motion stations of the Advanced National <span class="hlt">Seismic</span> System and six broadband stations. (The <span class="hlt">records</span> from six other broadband instruments in the region of interest were clipped.) The estimated peak stresses ranged from 1.2 bars to 3.5 bars with a mean of 2.3 bars, and generally occurred during the arrival of Love waves of ~15 sec period. These peak dynamic shear stress estimates are comparable to those obtained from <span class="hlt">recordings</span> of the 1992 Mw 7.3 Landers, California, earthquake in regions where the Landers earthquake triggered increased <span class="hlt">seismicity</span>. We plan to present more complete analyses of UUSS <span class="hlt">seismic</span> network data, further testing our hypothesis that the DFE remotely triggered <span class="hlt">seismicity</span> in Utah. This hypothesis is</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.usgs.gov/of/2006/1185/','USGSPUBS'); return false;" href="https://pubs.usgs.gov/of/2006/1185/"><span><span class="hlt">Seismicity</span> of Afghanistan and vicinity</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Dewey, James W.</p> <p>2006-01-01</p> <p>This publication describes the <span class="hlt">seismicity</span> of Afghanistan and vicinity and is intended for use in <span class="hlt">seismic</span> hazard studies of that nation. Included are digital files with information on earthquakes that have been <span class="hlt">recorded</span> in Afghanistan and vicinity through mid-December 2004. Chapter A provides an overview of the <span class="hlt">seismicity</span> and tectonics of Afghanistan and defines the earthquake parameters included in the 'Summary Catalog' and the 'Summary of Macroseismic Effects.' Chapter B summarizes compilation of the 'Master Catalog' and 'Sub-Threshold Catalog' and documents their formats. The 'Summary Catalog' itself is presented as a comma-delimited ASCII file, the 'Summary of Macroseismic Effects' is presented as an html file, and the 'Master Catalog' and 'Sub-Threshold Catalog' are presented as flat ASCII files. Finally, this report includes as separate plates a digital image of a map of epicenters of earthquakes occurring since 1964 (Plate 1) and a representation of areas of damage or strong shaking from selected past earthquakes in Afghanistan and vicinity (Plate 2).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMNH32A..02T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMNH32A..02T"><span>The Investigation of a Sinkhole Area in Germany by Near-Surface Active <span class="hlt">Seismic</span> Tomography</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tschache, S.; Becker, D.; Wadas, S. H.; Polom, U.; Krawczyk, C. M.</p> <p>2017-12-01</p> <p>In November 2010, a 30 m wide and 17 m deep sinkhole occurred in a residential area of Schmalkalden, Germany, which fortunately did not harm humans, but led to damage of buildings and property. Subsequent geoscientific investigations showed that the collapse was naturally caused by the subrosion of sulfates in a depth of about 80 m. In 2012, an early warning system was established including 3<span class="hlt">C</span> borehole geophones deployed in 50 m depth around the backfilled sinkhole. During the acquisition of two shallow 2D shear wave <span class="hlt">seismic</span> profiles, the signals generated by a micro-vibrator at the surface were additionally <span class="hlt">recorded</span> by the four borehole geophones of the early warning system and a VSP probe in a fifth borehole. The travel time analysis of the direct arrivals enhanced the understanding of wave propagation in the area. <span class="hlt">Seismic</span> velocity anomalies were detected and related to structural <span class="hlt">seismic</span> images of the 2D profiles. Due to the promising first results, the experiment was further extended by distributing vibration points throughout the whole area around the sinkhole. This time, micro-vibrators for P- and S-wave generation were used. The signals were <span class="hlt">recorded</span> by the borehole geophones and temporary installed seismometers at surface positions close to the boreholes. The travel times and signal attenuations are evaluated to detect potential instable zones. Furthermore, array analyses are performed. The first results reveal features in the active tomography datasets consistent with structures observed in the 2D <span class="hlt">seismic</span> images. The advantages of the presented method are the low effort and good repeatability due to the permanently installed borehole geophones. It has the potential to determine P-wave and S-wave velocities in 3D. It supports the interpretation of established investigation methods as 2D surface <span class="hlt">seismics</span> and VSP. In our further research we propose to evaluate the suitability of the method for the time lapse monitoring of changes in the <span class="hlt">seismic</span> wave</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.usgs.gov/of/1993/0322/report.pdf','USGSPUBS'); return false;" href="https://pubs.usgs.gov/of/1993/0322/report.pdf"><span>Observations and modeling of <span class="hlt">seismic</span> background noise</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Peterson, Jon R.</p> <p>1993-01-01</p> <p>The preparation of this report had two purposes. One was to present a catalog of <span class="hlt">seismic</span> background noise spectra obtained from a worldwide network of seismograph stations. The other purpose was to refine and document models of <span class="hlt">seismic</span> background noise that have been in use for several years. The second objective was, in fact, the principal reason that this study was initiated and influenced the procedures used in collecting and processing the data.With a single exception, all of the data used in this study were extracted from the digital data archive at the U.S. Geological Survey's Albuquerque Seismological Laboratory (ASL). This archive dates from 1972 when ASL first began deploying digital seismograph systems and collecting and distributing digital data under the sponsorship of the Defense Advanced Research Projects Agency (DARPA). There have been many changes and additions to the global seismograph networks during the past twenty years, but perhaps none as significant as the current deployment of very broadband seismographs by the U.S. Geological Survey (USGS) and the University of California San Diego (UCSD) under the scientific direction of the IRIS consortium. The new data acquisition systems have extended the bandwidth and resolution of <span class="hlt">seismic</span> <span class="hlt">recording</span>, and they utilize high-density <span class="hlt">recording</span> media that permit the continuous <span class="hlt">recording</span> of broadband data. The data improvements and continuous <span class="hlt">recording</span> greatly benefit and simplify surveys of <span class="hlt">seismic</span> background noise.Although there are many other sources of digital data, the ASL archive data were used almost exclusively because of accessibility and because the data systems and their calibration are well documented for the most part. Fortunately, the ASL archive contains high-quality data from other stations in addition to those deployed by the USGS. Included are data from UCSD IRIS/IDA stations, the Regional <span class="hlt">Seismic</span> Test Network (RSTN) deployed by Sandia National Laboratories (SNL), and the TERRAscope network</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.S34A..08T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.S34A..08T"><span>Spatial and temporal variation of <span class="hlt">seismic</span> velocity during earthquakes and volcanic eruptions in western Japan: Insight into mechanism for <span class="hlt">seismic</span> velocity variation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tsuji, T.; Ikeda, T.; Nimiya, H.</p> <p>2017-12-01</p> <p>We report spatio-temporal variations of <span class="hlt">seismic</span> velocity around the seismogenic faults in western Japan. We mainly focus on the <span class="hlt">seismic</span> velocity variation during (1) the 2016 Off-Mie earthquake in the Nankai subduction zone (Mw5.8) and (2) the 2016 Kumamoto earthquake in Kyushu Island (Mw7.0). We applied <span class="hlt">seismic</span> interferometry and surface wave analysis to the ambient noise data <span class="hlt">recorded</span> by Hi-net and DONET seismometers of National Research Institute for Earth Science and Disaster Resilience (NIED). <span class="hlt">Seismic</span> velocity near the rupture faults and volcano decreased during the earthquake. For example, we observed velocity reduction around the seismogenic Futagawa-Hinagu fault system and Mt Aso in the 2016 Kumamoto earthquake. We also identified velocity increase after the eruptions of Mt Aso. During the 2016 Off-Mie earthquake, we observed <span class="hlt">seismic</span> velocity variation in the Nankai accretionary prism. After the earthquakes, the <span class="hlt">seismic</span> velocity gradually returned to the pre-earthquake value. The velocity recovering process (healing process) is caused by several mechanisms, such as pore pressure reduction, strain change, and crack sealing. By showing the velocity variations obtained at different geologic settings (volcano, seismogenic fault, unconsolidated sediment), we discuss the mechanism of <span class="hlt">seismic</span> velocity variation as well as the post-<span class="hlt">seismic</span> fault healing process.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2013-title14-vol3/pdf/CFR-2013-title14-vol3-part135-appC.pdf','CFR2013'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2013-title14-vol3/pdf/CFR-2013-title14-vol3-part135-appC.pdf"><span>14 CFR Appendix <span class="hlt">C</span> to Part 135 - Helicopter Flight <span class="hlt">Recorder</span> Specifications</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2013&page.go=Go">Code of Federal Regulations, 2013 CFR</a></p> <p></p> <p>2013-01-01</p> <p>... 14 Aeronautics and Space 3 2013-01-01 2013-01-01 false Helicopter Flight <span class="hlt">Recorder</span> Specifications <span class="hlt">C</span>.... <span class="hlt">C</span> Appendix <span class="hlt">C</span> to Part 135—Helicopter Flight <span class="hlt">Recorder</span> Specifications Parameters Range Installed system... Maximum range +5% 1 1% 2 Engine torque Maximum range ±5% 1 1% 2 Flight Control—Hydraulic Pressure Primary...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1991SedG...73...13E','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1991SedG...73...13E"><span>The <span class="hlt">seismic</span> stratigraphy of Okanagan Lake, British Columbia; a <span class="hlt">record</span> of rapid deglaciation in a deep 'fiord-lake' basin</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Eyles, Nicholas; Mullins, Henry T.; Hine, Albert C.</p> <p>1991-09-01</p> <p>This paper presents the first detailed data regarding the newly discovered deep infill of Okanagan Lake. Okanagan Lake (50°00'N, 119°30'W) is 120 km long, ˜ 3-5 km wide and occupies a glacially overdeepened bedrock basin in the southern interior of British Columbia. This basin, and other elongate lakes of the region (e.g. Shuswap, Kootenay, Kalamalka, Canim and Mahood lakes), mark the site of westward flowing ice streams within successive Cordilleran ice sheets. An air gun <span class="hlt">seismic</span> survey of Okanagan Lake shows that the bedrock floor is nearly 650 m below sea-level, more than 2000 m below the rim of the surrounding plateau. The maximum thickness of Pleistocene sediment in Okanagan Lake basin approaches 800 m. Forty-six <span class="hlt">seismic</span> reflection traverses and an axial profile show a relatively simple stratigraphy composed of three <span class="hlt">seismic</span> sequences argued to be no older than the last glacial cycle (< 30 ka). A discontinuous basal unit (sequence I) characterized by large-scale diffractions, and up to 460 m thick, infills the narrow, V-shaped bedrock floor of the basin and is interpreted as a boulder gravel deposited by subglacial meltwaters. Overlying <span class="hlt">seismic</span> sequence II is composed of two sub-sequences. Sub-sequence IIa is a chaotic to massive facies up to 736 m thick. Lakeshore exposures close to where this unit reaches lake level show deformed and chaotically-bedded glaciolacustrine silts containing gravel lens and large ice-rafted boulders. The surface topography of this sub-sequence is irregular and in general mimics the form of the underlying bedrock as a result of compaction. This sequence passes laterally into stratified facies (sub-sequence IIb) at the northern end of the basin. <span class="hlt">Seismic</span> sequence II appears to <span class="hlt">record</span> rapid ice-proximal dumping of glaciolacustrine silt as the Okanagan glacier backwasted upvalley in a deep lake. A thin (60 m max.) laminated <span class="hlt">seismic</span> sequence (III) drapes the hummocky surface of sequence II and represents postglacial sedimentation</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2005AGUFM.S33A0299T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2005AGUFM.S33A0299T"><span>A Two-Radius Circular Array Method: Extracting Independent Information on Phase Velocities of Love Waves From Microtremor <span class="hlt">Records</span> From a Simple <span class="hlt">Seismic</span> Array</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tada, T.; Cho, I.; Shinozaki, Y.</p> <p>2005-12-01</p> <p>We have invented a Two-Radius (TR) circular array method of microtremor exploration, an algorithm that enables to estimate phase velocities of Love waves by analyzing horizontal-component <span class="hlt">records</span> of microtremors that are obtained with an array of <span class="hlt">seismic</span> sensors placed around circumferences of two different radii. The data <span class="hlt">recording</span> may be done either simultaneously around the two circles or in two separate sessions with sensors distributed around each circle. Both Rayleigh and Love waves are present in the horizontal components of microtremors, but in the data processing of our TR method, all information on the Rayleigh waves ends up cancelled out, and information on the Love waves alone are left to be analyzed. Also, unlike the popularly used frequency-wavenumber spectral (F-K) method, our TR method does not resolve individual plane-wave components arriving from different directions and analyze their "vector" phase velocities, but instead directly evaluates their "scalar" phase velocities --- phase velocities that contain no information on the arrival direction of waves --- through a mathematical procedure which involves azimuthal averaging. The latter feature leads us to expect that, with our TR method, it is possible to conduct phase velocity analysis with smaller numbers of sensors, with higher stability, and up to longer-wavelength ranges than with the F-K method. With a view to investigating the capabilities and limitations of our TR method in practical implementation to real data, we have deployed circular <span class="hlt">seismic</span> arrays of different sizes at a test site in Japan where the underground structure is well documented through geophysical exploration. Ten <span class="hlt">seismic</span> sensors were placed equidistantly around two circumferences, five around each circle, with varying combinations of radii ranging from several meters to several tens of meters, and simultaneous <span class="hlt">records</span> of microtremors around circles of two different radii were analyzed with our TR method to produce</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017E%26ES...95c2035M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017E%26ES...95c2035M"><span>MASW <span class="hlt">Seismic</span> Method in Brebu Landslide Area, Romania</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mihai, Marinescu; Paul, Cristea; Cristian, Marunteanu; Matei, Mezincescu</p> <p>2017-12-01</p> <p>This paper is focused on assessing the possibility of enhancing the geotechnical information in perimeters with landslides, especially through applications of the Multichannel Analysis of Surface Waves (MASW) method. The technology enables the determination of the phase velocities of Rayleigh waves and, recursively, the evaluation of shear wave velocities (Vs) related to depth. Finally, using longitudinal wave velocities (Vp), derived from the <span class="hlt">seismic</span> refraction measurements, in situ dynamic elastic properties in a shallow section can be obtained. The investigation was carried out in the Brebu landslide (3-5 m depth of bedrock), located on the southern flank of the Slanic Syncline (110 km North of Bucharest) and included a drilling program and geotechnical laboratory observations. The <span class="hlt">seismic</span> refraction <span class="hlt">records</span> (<span class="hlt">seismic</span> sources placed at the centre, ends and outside of the geophone spread) have been undertaken on two lines, 23 m and 46 m long respectively) approximately perpendicular to the downslope direction of the landslide and on different local morpho-structures. A Geode Geometrics seismograph was set for 1 ms sampling rate and pulse summations in real-time for five blows. Twenty-four vertical Geometrics SpaceTech geophones (14 Hz resonance frequency) were disposed at 1 m spacing. The <span class="hlt">seismic</span> source was represented by the impact of an 8kg weight sledge hammer on a metal plate. Regarding <span class="hlt">seismic</span> data processing, the distinctive feature is related to performing more detailed analyses of MASW <span class="hlt">records</span>. The proposed procedure consists of the spread split in groups with fewer receivers and several interval-geophones superposed. 2D Fourier analysis, f-k (frequency-wave number) spectrum, for each of these groups assures the information continuity and, all the more, accuracy to pick out the amplitude maximums of the f-k spectra. Finally, combining both values VS (calculated from 2D spectral analyses of Rayleigh waves) and VP (obtained from <span class="hlt">seismic</span> refraction <span class="hlt">records</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015JGRB..120.7536L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015JGRB..120.7536L"><span>Friction weakening in granular flows deduced from <span class="hlt">seismic</span> <span class="hlt">records</span> at the Soufrière Hills Volcano, Montserrat</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Levy, Clara; Mangeney, Anne; Bonilla, Fabian; Hibert, Clément; Calder, Eliza S.; Smith, Patrick J.</p> <p>2015-11-01</p> <p>Accurate modeling of rockfalls and pyroclastic flows is still an open issue, partly due to a lack of measurements related to their dynamics. Using <span class="hlt">seismic</span> data from the Soufrière Hills Volcano, Montserrat, and granular flow modeling, we show that the power laws relating the <span class="hlt">seismic</span> energy Es to the <span class="hlt">seismic</span> duration ts and relating the loss of potential energy ΔEp to the flow duration tf are very similar, like the power laws observed at Piton de la Fournaise, Reunion Island. Observations showing that tf≃ts suggest a constant ratio Es/ΔEp≃10-5. This similarity in these two power laws can be obtained only when the granular flow model uses a friction coefficient that decreases with the volume transported. Furthermore, with this volume-dependent friction coefficient, the simulated force applied by the flow to the ground correlates well with the <span class="hlt">seismic</span> energy, highlighting the signature of this friction weakening effect in <span class="hlt">seismic</span> data.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015EGUGA..1714642L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015EGUGA..1714642L"><span>Friction weakening in granular flows deduced from <span class="hlt">seismic</span> <span class="hlt">records</span> at the Soufrière Hills Volcano, Montserrat</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Levy, Clara; Mangeney, Anne; Bonilla, Fabian; Hibert, Clément; Calder, Eliza; Smith, Paddy</p> <p>2015-04-01</p> <p>Accurate modelling of rockfalls and pyroclastic flows is still an open issue, partly due the lack of measurements related to the dynamics of such events. Using <span class="hlt">seismic</span> data from the Soufrière Hills Volcano and granular flow modelling, we show that the power laws relating the <span class="hlt">seismic</span> energy Es to the <span class="hlt">seismic</span> duration ts and relating the loss of potential energy ΔEp to the flow duration tf are very similar (Ei ≈ tiβ with i = s,p), as observed previously at Piton de la Fournaise, Reunion Island. Observations showing that tf ≃ ts suggest a constant ratio Es/ΔEp ≃ 10-5. This similarity in the power laws can be obtained only when the granular flow model uses a friction coefficient that decreases with the volume involved. Furthermore, with this volume-dependent friction coefficient, the simulated force applied by the flow to the ground correlates well with the <span class="hlt">seismic</span> energy, highlighting the signature of this friction weakening effect in <span class="hlt">seismic</span> data.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EGUGA..1817365B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EGUGA..1817365B"><span><span class="hlt">Seismic</span> activity monitoring in the Izvorul Muntelui dam region</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Borleanu, Felix; Otilia Placinta, Anca; Popa, Mihaela; Adelin Moldovan, Iren; Popescu, Emilia</p> <p>2016-04-01</p> <p>Earthquakes occurrences near the artificial water reservoirs are caused by stress variation due to the weight of water, weakness of fractures or faults and increasing of pore pressure in crustal rocks. In the present study we aim to investigate how Izvorul Muntelui dam, located in the Eastern Carpathians influences local <span class="hlt">seismicity</span>. For this purpose we selected from the <span class="hlt">seismic</span> bulletins computed within National Data Center of National Institute for Earth Physics, Romania, crustal events occurred between 984 and 2015 in a range of 0.3 deg around the artificial lake. Subsequently to improve the <span class="hlt">seismic</span> monitoring of the region we applied a cross-correlation detector on the continuous <span class="hlt">recordings</span> of Bicaz (BIZ) <span class="hlt">seismic</span> stations. Besides the tectonic events we detected sources within this region that periodically generate artificial evens. We couldn't emphasize the existence of a direct correlation between the water level variations and natural <span class="hlt">seismicity</span> of the investigated area.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.usgs.gov/of/1998/0506/pdf/of98-506.pdf','USGSPUBS'); return false;" href="https://pubs.usgs.gov/of/1998/0506/pdf/of98-506.pdf"><span>Cruise report for a <span class="hlt">seismic</span> investigation of gas hydrates in the Mississippi Canyon region, northern Gulf of Mexico; cruise M1-98-GM</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Cooper, Alan K.; Hart, Patrick E.; Pecher, Ingo</p> <p>1998-01-01</p> <p>During the cruise about 850 km of multichannel and single-channel <span class="hlt">seismic</span> data were <span class="hlt">recorded</span>. <span class="hlt">Seismic</span> measurements at nine ocean-bottom seismometer (OBS) stations were <span class="hlt">recorded</span> for several of the multichannel tracklines (see Fig. 3 in report). The following report describes the field operations and equipment systems employed, gives two examples of ship-board <span class="hlt">seismic</span> <span class="hlt">records</span>, and outlines a few preliminary results.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1452746','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1452746"><span><span class="hlt">Seismic</span> Data from Roosevelt Hot Springs, Utah FORGE Study Area</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Miller, John</p> <p></p> <p>This set of data contains raw and processed 2D and 3D <span class="hlt">seismic</span> data from the Utah FORGE study area near Roosevelt Hot Springs. The zipped archives numbered from 1-100 to 1001-1122 contain 3D <span class="hlt">seismic</span> uncorrelated shot gatherers SEG-Y files. The zipped archives numbered from 1-100<span class="hlt">C</span> to 1001-1122<span class="hlt">C</span> contain 3D <span class="hlt">seismic</span> correlated shot gatherers SEG-Y files. Other data have intuitive names.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2005GeoJI.162..516G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2005GeoJI.162..516G"><span>Long-term <span class="hlt">seismicity</span> of the Reykjanes Ridge (North Atlantic) <span class="hlt">recorded</span> by a regional hydrophone array</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Goslin, Jean; Lourenço, Nuno; Dziak, Robert P.; Bohnenstiehl, DelWayne R.; Haxel, Joe; Luis, Joaquim</p> <p>2005-08-01</p> <p>The <span class="hlt">seismicity</span> of the northern Mid-Atlantic Ridge was <span class="hlt">recorded</span> by two hydrophone networks moored in the sound fixing and ranging (SOFAR) channel, on the flanks of the Mid-Atlantic Ridge, north and south of the Azores. During its period of operation (05/2002-09/2003), the northern `SIRENA' network, deployed between latitudes 40° 20'N and 50° 30'N, <span class="hlt">recorded</span> acoustic signals generated by 809 earthquakes on the hotspot-influenced Reykjanes Ridge. This activity was distributed between five spatio-temporal event clusters, each initiated by a moderate-to-large magnitude (4.0-5.6 M) earthquake. The rate of earthquake occurrence within the initial portion of the largest sequence (which began on 2002 October 6) is described adequately by a modified Omori law aftershock model. Although this is consistent with triggering by tectonic processes, none of the Reykjanes Ridge sequences are dominated by a single large-magnitude earthquake, and they appear to be of relatively short duration (0.35-4.5 d) when compared to previously described mid-ocean ridge aftershock sequences. The occurrence of several near-equal magnitude events distributed throughout each sequence is inconsistent with the simple relaxation of mainshock-induced stresses and may reflect the involvement of magmatic or fluid processes along this deep (>2000 m) section of the Reykjanes Ridge.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017IJASE...9..277B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017IJASE...9..277B"><span>Predicting the <span class="hlt">seismic</span> performance of typical R/<span class="hlt">C</span> healthcare facilities: emphasis on hospitals</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bilgin, Huseyin; Frangu, Idlir</p> <p>2017-09-01</p> <p>Reinforced concrete (RC) type of buildings constitutes an important part of the current building stock in earthquake prone countries such as Albania. <span class="hlt">Seismic</span> response of structures during a severe earthquake plays a vital role in the extent of structural damage and resulting injuries and losses. In this context, this study evaluates the expected performance of a five-story RC healthcare facility, representative of common practice in Albania, designed according to older codes. The design was based on the code requirements used in this region during the mid-1980s. Non-linear static and dynamic time history analyses were conducted on the structural model using the Zeus NL computer program. The dynamic time history analysis was conducted with a set of ground motions from real earthquakes. The building responses were estimated in global levels. FEMA 356 criteria were used to predict the <span class="hlt">seismic</span> performance of the building. The structural response measures such as capacity curve and inter-story drift under the set of ground motions and pushover analyses results were compared and detailed <span class="hlt">seismic</span> performance assessment was done. The main aim of this study is considering the application and methodology for the earthquake performance assessment of existing buildings. The <span class="hlt">seismic</span> performance of the structural model varied significantly under different ground motions. Results indicate that case study building exhibit inadequate <span class="hlt">seismic</span> performance under different <span class="hlt">seismic</span> excitations. In addition, reasons for the poor performance of the building is discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EP%26S...69..126K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EP%26S...69..126K"><span>On the <span class="hlt">seismic</span> response of instable rock slopes based on ambient vibration <span class="hlt">recordings</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kleinbrod, Ulrike; Burjánek, Jan; Fäh, Donat</p> <p>2017-09-01</p> <p>Rock slope failures can lead to huge human and economic loss depending on their size and exact location. Reasonable hazard mitigation requires thorough understanding of the underlying slope driving mechanisms and its rock mass properties. Measurements of <span class="hlt">seismic</span> ambient vibrations could improve the characterization and detection of rock instabilities since there is a link between <span class="hlt">seismic</span> response and internal structure of the unstable rock mass. An unstable slope near the village Gondo has been investigated. The unstable part shows strongly amplified ground motion with respect to the stable part of the rock slope. The amplification values reach maximum factors of 70. The <span class="hlt">seismic</span> response on the instable part is highly directional and polarized. Re-measurements have been taken 1 year later showing exactly the same results as the original measurements. Neither the amplified frequencies nor the amplification values have changed. Therefore, ambient vibration measurements are repeatable and stay the same, if the rock mass has not undergone any significant change in structure or volume, respectively. Additionally, four new points have been measured during the re-measuring campaign in order to better map the border of the instability.[Figure not available: see fulltext.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010AGUFM.T23E..02T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010AGUFM.T23E..02T"><span><span class="hlt">Seismic</span> anisotropy from walk-around VSP data in the Kumano basin south of Kii Peninsula (IODP Site <span class="hlt">C</span>0009A)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tsuji, T.; Hino, R.; Sanada, Y.; Park, J.; No, T.; Araki, E.; Kinoshita, M.; Bangs, N. L.; von Huene, R.; Moore, G. F.</p> <p>2010-12-01</p> <p>We estimated <span class="hlt">seismic</span> anisotropy from the walk-around Vertical <span class="hlt">Seismic</span> Profiling (VSP) data in Site <span class="hlt">C</span>0009A obtained during Integrated Ocean Drilling Program (IODP) Expedition 319. It is generally agreed that <span class="hlt">seismic</span> anisotropy within sediments is related to the cracks. For vertical cracks (Horizontal Transverse Isotropy; HTI), the fast velocity direction coincides with the direction of crack alignment, while the degree of velocity difference provides information about crack density (Crampin, 1985). If cracks are produced by a regional tectonic stress field, <span class="hlt">seismic</span> anisotropy can be used to estimate stress orientation and magnitude. In unconsolidated sequence, furthermore, the stress-induced anisotropy can be observed due to increasing contact between grains (Johnson et al., 1998). In this case (increasing grain-contact), the fast velocity direction from walk-around VSP experiment is also consistent with the principal horizontal stress direction. Site <span class="hlt">C</span>0009A is located in the Kumano basin where ~1350m unconsolidated Kumano basin sediment overlies the accretionary prism. During VSP operations, we obtained walk-away, walk-around, and zero-offset VSP data (Saffer et al., 2009). We used mainly walk-around VSP data to study <span class="hlt">seismic</span> anisotropy. In the walk-around VSP experiments, R/V Kairei deployed 4 air-gun strings (128 L total volume) and generated 275 shots. The shooting interval was 30s and the distance from the borehole was a constant 3.5 km. We deployed the Vertical <span class="hlt">Seismic</span> Imager (VSI) wireline tool into the borehole between 2989 and 3218m below the sea surface (935-1164m below seafloor). This interval corresponds to the bottom of the Kumano basin sediment section. From the walk-around VSP data, we obtained the following anisotropic parameters: (1) P-wave velocity anisotropy derived from azimuthal velocity analysis (Grechka and Tsvankin, 1998), (2) P-wave amplitude variation with azimuth (AVAZ), and (3) S-wave amplitude variation with azimuth associated with S</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.S23C0825P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.S23C0825P"><span>Geothermal Gradient impact on Induced <span class="hlt">Seismicity</span> in Raton Basin, Colorado and New Mexico</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pfeiffer, K.; Ge, S.</p> <p>2017-12-01</p> <p>Since 1999, Raton Basin, located in southeastern Colorado and northern New Mexico, is the site of wastewater injection for disposing a byproduct of coal bed methane production. During 1999-2016, 29 wastewater injection wells were active in Raton Basin. Induced <span class="hlt">seismicity</span> began in 2001 and the largest <span class="hlt">recorded</span> earthquake, an M5.3, occurred in August 2011. Although most injection occurs in the Dakota Formation, the majority of the <span class="hlt">seismicity</span> has been located in the crystalline basement. Previous studies involving Raton Basin focused on high injection rates and high volume wells to determine their effect on increased pore pressure. However, the geothermal gradient has yet to be studied as a potential catalyst of <span class="hlt">seismicity</span>. Enhanced Geothermal Systems throughout the world have experienced similar <span class="hlt">seismicity</span> problems due to water injection. Raton's geothermal gradient, which averages 49± 12°<span class="hlt">C</span>/km, is much higher then other areas experiencing <span class="hlt">seismicity</span>. Thermal differences between the hot subsurface and cooler wastewater injection have the potential to affect the strength of the rock and allow for failure. Therefore, we hypothesis that wells in high geothermal gradient areas will produce more frequent earthquakes due to thermal contrast from relatively cold wastewater injection. We model the geothermal gradient in the surrounding areas of the injection sites in Raton Basin to assess potential spatial relationship between high geothermal gradient and earthquakes. Preliminary results show that the fluid pressure increase from injecting cool water is above the threshold of 0.1MPa, which has been shown to induce earthquakes. In addition, temperatures in the subsurface could decrease up to 2°<span class="hlt">C</span> at approximately 80 m from the injection well, with a temperature effect reaching up to 100 m away from the injection well.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2003EAEJA....13070V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2003EAEJA....13070V"><span>Modernization of the Slovenian National <span class="hlt">Seismic</span> Network</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Vidrih, R.; Godec, M.; Gosar, A.; Sincic, P.; Tasic, I.; Zivcic, M.</p> <p>2003-04-01</p> <p>The Environmental Agency of the Republic of Slovenia, the Seismology Office is responsible for the fast and reliable information about earthquakes, originating in the area of Slovenia and nearby. In the year 2000 the project Modernization of the Slovenian National <span class="hlt">Seismic</span> Network started. The purpose of a modernized <span class="hlt">seismic</span> network is to enable fast and accurate automatic location of earthquakes, to determine earthquake parameters and to collect data of local, regional and global earthquakes. The modernized network will be finished in the year 2004 and will consist of 25 Q730 remote broadband data loggers based <span class="hlt">seismic</span> station subsystems transmitting in real-time data to the Data Center in Ljubljana, where the Seismology Office is located. The remote broadband station subsystems include 16 surface broadband seismometers CMG-40T, 5 broadband seismometers CMG-40T with strong motion accelerographs EpiSensor, 4 borehole broadband seismometers CMG-40T, all with accurate timing provided by GPS receivers. The <span class="hlt">seismic</span> network will cover the entire Slovenian territory, involving an area of 20,256 km2. The network is planned in this way; more <span class="hlt">seismic</span> stations will be around bigger urban centres and in regions with greater vulnerability (NW Slovenia, Krsko Brezice region). By the end of the year 2002, three old <span class="hlt">seismic</span> stations were modernized and ten new <span class="hlt">seismic</span> stations were built. All <span class="hlt">seismic</span> stations transmit data to UNIX-based computers running Antelope system software. The data is transmitted in real time using TCP/IP protocols over the Goverment Wide Area Network . Real-time data is also exchanged with <span class="hlt">seismic</span> networks in the neighbouring countries, where the data are collected from the <span class="hlt">seismic</span> stations, close to the Slovenian border. A typical <span class="hlt">seismic</span> station consists of the <span class="hlt">seismic</span> shaft with the sensor and the data acquisition system and, the service shaft with communication equipment (modem, router) and power supply with a battery box. which provides energy in case</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li class="active"><span>16</span></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_16 --> <div id="page_17" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li class="active"><span>17</span></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="321"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70169259','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70169259"><span>An economical educational <span class="hlt">seismic</span> system</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Lehman, J. D.</p> <p>1980-01-01</p> <p>There is a considerable interest in seismology from the nonprofessional or amateur standpoint. The operation of a <span class="hlt">seismic</span> system can be satisfying and educational, especially when you have built and operated the system yourself. A long-period indoor-type sensor and <span class="hlt">recording</span> system that works extremely well has been developed in the James Madison University Physics Deparment. The system can be built quite economically, and any educational institution that cannot commit themselves to a professional installation need not be without first-hand <span class="hlt">seismic</span> information. The system design approach has been selected by college students working a project or senior thesis, several elementary and secondary science teachers, as well as the more ambitious tinkerer or hobbyist at home </p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.S31A0794H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.S31A0794H"><span><span class="hlt">Seismic</span> reflection response from cross-correlations of ambient vibrations on non-conventional hidrocarbon reservoir</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Huerta, F. V.; Granados, I.; Aguirre, J.; Carrera, R. Á.</p> <p>2017-12-01</p> <p>Nowadays, in hydrocarbon industry, there is a need to optimize and reduce exploration costs in the different types of reservoirs, motivating the community specialized in the search and development of alternative exploration geophysical methods. This study show the reflection response obtained from a shale gas / oil deposit through the method of <span class="hlt">seismic</span> interferometry of ambient vibrations in combination with Wavelet analysis and conventional <span class="hlt">seismic</span> reflection techniques (CMP & NMO). The method is to generate <span class="hlt">seismic</span> responses from virtual sources through the process of cross-correlation of <span class="hlt">records</span> of Ambient <span class="hlt">Seismic</span> Vibrations (ASV), collected in different receivers. The <span class="hlt">seismic</span> response obtained is interpreted as the response that would be measured in one of the receivers considering a virtual source in the other. The acquisition of ASV <span class="hlt">records</span> was performed in northern of Mexico through semi-rectangular arrays of multi-component geophones with instrumental response of 10 Hz. The in-line distance between geophones was 40 m while in cross-line was 280 m, the sampling used during the data collection was 2 ms and the total duration of the <span class="hlt">records</span> was 6 hours. The results show the reflection response of two lines in the in-line direction and two in the cross-line direction for which the continuity of coherent events have been identified and interpreted as reflectors. There is certainty that the events identified correspond to reflections because the time-frequency analysis performed with the Wavelet Transform has allowed to identify the frequency band in which there are body waves. On the other hand, the CMP and NMO techniques have allowed to emphasize and correct the reflection response obtained during the correlation processes in the frequency band of interest. The results of the processing and analysis of ASV <span class="hlt">records</span> through the <span class="hlt">seismic</span> interferometry method have allowed us to see interesting results in light of the cross-correlation process in combination with</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/982573','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/982573"><span>Second Quarter Hanford <span class="hlt">Seismic</span> Report for Fiscal Year 2009</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Rohay, Alan C.; Sweeney, Mark D.; Hartshorn, Donald C.</p> <p>2009-07-31</p> <p>The Hanford <span class="hlt">Seismic</span> Assessment Program (HSAP) provides an uninterrupted collection of high-quality raw and processed <span class="hlt">seismic</span> data from the Hanford <span class="hlt">Seismic</span> Network for the U.S. Department of Energy and its contractors. The HSAP is responsible for locating and identifying sources of <span class="hlt">seismic</span> activity and monitoring changes in the historical pattern of <span class="hlt">seismic</span> activity at the Hanford Site. The data are compiled, archived, and published for use by the Hanford Site for waste management, natural phenomena hazards assessments, and engineering design and construction. In addition, the HSAP works with the Hanford Site Emergency Services Organization to provide assistance in the eventmore » of a significant earthquake on the Hanford Site. The Hanford <span class="hlt">Seismic</span> Network and the Eastern Washington Regional Network consist of 44 individual sensor sites and 15 radio relay sites maintained by the Hanford <span class="hlt">Seismic</span> Assessment Team. The Hanford <span class="hlt">Seismic</span> Network <span class="hlt">recorded</span> over 800 local earthquakes during the second quarter of FY 2009. Nearly all of these earthquakes were detected in the vicinity of Wooded Island, located about eight miles north of Richland just west of the Columbia River. Most of the events were considered minor (magnitude (Mc) less than 1.0) with 19 events in the 2.0-2.9 range. The estimated depths of the Wooded Island events are shallow (averaging less than 1.0 km deep) with a maximum depth estimated at 1.9 km. This places the Wooded Island events within the Columbia River Basalt Group (CRBG). The low magnitude and the shallowness of the Wooded Island events have made them undetectable to most area residents. However, some Hanford employees working within a few miles of the area of highest activity, and individuals living in homes directly across the Columbia River from the swarm center, have reported feeling some movement. The Hanford SMA network was triggered numerous times by the Wooded Island swarm events. The maximum acceleration values <span class="hlt">recorded</span> by the SMA network</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014EGUGA..1616844M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014EGUGA..1616844M"><span><span class="hlt">Seismic</span> Hazard Implication of the Seismotectonics of southern Africa</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Midzi, Vunganai; Mulabisana, Thifelimbilu; Manzunzu, Brassnavy</p> <p>2014-05-01</p> <p>The work presented in this report / presentation was prepared as part of the requirements for the SIDA/IGCP Project 601 titled "Seismotectonics and <span class="hlt">Seismic</span> Hazards in Africa" as well as part of the <span class="hlt">seismic</span> source characterisation of the GEM-Africa <span class="hlt">Seismic</span> hazard study. An effort was made to compile information necessary to prepare a seismotectonic map of Africa which can then be used in carrying out a <span class="hlt">seismic</span> hazard assessment of the continent or locations within the continent. Information on major faults, fault plane solutions, geophysical data as well as stress data has so far been collected and included in a database for the southern Africa region. Reports published by several experts contributed much to the collected information. The <span class="hlt">seismicity</span> data used are part of the earthquake catalogue being prepared for the GEM-Africa project, which includes historical and instrumental <span class="hlt">records</span> as collected from various sources. An effort has been made to characterise the identified major faults and through further analysis investigate their possible impact on the <span class="hlt">seismic</span> hazard of southern Africa.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1380104','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1380104"><span>Test to Extract Soil Properties Using the <span class="hlt">Seismic</span> HammerTM Active <span class="hlt">Seismic</span> Source</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Lee, Rebekah F.; Abbott, Robert E.</p> <p></p> <p>Geologic material properties are necessary parameters for ground motion modeling and are difficult and expensive to obtain via traditional methods. Alternative methods to estimate soil properties require a measurement of the ground's response to a force. A possible method of obtaining these measurements is active-source <span class="hlt">seismic</span> surveys, but measurements of the ground response at the source must also be available. The potential of <span class="hlt">seismic</span> sources to obtain soil properties is limited, however, by the repeatability of the source. Explosives, and hammer surveys are not repeatable because of variable ground coupling or swing strength. On the other hand, the <span class="hlt">Seismic</span> Hammermore » TM (SH) is consistent in the amount of energy it inputs into the ground. In addition, it leaves large physical depressions as a result of ground compaction. The volume of ground compaction varies by location. Here, we hypothesize that physical depressions left in the earth by the SH correlate to energy <span class="hlt">recorded</span> by nearby geophones, and therefore are a measurement of soil physical properties. Using measurements of the volume of shot holes, we compare the spatial distribution of the volume of ground compacted between the different shot locations. We then examine energy <span class="hlt">recorded</span> by the nearest 50 geophones and compare the change in amplitude across hits at the same location. Finally, we use the percent difference between the energy <span class="hlt">recorded</span> by the first and later hits at a location to test for a correlation to the volume of the shot depressions. We find that: * Ground compaction at the shot-depression does cluster geographically, but does not correlate to known surface features. * Energy <span class="hlt">recorded</span> by nearby geophones reflects ground refusal after several hits. * There is no correlation to shot volume and changes in energy at particular shot locations. Deeper material properties (i.e. below the depth of surface compaction) may be contributing to the changes in energy propagation. * Without further</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.V23A0468D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.V23A0468D"><span>InSAR Surface Deformation and Source Modelling at Semisopochnoi Island During the 2014 and 2015 <span class="hlt">Seismic</span> Swarms with Constraints from Geochemical and <span class="hlt">Seismic</span> Analysis</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>DeGrandpre, K.; Pesicek, J. D.; Lu, Z.</p> <p>2017-12-01</p> <p>During the summer of 2014 and the early spring of 2015 two notable increases in <span class="hlt">seismic</span> activity at Semisopochnoi Island in the western Aleutian islands were <span class="hlt">recorded</span> on AVO seismometers on Semisopochnoi and neighboring islands. These <span class="hlt">seismic</span> swarms did not lead to an eruption. This study employs interferometric synthetic aperture radar (InSAR) techniques using TerraSAR-X images in conjunction with more accurately relocating the <span class="hlt">recorded</span> <span class="hlt">seismic</span> events through simultaneous inversion of event travel times and a three-dimensional velocity model using tomoDD. The InSAR images exhibit surprising coherence and an island wide spatial distribution of inflation that is then used in Mogi, Okada, spheroid, and ellipsoid source models in order to define the three-dimensional location and volume change required for a source at the volcano to produce the observed surface deformation. The tomoDD relocations provide a more accurate and realistic three-dimensional velocity model as well as a tighter clustering of events for both swarms that clearly outline a linear <span class="hlt">seismic</span> void within the larger group of shallow (<10 km) <span class="hlt">seismicity</span>. The source models are fit to this void and pressure estimates from geochemical analysis are used to verify the storage depth of magmas at Semisopochnoi. Comparisons of calculated source cavity, magma injection, and surface deformation volumes are made in order to assess the reality behind the various modelling estimates. Incorporating geochemical and <span class="hlt">seismic</span> data to provide constraints on surface deformation source inversions provides an interdisciplinary approach that can be used to make more accurate interpretations of dynamic observations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010EGUGA..12.2567C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010EGUGA..12.2567C"><span>Kinematic <span class="hlt">Seismic</span> Rupture Parameters from a Doppler Analysis</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Caldeira, Bento; Bezzeghoud, Mourad; Borges, José F.</p> <p>2010-05-01</p> <p>The radiation emitted from extended <span class="hlt">seismic</span> sources, mainly when the rupture spreads in preferred directions, presents spectral deviations as a function of the observation location. This aspect, unobserved to point sources, and named as directivity, are manifested by an increase in the frequency and amplitude of <span class="hlt">seismic</span> waves when the rupture occurs in the direction of the <span class="hlt">seismic</span> station and a decrease in the frequency and amplitude if it occurs in the opposite direction. The model of directivity that supports the method is a Doppler analysis based on a kinematic source model of rupture and wave propagation through a structural medium with spherical symmetry [1]. A unilateral rupture can be viewed as a sequence of shocks produced along certain paths on the fault. According this model, the <span class="hlt">seismic</span> <span class="hlt">record</span> at any point on the Earth's surface contains a signature of the rupture process that originated the <span class="hlt">recorded</span> waveform. Calculating the rupture direction and velocity by a general Doppler equation, - the goal of this work - using a dataset of common time-delays read from waveforms <span class="hlt">recorded</span> at different distances around the epicenter, requires the normalization of measures to a standard value of slowness. This normalization involves a non-linear inversion that we solve numerically using an iterative least-squares approach. The evaluation of the performance of this technique was done through a set of synthetic and real applications. We present the application of the method at four real case studies, the following earthquakes: Arequipa, Peru (Mw = 8.4, June 23, 2001); Denali, AK, USA (Mw = 7.8; November 3, 2002); Zemmouri-Boumerdes, Algeria (Mw = 6.8, May 21, 2003); and Sumatra, Indonesia (Mw = 9.3, December 26, 2004). The results obtained from the dataset of the four earthquakes agreed, in general, with the values presented by other authors using different methods and data. [1] Caldeira B., Bezzeghoud M, Borges JF, 2009; DIRDOP: a directivity approach to determining</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016GeoRL..4310078S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016GeoRL..4310078S"><span>The shallow elastic structure of the lunar crust: New insights from <span class="hlt">seismic</span> wavefield gradient analysis</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sollberger, David; Schmelzbach, Cedric; Robertsson, Johan O. A.; Greenhalgh, Stewart A.; Nakamura, Yosio; Khan, Amir</p> <p>2016-10-01</p> <p>Enigmatic lunar seismograms <span class="hlt">recorded</span> during the Apollo 17 mission in 1972 have so far precluded the identification of shear-wave arrivals and hence the construction of a comprehensive elastic model of the shallow lunar subsurface. Here, for the first time, we extract shear-wave information from the Apollo active <span class="hlt">seismic</span> data using a novel waveform analysis technique based on spatial <span class="hlt">seismic</span> wavefield gradients. The star-like <span class="hlt">recording</span> geometry of the active <span class="hlt">seismic</span> experiment lends itself surprisingly well to compute spatial wavefield gradients and rotational ground motion as a function of time. These observables, which are new to <span class="hlt">seismic</span> exploration in general, allowed us to identify shear waves in the complex lunar seismograms, and to derive a new model of <span class="hlt">seismic</span> compressional and shear-wave velocities in the shallow lunar crust, critical to understand its lithology and constitution, and its impact on other geophysical investigations of the Moon's deep interior.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMNS23A0012G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMNS23A0012G"><span>High-Resolution <span class="hlt">Seismic</span> Imaging of Near-Surface Voids</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gritto, R.; Korneev, V. A.; Elobaid, E. A.; Mohamed, F.; Sadooni, F.</p> <p>2017-12-01</p> <p> to detect and locate the object. Furthermore, we show that ambient noise <span class="hlt">recordings</span> may generate data with sufficient signal-to-noise ratio to successfully detect and locate subsurface voids. Being able to use ambient noise <span class="hlt">recordings</span> would eliminate the need to employ active <span class="hlt">seismic</span> sources that are time consuming and more expensive to operate.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.S41F..03P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.S41F..03P"><span>High Temporal Resolution Mapping of <span class="hlt">Seismic</span> Noise Sources Using Heterogeneous Supercomputers</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Paitz, P.; Gokhberg, A.; Ermert, L. A.; Fichtner, A.</p> <p>2017-12-01</p> <p>The time- and space-dependent distribution of <span class="hlt">seismic</span> noise sources is becoming a key ingredient of modern real-time monitoring of various geo-systems like earthquake fault zones, volcanoes, geothermal and hydrocarbon reservoirs. We present results of an ongoing research project conducted in collaboration with the Swiss National Supercomputing Centre (CSCS). The project aims at building a service providing <span class="hlt">seismic</span> noise source maps for Central Europe with high temporal resolution. We use source imaging methods based on the cross-correlation of <span class="hlt">seismic</span> noise <span class="hlt">records</span> from all <span class="hlt">seismic</span> stations available in the region of interest. The service is hosted on the CSCS computing infrastructure; all computationally intensive processing is performed on the massively parallel heterogeneous supercomputer "Piz Daint". The solution architecture is based on the Application-as-a-Service concept to provide the interested researchers worldwide with regular access to the noise source maps. The solution architecture includes the following sub-systems: (1) data acquisition responsible for collecting, on a periodic basis, raw <span class="hlt">seismic</span> <span class="hlt">records</span> from the European <span class="hlt">seismic</span> networks, (2) high-performance noise source mapping application responsible for the generation of source maps using cross-correlation of <span class="hlt">seismic</span> <span class="hlt">records</span>, (3) back-end infrastructure for the coordination of various tasks and computations, (4) front-end Web interface providing the service to the end-users and (5) data repository. The noise source mapping itself rests on the measurement of logarithmic amplitude ratios in suitably pre-processed noise correlations, and the use of simplified sensitivity kernels. During the implementation we addressed various challenges, in particular, selection of data sources and transfer protocols, automation and monitoring of daily data downloads, ensuring the required data processing performance, design of a general service-oriented architecture for coordination of various sub-systems, and</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70035282','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70035282"><span><span class="hlt">Seismic</span> hazard and risk assessment in the intraplate environment: The New Madrid <span class="hlt">seismic</span> zone of the central United States</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Wang, Z.</p> <p>2007-01-01</p> <p>Although the causes of large intraplate earthquakes are still not fully understood, they pose certain hazard and risk to societies. Estimating hazard and risk in these regions is difficult because of lack of earthquake <span class="hlt">records</span>. The New Madrid <span class="hlt">seismic</span> zone is one such region where large and rare intraplate earthquakes (M = 7.0 or greater) pose significant hazard and risk. Many different definitions of hazard and risk have been used, and the resulting estimates differ dramatically. In this paper, <span class="hlt">seismic</span> hazard is defined as the natural phenomenon generated by earthquakes, such as ground motion, and is quantified by two parameters: a level of hazard and its occurrence frequency or mean recurrence interval; <span class="hlt">seismic</span> risk is defined as the probability of occurrence of a specific level of <span class="hlt">seismic</span> hazard over a certain time and is quantified by three parameters: probability, a level of hazard, and exposure time. Probabilistic <span class="hlt">seismic</span> hazard analysis (PSHA), a commonly used method for estimating <span class="hlt">seismic</span> hazard and risk, derives a relationship between a ground motion parameter and its return period (hazard curve). The return period is not an independent temporal parameter but a mathematical extrapolation of the recurrence interval of earthquakes and the uncertainty of ground motion. Therefore, it is difficult to understand and use PSHA. A new method is proposed and applied here for estimating <span class="hlt">seismic</span> hazard in the New Madrid <span class="hlt">seismic</span> zone. This method provides hazard estimates that are consistent with the state of our knowledge and can be easily applied to other intraplate regions. ?? 2007 The Geological Society of America.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PApGe.174.2523S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PApGe.174.2523S"><span>Attenuation Characteristics of High Frequency <span class="hlt">Seismic</span> Waves in Southern India</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sivaram, K.; Utpal, Saikia; Kanna, Nagaraju; Kumar, Dinesh</p> <p>2017-07-01</p> <p>We present a systematic study of <span class="hlt">seismic</span> attenuation and its related Q structure derived from the spectral analysis of P-, S-waves in the southern India. The study region is separated into parts of EDC (Eastern Dharwar Craton), Western Dharwar Craton (WDC) and Southern Granulite Terrain (SGT). The study is carried out in the frequency range 1-20 Hz, using a single-station spectral ratio technique. We make use of about 45 earthquakes, <span class="hlt">recorded</span> in a network of about 32 broadband 3-component seismograph-stations, having magnitudes ( M L) varying from 1.6 to 4.5, to estimate the average <span class="hlt">seismic</span> body wave attenuation quality factors; Q P and Q S. Their estimated average values are observed to be fitting to the power law form of Q = Q 0 f n . The averaged power law relations for Southern Indian region (as a whole) are obtained as Q P = (95 ± 1.12) f (1.32±0.01); Q S = (128 ± 1.84) f (1.49±0.01). Based on the stations and <span class="hlt">recorded</span> local earthquakes, for parts of EDC, WDC and SGT, the average power law estimates are obtained as: Q P = (97 ± 5) f (1.40±0.03), Q S = (116 ± 1.5) f (1.48±0.01) for EDC region; Q P = (130 ± 7) f (1.20±0.03), Q S = (103 ± 3) f (1.49±0.02) for WDC region; Q P = (68 ± 2) f (1.4±0.02), Q S = (152 ± 6) f (1.48±0.02) for SGT region. These estimates are weighed against coda Q ( Q <span class="hlt">C</span>) estimates, using the coda decay technique, which is based on a weak backscattering of S-waves. A major observation in the study of body wave analysis is the low body wave Q ( Q 0 < 200), moderately high value of the frequency-exponent, ` n' (>0.5) and Q S/ Q P ≫ 1, suggesting lateral stretches of dominant scattering mode of <span class="hlt">seismic</span> wave propagation. This primarily could be attributed to possible thermal anomalies and spread of partially fluid-saturated rock-masses in the crust and upper mantle of the southern Indian region, which, however, needs further laboratory studies. Such physical conditions might partly be correlated to the active <span class="hlt">seismicity</span> and</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010EGUGA..12.6657E','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010EGUGA..12.6657E"><span>Man-caused <span class="hlt">seismicity</span> of Kuzbass</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Emanov, Alexandr; Emanov, Alexey; Leskova, Ekaterina; Fateyev, Alexandr</p> <p>2010-05-01</p> <p>A natural <span class="hlt">seismicity</span> of Kuznetsk Basin is confined in the main to mountain frame of Kuznetsk hollow. In this paper materials of experimental work with local station networks within sediment basin are presented. Two types of <span class="hlt">seismicity</span> display within Kuznetsk hollow have been understood: first, man-caused <span class="hlt">seismic</span> processes, confined to mine working and concentrated on depths up to one and a half of km; secondly, <span class="hlt">seismic</span> activations on depths of 2-56 km, not coordinated in plan with coal mines. Every of studied <span class="hlt">seismic</span> activations consists of large quantity of earthquakes of small powers (Ms=1-3). From one to first tens of earthquakes were <span class="hlt">recorded</span> in a day. The earthquakes near mine working shift in space along with mine working, and <span class="hlt">seismic</span> process become stronger at the instant a coal-plough machine is operated, and slacken at the instant the preventive works are executed. The <span class="hlt">seismic</span> processes near three lavas in Kuznetsk Basin have been studied in detail. Uplift is the most typical focal mechanism. Activated zone near mine working reach in diameter 1-1,5 km. <span class="hlt">Seismic</span> activations not linked with mine working testify that the subsoil of Kuznetsk hollow remain in stress state in whole. The most probable causes of man-caused action on hollow are processes, coupled with change of physical state of rocks at loss of methane from large volume or change by mine working of rock watering in large volume. In this case condensed rocks, lost gas and water, can press out upwards, realizing the reverse fault mechanism of earthquakes. A combination of stress state of hollow with man-caused action at deep mining may account for incipient activations in Kuznetsk Basin. Today earthquakes happen mainly under mine workings, though damages of workings themselves do not happen, but intensive shaking on surface calls for intent study of so dangerous phenomena. In 2009 replicates of the experiment on research of <span class="hlt">seismic</span> activations in area of before investigated lavas have been conducted</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013PhDT.......106O','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013PhDT.......106O"><span>Studies of earthquakes and microearthquakes using near-field <span class="hlt">seismic</span> and geodetic observations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>O'Toole, Thomas Bartholomew</p> <p></p> <p>The Centroid-Moment Tensor (CMT) method allows an optimal point-source description of an earthquake to be recovered from a set of <span class="hlt">seismic</span> observations, and, for over 30 years, has been routinely applied to determine the location and source mechanism of teleseismically <span class="hlt">recorded</span> earthquakes. The CMT approach is, however, entirely general: any measurements of <span class="hlt">seismic</span> displacement fields could, in theory, be used within the CMT inversion formulation, so long as the treatment of the earthquake as a point source is valid for that data. We modify the CMT algorithm to enable a variety of near-field <span class="hlt">seismic</span> observables to be inverted for the source parameters of an earthquake. The first two data types that we implement are provided by Global Positioning System receivers operating at sampling frequencies of 1,Hz and above. When deployed in the <span class="hlt">seismic</span> near field, these instruments may be used as long-period-strong-motion seismometers, <span class="hlt">recording</span> displacement time series that include the static offset. We show that both the displacement waveforms, and static displacements alone, can be used to obtain CMT solutions for moderate-magnitude earthquakes, and that performing analyses using these data may be useful for earthquake early warning. We also investigate using waveform <span class="hlt">recordings</span> - made by conventional seismometers deployed at the surface, or by geophone arrays placed in boreholes - to determine CMT solutions, and their uncertainties, for microearthquakes induced by hydraulic fracturing. A similar waveform inversion approach could be applied in many other settings where induced <span class="hlt">seismicity</span> and microseismicity occurs..</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70013960','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70013960"><span><span class="hlt">Seismicity</span> and eruptive activity at Fuego Volcano, Guatemala: February 1975 -January 1977</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Yuan, A.T.E.; McNutt, S.R.; Harlow, D.H.</p> <p>1984-01-01</p> <p>We examine <span class="hlt">seismic</span> and eruptive activity at Fuego Volcano (14??29???N, 90?? 53???W), a 3800-m-high stratovolcano located in the active volcanic arc of Guatemala. Eruptions at Fuego are typically short-lived vulcanian eruptions producing ash falls and ash flows of high-alumina basalt. From February 1975 to December 1976, five weak ash eruptions occurred, accompanied by small earthquake swarms. Between 0 and 140 (average ??? 10) A-type or high-frequency <span class="hlt">seismic</span> events per day with M > 0.5 were <span class="hlt">recorded</span> during this period. Estimated thermal energies for each eruption are greater by a factor of 106 than cumulative <span class="hlt">seismic</span> energies, a larger ratio than that reported for other volcanoes. Over 4000 A-type events were <span class="hlt">recorded</span> January 3-7, 1977 (cumulative <span class="hlt">seismic</span> energy ??? 109 joules), yet no eruption occurred. Five 2-hour-long pulses of intense <span class="hlt">seismicity</span> separated by 6-hour intervals of quiescence accounted for the majority of events. Maximum likelihood estimates of b-values range from 0.7 ?? 0.2 to 2.1 ?? 0.4 with systematically lower values corresponding to the five intense pulses. The low values suggest higher stress conditions. During the 1977 swarm, a tiltmeter located 6 km southeast of Fuego <span class="hlt">recorded</span> a 14 ?? 3 microradian tilt event (down to SW). This value is too large to represent a simple change in the elastic strain field due to the earthquake swarm. We speculate that the earthquake swarm and tilt are indicative of subsurface magma movement. ?? 1984.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018GeoJI.tmp..176M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018GeoJI.tmp..176M"><span>The modest <span class="hlt">seismicity</span> of the northern Red Sea rift</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mitchell, Neil C.; Stewart, Ian C. F.</p> <p>2018-05-01</p> <p>Inferring tectonic movements from earthquakes (`seismotectonics') relies on earthquakes faithfully <span class="hlt">recording</span> tectonic motions. In the northern half of the Red Sea, however, events of magnitude 5.0 and above are almost entirely absent from global catalogues, even though GPS and other plate motion data suggest that the basin is actively rifting at ˜10 mm yr-1. <span class="hlt">Seismic</span> moments computed here from event magnitudes contributed to the International Seismology Centre (ISC) suggest that the moment release rate is more than an order of magnitude smaller than for the southern Red Sea and for the Southwest Indian Ridge (SWIR), which is spreading at a comparable rate to the central Red Sea and is more remote from <span class="hlt">recording</span> stations. A smaller moment release rate in the northern Red Sea might be anticipated from its smaller spreading rate, but <span class="hlt">seismic</span> coupling coefficients, which account for spreading rate variations, are also one order of magnitude smaller than for the other two areas. We explore potential explanations for this apparently reduced <span class="hlt">seismicity</span>. The northern Red Sea is almost continuously covered with thick evaporites and overlying Plio-Pleistocene sediments. These deposits may have reduced the thickness of the seismogenic layer, for example, by elevating lithosphere temperatures by a thermal blanketing effect or by leading to excess pore fluid pressures that reduce effective stress. The presence of subdued <span class="hlt">seismicity</span> here implies that tectonic movements can in places be poorly <span class="hlt">recorded</span> by earthquake data and requires that alternative data be sought when investigating the active tectonics of sedimented rifts in particular.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.S32A..08K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.S32A..08K"><span>MyShake: Initial Observations from a Global Smartphone <span class="hlt">Seismic</span> Network</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kong, Q.; Allen, R. M.; Schreier, L.</p> <p>2016-12-01</p> <p>MyShake is a global smartphone <span class="hlt">seismic</span> network that harnesses the power of crowdsourcing. It has two component: an android application running on the personal smartphones to detect earthquake-like motion, and a network detection algorithm to aggregate results from multiple smartphones to detect earthquakes. The MyShake application was released to the public on Feb 12th 2016. Within the first 5 months, there are more than 200 earthquakes <span class="hlt">recorded</span> by the smartphones all over the world, including events in Chile, Argentina, Mexico, Morocco, Greece, Nepal, New Zealand, Taiwan, Japan, and across North America. In this presentation, we will show the waveforms we <span class="hlt">recorded</span> from the smartphones for different earthquakes, and the evidences for using this data as a supplementary to the current earthquake early warning system. We will also show the performance of MyShake system during the some earthquakes in US. In short, MyShake smartphone <span class="hlt">seismic</span> network can be a nice complementary system to the current traditional <span class="hlt">seismic</span> network, at the same time, it can be a standalone system in places where few <span class="hlt">seismic</span> stations were installed to reduce the earthquake hazards.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EGUGA..1818351K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EGUGA..1818351K"><span>Fluid injection and induced <span class="hlt">seismicity</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kendall, Michael; Verdon, James</p> <p>2016-04-01</p> <p>The link between fluid injection, or extraction, and induced <span class="hlt">seismicity</span> has been observed in reservoirs for many decades. In fact spatial mapping of low magnitude events is routinely used to estimate a stimulated reservoir volume. However, the link between subsurface fluid injection and larger felt <span class="hlt">seismicity</span> is less clear and has attracted recent interest with a dramatic increase in earthquakes associated with the disposal of oilfield waste fluids. In a few cases, hydraulic fracturing has also been linked to induced <span class="hlt">seismicity</span>. Much can be learned from past case-studies of induced <span class="hlt">seismicity</span> so that we can better understand the risks posed. Here we examine 12 case examples and consider in particular controls on maximum event size, lateral event distributions, and event depths. Our results suggest that injection volume is a better control on maximum magnitude than past, natural <span class="hlt">seismicity</span> in a region. This might, however, simply reflect the lack of baseline monitoring and/or long-term <span class="hlt">seismic</span> <span class="hlt">records</span> in certain regions. To address this in the UK, the British Geological Survey is leading the deployment of monitoring arrays in prospective shale gas areas in Lancashire and Yorkshire. In most cases, <span class="hlt">seismicity</span> is generally located in close vicinity to the injection site. However, in some cases, the nearest events are up to 5km from the injection point. This gives an indication of the minimum radius of influence of such fluid injection projects. The most distant events are never more than 20km from the injection point, perhaps implying a maximum radius of influence. Some events are located in the target reservoir, but most occur below the injection depth. In fact, most events lie in the crystalline basement underlying the sedimentary rocks. This suggests that induced <span class="hlt">seismicity</span> may not pose a leakage risk for fluid migration back to the surface, as it does not impact caprock integrity. A useful application for microseismic data is to try and forecast induced <span class="hlt">seismicity</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFM.S53B2814M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFM.S53B2814M"><span>Bayesian Inference for Signal-Based <span class="hlt">Seismic</span> Monitoring</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Moore, D.</p> <p>2015-12-01</p> <p>Traditional <span class="hlt">seismic</span> monitoring systems rely on discrete detections produced by station processing software, discarding significant information present in the original <span class="hlt">recorded</span> signal. SIG-VISA (Signal-based Vertically Integrated <span class="hlt">Seismic</span> Analysis) is a system for global <span class="hlt">seismic</span> monitoring through Bayesian inference on <span class="hlt">seismic</span> signals. By modeling signals directly, our forward model is able to incorporate a rich representation of the physics underlying the signal generation process, including source mechanisms, wave propagation, and station response. This allows inference in the model to recover the qualitative behavior of recent geophysical methods including waveform matching and double-differencing, all as part of a unified Bayesian monitoring system that simultaneously detects and locates events from a global network of stations. We demonstrate recent progress in scaling up SIG-VISA to efficiently process the data stream of global signals <span class="hlt">recorded</span> by the International Monitoring System (IMS), including comparisons against existing processing methods that show increased sensitivity from our signal-based model and in particular the ability to locate events (including aftershock sequences that can tax analyst processing) precisely from waveform correlation effects. We also provide a Bayesian analysis of an alleged low-magnitude event near the DPRK test site in May 2010 [1] [2], investigating whether such an event could plausibly be detected through automated processing in a signal-based monitoring system. [1] Zhang, Miao and Wen, Lianxing. "Seismological Evidence for a Low-Yield Nuclear Test on 12 May 2010 in North Korea". Seismological Research Letters, January/February 2015. [2] Richards, Paul. "A <span class="hlt">Seismic</span> Event in North Korea on 12 May 2010". CTBTO SnT 2015 oral presentation, video at https://video-archive.ctbto.org/index.php/kmc/preview/partner_id/103/uiconf_id/4421629/entry_id/0_ymmtpps0/delivery/http</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMNH11A1704S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMNH11A1704S"><span>Retrieval of P wave Basin Response from Autocorrelation of <span class="hlt">Seismic</span> Noise-Jakarta, Indonesia</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Saygin, E.; Cummins, P. R.; Lumley, D. E.</p> <p>2016-12-01</p> <p>Indonesia's capital city, Jakarta, is home to a very large (over 10 million), vulnerable population and is proximate to known active faults, as well as to the subduction of Australian plate, which has a megathrust at abut 300 km distance, as well as intraslab <span class="hlt">seismicity</span> extending to directly beneath the city. It is also located in a basin filled with a thick layer of unconsolidated and poorly consolidated sediment, which increases the <span class="hlt">seismic</span> hazard the city is facing. Therefore, the information on the <span class="hlt">seismic</span> velocity structure of the basin is crucial for increasing our knowledge of the <span class="hlt">seismic</span> risk. We undertook a passive deployment of broadband seismographs throughout the city over a 3-month interval in 2013-2014, <span class="hlt">recording</span> ambient <span class="hlt">seismic</span> noise at over 90 sites for intervals of 1 month or more. Here we consider autocorrelations of the vertical component of the continuously <span class="hlt">recorded</span> <span class="hlt">seismic</span> wavefield across this dense network to image the shallow P wave velocity structure of Jakarta, Indonesia. Unlike the surface wave Green's functions used in ambient noise tomography, the vertical-component autocorrelograms are dominated by body wave energy that is potentially sensitive to sharp velocity contrasts, which makes them useful in <span class="hlt">seismic</span> imaging. Results show autocorrelograms at different <span class="hlt">seismic</span> stations with travel time variations that largely reflect changes in sediment thickness across the basin. We also confirm the validity our interpretation of the observed autocorrelation waveforms by conducting 2D finite difference full waveform numerical modeling for randomly distributed <span class="hlt">seismic</span> sources to retrieve the reflection response through autocorrelation.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li class="active"><span>17</span></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_17 --> <div id="page_18" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li class="active"><span>18</span></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="341"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMPP53E..06C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMPP53E..06C"><span><span class="hlt">Record</span> of <span class="hlt">C</span>4 Photosynthesis Through the Late Neogene and Pleistocene</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Cerling, T. E.</p> <p>2016-12-01</p> <p><span class="hlt">C</span>4 photosynthesis is an adaptation to the low atmospheric carbon dioxide concentrations experienced in the Neogene; it is found principally in tropical to sub-tropical/temperate regions where temperatures are high in the growing season. Although <span class="hlt">C</span>4 photosynthesis makes up about 50% of Net Primary Productivity in tropical regions, its macroscopic fossil <span class="hlt">record</span> is extremely sparse. Therefore, inferences to its significance in local ecosystems are based primarily on stable isotopes, with phytoliths become more important as phytolith morphology becomes better associated with plant structure and classification. Stable isotopes have been the principal <span class="hlt">recorder</span> for understanding the history of <span class="hlt">C</span>4 photosynthesis; however, different materials <span class="hlt">record</span> different aspects of the <span class="hlt">C</span>4 contribution to ecosystem structure and thus are telling different parts of the same story. With the fossil <span class="hlt">record</span> so poorly known, we often assume similar ecosystem structures and functions as we observe in modern analogues. It is likely that large evolutionary changes have taken place within <span class="hlt">C</span>4 plants as they went from < 1% tropical NPP to > 50% tropical NPP in the late Neogene.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://rosap.ntl.bts.gov/view/dot/25330','DOTNTL'); return false;" href="https://rosap.ntl.bts.gov/view/dot/25330"><span><span class="hlt">Seismic</span> vulnerability of new highway construction, executive summary.</span></a></p> <p><a target="_blank" href="http://ntlsearch.bts.gov/tris/index.do">DOT National Transportation Integrated Search</a></p> <p></p> <p>2002-03-01</p> <p>This executive summary gives an overview of the results of FHWA Contract DTFH61-92-<span class="hlt">C</span>-00112, <span class="hlt">Seismic</span> Research Program, : which performed a series of special studies addressing the <span class="hlt">seismic</span> design of new construction. The objectives of this project : we...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://rosap.ntl.bts.gov/view/dot/15495','DOTNTL'); return false;" href="https://rosap.ntl.bts.gov/view/dot/15495"><span><span class="hlt">Seismic</span> Vulnerability of New Highway Construction, Executive Summary.</span></a></p> <p><a target="_blank" href="http://ntlsearch.bts.gov/tris/index.do">DOT National Transportation Integrated Search</a></p> <p></p> <p>2002-03-01</p> <p>This executive summary gives an overview of the results of FHWA Contract DTFH61-92-<span class="hlt">C</span>-00112, <span class="hlt">Seismic</span> Research Program, which performed a series of special studies addressing the <span class="hlt">seismic</span> design of new construction. The objectives of this project were t...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/972560','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/972560"><span>Annual Hanford <span class="hlt">Seismic</span> Report for Fiscal Year 2009</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Rohay, Alan C.; Sweeney, Mark D.; Hartshorn, Donald C.</p> <p>2009-12-31</p> <p>The Hanford <span class="hlt">Seismic</span> Assessment Program (HSAP) provides an uninterrupted collection of high-quality raw and processed <span class="hlt">seismic</span> data from the Hanford <span class="hlt">Seismic</span> Network for the U.S. Department of Energy and its contractors. The HSAP is responsible for locating and identifying sources of <span class="hlt">seismic</span> activity and monitoring changes in the historical pattern of <span class="hlt">seismic</span> activity at the Hanford Site. The data are compiled, archived, and published for use by the Hanford Site for waste management, natural phenomena hazards assessments, and engineering design and construction. In addition, the HSAP works with the Hanford Site Emergency Services Organization to provide assistance in the eventmore » of a significant earthquake on the Hanford Site. The Hanford <span class="hlt">Seismic</span> Network and the Eastern Washington Regional Network consist of 44 individual sensor sites and 15 radio relay sites maintained by the Hanford <span class="hlt">Seismic</span> Assessment Team. During FY 2009, the Hanford <span class="hlt">Seismic</span> Network <span class="hlt">recorded</span> nearly 3000 triggers on the seismometer system, which included over 1700 <span class="hlt">seismic</span> events in the southeast Washington area and an additional 370 regional and teleseismic events. There were 1648 events determined to be local earthquakes relevant to the Hanford Site. Nearly all of these earthquakes were detected in the vicinity of Wooded Island, located about eight miles north of Richland just west of the Columbia River. <span class="hlt">Recording</span> of the Wooded Island events began in January with over 250 events per month through June 2009. The frequency of events decreased starting in July 2009 to approximately 10-15 events per month through September 2009. Most of the events were considered minor (coda-length magnitude [Mc] less than 1.0) with 47 events in the 2.0-3.0 range. The estimated depths of the Wooded Island events are shallow (averaging less than 1.0 km deep) with a maximum depth estimated at 2.3 km. This places the Wooded Island events within the Columbia River Basalt Group (CRBG). The highest-magnitude event (3</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70029890','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70029890"><span>Probabilistic <span class="hlt">seismic</span> demand analysis using advanced ground motion intensity measures</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Tothong, P.; Luco, N.</p> <p>2007-01-01</p> <p>One of the objectives in performance-based earthquake engineering is to quantify the <span class="hlt">seismic</span> reliability of a structure at a site. For that purpose, probabilistic <span class="hlt">seismic</span> demand analysis (PSDA) is used as a tool to estimate the mean annual frequency of exceeding a specified value of a structural demand parameter (e.g. interstorey drift). This paper compares and contrasts the use, in PSDA, of certain advanced scalar versus vector and conventional scalar ground motion intensity measures (IMs). One of the benefits of using a well-chosen IM is that more accurate evaluations of <span class="hlt">seismic</span> performance are achieved without the need to perform detailed ground motion <span class="hlt">record</span> selection for the nonlinear dynamic structural analyses involved in PSDA (e.g. <span class="hlt">record</span> selection with respect to <span class="hlt">seismic</span> parameters such as earthquake magnitude, source-to-site distance, and ground motion epsilon). For structural demands that are dominated by a first mode of vibration, using inelastic spectral displacement (Sdi) can be advantageous relative to the conventionally used elastic spectral acceleration (Sa) and the vector IM consisting of Sa and epsilon (??). This paper demonstrates that this is true for ordinary and for near-source pulse-like earthquake <span class="hlt">records</span>. The latter ground motions cannot be adequately characterized by either Sa alone or the vector of Sa and ??. For structural demands with significant higher-mode contributions (under either of the two types of ground motions), even Sdi (alone) is not sufficient, so an advanced scalar IM that additionally incorporates higher modes is used.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1990JVGR...41..297M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1990JVGR...41..297M"><span>Analysis of <span class="hlt">seismic</span> patterns observed at Nevado del Ruiz volcano, Colombia during August September 1985</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Martinelli, Bruno</p> <p>1990-07-01</p> <p>The <span class="hlt">seismic</span> activity of the Nevado del Ruiz volcano was monitored during August-September 1985 using a three-component portable seismograph station placed on the upper part of the volcano. The objective was to investigate the frequency content of the <span class="hlt">seismic</span> signals and the possible sources of the volcanic tremor. The <span class="hlt">seismicity</span> showed a wide spectrum of signals, especially at the beginning of September. Some relevant patterns from the collected <span class="hlt">records</span>, which have been analyzed by spectrum analysis, are presented. For the purpose of analysis, the <span class="hlt">records</span> have been divided into several categories such as long-period events, tremor, cyclic tremor episodes, and strong <span class="hlt">seismic</span> activity on September 8, 1985. The origin of the <span class="hlt">seismic</span> signals must be considered in relation to the dynamical and acoustical properties of fluids and the shape and dimensions of the volcano's conduits. The main results of the present experiment and analysis show that the sources of the <span class="hlt">seismic</span> signals are within the volcanic edifice. The signal characteristics indicate that the sources lie in fluid-phase interactions rather than in brittle fracturing of solid components.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFM.V14B..02W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFM.V14B..02W"><span><span class="hlt">Seismic</span> Forecasting of Eruptions at Dormant StratoVolcanoes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>White, R. A.</p> <p>2015-12-01</p> <p><span class="hlt">Seismic</span> monitoring data provide important constraints on tracking magmatic ascent and eruption. Based on direct experience with over 25 and review of over 10 additional eruption sequences at 24 volcanoes, we have identified 4 phases of precursory <span class="hlt">seismicity</span>. 1) Deep (>20 km) low frequency (DLF) earthquakes occur near the base of the crust as magma rises toward crustal reservoirs. This <span class="hlt">seismicity</span> is the most difficult to observe, owing to generally small magnitudes (M<2.5) the significant depth. 2) Distal volcano-tectonic (DVT) earthquakes occur on tectonic faults from a 2 to 30+ km distance laterally from (not beneath) the eventual eruption site as magma intrudes into and rises out of upper crustal reservoirs to depths of 2-3 km. A survey of 111 eruptions of 83 previously dormant volcanoes, (including all eruptions of VEI >4 since 1955) shows they were all preceded by significant DVT <span class="hlt">seismicity</span>, usually felt. This DVT <span class="hlt">seismicity</span> is easily observed owing to magnitudes generally reaching M>3.5. The cumulative DVT energy correlates to the intruding magma volume. 3) Low frequency (LF) earthquakes, LF tremor and contained explosions occur as magma interacts with the shallow hydrothermal system (<2 km depth), while the distal <span class="hlt">seismicity</span> dies off.4) Shortly after this, repetitive self-similar proximal <span class="hlt">seismicity</span> may occur and may dominate the <span class="hlt">seismic</span> <span class="hlt">records</span> as magma rises to the surface. We present some examples of this <span class="hlt">seismic</span> progression to demonstrate that data from a single short-period vertical station are often sufficient to forecast eruption onsets.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20130008794','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20130008794"><span><span class="hlt">Seismic</span> Imager Space Telescope</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Sidick, Erkin; Coste, Keith; Cunningham, J.; Sievers,Michael W.; Agnes, Gregory S.; Polanco, Otto R.; Green, Joseph J.; Cameron, Bruce A.; Redding, David C.; Avouac, Jean Philippe; <a style="text-decoration: none; " href="javascript:void(0); " onClick="displayelement('author_20130008794'); toggleEditAbsImage('author_20130008794_show'); toggleEditAbsImage('author_20130008794_hide'); "> <img style="display:inline; width:12px; height:12px; " src="images/arrow-up.gif" width="12" height="12" border="0" alt="hide" id="author_20130008794_show"> <img style="width:12px; height:12px; display:none; " src="images/arrow-down.gif" width="12" height="12" border="0" alt="hide" id="author_20130008794_hide"></p> <p>2012-01-01</p> <p>A concept has been developed for a geostationary <span class="hlt">seismic</span> imager (GSI), a space telescope in geostationary orbit above the Pacific coast of the Americas that would provide movies of many large earthquakes occurring in the area from Southern Chile to Southern Alaska. The GSI movies would cover a field of view as long as 300 km, at a spatial resolution of 3 to 15 m and a temporal resolution of 1 to 2 Hz, which is sufficient for accurate measurement of surface displacements and photometric changes induced by <span class="hlt">seismic</span> waves. Computer processing of the movie images would exploit these dynamic changes to accurately measure the rapidly evolving surface waves and surface ruptures as they happen. These measurements would provide key information to advance the understanding of the mechanisms governing earthquake ruptures, and the propagation and arrest of damaging <span class="hlt">seismic</span> waves. GSI operational strategy is to react to earthquakes detected by ground seismometers, slewing the satellite to point at the epicenters of earthquakes above a certain magnitude. Some of these earthquakes will be foreshocks of larger earthquakes; these will be observed, as the spacecraft would have been pointed in the right direction. This strategy was tested against the historical <span class="hlt">record</span> for the Pacific coast of the Americas, from 1973 until the present. Based on the <span class="hlt">seismicity</span> <span class="hlt">recorded</span> during this time period, a GSI mission with a lifetime of 10 years could have been in position to observe at least 13 (22 on average) earthquakes of magnitude larger than 6, and at least one (2 on average) earthquake of magnitude larger than 7. A GSI would provide data unprecedented in its extent and temporal and spatial resolution. It would provide this data for some of the world's most <span class="hlt">seismically</span> active regions, and do so better and at a lower cost than could be done with ground-based instrumentation. A GSI would revolutionize the understanding of earthquake dynamics, perhaps leading ultimately to effective warning</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PApGe.174.2475S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PApGe.174.2475S"><span>A Reappraisal of <span class="hlt">Seismicity</span> and Eruptions of Pantelleria Island and the Sicily Channel (Italy)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Spampinato, Salvatore; Ursino, Andrea; Barbano, Maria Serafina; Pirrotta, Claudia; Rapisarda, Salvatore; Larocca, Graziano; Platania, Pier Raffaele</p> <p>2017-07-01</p> <p>Three main tectonic depressions (the Pantelleria, Linosa and Malta troughs), the expression of a continental rift, characterize the Sicily Channel, a region with recent volcanic activity attested by the Pantelleria and Linosa volcanic islands, as well as numerous seamounts. To understand the <span class="hlt">seismic</span> and eruptive behaviour of this area, we compare historical and instrumental <span class="hlt">seismicity</span> retrieved from catalogues with <span class="hlt">recordings</span> from both a mobile <span class="hlt">seismic</span> network and a permanent station deployed at Pantelleria. A review of historical eruptions affecting the Sicily Channel is also presented. Recent instrumental <span class="hlt">seismicity</span> shows that the Sicily Channel is characterized by a low level of <span class="hlt">seismicity</span>, with earthquakes mainly occurring as isolated events, rather than swarms as observed during the few documented eruptive periods. The results of a <span class="hlt">seismic</span> survey in 2006-2007, as well as the signals <span class="hlt">recorded</span> by a permanent station in 2010-2014, enable stating that also Pantelleria is characterized by a very low rate of <span class="hlt">seismicity</span>. The available, though scant, historical information suggests a recurrence time of about a century for the volcanic activity and that eruptions are usually preceded by <span class="hlt">seismic</span> swarms. In the only historical known eruption of Pantelleria, in addition to shocks, uplifting and increasing fumarole activity, were observed. Notwithstanding the lack of eruptions over the past century, and despite the low recent <span class="hlt">seismic</span> rate, we believe that the geophysical monitoring of the Sicily Channel needs improving since it is an area of potentially high <span class="hlt">seismic</span> and volcanic hazard given the presence of several active submarine eruptive centres.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFMNS33B..05O','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFMNS33B..05O"><span>Noise-based body-wave <span class="hlt">seismic</span> tomography in an active underground mine.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Olivier, G.; Brenguier, F.; Campillo, M.; Lynch, R.; Roux, P.</p> <p>2014-12-01</p> <p>Over the last decade, ambient noise tomography has become increasingly popular to image the earth's upper crust. The <span class="hlt">seismic</span> noise <span class="hlt">recorded</span> in the earth's crust is dominated by surface waves emanating from the interaction of the ocean with the solid earth. These surface waves are low frequency in nature ( < 1 Hz) and not usable for imaging smaller structures associated with mining or oil and gas applications. The <span class="hlt">seismic</span> noise <span class="hlt">recorded</span> at higher frequencies are typically from anthropogenic sources, which are short lived, spatially unstable and not well suited for constructing <span class="hlt">seismic</span> Green's functions between sensors with conventional cross-correlation methods. To examine the use of ambient noise tomography for smaller scale applications, continuous data were <span class="hlt">recorded</span> for 5 months in an active underground mine in Sweden located more than 1km below surface with 18 high frequency <span class="hlt">seismic</span> sensors. A wide variety of broadband (10 - 3000 Hz) <span class="hlt">seismic</span> noise sources are present in an active underground mine ranging from drilling, scraping, trucks, ore crushers and ventilation fans. Some of these sources generate favorable <span class="hlt">seismic</span> noise, while others are peaked in frequency and not usable. In this presentation, I will show that the noise generated by mining activity can be useful if periods of <span class="hlt">seismic</span> noise are carefully selected. Although noise sources are not temporally stable and not evenly distributed around the sensor array, good estimates of the <span class="hlt">seismic</span> Green's functions between sensors can be retrieved for a broad frequency range (20 - 400 Hz) when a selective stacking scheme is used. For frequencies below 100 Hz, the reconstructed Green's functions show clear body-wave arrivals for almost all of the 153 sensor pairs. The arrival times of these body-waves are picked and used to image the local velocity structure. The resulting 3-dimensional image shows a high velocity structure that overlaps with a known ore-body. The material properties of the ore-body differ from</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010E%26PSL.290..214M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010E%26PSL.290..214M"><span>The <span class="hlt">seismic</span>-stratigraphic <span class="hlt">record</span> of lake-level fluctuations in Lake Challa: Hydrological stability and change in equatorial East Africa over the last 140 kyr</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Moernaut, J.; Verschuren, D.; Charlet, F.; Kristen, I.; Fagot, M.; De Batist, M.</p> <p>2010-02-01</p> <p><span class="hlt">Seismic</span>-reflection data from crater lake Challa (Mt. Kilimanjaro, equatorial East Africa) reveal a ˜ 210-m thick sedimentary infill containing distinct <span class="hlt">seismic</span>-stratigraphic signatures of late-Quaternary lake-level fluctuations. Extrapolation of a well-constrained age model on the cored upper part of the sequence suggests that these lake-level fluctuations represent a detailed and continuous <span class="hlt">record</span> of moisture-balance variation in equatorial East Africa over the last 140 kyr. This <span class="hlt">record</span> indicates that the most severe aridity occurred during peak Penultimate glaciation immediately before ˜ 128 kyr BP (coeval with Heinrich event 11) and during a Last Interglacial 'megadrought' period between ˜ 114 and ˜ 97 kyr BP; in comparison, Last Glacial Maximum (LGM) aridity was modest. It was preceded by ˜ 75 000 years of relatively stable and moist climate conditions interrupted by eleven short-lived dry spells, five of which match the timing of Heinrich events 2 to 6. Climate history near the East African equator reflects variation in the precessional forcing of monsoon rainfall modulated by orbital eccentricity, but precession-driven moisture fluctuations were less extreme than those observed in northern and southern tropical Africa. The near-continuous moist climate from ˜ 97 to 20.5 kyr BP <span class="hlt">recorded</span> in the Lake Challa <span class="hlt">record</span> contrasts with the trend towards greater aridity after ˜ 70 kyr BP documented in equatorial West Africa. This long period of moist glacial climate and a short, relatively modest LGM drought can be attributed to greater independence of western Indian Ocean monsoon dynamics from northern high-latitude glaciation than those in the tropical Atlantic Ocean. This rather persistent moist glacial climate regime may have helped maintain high biodiversity in the tropical forest ecosystems of the Eastern Arc mountains in Tanzania.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018E%26PSL.487...84M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018E%26PSL.487...84M"><span>Brittle deformation during Alpine basal accretion and the origin of <span class="hlt">seismicity</span> nests above the subduction interface</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Menant, Armel; Angiboust, Samuel; Monié, Patrick; Oncken, Onno; Guigner, Jean-Michel</p> <p>2018-04-01</p> <p>Geophysical observations on active subduction zones have evidenced high <span class="hlt">seismicity</span> clusters at 20-40 km depth in the fore-arc region whose origin remains controversial. We report here field observations of pervasive pseudotachylyte networks (interpreted as evidence for paleo-<span class="hlt">seismicity</span>) in the now-exhumed Valpelline continental unit (Dent Blanche complex, NW. Alps, Italy), a tectonic sliver accreted to the upper plate at <span class="hlt">c</span>. 30 km depth during the Paleocene Alpine subduction. Pre-alpine granulite-facies paragneiss from the core of the Valpelline unit are crosscut by widespread, mm to cm-thick pseudotachylyte veins. Co-<span class="hlt">seismic</span> heating and subsequent cooling led to the formation of Ti-rich garnet rims, ilmenite needles, Ca-rich plagioclase, biotite microliths and hercynite micro-crystals. 39Ar-40Ar dating yields a 51-54 Ma age range for these veins, thus suggesting that frictional melting events occurred near peak burial conditions while the Valpelline unit was already inserted inside the duplex structure. In contrast, the base of the Valpelline unit underwent synchronous ductile and brittle, <span class="hlt">seismic</span> deformation under water-bearing conditions followed by a re-equilibration at <span class="hlt">c</span>. 40 Ma (39Ar-40Ar on retrograded pseudotachylyte veins) during exhumation-related deformation. Calculated rheological profiles suggest that pseudotachylyte veins from the dry core of the granulite unit <span class="hlt">record</span> upper plate micro-<span class="hlt">seismicity</span> (Mw 2-3) formed under very high differential stresses (>500 MPa) while the sheared base of the unit underwent repeated brittle-ductile deformation at much lower differential stresses (<40 MPa) in a fluid-saturated environment. These results demonstrate that some of the <span class="hlt">seismicity</span> clusters nested along and above the plate interface may reflect the presence of stiff tectonic slivers rheologically analogous to the Valpelline unit acting as repeatedly breaking asperities in the basal accretion region of active subduction zones.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70011180','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70011180"><span><span class="hlt">Seismicity</span> at Fuego, Pacaya, Izalco, and San Cristobal Volcanoes, Central America, 1973-1974</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>McNutt, S.R.; Harlow, D.H.</p> <p>1983-01-01</p> <p><span class="hlt">Seismic</span> data collected at four volcanoes in Central America during 1973 and 1974 indicate three sources of <span class="hlt">seismicity</span>: regional earthquakes with hypocentral distances greater than 80 km, earthquakes within 40 km of each volcano, and <span class="hlt">seismic</span> activity originating at the volcanoes due to eruptive processes. Regional earthquakes generated by the underthrusting and subduction of the Cocos Plate beneath the Caribbean Plate are the most prominent <span class="hlt">seismic</span> feature in Central America. Earthquakes in the vicinity of the volcanoes occur on faults that appear to be related to volcano formation. Faulting near Fuego and Pacaya volcanoes in Guatemala is more complex due to motion on a major E-W striking transform plate boundary 40 km north of the volcanoes. Volcanic activity produces different kinds of <span class="hlt">seismic</span> signatures. Shallow tectonic or A-type events originate on nearby faults and occur both singly and in swarms. There are typically from 0 to 6 A-type events per day with b value of about 1.3. At very shallow depths beneath Pacaya, Izalco, and San Cristobal large numbers of low-frequency or B-type events are <span class="hlt">recorded</span> with predominant frequencies between 2.5 and 4.5 Hz and with b values of 1.7 to 2.9. The relative number of B-type events appears to be related to the eruptive states of the volcanoes; the more active volcanoes have higher levels of <span class="hlt">seismicity</span>. At Fuego Volcano, however, low-frequency events have unusually long codas and appear to be similar to tremor. High-amplitude volcanic tremor is <span class="hlt">recorded</span> at Fuego, Pacaya, and San Cristobal during eruptive periods. Large explosion earthquakes at Fuego are well <span class="hlt">recorded</span> at five stations and yield information on near-surface <span class="hlt">seismic</span> wave velocities (??=3.0??0.2 km/sec.). ?? 1983 Intern. Association of Volcanology and Chemistry of the Earth's Interior.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..1910049S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..1910049S"><span>On the potential of <span class="hlt">seismic</span> rotational motion measurements for extraterrestrial seismology</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Schmelzbach, Cedric; Sollberger, David; Khan, Amir; Greenhalgh, Stewart; Van Renterghem, Cederic; Robertsson, Johan</p> <p>2017-04-01</p> <p>Classically, seismological <span class="hlt">recordings</span> consist of measurements of translational ground motion only. However, in addition to three vector components of translation there are three components of rotation to consider, leading to six degrees of freedom. Of particular interest is thereby the fact that measuring rotational motion means isolating shear (S) waves. <span class="hlt">Recording</span> the rotational motion requires dedicated rotational sensors. Alternatively, since the rotational motion is given by the curl of the vectorial displacements, the rotational motion around the two horizontal axes can be computed from the horizontal spatial gradients of vertical translational <span class="hlt">recordings</span> if standard translational seismometers are placed in an areal array at the free surface. This follows from the zero stress free surface condition. Combining rotational and translational motion measurements opens up new ways of analyzing <span class="hlt">seismic</span> data, such as facilitating much improved arrival identification and wavefield separation (e.g., P-/S-wave separation), and local slowness (arrival direction and velocity) determination. Such combined measurements maximize the <span class="hlt">seismic</span> information content that a single six-component station or a small station array can provide, and are of particular interest for sparse or single-station measurements such as in extraterrestrial seismology. We demonstrate the value of the analysis of combined translational and rotational <span class="hlt">recordings</span> by re-evaluating data from the Apollo 17 lunar <span class="hlt">seismic</span> profiling experiment (LSPE). The LSPE setup consisted of four vertical-component geophones arranged in a star-like geometry. This areal receiver layout enables computing the horizontal spatial gradients by spatial finite differencing of the vertical-component data for two perpendicular directions and, hence, the estimation of rotational motion around two horizontal axes. Specifically, the <span class="hlt">recorded</span> <span class="hlt">seismic</span> waveform data originated from eight explosive packages as well as from continuously</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.usgs.gov/tm/12b1/','USGSPUBS'); return false;" href="https://pubs.usgs.gov/tm/12b1/"><span>SLAMMER: <span class="hlt">Seismic</span> LAndslide Movement Modeled using Earthquake <span class="hlt">Records</span></span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Jibson, Randall W.; Rathje, Ellen M.; Jibson, Matthew W.; Lee, Yong W.</p> <p>2013-01-01</p> <p>This program is designed to facilitate conducting sliding-block analysis (also called permanent-deformation analysis) of slopes in order to estimate slope behavior during earthquakes. The program allows selection from among more than 2,100 strong-motion <span class="hlt">records</span> from 28 earthquakes and allows users to add their own <span class="hlt">records</span> to the collection. Any number of earthquake <span class="hlt">records</span> can be selected using a search interface that selects <span class="hlt">records</span> based on desired properties. Sliding-block analyses, using any combination of rigid-block (Newmark), decoupled, and fully coupled methods, are then conducted on the selected group of <span class="hlt">records</span>, and results are compiled in both graphical and tabular form. Simplified methods for conducting each type of analysis are also included.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/5310443-seismic-reflection-studies-offshore-santa-maria-province-california','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/5310443-seismic-reflection-studies-offshore-santa-maria-province-california"><span><span class="hlt">Seismic</span>-reflection studies, offshore Santa Maria Province, California</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Bird, K.J.; Childs, J.R.; Taylor, D.J.</p> <p>1991-02-01</p> <p>Well data and <span class="hlt">seismic</span>-reflection <span class="hlt">records</span> are being analyzed to provide a subsurface geologic framework for the US Geological Survey's Santa Maria Province project. This project, jointly sponsored by the Evolution of Sedimentary Basins and Onshore Oil and Gas Investigations Programs, in a basin-evolution and petroleum geology study focusing on the geologically complex and tectonically active south-central California margin. The area embraces several basins and basin fragments including the onshore Santa Maria, offshore Santa Maria, Pismo, Huasna, Sur, Santa Lucia, and western Santa Barbara-Ventura. These basins have many similarities, including generally synchronous formation at about the end of the Oligocene, developmentmore » on a complex assemblage of Mesozoic tectonostratigraphic terranes, and basin fill consisting of Neogene clastic marine and nonmarine deposits, minor volcanic rocks, and organic-rich biogenous deposits of the Monterey Formation. Despite these similarities, basin origins are controversial and paleogeographies uncertain. In 1990, the US Geological Survey collected approximately 130 line-mi of multichannel <span class="hlt">seismic</span> reflection data in seven profiles off-shore California from Morro Bay south to the western Santa Barbara Channel. These are the first US Geological Survey <span class="hlt">seismic</span> data collected in this area since the early 1980s exploratory drilling began in the offshore Santa Maria basin. Profiles were generally oriented perpendicular to structural grain and located to intersect as many well-sites and pre-existing <span class="hlt">seismic</span> profiles as possible. Profile orientation and spacing were designed to provide the offshore extensions of onshore well-correlation profiles currently under construction. With synthetic seismograms the authors are integrating the stratigraphy of the wells with these <span class="hlt">seismic</span>-reflection <span class="hlt">records</span>.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70023299','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70023299"><span>Earthquake triggering by <span class="hlt">seismic</span> waves following the landers and hector mine earthquakes</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Gomberg, J.; Reasenberg, P.A.; Bodin, P.; Harris, R.A.</p> <p>2001-01-01</p> <p>The proximity and similarity of the 1992, magnitude 7.3 Landers and 1999, magnitude 7.1 Hector Mine earthquakes in California permit testing of earthquake triggering hypotheses not previously possible. The Hector Mine earthquake confirmed inferences that transient, oscillatory 'dynamic' deformations radiated as <span class="hlt">seismic</span> waves can trigger <span class="hlt">seismicity</span> rate increases, as proposed for the Landers earthquake1-6. Here we quantify the spatial and temporal patterns of the <span class="hlt">seismicity</span> rate changes7. The <span class="hlt">seismicity</span> rate increase was to the north for the Landers earthquake and primarily to the south for the Hector Mine earthquake. We suggest that rupture directivity results in elevated dynamic deformations north and south of the Landers and Hector Mine faults, respectively, as evident in the asymmetry of the <span class="hlt">recorded</span> <span class="hlt">seismic</span> velocity fields. Both dynamic and static stress changes seem important for triggering in the near field with dynamic stress changes dominating at greater distances. Peak <span class="hlt">seismic</span> velocities <span class="hlt">recorded</span> for each earthquake suggest the existence of, and place bounds on, dynamic triggering thresholds. These thresholds vary from a few tenths to a few MPa in most places, depend on local conditions, and exceed inferred static thresholds by more than an order of magnitude. At some sites, the onset of triggering was delayed until after the dynamic deformations subsided. Physical mechanisms consistent with all these observations may be similar to those that give rise to liquefaction or cyclic fatigue.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFM.H51M1566R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFM.H51M1566R"><span>Relocation of Groningen <span class="hlt">seismicity</span> using refracted waves</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ruigrok, E.; Trampert, J.; Paulssen, H.; Dost, B.</p> <p>2015-12-01</p> <p>The Groningen gas field is a giant natural gas accumulation in the Northeast of the Netherlands. The gas is in a reservoir at a depth of about 3 km. The naturally-fractured gas-filled sandstone extends roughly 45 by 25 km laterally and 140 m vertically. Decades of production have led to significant compaction of the sandstone. The (differential) compaction is thought to have reactivated existing faults and being the main driver of induced <span class="hlt">seismicity</span>. Precise earthquake location is difficult due to a complicated subsurface, and that is the likely reason, the current hypocentre estimates do not clearly correlate with the well-known fault network. The <span class="hlt">seismic</span> velocity model down to reservoir depth is quite well known from extensive <span class="hlt">seismic</span> surveys and borehole data. Most to date earthquake detections, however, were made with a sparse pre-2015 <span class="hlt">seismic</span> network. For shallow <span class="hlt">seismicity</span> (<5 km depth) horizontal source-receiver distances tend to be much larger than vertical distances. Consequently, preferred source-receiver travel paths are refractions over high-velocity layers below the reservoir. However, the <span class="hlt">seismic</span> velocities of layers below the reservoir are poorly known. We estimated an effective velocity model of the main refracting layer below the reservoir and use this for relocating past <span class="hlt">seismicity</span>. We took advantage of vertical-borehole <span class="hlt">recordings</span> for estimating precise P-wave (refraction) onset times and used a tomographic approach to find the laterally varying velocity field of the refracting layer. This refracting layer is then added to the known velocity model, and the combined model is used to relocate the past <span class="hlt">seismicity</span>. From the resulting relocations we assess which of the faults are being reactivated.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFM.S41B2714W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFM.S41B2714W"><span><span class="hlt">Seismic</span> While Drilling Case Study in Shengli Oilfield, Eastern China</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wang, L.; Liu, H.; Tong, S.; Zou, Z.</p> <p>2015-12-01</p> <p><span class="hlt">Seismic</span> while drilling (SWD) is a promising borehole <span class="hlt">seismic</span> technique with reduction of drilling risk, cost savings and increased efficiency. To evaluate the technical and economic benefits of this new technique, we carried out SWD survey at well G130 in Shengli Oilfield of Eastern China. Well G130 is an evaluation well, located in Dongying depression at depth more than 3500m. We used an array of portable seismometers to <span class="hlt">record</span> the surface SWD-data, during the whole drilling progress. The pilot signal was being <span class="hlt">recorded</span> continuously, by an accelerometer mounted on the top of the drill string. There were also two seismometers buried in the drill yard, one near diesel engine and another near derrick. All the data was being <span class="hlt">recorded</span> continuously. According to mud logging data, we have processed and analyzed all the data. It demonstrates the drill yard noise is the primary noise among the whole surface wavefield and its dominant frequency is about 20Hz. Crosscorrelation of surface signal with the pilot signal shows its SNR is severely low and there is no any obvious event of drill-bit signals. Fortunately, the autocorrelation of the pilot signal shows clear BHA multiple and drill string multiple. The period of drill string multiple can be used for establishing the reference time (so-called zero time). We identified and removed different noises from the surface SWD-data, taking advantages of wavefield analysis. The drill-bit signal was retrieved from surface SWD-data, using <span class="hlt">seismic</span> interferometry. And a reverse vertical <span class="hlt">seismic</span> profile (RVSP) data set for the continuous drilling depth was established. The subsurface images derived from these data compare well with the corresponding images of 3D surface <span class="hlt">seismic</span> survey cross the well.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014EGUGA..16.8700D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014EGUGA..16.8700D"><span>Fault Specific <span class="hlt">Seismic</span> Hazard Maps as Input to Loss Reserves Calculation for Attica Buildings</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Deligiannakis, Georgios; Papanikolaou, Ioannis; Zimbidis, Alexandros; Roberts, Gerald</p> <p>2014-05-01</p> <p>Greece is prone to various natural disasters, such as wildfires, floods, landslides and earthquakes, due to the special environmental and geological conditions dominating in tectonic plate boundaries. <span class="hlt">Seismic</span> is the predominant risk, in terms of damages and casualties in the Greek territory. The historical <span class="hlt">record</span> of earthquakes in Greece has been published from various researchers, providing useful data in <span class="hlt">seismic</span> hazard assessment of Greece. However, the completeness of the historical <span class="hlt">record</span> in Greece, despite being one of the longest worldwide, reaches only 500 years for M ≥ 7.3 and less than 200 years for M ≥ 6.5. Considering that active faults in the area have recurrence intervals of a few hundred to several thousands of years, it is clear that many active faults have not been activated during the completeness period covered by the historical <span class="hlt">records</span>. New <span class="hlt">Seismic</span> Hazard Assessment methodologies tend to follow fault specific approaches where <span class="hlt">seismic</span> sources are geologically constrained active faults, in order to address problems related to the historical <span class="hlt">records</span> incompleteness, obtain higher spatial resolution and calculate realistic source locality distances, since <span class="hlt">seismic</span> sources are very accurately located. Fault specific approaches provide quantitative assessments as they measure fault slip rates from geological data, providing a more reliable estimate of <span class="hlt">seismic</span> hazard. We used a fault specific <span class="hlt">seismic</span> hazard assessment approach for the region of Attica. The method of <span class="hlt">seismic</span> hazard mapping from geological fault throw-rate data combined three major factors: Empirical data which combine fault rupture lengths, earthquake magnitudes and coseismic slip relationships. The radiuses of VI, VII, VIII and IX isoseismals on the Modified Mercalli (MM) intensity scale. Attenuation - amplification functions for <span class="hlt">seismic</span> shaking on bedrock compared to basin filling sediments. We explicitly modeled 22 active faults that could affect the region of Attica, including</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li class="active"><span>18</span></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_18 --> <div id="page_19" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li class="active"><span>19</span></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="361"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/15101661','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/15101661"><span>Low-frequency whale and <span class="hlt">seismic</span> airgun sounds <span class="hlt">recorded</span> in the mid-Atlantic Ocean.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Nieukirk, Sharon L; Stafford, Kathleen M; Mellinger, David K; Dziak, Robert P; Fox, Christopher G</p> <p>2004-04-01</p> <p>Beginning in February 1999, an array of six autonomous hydrophones was moored near the Mid-Atlantic Ridge (35 degrees N-15 degrees N, 50 degrees W-33 degrees W). Two years of data were reviewed for whale vocalizations by visually examining spectrograms. Four distinct sounds were detected that are believed to be of biological origin: (1) a two-part low-frequency moan at roughly 18 Hz lasting 25 s which has previously been attributed to blue whales (Balaenoptera musculus); (2) series of short pulses approximately 18 s apart centered at 22 Hz, which are likely produced by fin whales (B. physalus); (3) series of short, pulsive sounds at 30 Hz and above and approximately 1 s apart that resemble sounds attributed to minke whales (B. acutorostrata); and (4) downswept, pulsive sounds above 30 Hz that are likely from baleen whales. Vocalizations were detected most often in the winter, and blue- and fin whale sounds were detected most often on the northern hydrophones. Sounds from <span class="hlt">seismic</span> airguns were <span class="hlt">recorded</span> frequently, particularly during summer, from locations over 3000 km from this array. Whales were detected by these hydrophones despite its location in a very remote part of the Atlantic Ocean that has traditionally been difficult to survey.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA276626','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA276626"><span>Application of Neutral Networks to <span class="hlt">Seismic</span> Signal Discrimination</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>1993-05-15</p> <p>AD-A276 626 PL-TR-93-2154 Application of Neural Networks to <span class="hlt">Seismic</span> Signal Discrimination James A. Cercone V. Shane Foster W. Mike Clark Larry... Networks to <span class="hlt">Seismic</span> Signal Discrimination PE 61101E PR 1DMO TA DA WU AA .AUTHOR(S) Stephen Goodman John Martin <span class="hlt">C</span> James A. Cercone Don J. Smith G...of Technology Applications of Neural Networks to <span class="hlt">Seismic</span> Classification project. The first year of research focused on identification and collection</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2001AGUFM.S12C0624K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2001AGUFM.S12C0624K"><span>GEODIS: A Portable Ocean Bottom Very Broadband <span class="hlt">Seismic</span> Station</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>KARCZEWSKI, J.; MONTAGNER, J.; BEGUERY, L.; STUTZMANN, E.; ROULT, G.; LOGNONNE, P.; CACHO, S.; KOENIG, J.; SAVARY, J.</p> <p>2001-12-01</p> <p>The last ten years have seen the simultaneous development of a global <span class="hlt">seismic</span> network coordinated through the FDSN (Federation of Digital Seismograph Networks) and of portable broadband <span class="hlt">seismic</span> arrays. The same approach can be followed for improving our scientific understanding of the Earth processes below oceanic areas. Both components of ocean bottom geophysical networks, will be coordinated by ION (international Ocean Network). They are complementary since they enable to investigate the Earth structure and processes at different spatial and temporal scales. Geophysical Ocean bottom observatories (hereafter referred as GOBO) and portable <span class="hlt">seismic</span> stations are sharing common technological problems. However, the issues of power supply and real-time data transmission are more crucial for a GOBO than for a portable temporary station. Since 1999, our group is developing a new "portable" geophysical ocean bottom autonomous station, named GEODIS. This station might be a basic element for a GOBO. It relies on the use of adapted VBB sensors issued from space experiments and technology and on improved electronics compared with previous ocean bottom experiments (SISMOBS/OFM 1992; MOISE 1997). The main characteristics of GEODIS are the following: - 3 axes VBB <span class="hlt">seismic</span> sensors with a classical flat velocity response 360-0.2s. at 2500V/m/s (intrinsic noise level smaller than LNM). - Automatic (under software control) installation, levelling, centring of the 3 component <span class="hlt">seismic</span> sensors. - 24 bit digitiser <span class="hlt">recording</span> at 20sps, 3 <span class="hlt">seismic</span> component and 1 infrasonic sensor. - <span class="hlt">Recording</span> by a 16 bit converter at 1sps of the sea temperature in the vicinity of the instrument and housekeeping parameters (temperature, inclinations, power,...). - 1 year autonomy by using Lithium batteries. - Storage of data on Flash card and <span class="hlt">recording</span> on hard disk every day. - Weight of GEODIS: 186kg in air and 110kg in water. - Overall dimensions: 930 x 930 x 440 mm. GEODIS can be easily installed by a</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFM.S22C..03H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFM.S22C..03H"><span>Large-N Nodal <span class="hlt">Seismic</span> Deployment at Mount St Helens</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hansen, S. M.; Schmandt, B.; Vidale, J. E.; Creager, K. C.; Levander, A.; Kiser, E.; Barklage, M.; Hollis, D.</p> <p>2014-12-01</p> <p>In late July of 2014 over 900 autonomous short period seismometers were deployed within 12 km of the summit crater at Mount St Helens. In concert with the larger iMUSH experiment, these data constitute the largest <span class="hlt">seismic</span> interrogation of an active volcano ever conducted. The array was deployed along the road and trail system of the national volcanic monument and adjacent regions with an average station spacing of 250 meters and included several station clusters with increased sampling density. The 10 Hz phones <span class="hlt">recorded</span> the vertical component wavefield continuously at 250 Hz sampling rate over a period of approximately two weeks. During the <span class="hlt">recording</span> time, the Pacific Northwest <span class="hlt">Seismic</span> Network detected ~65 earthquakes within the array footprint ranging in magnitude from -0.9 to 1.1, the majority of which were located beneath the crater at less than 10 km depth. In addition to the natural <span class="hlt">seismicity</span>, 23 explosion sources from the iMUSH active source experiment were <span class="hlt">recorded</span>, several of which exceeded magnitude 2. Preliminary results for this project will include an expanded event catalog as the array should significantly reduce the detection threshold. The sheer number of instruments allows for stacking of station clusters producing high signal-to-noise beam traces which can be used for event triggering and for creating waveform templates to measure relative travel-times across the array via cross-correlation. The ability of the array to estimate focal mechanisms from event radiation patterns and delineate complex path effects will also be investigated. The density and azimuthal coverage provide by this array offers an excellent opportunity to investigate short-wavelength variations of the <span class="hlt">seismic</span> wavefield in a complex geologic environment. Previous <span class="hlt">seismic</span> tomography results suggest the presence of a shallow magma chamber at 1-3 km depth near the region of shallow <span class="hlt">seismicity</span> as evidenced by a P wave low-velocity anomaly of at least -5.5% [Waite and Moran, 2009</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.S13A0640A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.S13A0640A"><span>a Comparative Case Study of Reflection <span class="hlt">Seismic</span> Imaging Method</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Alamooti, M.; Aydin, A.</p> <p>2017-12-01</p> <p><span class="hlt">Seismic</span> imaging is the most common means of gathering information about subsurface structural features. The accuracy of <span class="hlt">seismic</span> images may be highly variable depending on the complexity of the subsurface and on how <span class="hlt">seismic</span> data is processed. One of the crucial steps in this process, especially in layered sequences with complicated structure, is the time and/or depth migration of <span class="hlt">seismic</span> data.The primary purpose of the migration is to increase the spatial resolution of <span class="hlt">seismic</span> images by repositioning the <span class="hlt">recorded</span> <span class="hlt">seismic</span> signal back to its original point of reflection in time/space, which enhances information about complex structure. In this study, our objective is to process a <span class="hlt">seismic</span> data set (courtesy of the University of South Carolina) to generate an image on which the Magruder fault near Allendale SC can be clearly distinguished and its attitude can be accurately depicted. The data was gathered by common mid-point method with 60 geophones equally spaced along an about 550 m long traverse over a nearly flat ground. The results obtained from the application of different migration algorithms (including finite-difference and Kirchhoff) are compared in time and depth domains to investigate the efficiency of each algorithm in reducing the processing time and improving the accuracy of <span class="hlt">seismic</span> images in reflecting the correct position of the Magruder fault.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/6400316-deployment-oklahoma-borehole-seismic-experiment','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/6400316-deployment-oklahoma-borehole-seismic-experiment"><span>Deployment of the Oklahoma borehole <span class="hlt">seismic</span> experiment</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Harben, P.E.; Rock, D.W.</p> <p>1989-01-20</p> <p>This paper discusses the Oklahoma borehole <span class="hlt">seismic</span> experiment, currently in operation, set up by members of the Lawrence Livermore National Laboratory Treaty Verification Program and the Oklahoma Geophysical Observatory to determine deep-borehole <span class="hlt">seismic</span> characteristics in geology typical of large regions in the Soviet Union. We evaluated and logged an existing 772-m deep borehole on the Observatory site by running caliper, cement bonding, casing inspection, and hole-deviation logs. Two Teledyne Geotech borehole-clamping seismometers were placed at various depths and spacings in the deep borehole. Currently, they are deployed at 727 and 730 m. A Teledyne Geotech shallow-borehole seismometer was mounted inmore » a 4.5-m hole, one meter from the deep borehole. The seismometers' system coherency were tested and found to be excellent to 35 Hz. We have <span class="hlt">recorded</span> <span class="hlt">seismic</span> noise, quarry blasts, regional earthquakes and teleseisms in the present configuration. We will begin a study of <span class="hlt">seismic</span> noise and attenuation as a function of depth in the near future. 7 refs., 18 figs.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012AGUFM.T21B2561S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012AGUFM.T21B2561S"><span>The Propagation of <span class="hlt">Seismic</span> Waves in the Presence of Strong Elastic Property Contrasts</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Saleh, R.; Jeyaraj, R.; Milkereit, B.; Liu, Q.; Valley, B.</p> <p>2012-12-01</p> <p> distribution of <span class="hlt">seismic</span> sensors in a mine and the presence of <span class="hlt">seismic</span> events within a mine, the <span class="hlt">recorded</span> wavefield may represent a near-field displacement, which is not the case for most of <span class="hlt">seismic</span> studies. The role of receiver characterization on the <span class="hlt">recorded</span> event near the surface or around fault zones is also investigated. Using 2D/3D modeling, the effects of Vp/Vs variation on vertical and horizontal components of <span class="hlt">recorded</span> amplitude has been shown.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1001791','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/1001791"><span>Tube-wave <span class="hlt">seismic</span> imaging</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Korneev, Valeri A [Lafayette, CA; Bakulin, Andrey [Houston, TX</p> <p>2009-10-13</p> <p>The detailed analysis of cross well <span class="hlt">seismic</span> data for a gas reservoir in Texas revealed two newly detected <span class="hlt">seismic</span> wave effects, <span class="hlt">recorded</span> approximately 2000 feet above the reservoir. A tube-wave (150) is initiated in a source well (110) by a source (111), travels in the source well (110), is coupled to a geological feature (140), propagates (151) through the geological feature (140), is coupled back to a tube-wave (152) at a receiver well (120), and is and received by receiver(s) (121) in either the same (110) or a different receiving well (120). The tube-wave has been shown to be extremely sensitive to changes in reservoir characteristics. Tube-waves appear to couple most effectively to reservoirs where the well casing is perforated, allowing direct fluid contact from the interior of a well case to the reservoir.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/988156','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/988156"><span>Tube-wave <span class="hlt">seismic</span> imaging</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Korneev, Valeri A [LaFayette, CA</p> <p>2009-05-05</p> <p>The detailed analysis of cross well <span class="hlt">seismic</span> data for a gas reservoir in Texas revealed two newly detected <span class="hlt">seismic</span> wave effects, <span class="hlt">recorded</span> approximately 2000 feet above the reservoir. A tube-wave (150) is initiated in a source well (110) by a source (111), travels in the source well (110), is coupled to a geological feature (140), propagates (151) through the geological feature (140), is coupled back to a tube-wave (152) at a receiver well (120), and is and received by receiver(s) (121) in either the same (110) or a different receiving well (120). The tube-wave has been shown to be extremely sensitive to changes in reservoir characteristics. Tube-waves appear to couple most effectively to reservoirs where the well casing is perforated, allowing direct fluid contact from the interior of a well case to the reservoir.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017GeoRL..44.3509M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017GeoRL..44.3509M"><span>Bayesian identification of multiple <span class="hlt">seismic</span> change points and varying <span class="hlt">seismic</span> rates caused by induced <span class="hlt">seismicity</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Montoya-Noguera, Silvana; Wang, Yu</p> <p>2017-04-01</p> <p>The Central and Eastern United States (CEUS) has experienced an abnormal increase in <span class="hlt">seismic</span> activity, which is believed to be related to anthropogenic activities. The U.S. Geological Survey has acknowledged this situation and developed the CEUS 2016 1 year <span class="hlt">seismic</span> hazard model using the catalog of 2015 by assuming stationary <span class="hlt">seismicity</span> in that period. However, due to the nonstationary nature of induced <span class="hlt">seismicity</span>, it is essential to identify change points for accurate probabilistic <span class="hlt">seismic</span> hazard analysis (PSHA). We present a Bayesian procedure to identify the most probable change points in <span class="hlt">seismicity</span> and define their respective <span class="hlt">seismic</span> rates. It uses prior distributions in agreement with conventional PSHA and updates them with recent data to identify <span class="hlt">seismicity</span> changes. It can determine the change points in a regional scale and may incorporate different types of information in an objective manner. It is first successfully tested with simulated data, and then it is used to evaluate Oklahoma's regional <span class="hlt">seismicity</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24994652','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24994652"><span>Earthquake dynamics. Mapping pressurized volcanic fluids from induced crustal <span class="hlt">seismic</span> velocity drops.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Brenguier, F; Campillo, M; Takeda, T; Aoki, Y; Shapiro, N M; Briand, X; Emoto, K; Miyake, H</p> <p>2014-07-04</p> <p>Volcanic eruptions are caused by the release of pressure that has accumulated due to hot volcanic fluids at depth. Here, we show that the extent of the regions affected by pressurized fluids can be imaged through the measurement of their response to transient stress perturbations. We used <span class="hlt">records</span> of <span class="hlt">seismic</span> noise from the Japanese Hi-net <span class="hlt">seismic</span> network to measure the crustal <span class="hlt">seismic</span> velocity changes below volcanic regions caused by the 2011 moment magnitude (M(w)) 9.0 Tohoku-Oki earthquake. We interpret coseismic crustal <span class="hlt">seismic</span> velocity reductions as related to the mechanical weakening of the pressurized crust by the dynamic stress associated with the <span class="hlt">seismic</span> waves. We suggest, therefore, that mapping <span class="hlt">seismic</span> velocity susceptibility to dynamic stress perturbations can be used for the imaging and characterization of volcanic systems. Copyright © 2014, American Association for the Advancement of Science.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.V51D0395M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.V51D0395M"><span>In-situ <span class="hlt">seismic</span> <span class="hlt">record</span> of potential sill intrusion at the ultraslow spreading Southwest Indian Ridge</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Meier, M.; Schlindwein, V. S. N.</p> <p>2017-12-01</p> <p>Ultraslow spreading mid-ocean ridges with full spreading rates up to 15 mm/yr are described as the melt poor endmember of the entire mid-ocean ridge system. The melt supply along ultraslow spreading ridges is uneven resulting in the formation of volcanic centres and amagmatic segments. Amagmatic segments show thicker brittle lithosphere of up to 30 km, whereas magmatic segments have much thinner lithosphere of up to less than 15 km. It is supposed that melt travels along the lithosphere asthenosphere boundary from amagmatic segments to magmatic segments, where it can reach the seafloor and erupt. These spreading events are rare at ultraslow spreading ridges compared to faster spreading ridges and insitu observations hardly exist. During an ocean bottom seismometer (OBS) experiment at the eastern Southwest Indian Ridge two earthquake swarms were accidentally <span class="hlt">recorded</span>. The swarms occurred in January and April 2013 and both lasted for a few days. The events of the earthquake swarms were relatively located with HypoDD for better spatial resolution. This unique dataset allowed for studying active spreading processes at an ultraslow spreading ridge. The earthquakes occurred in depths, where the magma chamber of the nearby Segment-8 volcano is located. This magma chamber potentially fed a sill intrusion, which was <span class="hlt">recorded</span> as earthquake swarms. During the first hours of the first earthquake swarm a migration pattern was identified. The hypocentres migrated away from the Segment-8 volcanic centre and slightly downwards. Later events occurred more randomly in the active area. Simultaneously <span class="hlt">seismic</span> tremor was <span class="hlt">recorded</span> at the station closest to the swarm locations. The tremor lasted longer for the shorter earthquake swarm in April. During both tremor phases the signal was modulated with a 12 hour period. We speculate that a hydrothermal system was affected by the intrusion and fluid flow modulated by the tides produced the tremor signal.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFM.S21A2669S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFM.S21A2669S"><span>a Borehole <span class="hlt">Seismic</span> System for Active and Passive Seimsic Studies to 3 KM at Ptrc's Aquistore Project</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Schmitt, D. R.; Nixon, C.; Kofman, R.; White, D. J.; Worth, K.</p> <p>2015-12-01</p> <p>We have constructed a downhole <span class="hlt">seismic</span> <span class="hlt">recording</span> system for application to depths of nearly 3 km and temperatures up to 135 °<span class="hlt">C</span> at Aquistore, an independent research and monitoring project in which liquid CO2 is being stored in a brine and sandstone water formation. The key component to this system is a set of commercially available slim-hole 3-<span class="hlt">C</span> sondes carrying 15 Hz geophones deployable in open and cased boreholes with diameters as small as 57 mm. The system is currently hosted on a 4-conductor wireline with digital information streamed to the surface <span class="hlt">recording</span> unit. We have further incorporated these sondes into a mobile passive monitoring unit that includes a number of redundancies such as a multiple Tbyte network accessible RAID hard-drive system (NAS) and a self-designed uninterruptible power supply. The system can be remotely controlled via the internet. The system is currently deployed covering a range of depths from 2850 m to 2910 m. Ambient temperatures at this depth are approximately 110 °<span class="hlt">C</span> with onboard tool temperatures running at 115 °<span class="hlt">C</span>. Data is continuously streamed to the NAS for archiving, approximately 11 GBytes of data is <span class="hlt">recorded</span> per day at the sampling period of 0.5 ms. The lack of noise at this depth allows short data snippets to be flagged with a simple amplitude threshold criteria. The greatly reduced data volume of the snippets allows for ready access via the internet to the system for ongoing quality control. Spurious events, mostly small amplitude tube waves originating at or near the surface, are readily discounted. Active <span class="hlt">seismic</span> measurements are carried out simultaneously but these require that an appropriately accurate independent GPS based time synchronization be used. Various experiences with event detection, orientation of sondes using both explosives and <span class="hlt">seismic</span> vibrator, potential overheating of the surface electronics, and issues related to loss of shore power provide for a detailed case study. Aquistore, managed by the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFMNH14A..02M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFMNH14A..02M"><span>Non-<span class="hlt">seismic</span> tsunamis: filling the forecast gap</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Moore, C. W.; Titov, V. V.; Spillane, M. C.</p> <p>2015-12-01</p> <p>Earthquakes are the generation mechanism in over 85% of tsunamis. However, non-<span class="hlt">seismic</span> tsunamis, including those generated by meteorological events, landslides, volcanoes, and asteroid impacts, can inundate significant area and have a large far-field effect. The current National Oceanographic and Atmospheric Administration (NOAA) tsunami forecast system falls short in detecting these phenomena. This study attempts to classify the range of effects possible from these non-<span class="hlt">seismic</span> threats, and to investigate detection methods appropriate for use in a forecast system. Typical observation platforms are assessed, including DART bottom pressure <span class="hlt">recorders</span> and tide gauges. Other detection paths include atmospheric pressure anomaly algorithms for detecting meteotsunamis and the early identification of asteroids large enough to produce a regional hazard. Real-time assessment of observations for forecast use can provide guidance to mitigate the effects of a non-<span class="hlt">seismic</span> tsunami.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2004AGUFM.T21C0542G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2004AGUFM.T21C0542G"><span>Long-Term <span class="hlt">Seismicity</span> of Northern (15° N-60° N) Mid-Atlantic Ridge (MAR) <span class="hlt">Recorded</span> by two Regional Hydrophone Arrays: a Widespread Along-Ridge Influence of the Azores and Iceland Hotspots</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Goslin, J.; Bazin, S.; Dziak, R. P.; Fox, C.; Fowler, M.; Haxel, J.; Lourenco, N.; Luis, J.; Martin, C.; Matsumoto, H.; Perrot, J.; Royer, J.</p> <p>2004-12-01</p> <p>The <span class="hlt">seismicity</span> of the North Atlantic was <span class="hlt">recorded</span> by two networks of hydrophones moored in the SOFAR channel, north and south of the Azores Plateau. The interpretation of the hydro-acoustic signals <span class="hlt">recorded</span> during the first six-month common period of operation of the two networks (June 2002 to Nov. 2002) provides a unique data set on the spatial and time distributions of the numerous low-magnitude earthquakes which occurred along the Mid-Atlantic Ridge. Close to 2000 events were localized during this six-month period between latitudes 15° N and 63° N, 501 of which are localized within the SIRENA network (40° N-51° N) and 692 within the wider South Azores network (17° N-33° N). Using hydrophones to locate seafloor earthquakes by interpreting T-wave signals lowers the detection threshold of Mid-Atlantic Ridge events to 3.0 mb from the 4.7 mb of global <span class="hlt">seismic</span> networks. This represents an average thirty-fold increase in the number of events: 62 events were detected by global seismological networks within the same area during the same period. An along-ridge spatial distribution of the <span class="hlt">seismicity</span> is obtained by computing the cumulated numbers of events in 1° -wide latitudinal bins. When plotted vs. latitude, this first-order distribution shows remarkable long-wavelength patterns: the <span class="hlt">seismicity</span> rate is low when approaching the Azores and Iceland (reaching values as low as 10 events/d° ), while it peaks to 70 events/d° in the vicinity of the Gibbs FZ. Moreover, the latitudinal distribution of the <span class="hlt">seismicity</span> hints at an asymmetric influence of the Azores hotpot on the MAR. Finally, the spatial distribution of the <span class="hlt">seismicity</span> anti-correlates well at long wavelengths with the zero-age depths along the MAR and correlates with the zero-age Mantle Bouguer (MBA) anomaly values and the Vs velocity anomalies at 100 km in the upper mantle. It is thus proposed that the <span class="hlt">seismicity</span> level would be partly tied to the rheology and thickness of the brittle layer and be thus</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..19.8807L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..19.8807L"><span>Surface wave tomography of Europe from ambient <span class="hlt">seismic</span> noise</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lu, Yang; Stehly, Laurent; Paul, Anne</p> <p>2017-04-01</p> <p>We present a European scale high-resolution 3-D shear wave velocity model derived from ambient <span class="hlt">seismic</span> noise tomography. In this study, we collect 4 years of continuous <span class="hlt">seismic</span> <span class="hlt">recordings</span> from 1293 stations across much of the European region (10˚W-35˚E, 30˚N-75˚N), which yields more than 0.8 million virtual station pairs. This data set compiles <span class="hlt">records</span> from 67 <span class="hlt">seismic</span> networks, both permanent and temporary from the EIDA (European Integrated Data Archive). Rayleigh wave group velocity are measured at each station pair using the multiple-filter analysis technique. Group velocity maps are estimated through a linearized tomographic inversion algorithm at period from 5s to 100s. Adaptive parameterization is used to accommodate heterogeneity in data coverage. We then apply a two-step data-driven inversion method to obtain the shear wave velocity model. The two steps refer to a Monte Carlo inversion to build the starting model, followed by a linearized inversion for further improvement. Finally, Moho depth (and its uncertainty) are determined over most of our study region by identifying and analysing sharp velocity discontinuities (and sharpness). The resulting velocity model shows good agreement with main geological features and previous geophyical studies. Moho depth coincides well with that obtained from active <span class="hlt">seismic</span> experiments. A focus on the Greater Alpine region (covered by the AlpArray <span class="hlt">seismic</span> network) displays a clear crustal thinning that follows the arcuate shape of the Alps from the southern French Massif Central to southern Germany.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008AGUFM.P51D..08L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008AGUFM.P51D..08L"><span>The MOON micro-<span class="hlt">seismic</span> noise : first estimates from meteorites flux simulations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lognonne, P.; Lefeuvre, M.; Johnson, C.; Weber, R.</p> <p>2008-12-01</p> <p>The Moon is considered to be a <span class="hlt">seismically</span> quiet planet and most of the time, the Apollo seismograms were flat when not quakes was occuring. We show in this paper that this might not be the case if more sensitive data are <span class="hlt">recorded</span> by future instruments and that a permanent micro-<span class="hlt">seismic</span> noise is existing due to the continuous impacts of meteorites. We perform a modeling of this noise by using, as calibrated <span class="hlt">seismic</span> data, those generated by the impacts of the Apollo S4B or LEM, by taking care on the scaling law, necessary to express the <span class="hlt">seismic</span> force with respect to the mass and velocity of the impactors. We also parametrize the dependence of the amplitude of the <span class="hlt">seismic</span> coda, associated to the maximum amplitude of the seismograms, with respect to the epicentral distance and to the source geometry. This enabling us to use the <span class="hlt">seismic</span> data of the S4B impacts as empirical waveforms for the modeling of the natural impacts. The frequency/size law of meteoroids impacting the Moon and the associated probability of NEO impacts are however not known precisely. Uncertainties as large as a factor of 3-5 remain, especially for the moderate-sized impacts which are not observed on the Earth, due to the shielding by the atmosphere. We therefore use several meteoroid mass/frequency laws from the literature to generate, with a random simulator, a history of impacts on the Moon during a given period. The <span class="hlt">seismic</span> signals generated by succession of <span class="hlt">seismic</span> sources and estimate the frequency/amplitude relationship of such <span class="hlt">seismic</span> signals. Our results finally provide an estimate for the meteoritic <span class="hlt">seismic</span> background on the Moon. This background noise was not <span class="hlt">recorded</span> by the Apollo <span class="hlt">seismic</span> experiment due insufficient resolution. Such an estimate can be used in designing a new generation of lunar seismometers, for estimating the probability of detecting proposed impacts due to nuggets of strange quark matter , and to inform future lunar based experiments, which require very stable ground</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.T31C2914S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.T31C2914S"><span><span class="hlt">Seismicity</span> around the source areas of the 1946 Nankai and the 1944 Tonankai earthquakes detected from data <span class="hlt">recorded</span> at DONET stations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Suzuki, K.; Kamiya, S.; Takahashi, N.</p> <p>2016-12-01</p> <p>The Japan Agency for Marine-Earth Science and Technology (JAMSTEC) installed DONET (Dense Oceanfloor Network System for Earthquakes and Tsunamis) off the Kii Peninsula, southwest of Japan, to monitor earthquakes and tsunamis. Stations of DONET1, which are distributed in Kumano-nada, and DONET2, which are distributed off Muroto, were installed by August 2011 and April 2016, respectively. After the installation of all of the 51 stations, DONET was transferred to National Research Institute for Earth Science and Disaster Resilience (NIED). NIED and JAMSTEC have now corroborated in the operation of DONET since April 2016. To investigate the <span class="hlt">seismicity</span> around the source areas of the 1946 Nankai and the 1944 Tonankai earthquakes, we detected earthquakes from the <span class="hlt">records</span> of the broadband seismometers installed to DONET. Because DONET stations are apart from land stations, we can detect smaller earthquakes than by using only land stations. It is important for understanding the stress state and seismogenic mechanism to monitoring the spatial-temporal <span class="hlt">seismicity</span> change. In this study we purpose to evaluate to the <span class="hlt">seismicity</span> around the source areas of the Nankai and the Tonankai earthquakes by using our earthquake catalogue. The frequency-magnitude relationships of earthquakes in the areas of DONET1&2 had an almost constant slope of about -1 for earthquakes of ML larger than 1.5 and 2.5, satisfying the Gutenberg-Richter law, and the slope of smaller earthquakes approached 0, reflecting the detection limits. While the most of the earthquakes occurred in the aftershock area of the 2004 off the Kii Peninsula earthquakes, very limited activity was detected in the source region of the Nankai and Tonankai earthquake except for the large earthquake (MJMA = 6.5) on 1st April 2016 and its aftershocks. We will evaluate the detection limit of the earthquake in more detail and investigate the spatial-temporal <span class="hlt">seismicity</span> change with waiting the data store.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFM.S33B2758S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFM.S33B2758S"><span>Implementing a <span class="hlt">C</span>++ Version of the Joint <span class="hlt">Seismic</span>-Geodetic Algorithm for Finite-Fault Detection and Slip Inversion for Earthquake Early Warning</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Smith, D. E.; Felizardo, C.; Minson, S. E.; Boese, M.; Langbein, J. O.; Guillemot, C.; Murray, J. R.</p> <p>2015-12-01</p> <p>The earthquake early warning (EEW) systems in California and elsewhere can greatly benefit from algorithms that generate estimates of finite-fault parameters. These estimates could significantly improve real-time shaking calculations and yield important information for immediate disaster response. Minson et al. (2015) determined that combining FinDer's <span class="hlt">seismic</span>-based algorithm (Böse et al., 2012) with BEFORES' geodetic-based algorithm (Minson et al., 2014) yields a more robust and informative joint solution than using either algorithm alone. FinDer examines the distribution of peak ground accelerations from <span class="hlt">seismic</span> stations and determines the best finite-fault extent and strike from template matching. BEFORES employs a Bayesian framework to search for the best slip inversion over all possible fault geometries in terms of strike and dip. Using FinDer and BEFORES together generates estimates of finite-fault extent, strike, dip, preferred slip, and magnitude. To yield the quickest, most flexible, and open-source version of the joint algorithm, we translated BEFORES and FinDer from Matlab into <span class="hlt">C</span>++. We are now developing a <span class="hlt">C</span>++ Application Protocol Interface for these two algorithms to be connected to the <span class="hlt">seismic</span> and geodetic data flowing from the EEW system. The interface that is being developed will also enable communication between the two algorithms to generate the joint solution of finite-fault parameters. Once this interface is developed and implemented, the next step will be to run test <span class="hlt">seismic</span> and geodetic data through the system via the Earthworm module, Tank Player. This will allow us to examine algorithm performance on simulated data and past real events.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70191530','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70191530"><span>Efforts to monitor and characterize the recent increasing <span class="hlt">seismicity</span> in central Oklahoma</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>McNamara, Daniel E.; Rubinstein, Justin L.; Myers, Emma; Smoczyk, Gregory M.; Benz, Harley M.; Williams, Robert; Hayes, Gavin; Wilson, David; Herrmann, Robert B.; McMahon, Nicole D; Aster, R.C.; Bergman, E.; Holland, Austin; Earle, Paul</p> <p>2015-01-01</p> <p>The sharp increase in <span class="hlt">seismicity</span> over a broad region of central Oklahoma has raised concerns regarding the source of the activity and its potential hazard to local communities and energy-industry infrastructure. Efforts to monitor and characterize the earthquake sequences in central Oklahoma are reviewed. Since early 2010, numerous organizations have deployed temporary portable <span class="hlt">seismic</span> stations in central Oklahoma to <span class="hlt">record</span> the evolving <span class="hlt">seismicity</span>. A multiple-event relocation method is applied to produce a catalog of central Oklahoma earthquakes from late 2009 into early 2015. Regional moment tensor (RMT) source parameters were determined for the largest and best-<span class="hlt">recorded</span> earthquakes. Combining RMT results with relocated <span class="hlt">seismicity</span> enabled determination of the length, depth, and style of faulting occurring on reactivated subsurface fault systems. It was found that the majority of earthquakes occur on near-vertical, optimally oriented (northeast-southwest and northwest-southeast) strike-slip faults in the shallow crystalline basement. In 2014, 17 earthquakes occurred with magnitudes of 4 or larger. It is suggested that these recently reactivated fault systems pose the greatest potential hazard to the region.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li class="active"><span>19</span></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_19 --> <div id="page_20" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li class="active"><span>20</span></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="381"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.S11C0616Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.S11C0616Y"><span>Monitoring Instrument Performance in Regional Broadband <span class="hlt">Seismic</span> Network Using Ambient <span class="hlt">Seismic</span> Noise</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ye, F.; Lyu, S.; Lin, J.</p> <p>2017-12-01</p> <p>In the past ten years, the number of <span class="hlt">seismic</span> stations has increased significantly, and regional <span class="hlt">seismic</span> networks with advanced technology have been gradually developed all over the world. The resulting broadband data help to improve the seismological research. It is important to monitor the performance of broadband instruments in a new network in a long period of time to ensure the accuracy of <span class="hlt">seismic</span> <span class="hlt">records</span>. Here, we propose a method that uses ambient noise data in the period range 5-25 s to monitor instrument performance and check data quality in situ. The method is based on an analysis of amplitude and phase index parameters calculated from pairwise cross-correlations of three stations, which provides multiple references for reliable error estimates. Index parameters calculated daily during a two-year observation period are evaluated to identify stations with instrument response errors in near real time. During data processing, initial instrument responses are used in place of available instrument responses to simulate instrument response errors, which are then used to verify our results. We also examine feasibility of the tailing noise using data from stations selected from USArray in different locations and analyze the possible instrumental errors resulting in time-shifts used to verify the method. Additionally, we show an application that effects of instrument response errors that experience pole-zeros variations on monitoring temporal variations in crustal properties appear statistically significant velocity perturbation larger than the standard deviation. The results indicate that monitoring <span class="hlt">seismic</span> instrument performance helps eliminate data pollution before analysis begins.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.usgs.gov/of/1978/0591/report.pdf','USGSPUBS'); return false;" href="https://pubs.usgs.gov/of/1978/0591/report.pdf"><span>The utility of petroleum <span class="hlt">seismic</span> exploration data in delineating structural features within salt anticlines</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Stockton, S.L.; Balch, Alfred H.</p> <p>1978-01-01</p> <p>The Salt Valley anticline, in the Paradox Basin of southeastern Utah, is under investigation for use as a location for storage of solid nuclear waste. Delineation of thin, nonsalt interbeds within the upper reaches of the salt body is extremely important because the nature and character of any such fluid- or gas-saturated horizons would be critical to the mode of emplacement of wastes into the structure. Analysis of 50 km of conventional <span class="hlt">seismic</span>-reflection data, in the vicinity of the anticline, indicates that mapping of thin beds at shallow depths may well be possible using a specially designed adaptation of state-of-the-art <span class="hlt">seismic</span> oil-exploration procedures. Computer ray-trace modeling of thin beds in salt reveals that the frequency and spatial resolution required to map the details of interbeds at shallow depths (less than 750 m) may be on the order of 500 Hz, with surface-spread lengths of less than 350 m. Consideration should be given to the burial of sources and receivers in order to attenuate surface noise and to <span class="hlt">record</span> the desired high frequencies. Correlation of the <span class="hlt">seismic</span>-reflection data with available well data and surface geology reveals the complex, structurally initiated diapir, whose upward flow was maintained by rapid contemporaneous deposition of continental clastic sediments on its flanks. Severe collapse faulting near the crests of these structures has distorted the <span class="hlt">seismic</span> response. Evidence exists, however, that intrasalt thin beds of anhydrite, dolomite, and black shale are mappable on <span class="hlt">seismic</span> <span class="hlt">record</span> sections either as short, discontinuous reflected events or as amplitude anomalies that result from focusing of the reflected <span class="hlt">seismic</span> energy by the thin beds; computer modeling of the folded interbeds confirms both of these as possible causes of <span class="hlt">seismic</span> response from within the salt diapir. Prediction of the <span class="hlt">seismic</span> signatures of the interbeds can be made from computer-model studies. Petroleum <span class="hlt">seismic</span>-reflection data are unsatisfactory for</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014EGUGA..16.1351T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014EGUGA..16.1351T"><span>Analysis of the low-level <span class="hlt">seismicity</span> along the Southern Indian Ocean spreading ridges <span class="hlt">recorded</span> by the OHASISBIO array of hydrophones in 2012</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tsang-Hin-Sun, Eve; Royer, Jean-Yves; Sukhovich, Alexey; Perrot, Julie</p> <p>2014-05-01</p> <p>Arrays of autonomous hydrophones (AUHs) proved to be a very valuable tool for monitoring the <span class="hlt">seismic</span> activity of mid-ocean ridges. AUHs take advantage of the ocean acoustic properties to detect many low-magnitude underwater earthquakes undetected by land-based stations. This allows for a significant improvement in the magnitude completeness level of <span class="hlt">seismic</span> catalogs in remote oceanic areas. This study presents some results from the deployment of the OHASISBIO array comprising 7 AUHs deployed in the southern Indian Ocean. The source of acoustic events, i.e. site where - conversion from <span class="hlt">seismic</span> to acoustic waves occur and proxy to epicenters for shallow earthquakes - can be precisely located within few km, inside the AUH array. The distribution of the uncertainties in the locations and time-origins shows that the OHASISBIO array reliably covers a wide region encompassing the Indian Ocean triple junction and large extent of the three mid-oceanic Indian spreading ridges, from 52°E to 80°E and from 25°S to 40°S. During its one year long deployment in 2012 and in this area the AUH array <span class="hlt">recorded</span> 1670 events, while, for the same period, land-based networks only detected 470 events. A comparison of the background <span class="hlt">seismicity</span> along the South-east (SEIR) and South-west (SWIR) Indian ridges suggests that the microseismicity, even over a year period, could be representative of the steady-state of stress along the SEIR and SWIR; this conclusion is based on very high Spearman's correlations between our one-year long AUH catalog and teleseismic catalogs over nearly 40 years. <span class="hlt">Seismicity</span> along the ultra-slow spreading SWIR is regularly distributed in space and time, along spreading segments and transform faults, whereas the intermediate spreading SEIR diplays clusters of events in the vicinity of some transform faults or near specific geological structures such as the St-Paul and Amsterdam hotspot. A majority of these clusters seem to be related to magmatic processes, such as</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFM.V31D4782O','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFM.V31D4782O"><span>Slab dehydration <span class="hlt">recorded</span> in subducted serpentine sea-mount</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Okamoto, K.; Fukumura, S.; Ishimori, C.; Jung, H.</p> <p>2014-12-01</p> <p>It has been considered that there is a correlation between the double <span class="hlt">seismic</span> zones and metamorphic dehydration reaction in deep slab. The lower <span class="hlt">seismic</span> plane of the double <span class="hlt">seismic</span> zone is considered to be located on the 600 o<span class="hlt">C</span> isotherm in the subducting lithosphere. Antigorite terminal reaction is highly temperature sensitive around 600 o<span class="hlt">C</span>. Therefore it has been proposed that the oceanic lithosphere was hydrated forming serpentine prior to subduction, then serpentine was decomposed to release fluid causing dehydration embrittlement in the slab. In order to unravel relation between dehydration and <span class="hlt">seismic</span> deformation, we have investigated dehydration process of natural metamorphic rocks <span class="hlt">recording</span> very cold geothermal history in the crust and lithosphere in the slab. Metamorphic olivine after antigorite has been described in Italian Alps and also from the Mt. Shiraga, Japan [1]. However, the olivine was formed with talc and fluid by antigorite breakdown reaction in pressures lower than 1.5 GPa. Spinifex olivine with opx in the Cerro del Almirez [2], is the product at pressures (P > 1.5 GPa) relevant to the lower <span class="hlt">seismic</span> plane beneath Northeast Japan. It clearly indicates the presence of large amount of water facilitate crystallization of elongated olivine with opx. It is also supported by LPO pattern of olivines determined by EBSD. Fine-grained olivine-rich samples shows that Type-<span class="hlt">C</span> fabric pattern is dominant, suggesting deformation under water-rich condition [3]. With metamorphic olivines, chlorite was also recrystallized, suggesting that water would be transported farther down to deep. The estimated dehydration reaction has a negative P-T slope at pressures higher than 1.5 GPa. The reaction is volume reducing reaction and the olivine-opx spinifex texture was formed under volume reducing reaction. In the warm slab beneath SW Japan, the reaction has a positive slope in P-T space and forms olivine+talc+fluid. From microstrucral and petrological analysis of the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1996EOSTr..77..289H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1996EOSTr..77..289H"><span>Multi-Use <span class="hlt">seismic</span> stations offer strong deterrent to clandestine nuclear weapons testing</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hennet, C. B.; Van der Vink, G. E.; Richards, P. G.; Adushkin, V. V.; Kopnichev, Y. F.; Geary, R.</p> <p></p> <p>As the United States and other nations push for the signing of a Comprehensive Test Ban Treaty, representatives are meeting in Geneva this year to develop an International <span class="hlt">Seismic</span> Monitoring System to verify compliance with the treaty's restrictions. In addition to the official monitoring system, regional networks developed for earthquake studies and basic research can provide a strong deterrent against clandestine testing. The recent release of information by the U.S. Department of Energy (DoE) on previously unannounced nuclear tests provides an opportunity to assess the ability of multi-use <span class="hlt">seismic</span> networks to help monitor nuclear testing across the globe.Here we look at the extent to which the formerly unannounced tests were <span class="hlt">recorded</span> and identified on the basis of publicly available seismographic data <span class="hlt">recorded</span> by five <span class="hlt">seismic</span> networks. The data were <span class="hlt">recorded</span> by networks in southern Nevada and northern California at stations less than 1500 km from the Nevada Test Site (NTS), and two networks in the former Soviet Union at stations farther than 1500 km from the NTS.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.S51A2759C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.S51A2759C"><span>Velocity Model Using the Large-N <span class="hlt">Seismic</span> Array from the Source Physics Experiment (SPE)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chen, T.; Snelson, C. M.</p> <p>2016-12-01</p> <p>The Source Physics Experiment (SPE) is a multi-institutional, multi-disciplinary project that consists of a series of chemical explosions conducted at the Nevada National Security Site (NNSS). The goal of SPE is to understand the complicated effect of geological structures on <span class="hlt">seismic</span> wave propagation and source energy partitioning, develop and validate physics-based modeling, and ultimately better monitor low-yield nuclear explosions. A Large-N <span class="hlt">seismic</span> array was deployed at the SPE site to image the full 3D wavefield from the most recent SPE-5 explosion on April 26, 2016. The Large-N <span class="hlt">seismic</span> array consists of 996 geophones (half three-component and half vertical-component sensors), and operated for one month, <span class="hlt">recording</span> the SPE-5 shot, ambient noise, and additional controlled-sources (a large hammer). This study uses Large-N array <span class="hlt">recordings</span> of the SPE-5 chemical explosion to develop high resolution images of local geologic structures. We analyze different phases of <span class="hlt">recorded</span> <span class="hlt">seismic</span> data and construct a velocity model based on arrival times. The results of this study will be incorporated into the large modeling and simulation efforts as ground-truth further validating the models.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.usgs.gov/of/1982/0607/ofr1982607.pdf','USGSPUBS'); return false;" href="https://pubs.usgs.gov/of/1982/0607/ofr1982607.pdf"><span>High-resolution <span class="hlt">seismic</span>-reflection profiles from the R/V Columbus Iselin, cruise CI 7-78-2, over the continental shelf and slope in the Georges Bank area</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Bailey, Norman G.; Aaron, John M.</p> <p>1982-01-01</p> <p>In September 1978, the U. S. Geological Survey (USGS) collected 5,029 km of single-channel <span class="hlt">seismic</span>-reflection data from the Georges Bank area of the Atlantic Continental Shelf and Slope during the R/V COLUMBUS ISELIN cruise CI 7-78-2. The purpose of the cruise was to determine the location and frequency of mass sediment movement and other geologic hazards along the Continental Slope.Navigation of the COLUMBUS ISELIN was by LORAN-<span class="hlt">C</span>; position fixes were automatically <span class="hlt">recorded</span> at 5-minute intervals and manually plotted and <span class="hlt">recorded</span> at 15-minute intervals. The navigation equipment included a Northstar 6000 LORAN receiver and a Texas Instruments Silent 700 tape and paper <span class="hlt">recorder</span>.The <span class="hlt">seismic</span> equipment consisted of a 40-in3 airgun, a 5-in3 airgun, a Teledyne 600-joule mnisparker, and ORE (Ocean Research Equipment Inc.) 3.5-kHz transducer. The <span class="hlt">seismic</span> profiles obtained were <span class="hlt">recorded</span> on paper by EPC (EPC Labs Inc.) <span class="hlt">recorders</span> and on magnetic tape by a 7-channel analog tape <span class="hlt">recorder</span>. Overall, the data quality is excellent, and penetration and resolution are good although in some areas, the underlying structure was obscured by rough topography.The original <span class="hlt">records</span> may be viewed at the USGS office in Woods Hole, Massachusetts. Microfilm copies of the data may be purchased only from the National Geophysical and Solar-Terrestrial Data Center, NOAA/EDIS/NGSDC, Code D621, 325 Broadway, Boulder, CO 80303 (Telephone: 303-497-6338).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUFM.V41B2780O','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUFM.V41B2780O"><span>Updated Tomographic <span class="hlt">Seismic</span> Imaging at Kilauea Volcano, Hawaii</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Okubo, P.; Johnson, J.; Felts, E. S.; Flores, N.</p> <p>2013-12-01</p> <p>. We also look forward to more complete implementation at HVO of <span class="hlt">seismic</span> imaging techniques that use ambient <span class="hlt">seismic</span> noise retrieved from continuous <span class="hlt">seismic</span> <span class="hlt">recordings</span>, and to using earthquake arrival times and ambient <span class="hlt">seismic</span> noise jointly to tomographically image Kilauea.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018E%26PSL.484..287G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018E%26PSL.484..287G"><span>The persistent signature of tropical cyclones in ambient <span class="hlt">seismic</span> noise</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gualtieri, Lucia; Camargo, Suzana J.; Pascale, Salvatore; Pons, Flavio M. E.; Ekström, Göran</p> <p>2018-02-01</p> <p>The spectrum of ambient <span class="hlt">seismic</span> noise shows strong signals associated with tropical cyclones, yet a detailed understanding of these signals and the relationship between them and the storms is currently lacking. Through the analysis of more than a decade of <span class="hlt">seismic</span> data <span class="hlt">recorded</span> at several stations located in and adjacent to the northwest Pacific Ocean, here we show that there is a persistent and frequency-dependent signature of tropical cyclones in ambient <span class="hlt">seismic</span> noise that depends on characteristics of the storm and on the detailed location of the station relative to the storm. An adaptive statistical model shows that the spectral amplitude of ambient <span class="hlt">seismic</span> noise, and notably of the short-period secondary microseisms, has a strong relationship with tropical cyclone intensity and can be employed to extract information on the tropical cyclones.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014NHESD...2.1505B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014NHESD...2.1505B"><span><span class="hlt">Seismic</span> and mechanical studies of the artificially triggered rockfall at the Mount Néron (French Alps, December 2011)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bottelin, P.; Jongmans, D.; Daudon, D.; Mathy, A.; Helmstetter, A.; Bonilla-Sierra, V.; Cadet, H.; Amitrano, D.; Richefeu, V.; Lorier, L.; Baillet, L.; Villard, P.; Donzé, F.</p> <p>2014-02-01</p> <p>The eastern limestone cliff of Mount Néron (French Alps) was the theatre of two medium-size rockfalls between summer and winter 2011. On 14 August 2011, a ~ 2000 m3 rock compartment detached from the cliff, fell 100 m below and propagated down the slope. Although most of the fallen rocks deposited in the upper part of the slope, about 15 meter-size blocks were stopped by a ditch and an earthen barrier after a runout of 800 m. An unstable overhanging ~ 2600 m3 compartment remained attached to the cliff and was blasted on 13 December 2011. During this artificially triggered event, 7 blocks reached the same ditch, with volumes ranging from 0.8 to 12 m3. A semi-permanent <span class="hlt">seismic</span> array located about 2.5 km from the site <span class="hlt">recorded</span> the two events, providing a unique opportunity to understand and to compare the <span class="hlt">seismic</span> phases generated during natural and artificially triggered rockfalls. Both events have signal duration of ~ 100 s with comparable maximum amplitudes <span class="hlt">recorded</span> at large distances (computed local magnitude of 1.14 and 1.05, respectively), most of the energy lying below 20 Hz. Remote sensing techniques (photogrammetry and LiDAR) were employed before and after the provoked rockfall, allowing the volume and fracturing to be characterized. This event was filmed by two video cameras and the generated ground motions were <span class="hlt">recorded</span> using two temporary 3<span class="hlt">C</span> <span class="hlt">seismic</span> sensors and 3 <span class="hlt">seismic</span> arrays deployed at the slope toe. Movie and seismogram processing provided estimates of the propagation velocity during the successive rockfall phases, which ranges from 12 m s-1 to 30 m s-1. The main <span class="hlt">seismic</span> phases were obtained from combined video and <span class="hlt">seismic</span> signal analyses. The two most energetic phases are related to the ground impact of fallen material after free-fall, and to individual rock block impacts into the ditch and the earthen barrier. These two phases are characterized by similar low-frequency content but show very different particle motions. The discrete element technique</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.S53B0698D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.S53B0698D"><span>The recent <span class="hlt">seismicity</span> of Teide volcano, Tenerife (Canary Islands, Spain)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>D'Auria, L.; Albert, G. W.; Calvert, M. M.; Gray, A.; Vidic, C.; Barrancos, J.; Padilla, G.; García-Hernández, R.; Perez, N. M.</p> <p>2017-12-01</p> <p>Tenerife is an active volcanic island which experienced several eruptions of moderate intensity in historical times, and few explosive eruptions in the Holocene. The increasing population density and the consistent number of tourists are constantly raising the volcanic risk of the island.On 02/10/2016 a remarkable swarm of long-period events was <span class="hlt">recorded</span> and was interpreted as the effect of a transient massive fluid discharge episode occurring within the deep hydrothermal system of Teide volcano. Actually, since Oct. 2016, the hydrothermal system of the volcano underwent a progressive pressurization, testified by the marked variation of different geochemical parameters. The most striking observation is the increase in the diffuse CO2 emission from the summit crater of Teide volcano which started increasing from a background value of about 20 tons/day and reaching a peak of 175 tons/day in Feb. 2017.The pressurization process has been accompanied by an increase in the volcano-tectonic <span class="hlt">seismicity</span> of. Teide volcano, <span class="hlt">recorded</span> by the Red Sísmica Canaria, managed by Instituto Volcanológico de Canarias (INVOLCAN). The network began its full operativity in Nov. 2016 and currently consists of 15 broadband <span class="hlt">seismic</span> stations. Since Nov. 2016 the network detected more than 100 small magnitude earthquakes, located beneath Teide volcano at depths usually ranging between 5 and 15 km. On January 6th 2017 a M=2.5 earthquake was <span class="hlt">recorded</span> in the area, being one of the strongest ever <span class="hlt">recorded</span> since decades. Most of the events show typical features of the microseismicity of hydrothermal systems: high spatial and temporal clustering and similar waveforms of individual events which often are overlapped.We present the spatial and temporal distribution of the <span class="hlt">seismicity</span> of Teide volcano since Nov. 2016, comparing it also with the past <span class="hlt">seismicity</span> of the volcano. Furthermore we analyze the statistical properties of the numerous swarms <span class="hlt">recorded</span> until now with the aid of a template</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.S43A2813D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.S43A2813D"><span>Tide-related <span class="hlt">seismic</span> velocity changes across the English Channel</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>de Ridder, S.; Valova, V.; Curtis, A.</p> <p>2016-12-01</p> <p>Temporal changes in the <span class="hlt">seismic</span> velocities in the Earth's subsurface are known to occur due to a range of phenomena including seasonal variations, magmatic activity, nonlinear healing after strong ground motion, and glacial loading and unloading. Our goal is to extend observations of small velocity changes towards shorter timescales. Earth tides caused by the gravitational attraction between the Earth and the Moon might affect <span class="hlt">seismic</span> properties. If tidal velocity variations can be recovered from long range cross-correlations, and can also be coupled to stress-strain induced variations in the elastic properties, that would pave the way for systematic imaging of rheological properties of the upper crust. With this long-term goal, we studied data <span class="hlt">recorded</span> between January 2010 and December 2015 by four broad-band instruments from the British Geological Survey network. One station is located in Cornwall, two in Devon, and one across the English Channel on the island of Jersey. Continuous <span class="hlt">seismic</span> <span class="hlt">recordings</span> of the vertical components of particle velocity were divided into one hour intervals, bandpass filtered between 0.02 and 0.11 Hz, spectrally whitened, and cross-correlated between station pairs. The resulting cross-correlations were stacked into bins corresponding to the average water levels observed at nearby ports resulting in cross-correlation traces as a function of water level, for each station pair. To detect temporal changes, a multi-window time-shift analysis is applied to these inter-station traces. We find a stretch factor that best translates one trace into another: this stretch is indicative of changes in average <span class="hlt">seismic</span> velocities between the pair of tidal phases. We detected systematic <span class="hlt">seismic</span> velocity variations as a function of water level. We find that increasing water level coincided with decreasing <span class="hlt">seismic</span> velocities. Separating the data according to up- and down-going tidal tracts reveals that the observed velocity changes exhibit a time</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014EGUGA..16..791L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014EGUGA..16..791L"><span>Mapping the North Sea base-Quaternary: using 3D <span class="hlt">seismic</span> to fill a gap in the geological <span class="hlt">record</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lamb, Rachel; Huuse, Mads; Stewart, Margaret; Brocklehurst, Simon H.</p> <p>2014-05-01</p> <p> water currents. This has strong implications for both the Quaternary climate archive and petroleum systems in the North Sea. Key Words: base-Quaternary; chronostratigraphy: <span class="hlt">seismic</span> interpretation; paleoenvironments References Buckley, F.A., (2012) 'An Early Pleistocene grounded ice sheet in the Central North Sea' From: Huuse, M., Redfern, J., Le Heron, D.P., Dixon, R.J., Moscariello, A., Craig, J. (eds) 'Glaciogenic reservoirs and Hydrocarbon Systems' Geological Society, London, Special Publications, 368 Cameron, T.D.J., Stoker, M.S., Long, D., (1987) 'The history of Quaternary sedimentation in the UK sector of the North Sea Basin' Journal of the Geological Society, 144, 43-58 Gatliff, R.W, Richards, P.<span class="hlt">C</span>, Smith, K, Graham, <span class="hlt">C.C</span>, McCormac, M, Smith, N.J.P, Long, D, Cameron, T.D.J, Evans, D, Stevenson, A.G, Bulat, J, Ritchie, J.D, (1994) 'United Kingdom offshore regional report: the geology of the central North Sea.' London: HMSO for the British Geological Survey Kulhmann, G., Langereis <span class="hlt">C</span>.G., Munsterman, D., van Leeuwen, R.-J., Verreussel, R., Meulenkamp, J.E., Wong, Th.E., 2006 'Intergrated chronostratigraphy of the Pliocene-Pliestocene interval and its relation to the regional stratigraphical stages in the Southern North Sea region' Netherlands Journal of Geosciences 85(1), 29-45 Rasmussen, E.A., Vejb?k O.V., Bidstrup, T., Piasecki, S., Dybkj?r, K., 2005 'Late Cenozoic depositional history of the Danish North Sea Basin: implications for the petroleum systems in the Kraka, Halfdan, Siri and Nini fields', Petroleum Geology Conference series 6, 1347-1358 Sejrup, H.P., Aareseth, I., Haflidason, H., 1991 'The Quaternary succession in the northern North Sea' Marine Geology 101 103-111</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA489457','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA489457"><span>Overview of <span class="hlt">Seismic</span> Noise and it’s Relevance to Personnel Detection</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2008-04-01</p> <p>production sites. Young et al. (1996) measured <span class="hlt">seismic</span> noise with seismometers at the surface and within boreholes at three sites, and generated...ER D <span class="hlt">C</span>/ CR R EL T R -0 8 -5 Overview of <span class="hlt">Seismic</span> Noise and its Relevance to Personnel Detection Lindamae Peck April 2008 <span class="hlt">C</span> ol d R...April 2008 Overview of <span class="hlt">Seismic</span> Noise and its Relevance to Personnel Detection Lindamae Peck Cold Regions Research and Engineering Laboratory</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011EEEV...10..115M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011EEEV...10..115M"><span>Assessment of <span class="hlt">seismic</span> design response factors of concrete wall buildings</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mwafy, Aman</p> <p>2011-03-01</p> <p>To verify the <span class="hlt">seismic</span> design response factors of high-rise buildings, five reference structures, varying in height from 20- to 60-stories, were selected and designed according to modern design codes to represent a wide range of concrete wall structures. Verified fiber-based analytical models for inelastic simulation were developed, considering the geometric nonlinearity and material inelasticity of the structural members. The ground motion uncertainty was accounted for by employing 20 earthquake <span class="hlt">records</span> representing two <span class="hlt">seismic</span> scenarios, consistent with the latest understanding of the tectonic setting and <span class="hlt">seismicity</span> of the selected reference region (UAE). A large number of Inelastic Pushover Analyses (IPAs) and Incremental Dynamic Collapse Analyses (IDCAs) were deployed for the reference structures to estimate the <span class="hlt">seismic</span> design response factors. It is concluded that the factors adopted by the design code are adequately conservative. The results of this systematic assessment of <span class="hlt">seismic</span> design response factors apply to a wide variety of contemporary concrete wall buildings with various characteristics.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2004JSAES..16..759B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2004JSAES..16..759B"><span>Crustal <span class="hlt">seismicity</span> in central Chile</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Barrientos, S.; Vera, E.; Alvarado, P.; Monfret, T.</p> <p>2004-06-01</p> <p>Both the genesis and rates of activity of shallow intraplate <span class="hlt">seismic</span> activity in central Chile are poorly understood, mainly because of the lack of association of <span class="hlt">seismicity</span> with recognizable fault features at the surface and a poor <span class="hlt">record</span> of <span class="hlt">seismic</span> activity. The goal of this work is to detail the characteristics of <span class="hlt">seismicity</span> that takes place in the western flank of the Andes in central Chile. This region, located less than 100 km from Santiago, has been the site of earthquakes with magnitudes up to 6.9, including several 5+ magnitude shocks in recent years. Because most of the events lie outside the Central Chile <span class="hlt">Seismic</span> Network, at distances up to 60 km to the east, it is essential to have adequate knowledge of the velocity structure in the Andean region to produce the highest possible quality of epicentral locations. For this, a N-S refraction line, using mining blasts of the Disputada de Las Condes open pit mine, has been acquired. These blasts were detected and <span class="hlt">recorded</span> as far as 180 km south of the mine. Interpretation of the travel times indicates an upper crustal model consisting of three layers: 2.2-, 6.7-, and 6.1-km thick, overlying a half space; their associated P wave velocities are 4.75-5.0 (gradient), 5.8-6.0 (gradient), 6.2, and 6.6 km/s, respectively. Hypocentral relocation of earthquakes in 1986-2001, using the newly developed velocity model, reveals several regions of concentrated <span class="hlt">seismicity</span>. One clearly delineates the fault zone and extensions of the strike-slip earthquake that took place in September 1987 at the source of the Cachapoal River. Other regions of activity are near the San José volcano, the source of the Maipo River, and two previously recognized lineaments that correspond to the southern extension of the Pocuro fault and Olivares River. A temporary array of seismographs, installed in the high Maipo River (1996) and San José volcano (1997) regions, established the hypocentral location of events with errors of less than 1 km</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3274221','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3274221"><span>GFZ Wireless <span class="hlt">Seismic</span> Array (GFZ-WISE), a Wireless Mesh Network of <span class="hlt">Seismic</span> Sensors: New Perspectives for <span class="hlt">Seismic</span> Noise Array Investigations and Site Monitoring</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Picozzi, Matteo; Milkereit, Claus; Parolai, Stefano; Jaeckel, Karl-Heinz; Veit, Ingo; Fischer, Joachim; Zschau, Jochen</p> <p>2010-01-01</p> <p>Over the last few years, the analysis of <span class="hlt">seismic</span> noise <span class="hlt">recorded</span> by two dimensional arrays has been confirmed to be capable of deriving the subsoil shear-wave velocity structure down to several hundred meters depth. In fact, using just a few minutes of <span class="hlt">seismic</span> noise <span class="hlt">recordings</span> and combining this with the well known horizontal-to-vertical method, it has also been shown that it is possible to investigate the average one dimensional velocity structure below an array of stations in urban areas with a sufficient resolution to depths that would be prohibitive with active source array surveys, while in addition reducing the number of boreholes required to be drilled for site-effect analysis. However, the high cost of standard seismological instrumentation limits the number of sensors generally available for two-dimensional array measurements (i.e., of the order of 10), limiting the resolution in the estimated shear-wave velocity profiles. Therefore, new themes in site-effect estimation research by two-dimensional arrays involve the development and application of low-cost instrumentation, which potentially allows the performance of dense-array measurements, and the development of dedicated signal-analysis procedures for rapid and robust estimation of shear-wave velocity profiles. In this work, we present novel low-cost wireless instrumentation for dense two-dimensional ambient <span class="hlt">seismic</span> noise array measurements that allows the real–time analysis of the surface-wavefield and the rapid estimation of the local shear-wave velocity structure for site response studies. We first introduce the general philosophy of the new system, as well as the hardware and software that forms the novel instrument, which we have tested in laboratory and field studies. PMID:22319298</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008AGUFM.S43D1907N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008AGUFM.S43D1907N"><span>Recent Studies on the increase in <span class="hlt">Seismicity</span> in the Antarctic Plate: Observations from BB Seismological Observatory (MAIT) at Maitri, Antarctica</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>N, R.; Ec, M.</p> <p>2008-12-01</p> <p>The permanent Seismological Observatory was established in 1997 at Maitri in Central Dronning Maud Land, East Antarctica (70 °45' South 11 °43' East) primarily to monitor the <span class="hlt">seismicity</span> in and around Antarctica, the space and time distribution of earthquake occurrences and obtain hypocentral parameters, magnitudes of earthquakes, velocity inversion for underground structure and earthquake source mechanism. The observatory has been upgraded during 25th Indian Silver Jubilee Scientific Expedition to Antarctica (December 2005 to February 2007) and 26th Indian Antarctic Expedition (IAE) with the new generation Geotech KS-2000M Seismometer and Smart 24R digitizer. During the 27th IAE the <span class="hlt">Seismic</span> Observatory was further upgraded by adding Reftek 130 <span class="hlt">seismic</span> system. Uninterrupted good quality digital Broad Band <span class="hlt">Seismic</span> data is continuously being acquired. The SEISAN 8.1 software was used for final processing and analysis of about 300 earthquakes <span class="hlt">recorded</span>. During the year 2006 the tele-<span class="hlt">seismic</span> events, and quite a number of regional earthquakes of the order of 4 to 6.0 magnitude within Antarctic Plate, 23 in South Sandwich Islands, 7 in Scotia Sea, 2 in Macqurie Islands and 23 in Mid Oceanic Ridges in the Indian Ocean were <span class="hlt">recorded</span>. 48 earthquakes of the magnitude above 4.5 from the nearby South Indian Ocean, South of South Africa, Chile, Argentina, Bolivia and about 40 earthquakes of the magnitude above 5.0 from the Indonesian Region were analysed. An earthquake of magnitude Ms=7.3 from the <span class="hlt">seismically</span> active region of South Sandwich Islands Δ =16.5 °, Mb=7.8 earthquake from Tonga Islands and Mb=7.2 earthquake from Java were the large earthquakes that were <span class="hlt">recorded</span>. Along with this the MOHO depth beneath MAIT was also estimated to be about 40km using receiver function analysis. All the analysed monthly data was reported to the I.S.<span class="hlt">C</span>., U.K.,Global Data Centre for the final processing and inclusion in the yearly ISC <span class="hlt">Seismic</span> Bulletin. The increasing <span class="hlt">seismic</span> activity in</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70021549','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70021549"><span><span class="hlt">Seismic</span> hazard map of the western hemisphere</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Shedlock, K.M.; Tanner, J.G.</p> <p>1999-01-01</p> <p> horizontal force a building should be able to withstand during an earthquake. This <span class="hlt">seismic</span> hazard map of the Americas depicts the likely level of short-period ground motion from earthquakes in a fifty-year window. Short-period ground motions effect short-period structures (e.g., one-to-two story buildings). The largest <span class="hlt">seismic</span> hazard values in the western hemisphere generally occur in areas that have been, or are likely to be, the sites of the largest plate boundary earthquakes. Although the largest earthquakes ever <span class="hlt">recorded</span> are the 1960 Chile and 1964 Alaska subduction zone earthquakes, the largest <span class="hlt">seismic</span> hazard (PGA) value in the Americas is in Southern California (U.S.), along the San Andreas fault.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFM.S41B2732F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFM.S41B2732F"><span>Deep structure of Llaima Volcano from <span class="hlt">seismic</span> ambient noise tomography: Preliminary results</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Franco, L.; Mikesell, T. D.; Rodd, R.; Lees, J. M.; Johnson, J. B.; Ronan, T.</p> <p>2015-12-01</p> <p>The ambient <span class="hlt">seismic</span> noise tomography (ANT) method has become an important tool to image crustal structures and magmatic bodies at volcanoes. The frequency band of ambient noise provides complimentary data and added resolution to the deeper volcanic structures when compared to traditional tomography based on local earthquakes. The Llaima Volcano (38° 41.9' S and 71° 43.8' W) is a stratovolcano of basaltic-andesitic composition. Llaima is located in the South Volcanic Zone (ZVS) of the Andes and is listed as one of the most active volcanoes in South America, with a long documented historical <span class="hlt">record</span> dating back to 1640. Llaima experienced violent eruptions in 1927 and 1957 (Naranjo and Moreno, 1991), and its last eruptive cycle (2008-2010) is considered the most important after the 1957 eruption. Lacking <span class="hlt">seismic</span> constraints on the deep structure under Llaima, petrologic data have suggested the presence of magmatic bodies (dikes). These bodies likely play an important role in the eruptive dynamics of Llaima (Bouvet de Maisonneuve, <span class="hlt">C</span>., et al 2012). Analysis of the 2008-2010 <span class="hlt">seismicity</span> shows a southern zone (approx. 15 km from the Llaima summit) where there were many Very Long Period events occurring prior to the eruptions. This is in agreement with a deformation zone determined by InSAR analysis (Fournier et al, 2010 and Bathke, 2011), but no geologic model based on geophysical imaging has been created yet. Beginning in 2009, staff from the Chilean Geological Survey (SERNAGEOMIN) started to install a permanent <span class="hlt">seismic</span> network consisting of nine stations. These nine stations have allowed Chilean seismologists to closely monitor the activity at Llaima, but prevented a high-resolution tomographic imaging study. During the summer of 2015, a temporary <span class="hlt">seismic</span> network consisting of 26 stations was installed around Llaima. In the work presented here, we analyze continuous waveforms <span class="hlt">recorded</span> between January and April 2015 from a total of 35 broadband stations (permanent and</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li class="active"><span>20</span></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_20 --> <div id="page_21" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li class="active"><span>21</span></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="401"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012AGUFMOS43C1837R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012AGUFMOS43C1837R"><span>Testing 8000 years of submarine paleoseismicity <span class="hlt">record</span> offshore western Algeria : First evidence for irregular <span class="hlt">seismic</span> cycles</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ratzov, G.; Cattaneo, A.; Babonneau, N.; Yelles, K.; Bracene, R.; Deverchere, J.</p> <p>2012-12-01</p> <p>It is commonly assumed that stress buildup along a given fault is proportional to the time elapsed since the previous earthquake. Although the resulting « <span class="hlt">seismic</span> gap » hypothesis suits well for moderate magnitude earthquakes (Mw 4-5), large events (Mw>6) are hardly predictable and depict great variation in recurrence intervals. Models based on stress transfer and interactions between faults argue that an earthquake may promote or delay the occurrence of next earthquakes on adjacent faults by increasing or lowering the level of static stress. The Algerian margin is a Cenozoic passive margin presently inverted within the slow convergence between Africa and Eurasia plates (~3-6 mm/yr). The western margin experienced two large earthquakes in 1954 (Orléansville, M 6.7) and 1980 (El Asnam, M 7.3), supporting an interaction between the two faults. To get meaningful statistics of large earthquakes recurrence intervals over numerous <span class="hlt">seismic</span> cycles, we conducted a submarine paleoseismicity investigation based on turbidite chronostratigraphy. As evidenced on the Cascadia subduction zone, synchronous turbidites accumulated over a large area and originated from independent sources are likely triggered by an earthquake. To test the method on a slowly convergent margin, we analyze turbidites from three sediment cores collected during the Maradja (2003) and Prisme (2007) cruises off the 1954-1980 source areas. We use X-ray radioscopy, XRF major elements counter, magnetic susceptibility, and grain-size distribution to accurately discriminate turbidites from hemipelagites. We date turbidites by calculating hemipelagic sedimentation rates obtained with radiocarbon ages, and interpolate the rates between turbidites. Finally, the age of events is compared with the only paleoseismic study available on land (El Asnam fault). Fourteen possible <span class="hlt">seismic</span> events are identified by the counting and correlation of turbidites over the last 8 ka. Most events are correlated with the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1989PhDT.......188K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1989PhDT.......188K"><span><span class="hlt">Seismic</span> and potential field studies over the East Midlands</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kirk, Wayne John</p> <p></p> <p>A <span class="hlt">seismic</span> refraction profile was undertaken to investigate the source of an aeromagnetic anomaly located above the Widmerpool Gulf, East Midlands. Ten shots were fired into 51 stations at <span class="hlt">c</span>. 1.5km spacing in a 70km profile during 41 days <span class="hlt">recording</span>. The refraction data were processed using standard techniques to improve the data quality. A new filtering technique, known as Correlated Adaptive Noise Cancellation was tested on synthetic data and successfully applied to controlled source and quarry blast data. Study of strong motion data reveals that the previous method of site calibration is invalid. A new calibration technique, known as the Scaled Amplitude method is presented to provide safer charge size estimation. Raytrace modelling of the refraction data and two dimensional gravity interpretation confirms the presence of the Widmerpool Gulf but no support is found for the postulated intrusion. Two dimensional magnetic interpretation revealed that the aeromagnetic anomaly could be modelled with a Carboniferous igneous source. A Lower Palaeozoic refractor with a velocity of 6.0 km/s is identified at a maximum depth of <span class="hlt">c</span>. 2.85km beneath the Widmerpool Gulf. Carboniferous and post-Carboniferous sediments within the gulf have velocities between 2.6-5.5 km/s with a strong vertical gradient. At the gulf margins, a refractor with a constant velocity of 5.2 km/s is identified as Dinantian limestone. A low velocity layer of proposed unaltered Lower Palaeozoics is identified beneath the limestone at the eastern edge of the Derbyshire Dome. The existence and areal extent of this layer are also determined from <span class="hlt">seismic</span> reflection data. Image analysis of potential field data, presents a model identifying 3 structural provinces, the Midlands Microcraton, the Welsh and English Caledonides and a central region of complex linears. This model is used to explain the distribution of basement rocks determined from <span class="hlt">seismic</span> and gravity profiles.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013JPhCS.433a2039O','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013JPhCS.433a2039O"><span>Recent Progress of <span class="hlt">Seismic</span> Observation Networks in Japan</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Okada, Y.</p> <p>2013-04-01</p> <p>Before the occurrence of disastrous Kobe earthquake in 1995, the number of high sensitivity seismograph stations operated in Japan was nearly 550 and was concentrated in the Kanto and Tokai districts, central Japan. In the wake of the Kobe earthquake, Japanese government has newly established the Headquarters for Earthquake Research Promotion and started the reconstruction of <span class="hlt">seismic</span> networks to evenly cover the whole Japan. The basic network is composed of three seismographs, i.e. high sensitivity seismograph (Hi-net), broadband seismograph (F-net), and strong motion seismograph (K-NET). A large majority of Hi-net stations are also equipped with a pair of strong motion sensors at the bottom of borehole and the ground surface (KiK-net). A plenty of high quality data obtained from these networks are circulated at once and is producing several new seismological findings as well as providing the basis for the Earthquake Early Warning system. In March 11, 2011, "Off the Pacific coast of Tohoku Earthquake" was generated with magnitude 9.0, which <span class="hlt">records</span> the largest in the history of <span class="hlt">seismic</span> observation in Japan. The greatest disaster on <span class="hlt">record</span> was brought by huge tsunami with nearly 20 thousand killed or missing people. We are again noticed that <span class="hlt">seismic</span> observation system is quite poor in the oceanic region compared to the richness of it in the inland region. In 2012, NIED has started the construction of ocean bottom <span class="hlt">seismic</span> and tsunami observation network along the Japan Trench. It is planned to layout 154 stations with an average spacing of 30km, each of which is equipped with an accelerometer for <span class="hlt">seismic</span> observation and a water pressure gauge for tsunami observation. We are expecting that more rapid and accurate warning of earthquake and tsunami becomes possible by this observing network.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.S41B0768K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.S41B0768K"><span>New strong motion network in Georgia: basis for specifying <span class="hlt">seismic</span> hazard</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kvavadze, N.; Tsereteli, N. S.</p> <p>2017-12-01</p> <p>Risk created by hazardous natural events is closely related to sustainable development of the society. Global observations have confirmed tendency of growing losses resulting from natural disasters, one of the most dangerous and destructive if which are earthquakes. Georgia is located in <span class="hlt">seismically</span> active region. So, it is imperative to evaluate probabilistic <span class="hlt">seismic</span> hazard and <span class="hlt">seismic</span> risk with proper accuracy. National network of Georgia includes 35 station all of which are seismometers. There are significant gaps in strong motion <span class="hlt">recordings</span>, which essential for <span class="hlt">seismic</span> hazard assessment. To gather more accelerometer <span class="hlt">recordings</span>, we have built a strong motion network distributed on the territory of Georgia. The network includes 6 stations for now, with Basalt 4x datalogger and strong motion sensor Episensor ES-T. For each site, Vs30 and soil resonance frequencies have been measured. Since all but one station (Tabakhmelam near Tbilisi), are located far from power and internet lines special system was created for instrument operation. Solar power is used to supply the system with electricity and GSM/LTE modems for internet access. VPN tunnel was set up using Raspberry pi, for two-way communication with stations. Tabakhmela station is located on grounds of Ionosphere Observatory, TSU and is used as a hub for the network. This location also includes a broadband seismometer and VLF electromagnetic waves observation antenna, for possible earthquake precursor studies. On server, located in Tabakhmela, the continues data is collected from all the stations, for later use. The <span class="hlt">recordings</span> later will be used in different seismological and engineering problems, namely selecting and creating GMPE model for Caucasus, for probabilistic <span class="hlt">seismic</span> hazard and <span class="hlt">seismic</span> risk evaluation. These stations are a start and in the future expansion of strong motion network is planned. Along with this, electromagnetic wave observations will continue and additional antennas will be implemented</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.T12B..08G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.T12B..08G"><span>Rheology and <span class="hlt">Seismic</span> Potential of Experimentally-Deformed Natural Serpentinites</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gasc, J.; Hilairet, N.; Wang, Y.; Yu, T.; Ferrand, T. P.; Schubnel, A.</p> <p>2016-12-01</p> <p>The origin of intermediate-depth earthquakes, which occur at depths of 60-300 km along subducting slabs, remains somehow enigmatic. In the pressure and temperature conditions involved, rocks should indeed deform in a ductile fashion. One, or more, mechanism is therefore responsible for mechanical instabilities. Dehydration embrittlement, due to serpentine breakdown, was long considered a good candidate. However, in recent years, experimental studies have challenged this theory, by showing that deformation and faulting of serpentinites, related to dehydration, occurs in a stable and aseismic way (Chernak and Hirth, 2011; Gasc et al., 2011). In order to assess the <span class="hlt">seismic</span> potential of serpentinites, high pressure deformation experiments were carried out on natural samples, during which micro-<span class="hlt">seismicity</span> was monitored by <span class="hlt">recording</span> Acoustic Emissions (AE's). Deformation was performed at pressures of 3-5 GPa, using a Deformation-DIA device, and over a wide range of temperatures, both within and outside antigorite's stability field. The results show that, below 400 <span class="hlt">C</span>, serpentinite deformation involves aseismic semi-brittle mechanisms, even in cases where strain localization is observed. At high temperature (i.e., above 600 <span class="hlt">C</span>), despite conditions propitious to dehydration embrittlement (i.e., with fast strain rates and reaction kinetics), joint deformation and dehydration leads to ductile shear, without generation of AE's. On the other hand, a brittle temperature window, centered at ca. 500 <span class="hlt">C</span>, is evidenced. In this latter case, AE's are consistently collected upon deformation and faulting with extremely sharp strain localization is observed. This brittle field may therefore be a source of <span class="hlt">seismicity</span> in subducting slabs at mantle pressures. However, analysis of the acoustic signal shows that it is relatively orders of magnitude weaker than its real-earth counterparts, which suggests that other mechanisms are responsible for larger intermediate-depth earthquakes. In fact</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012JGRF..117.3004C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012JGRF..117.3004C"><span><span class="hlt">Seismic</span> multiplet response triggered by melt at Blood Falls, Taylor Glacier, Antarctica</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Carmichael, Joshua D.; Pettit, Erin C.; Hoffman, Matt; Fountain, Andrew; Hallet, Bernard</p> <p>2012-09-01</p> <p>Meltwater input often triggers a <span class="hlt">seismic</span> response from glaciers and ice sheets. It is difficult, however, to measure melt production on glaciers directly, while subglacial water storage is not directly observable. Therefore, we document temporal changes in <span class="hlt">seismicity</span> from a dry-based polar glacier (Taylor Glacier, Antarctica) during a melt season using a synthesis of <span class="hlt">seismic</span> observation and melt modeling. We <span class="hlt">record</span> icequakes using a dense six-receiver network of three-component geophones and compare this with melt input generated from a calibrated surface energy balance model. In the absence of modeled surface melt, we find that <span class="hlt">seismicity</span> is well-described by a diurnal signal composed of microseismic events in lake and glacial ice. During melt events, the diurnal signal is suppressed and <span class="hlt">seismicity</span> is instead characterized by large glacial icequakes. We perform network-based correlation and clustering analyses of <span class="hlt">seismic</span> <span class="hlt">record</span> sections and determine that 18% of melt-season icequakes are repetitive (multiplets). The epicentral locations for these multiplets suggest that they are triggered by meltwater produced near a brine seep known as Blood Falls. Our observations of the correspondingp-wave first motions are consistent with volumetric source mechanisms. We suggest that surface melt enables a persistent pathway through this cold ice to an englacial fracture system that is responsible for brine release episodes from the Blood Falls seep. The scalar moments for these events suggest that the volumetric increase at the source region can be explained by melt input.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1305883','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1305883"><span>Probabilistic <span class="hlt">Seismic</span> Hazard Assessment for Iraq</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Onur, Tuna; Gok, Rengin; Abdulnaby, Wathiq</p> <p></p> <p>Probabilistic <span class="hlt">Seismic</span> Hazard Assessments (PSHA) form the basis for most contemporary <span class="hlt">seismic</span> provisions in building codes around the world. The current building code of Iraq was published in 1997. An update to this edition is in the process of being released. However, there are no national PSHA studies in Iraq for the new building code to refer to for <span class="hlt">seismic</span> loading in terms of spectral accelerations. As an interim solution, the new draft building code was considering to refer to PSHA results produced in the late 1990s as part of the Global <span class="hlt">Seismic</span> Hazard Assessment Program (GSHAP; Giardini et al.,more » 1999). However these results are: a) more than 15 years outdated, b) PGA-based only, necessitating rough conversion factors to calculate spectral accelerations at 0.3s and 1.0s for <span class="hlt">seismic</span> design, and <span class="hlt">c</span>) at a probability level of 10% chance of exceedance in 50 years, not the 2% that the building code requires. Hence there is a pressing need for a new, updated PSHA for Iraq.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014GeoRL..41.1964M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014GeoRL..41.1964M"><span>Infrasonic component of volcano-<span class="hlt">seismic</span> eruption tremor</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Matoza, Robin S.; Fee, David</p> <p>2014-03-01</p> <p>Air-ground and ground-air elastic wave coupling are key processes in the rapidly developing field of seismoacoustics and are particularly relevant for volcanoes. During a sustained explosive volcanic eruption, it is typical to <span class="hlt">record</span> a sustained broadband signal on seismometers, termed eruption tremor. Eruption tremor is usually attributed to a subsurface <span class="hlt">seismic</span> source process, such as the upward migration of magma and gases through the shallow conduit and vent. However, it is now known that sustained explosive volcanic eruptions also generate powerful tremor signals in the atmosphere, termed infrasonic tremor. We investigate infrasonic tremor coupling down into the ground and its contribution to the observed <span class="hlt">seismic</span> tremor. Our methodology builds on that proposed by Ichihara et al. (2012) and involves cross-correlation, coherence, and cross-phase spectra between waveforms from nearly collocated <span class="hlt">seismic</span> and infrasonic sensors; we apply it to datasets from Mount St. Helens, Tungurahua, and Redoubt Volcanoes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.S13B0642P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.S13B0642P"><span>National Earthquake Information Center <span class="hlt">Seismic</span> Event Detections on Multiple Scales</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Patton, J.; Yeck, W. L.; Benz, H.; Earle, P. S.; Soto-Cordero, L.; Johnson, C. E.</p> <p>2017-12-01</p> <p>The U.S. Geological Survey National Earthquake Information Center (NEIC) monitors <span class="hlt">seismicity</span> on local, regional, and global scales using automatic picks from more than 2,000 near-real time <span class="hlt">seismic</span> stations. This presents unique challenges in automated event detection due to the high variability in data quality, network geometries and density, and distance-dependent variability in observed <span class="hlt">seismic</span> signals. To lower the overall detection threshold while minimizing false detection rates, NEIC has begun to test the incorporation of new detection and picking algorithms, including multiband (Lomax et al., 2012) and kurtosis (Baillard et al., 2014) pickers, and a new bayesian associator (Glass 3.0). The Glass 3.0 associator allows for simultaneous processing of variably scaled detection grids, each with a unique set of nucleation criteria (e.g., nucleation threshold, minimum associated picks, nucleation phases) to meet specific monitoring goals. We test the efficacy of these new tools on event detection in networks of various scales and geometries, compare our results with previous catalogs, and discuss lessons learned. For example, we find that on local and regional scales, rapid nucleation of small events may require event nucleation with both P and higher-amplitude secondary phases (e.g., S or Lg). We provide examples of the implementation of a scale-independent associator for an induced <span class="hlt">seismicity</span> sequence (local-scale), a large aftershock sequence (regional-scale), and for monitoring global <span class="hlt">seismicity</span>. Baillard, <span class="hlt">C</span>., Crawford, W. <span class="hlt">C</span>., Ballu, V., Hibert, <span class="hlt">C</span>., & Mangeney, A. (2014). An automatic kurtosis-based P-and S-phase picker designed for local <span class="hlt">seismic</span> networks. Bulletin of the Seismological Society of America, 104(1), 394-409. Lomax, A., Satriano, <span class="hlt">C</span>., & Vassallo, M. (2012). Automatic picker developments and optimization: FilterPicker - a robust, broadband picker for real-time <span class="hlt">seismic</span> monitoring and earthquake early-warning, Seism. Res. Lett. , 83, 531-540, doi: 10</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA215943','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA215943"><span>Investigating the Effects Fracture Systems Have on <span class="hlt">Seismic</span> Wave Velocities at the Lajitas, Texas <span class="hlt">Seismic</span> Station</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>1989-05-01</p> <p>Victoria L. Sandidge-Bodoh % S Southern Methodist University Department of Geological Sciences Dallas, TX 75275 1 May 1989 Final Report 3 March 1987 - 2...Projects Agency or the U.S. Government. This technical report has been reviewed and is approved for publicj ion. JAME F. LEWKOW(CZ J/ S F. LEWKOWi<span class="hlt">C</span>...Effects Fracture Systems Have on <span class="hlt">Seismic</span> Wave Velocities at the Lajitas, Texas <span class="hlt">Seismic</span> Station 12. PERSONAL AUTHOR( S ) Victoria L. Sandidge-Bodoh 13a. TYPE</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFMNS33A..07W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFMNS33A..07W"><span>Investigating the <span class="hlt">seismic</span> signal of elephants: using seismology to mitigate elephant human conflict</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Webb, S. J.; Manzi, M.; Naidoo, A.; Raveloson, A.</p> <p>2015-12-01</p> <p>Human interactions with wild elephants are often a source of conflict, as elephants invade inhabited lands looking for sustenance. In order to mitigate these interactions, a number of elephant defense systems are under development. These include electric fences, bees and the playback of warning calls <span class="hlt">recorded</span> from elephants. With the discovery that elephants use <span class="hlt">seismic</span> signals to communicate (O'Connell-Rodwell et al., 2006, Behav. Ecol. Sociobiol.), it is hoped that <span class="hlt">seismic</span> signals can also be used to help reduce conflict. Our current research project investigates the spectral content of the elephant <span class="hlt">seismic</span> signal that travels through the ground using a variety of geophones and seismometers. Our experimental setup used a Geometrics Geode 24 channel <span class="hlt">seismic</span> system with an array of 24 geophones spaced 1 m apart in an area of compact soil overlying weathered granites. Initially we used 14 Hz vertical geophones. The ground and ambient noise conditions were characterized by <span class="hlt">recording</span> several hammer shots. These were used to identify the air wave, wind noise, and the direct wave, which had a dominant frequency of ~50 Hz. Several trained elephants that 'rumble' on command were then deployed ~5 m perpendicular to a line of 24 (14 Hz) vertical geophones between the 1 and 10 m geophone positions. We <span class="hlt">recorded</span> a number of different elephants and configurations, and digitally <span class="hlt">recorded</span> video for comparison. An additional deployment of 20 (14 Hz) horizontal geophones was also used. For all data, the sample interval was 0.25 ms and the <span class="hlt">recording</span> length was 16 s as the timing of the rumbles could not be precisely controlled. We were able to identify the airwave due to the elephant's rumble with velocities between 305-310 m/s and the ground <span class="hlt">seismic</span> signal due to the rumble with frequencies between 20-30 Hz. Our next experiment will include broadband seismometers at a further distance, to more fully characterize the frequency content of the elephant signal.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA487650','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA487650"><span>Estimating Local and Near-Regional Velocity and Attenuation Structure from <span class="hlt">Seismic</span> Noise</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2008-09-30</p> <p><span class="hlt">seismic</span> array in Costa Rica and Nicaragua from ambient <span class="hlt">seismic</span> noise using two independent methods, noise cross correlation and beamforming. The noise...Mean-phase velocity-dispersion curves are calculated for the TUCAN <span class="hlt">seismic</span> array in Costa Rica and Nicaragua from ambient <span class="hlt">seismic</span> noise using two...stations of the TUCAN <span class="hlt">seismic</span> array (Figure 4<span class="hlt">c</span>) using a method similar to Harmon et al. (2007). Variations from Harmon et al. (2007) include removing the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/11816991','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/11816991"><span>Time-lapse 3-D <span class="hlt">seismic</span> imaging of shallow subsurface contaminant flow.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>McKenna, J; Sherlock, D; Evans, B</p> <p>2001-12-01</p> <p>This paper presents a physical modelling study outlining a technique whereby buoyant contaminant flow within water-saturated unconsolidated sand was remotely monitored utilizing the time-lapse 3-D (TL3-D) <span class="hlt">seismic</span> response. The controlled temperature and pressure conditions, along with the high level of acquisition repeatability attainable using sandbox physical models, allow the TL3-D <span class="hlt">seismic</span> response to pore fluid movement to be distinguished from all other effects. TL3-D <span class="hlt">seismic</span> techniques are currently being developed to monitor hydrocarbon reserves within producing reservoirs in an endeavour to improve overall recovery. However, in many ways, sandbox models under atmospheric conditions more accurately simulate the shallow subsurface than petroleum reservoirs. For this reason, perhaps the greatest application for analogue sandbox modelling is to improve our understanding of shallow groundwater and environmental flow mechanisms. Two fluid flow simulations were conducted whereby air and kerosene were injected into separate water-saturated unconsolidated sand models. In both experiments, a base 3-D <span class="hlt">seismic</span> volume was <span class="hlt">recorded</span> and compared with six later monitor surveys <span class="hlt">recorded</span> while the injection program was conducted. Normal incidence amplitude and P-wave velocity information were extracted from the TL3-D <span class="hlt">seismic</span> data to provide visualization of contaminant migration. Reflection amplitudes displayed qualitative areal distribution of fluids when a suitable impedance contrast existed between pore fluids. TL3-D <span class="hlt">seismic</span> reflection tomography can potentially monitor the change in areal distribution of fluid contaminants over time, indicating flow patterns. However, other research and this current work have not established a quantifiable relationship between either normal reflection amplitudes and attenuation and fluid saturation. Generally, different pore fluids will have unique <span class="hlt">seismic</span> velocities due to differences in compressibility and density. The predictable</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015EGUGA..17.8612L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015EGUGA..17.8612L"><span>Carbon cycle dynamics and solar activity embedded in a high-resolution 14<span class="hlt">C</span> speleothem <span class="hlt">record</span> from Belize, Central America</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lechleitner, Franziska A.; Breitenbach, Sebastian F. M.; McIntyre, Cameron; Asmerom, Yemane; Prufer, Keith M.; Polyak, Victor; Culleton, Brendan J.; Kennett, Douglas J.; Eglinton, Timothy I.; Baldini, James U. L.</p> <p>2015-04-01</p> <p> of old recalcitrant carbon to the soil water, and resulting in closer coupling between atmosphere and cave environment. The resolution of the <span class="hlt">record</span> (0.3-0.7 mm/sample) permits identification of the dominant drivers of stalagmite 14<span class="hlt">C</span> during different intervals. For example, hydrologic control on 14<span class="hlt">C</span> appears dominant during the 11th century drought, while in the 16th to 18th century a clear solar influence exists. Solar activity is reflected in YOK-I as lower a14Cinit, reflecting the atmospheric a14<span class="hlt">C</span>. We apply simple hydrological models to investigate the different factors influencing 14<span class="hlt">C</span> in YOK-I. We estimate the importance of mean SOM age to signal dampening, and quantify the strength of the solar influence and the global carbon cycle on the <span class="hlt">record</span>. References: Genty, D., Baker, A., Massault, M., Proctor, <span class="hlt">C</span>., Gilmour, M., Pons-Branchu, E., Hamelin, B. (2001) Dead carbon in stalagmites: carbonate bedrock paleodissolution vs. ageing of soil organic matter. Implications for 13<span class="hlt">C</span> variations in speleothems, GCA, 65 Griffiths, M.L., Fohlmeister, J., Drysdale, R.N., Hua, Q., Johnson, K.R., Hellstrom, J.<span class="hlt">C</span>., Gagan, M.K., Zhao, J.-x. (2012) Hydrological control of the dead carbon fraction in a Holocene tropical speleothem, Quat. Geochron. 14 Ridley, H.E., Baldini, J.U.L., Prufer, K.M., Walczak, I.W., Breitenbach, S.F.M. (in press) High resolution monitoring of a tropical cave system reveals dynamic ventilation and hydrologic resilience to <span class="hlt">seismic</span> activity, Journal of Cave and Karst Studies</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PNAS..114.4893W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PNAS..114.4893W"><span>Reading a 400,000-year <span class="hlt">record</span> of earthquake frequency for an intraplate fault</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Williams, Randolph T.; Goodwin, Laurel B.; Sharp, Warren D.; Mozley, Peter S.</p> <p>2017-05-01</p> <p>Our understanding of the frequency of large earthquakes at timescales longer than instrumental and historical <span class="hlt">records</span> is based mostly on paleoseismic studies of fast-moving plate-boundary faults. Similar study of intraplate faults has been limited until now, because intraplate earthquake recurrence intervals are generally long (10s to 100s of thousands of years) relative to conventional paleoseismic <span class="hlt">records</span> determined by trenching. Long-term variations in the earthquake recurrence intervals of intraplate faults therefore are poorly understood. Longer paleoseismic <span class="hlt">records</span> for intraplate faults are required both to better quantify their earthquake recurrence intervals and to test competing models of earthquake frequency (e.g., time-dependent, time-independent, and clustered). We present the results of U-Th dating of calcite veins in the Loma Blanca normal fault zone, Rio Grande rift, New Mexico, United States, that constrain earthquake recurrence intervals over much of the past ˜550 ka—the longest direct <span class="hlt">record</span> of <span class="hlt">seismic</span> frequency documented for any fault to date. The 13 distinct <span class="hlt">seismic</span> events delineated by this effort demonstrate that for >400 ka, the Loma Blanca fault produced periodic large earthquakes, consistent with a time-dependent model of earthquake recurrence. However, this time-dependent series was interrupted by a cluster of earthquakes at ˜430 ka. The carbon isotope composition of calcite formed during this <span class="hlt">seismic</span> cluster <span class="hlt">records</span> rapid degassing of CO2, suggesting an interval of anomalous fluid source. In concert with U-Th dates <span class="hlt">recording</span> decreased recurrence intervals, we infer <span class="hlt">seismicity</span> during this interval <span class="hlt">records</span> fault-valve behavior. These data provide insight into the long-term <span class="hlt">seismic</span> behavior of the Loma Blanca fault and, by inference, other intraplate faults.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.usgs.gov/of/1980/0509/ofr1980509.pdf','USGSPUBS'); return false;" href="https://pubs.usgs.gov/of/1980/0509/ofr1980509.pdf"><span>Single-channel <span class="hlt">seismic</span>-reflection profiles from Massachusetts coastal waters and the western part of Georges Bank</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Eskenasy, Diane M.</p> <p>1980-01-01</p> <p>The U.S. Geological Survey collected approximately 1,200 km each of airgun and minisparker single-channel <span class="hlt">seismic</span>-reflection profiles during the R/V FAY cruise 023 in September 1976. The purpose of the 6-day cruise was to study the shallow sedimentary structure south and east of southern Massachusetts and to obtain magnetic and gravity data in these areas and in the vicinity of Great South Channel and Cape Ann. The survey was conducted by the U.S. Geo­logical Survey as part of the Massachusetts Cooperative Marine Geologic Program.<span class="hlt">Seismic</span> instruments used include a 1Teledyne 600-joule minisparker system and a 20-in3 airgun system. Navigational data during the cruise were obtained by the use of an Integrated Navigation System, which included the following sub­systems:Teledyne Loran-<span class="hlt">C</span> for both range-range and hyperbofic positions;Magnovox s'atellite receiver;Sperry Mark-29 gyrocompass; andHewlett-Packard 21 MX computer system with dual 9-track magnetic tape <span class="hlt">recording</span>.The original <span class="hlt">records</span> may be studied at the U.S. Geological Survey offices in Woods Hole, Mass. Copies of the <span class="hlt">records</span> can be purchased only from the National Geophysical and Solar-Terrestrial Data Center, NOAA/EDIS/NGSDC, Code D621, 325 Broadway, Boulder CO 80303- (303-497-6338).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFM.T24B..08B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFM.T24B..08B"><span>Characterizing the Inner Accretionary Prism of the Nankai Trough with 3D <span class="hlt">Seismic</span> and Logging While Drilling at IODP Site <span class="hlt">C</span>0002</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Boston, B.; Moore, G. F.; Jurado, M. J.; Sone, H.; Tobin, H. J.; Saffer, D. M.; Hirose, T.; Toczko, S.; Maeda, L.</p> <p>2014-12-01</p> <p>The deeper, inner parts of active accretionary prisms have been poorly studied due the lack of drilling data, low <span class="hlt">seismic</span> image quality and typically thick overlying sediments. Our project focuses on the interior of the Nankai Trough inner accretionary prism using deep scientific drilling and a 3D <span class="hlt">seismic</span> cube. International Ocean Discovery Program (IODP) Expedition 348 extended the existing riser hole to more than 3000 meters below seafloor (mbsf) at Site <span class="hlt">C</span>0002. Logging while drilling (LWD) data included gamma ray, resistivity, resistivity image, and sonic logs. LWD analysis of the lower section revealed on the borehole images intense deformation characterized by steep bedding, faults and fractures. Bedding plane orientations were measured throughout, with minor gaps at heavily deformed zones disrupting the quality of the resistivity images. Bedding trends are predominantly steeply dipping (60-90°) to the NW. Interpretation of fractures and faults in the image log revealed the existence of different sets of fractures and faults and variable fracture density, remarkably high at fault zones. Gamma ray, resistivity and sonic logs indicated generally homogenous lithology interpretation along this section, consistent with the "silty-claystone" predominant lithologies described on cutting samples. Drops in sonic velocity were observed at the fault zones defined on borehole images. <span class="hlt">Seismic</span> reflection interpretation of the deep faults in the inner prism is exceedingly difficult due to a strong seafloor multiple, high-angle bedding dips, and low frequency of the data. Structural reconstructions were employed to test whether folding of <span class="hlt">seismic</span> horizons in the overlying forearc basin could be from an interpreted paleothrust within the inner prism. We used a trishear-based restoration to estimate fault slip on folded horizons landward of <span class="hlt">C</span>0002. We estimate ~500 m of slip from a steeply dipping deep thrust within the last ~0.9 Ma. Folding is not found in the Kumano sediments</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..19.9372G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..19.9372G"><span>High temporal resolution mapping of <span class="hlt">seismic</span> noise sources using heterogeneous supercomputers</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gokhberg, Alexey; Ermert, Laura; Paitz, Patrick; Fichtner, Andreas</p> <p>2017-04-01</p> <p>Time- and space-dependent distribution of <span class="hlt">seismic</span> noise sources is becoming a key ingredient of modern real-time monitoring of various geo-systems. Significant interest in <span class="hlt">seismic</span> noise source maps with high temporal resolution (days) is expected to come from a number of domains, including natural resources exploration, analysis of active earthquake fault zones and volcanoes, as well as geothermal and hydrocarbon reservoir monitoring. Currently, knowledge of noise sources is insufficient for high-resolution subsurface monitoring applications. Near-real-time <span class="hlt">seismic</span> data, as well as advanced imaging methods to constrain <span class="hlt">seismic</span> noise sources have recently become available. These methods are based on the massive cross-correlation of <span class="hlt">seismic</span> noise <span class="hlt">records</span> from all available <span class="hlt">seismic</span> stations in the region of interest and are therefore very computationally intensive. Heterogeneous massively parallel supercomputing systems introduced in the recent years combine conventional multi-core CPU with GPU accelerators and provide an opportunity for manifold increase and computing performance. Therefore, these systems represent an efficient platform for implementation of a noise source mapping solution. We present the first results of an ongoing research project conducted in collaboration with the Swiss National Supercomputing Centre (CSCS). The project aims at building a service that provides <span class="hlt">seismic</span> noise source maps for Central Europe with high temporal resolution (days to few weeks depending on frequency and data availability). The service is hosted on the CSCS computing infrastructure; all computationally intensive processing is performed on the massively parallel heterogeneous supercomputer "Piz Daint". The solution architecture is based on the Application-as-a-Service concept in order to provide the interested external researchers the regular access to the noise source maps. The solution architecture includes the following sub-systems: (1) data acquisition responsible for</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010AGUFMOS43A1599A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010AGUFMOS43A1599A"><span>Development of Vertical Cable <span class="hlt">Seismic</span> System for Hydrothermal Deposit Survey (2) - Feasibility Study</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Asakawa, E.; Murakami, F.; Sekino, Y.; Okamoto, T.; Mikada, H.; Takekawa, J.; Shimura, T.</p> <p>2010-12-01</p> <p>In 2009, Ministry of Education, Culture, Sports, Science and Technology(MEXT) started the survey system development for Hydrothermal deposit. We proposed the Vertical Cable <span class="hlt">Seismic</span> (VCS), the reflection <span class="hlt">seismic</span> survey with vertical cable above seabottom. VCS has the following advantages for hydrothermal deposit survey. . (1) VCS is an effective high-resolution 3D <span class="hlt">seismic</span> survey within limited area. (2) It achieves high-resolution image because the sensors are closely located to the target. (3) It avoids the coupling problems between sensor and seabottom that cause serious damage of <span class="hlt">seismic</span> data quality. (4) Various types of marine source are applicable with VCS such as sea-surface source (air gun, water gun etc.) , deep-towed or ocean bottom sources. (5) Autonomous <span class="hlt">recording</span> system. Our first experiment of 2D/3D VCS surveys has been carried out in Lake Biwa, JAPAN. in November 2009. The 2D VCS data processing follows the walk-away VSP, including wave field separation and depth migration. The result gives clearer image than the conventional surface <span class="hlt">seismic</span>. Prestack depth migration is applied to 3D data to obtain good quality 3D depth volume. Uncertainty of the source/receiver poisons in water causes the serious problem of the imaging. We used several transducer/transponder to estimate these positions. The VCS <span class="hlt">seismic</span> <span class="hlt">records</span> themselves can also provide sensor position using the first break of each trace and we calibrate the positions. We are currently developing the autonomous <span class="hlt">recording</span> VCS system and planning the trial experiment in actual ocean to establish the way of deployment/recovery and the examine the position through the current flow in November, 2010. The second VCS survey will planned over the actual hydrothermal deposit with deep-towed source in February, 2011.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.C41D1257M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.C41D1257M"><span>Lake Generated Microseisms at Yellowstone Lake as a <span class="hlt">Record</span> of Ice Phenology</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mohd Mokhdhari, A. A.; Koper, K. D.; Burlacu, R.</p> <p>2017-12-01</p> <p>It has recently been shown that wave action in lakes produces microseisms, which generate noise peaks in the period range of 0.8-1.2 s as <span class="hlt">recorded</span> by nearby <span class="hlt">seismic</span> stations. Such noise peaks have been observed at seven <span class="hlt">seismic</span> stations (H17A, LKWY, B208, B944, YTP, YLA, and YLT) located within 2 km of the Yellowstone Lake shoreline. Initial work using 2016 data shows that the variations in the microseism signals at Yellowstone Lake correspond with the freezing and thawing of lake ice: the <span class="hlt">seismic</span> noise occurs more frequently in the spring, summer, and fall, and less commonly in the winter. If this can be confirmed, then lake-generated microseisms could provide a consistent measure of the freezing and melting dates of high-latitude lakes in remote areas. The <span class="hlt">seismic</span> data would then be useful in assessing the effects of climate change on the ice phenology of those lakes. In this work, we analyze continuous <span class="hlt">seismic</span> data <span class="hlt">recorded</span> by the seven <span class="hlt">seismic</span> stations around Yellowstone Lake for the years of 1995 to 2016. We generate probability distribution functions of power spectral density for each station to observe the broad elevation of energy near a period of 1 s. The time dependence of this 1-s <span class="hlt">seismic</span> noise energy is analyzed by extracting the power spectral density at 1 s from every processed hour. The <span class="hlt">seismic</span> observations are compared to direct measurements of the dates of ice-out and freeze-up as reported by rangers at Yellowstone National Park. We examine how accurate the <span class="hlt">seismic</span> data are in <span class="hlt">recording</span> the freezing and melting of Yellowstone Lake, and how the accuracy changes as a function of the number of stations used. We also examine how sensitive the results are to the particular range of periods that are analyzed.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li class="active"><span>21</span></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_21 --> <div id="page_22" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li class="active"><span>22</span></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="421"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EGUGA..18.4512C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EGUGA..18.4512C"><span><span class="hlt">Seismic</span> Risk Perception compared with <span class="hlt">seismic</span> Risk Factors</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Crescimbene, Massimo; La Longa, Federica; Pessina, Vera; Pino, Nicola Alessandro; Peruzza, Laura</p> <p>2016-04-01</p> <p>The communication of natural hazards and their consequences is one of the more relevant ethical issues faced by scientists. In the last years, social studies have provided evidence that risk communication is strongly influenced by the risk perception of people. In order to develop effective information and risk communication strategies, the perception of risks and the influencing factors should be known. A theory that offers an integrative approach to understanding and explaining risk perception is still missing. To explain risk perception, it is necessary to consider several perspectives: social, psychological and cultural perspectives and their interactions. This paper presents the results of the CATI survey on <span class="hlt">seismic</span> risk perception in Italy, conducted by INGV researchers on funding by the DPC. We built a questionnaire to assess <span class="hlt">seismic</span> risk perception, with a particular attention to compare hazard, vulnerability and exposure perception with the real data of the same factors. The <span class="hlt">Seismic</span> Risk Perception Questionnaire (SRP-Q) is designed by semantic differential method, using opposite terms on a Likert scale to seven points. The questionnaire allows to obtain the scores of five risk indicators: Hazard, Exposure, Vulnerability, People and Community, Earthquake Phenomenon. The questionnaire was administered by telephone interview (<span class="hlt">C</span>.A.T.I.) on a statistical sample at national level of over 4,000 people, in the period January -February 2015. Results show that risk perception seems be underestimated for all indicators considered. In particular scores of <span class="hlt">seismic</span> Vulnerability factor are extremely low compared with house information data of the respondents. Other data collected by the questionnaire regard Earthquake information level, Sources of information, Earthquake occurrence with respect to other natural hazards, participation at risk reduction activities and level of involvement. Research on risk perception aims to aid risk analysis and policy-making by</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70178111','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70178111"><span>Observations of <span class="hlt">seismicity</span> and ground motion in the northeast U.S. Atlantic margin from ocean bottom seismometer data</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Flores, Claudia; ten Brink, Uri S.; McGuire, Jeffrey J.; Collins, John A.</p> <p>2017-01-01</p> <p>Earthquake data from two short-period ocean-bottom seismometer (OBS) networks deployed for over a year on the continental slope off New York and southern New England were used to evaluate <span class="hlt">seismicity</span> and ground motions along the continental margin. Our OBS networks located only one earthquake of Mc∼1.5 near the shelf edge during six months of <span class="hlt">recording</span>, suggesting that <span class="hlt">seismic</span> activity (MLg>3.0) of the margin as far as 150–200 km offshore is probably successfully monitored by land stations without the need for OBS deployments. The spectral acceleration from two local earthquakes <span class="hlt">recorded</span> by the OBS was found to be generally similar to the acceleration from these earthquakes <span class="hlt">recorded</span> at several <span class="hlt">seismic</span> stations on land and to hybrid empirical acceleration relationships for eastern North America. Therefore, the <span class="hlt">seismic</span> attenuation used for eastern North America can be extended in this region at least to the continental slope. However, additional offshore studies are needed to verify these preliminary conclusions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2004ASAJ..115.2555N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2004ASAJ..115.2555N"><span>Ground sounds: <span class="hlt">Seismic</span> detection in the golden mole</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Narins, Peter M.; Lewis, Edwin R.</p> <p>2004-05-01</p> <p>The Namib Desert golden mole is a nocturnal, surface-foraging mammal, possessing a massively hypertrophied malleus which presumably confers low-frequency, substrate-vibration sensitivity through inertial bone conduction. Foraging trails are punctuated with characteristic sand disturbances in which the animal's head dips under the sand. The function of this behavior is not known but it is thought that it may be used to obtain a <span class="hlt">seismic</span> fix on the next mound to be visited. To test this, we measured the local <span class="hlt">seismic</span> vibrations both on the top of a mound and on the flats. The spectrum <span class="hlt">recorded</span> on the flats shows a relatively low-amplitude peak at about 120 Hz, whereas the spectral peak <span class="hlt">recorded</span> from the mound is nearly 17 dB greater in amplitude and centered at 310 Hz. This suggests that mounds act as <span class="hlt">seismic</span> beacons for the golden moles that would be detectable from distances corresponding to typical intermound distances of 20-25 m. In addition, out of the 117 species for which data are available, these golden moles have the greatest ossicular mass relative to body size (Mason, personal communication). Functionally, they appear to be low-frequency specialists, and it is likely that golden moles hear through substrate conduction. [Work supported by NIH.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018E3SWC..3503003S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018E3SWC..3503003S"><span><span class="hlt">Seismic</span> Linear Noise Attenuation with Use of Radial Transform</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Szymańska-Małysa, Żaneta</p> <p>2018-03-01</p> <p>One of the goals of <span class="hlt">seismic</span> data processing is to attenuate the <span class="hlt">recorded</span> noise in order to enable correct interpretation of the image. Radial transform has been used as a very effective tool in the attenuation of various types of linear noise, both numerical and real (such as ground roll, direct waves, head waves, guided waves etc). The result of transformation from offset - time (X - T) domain into apparent velocity - time (R - T) domain is frequency separation between reflections and linear events. In this article synthetic and real <span class="hlt">seismic</span> shot gathers were examined. One example was targeted at far offset area of dataset where reflections and noise had similar apparent velocities and frequency bands. Another example was a result of elastic modelling where linear artefacts were produced. Bandpass filtering and scaling operation executed in radial domain attenuated all discussed types of linear noise very effectively. After noise reduction all further processing steps reveal better results, especially velocity analysis, migration and stacking. In all presented cases signal-to-noise ratio was significantly increased and reflections covered previously by noise were revealed. Power spectra of filtered <span class="hlt">seismic</span> <span class="hlt">records</span> preserved real dynamics of reflections.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUFM.S33D2485R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUFM.S33D2485R"><span>Seasonal variability in Tibetan <span class="hlt">seismicity</span> 1991-2013</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Randolph-Flagg, N. G.; Day, J.; Burgmann, R.; Manga, M.</p> <p>2013-12-01</p> <p><span class="hlt">Seismicity</span> in the High Himalaya in Nepal (Bollinger et al., GRL, 2007, Bettinelli et al., EPSL, 2008), the San Andreas fault near Parkfield, California (Christiansen et al., 2007), Mt. Hochstaufen in Germany (Hainzl et al., 2006), and some Cascade Range volcanoes (Christiansen et al., GRL, 2005; Saar and Manga, EPSL, 2003) shows seasonal modulation. From 1991 to 2013, <span class="hlt">seismicity</span> throughout the ~500 km by ~1000 km Tibetan Plateau also appears to be modulated with 66% more shallow (depth < 20km) earthquakes in spring and fall than in the summer and winter. This variation cannot be explained by seasonal changes in <span class="hlt">seismic</span> network coverage or triggering by (or occurrence of) large magnitude earthquakes. Significant foreshocks and aftershocks of the 2008 M7.9 Wenchuan earthquake in Sichuan dominate the <span class="hlt">seismic</span> <span class="hlt">record</span> from 2008 to 2009 and those years are not considered in the statistical analysis. The Tibetan <span class="hlt">seismicity</span>, although weaker, is very similar to the modulation observed in Nepal and in the locked section of the San Andreas fault at Parkfield. To explain this biannual signal, we assess the possible effects of hydrologic loading (and unloading), pore pressure diffusion, fault plane orientation, evapotranspiration, earth tides, and atmospheric pressure. The similarity in seasonal signals throughout the area suggests that many faults on the Tibetan Plateau are critically stressed and sensitive to small transient stresses.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014PhDT.......265R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014PhDT.......265R"><span>A <span class="hlt">seismic</span> reflection velocity study of a Mississippian mud-mound in the Illinois basin</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ranaweera, Chamila Kumari</p> <p></p> <p>Two mud-mounds have been reported in the Ullin limestone near, but not in, the Aden oil field in Hamilton County, Illinois. One mud-mound is in the Broughton oil field of Hamilton County 25 miles to the south of Aden. The second mud-mound is in the Johnsonville oil field in Wayne County 20 miles to the north of Aden. <span class="hlt">Seismic</span> reflection profiles were shot in 2012 adjacent to the Aden oil field to evaluate the oil prospects and to investigate the possibility of detecting Mississippian mud-mounds near the Aden field. A feature on one of the <span class="hlt">seismic</span> profiles was interpreted to be a mud-mound or carbonate buildup. A well drilled at the location of this interpreted structure provided digital geophysical logs and geological logs used to refine the interpretation of the <span class="hlt">seismic</span> profiles. Geological data from the new well at Aden, in the form of drill cuttings, have been used to essentially confirm the existence of a mud-mound in the Ullin limestone at a depth of 4300 feet. Geophysical well logs from the new well near Aden were used to create 1-D computer models and synthetic seismograms for comparison to the <span class="hlt">seismic</span> data. The reflection <span class="hlt">seismic</span> method is widely used to aid interpreting subsurface geology. Processing <span class="hlt">seismic</span> data is an important step in the method as a properly processed <span class="hlt">seismic</span> section can give a better image of the subsurface geology whereas a poorly processed section could mislead the interpretation. <span class="hlt">Seismic</span> reflections will be more accurately depicted with careful determination of <span class="hlt">seismic</span> velocities and by carefully choosing the processing steps and parameters. Various data processing steps have been applied and parameters refined to produce improved stacked <span class="hlt">seismic</span> <span class="hlt">records</span>. The resulting <span class="hlt">seismic</span> <span class="hlt">records</span> from the Aden field area indicate a <span class="hlt">seismic</span> response similar to what is expected from a carbonate mud-mound. One-dimensional synthetic seismograms were created using the available sonic and density logs from the well drilled near the Aden <span class="hlt">seismic</span> lines</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFM.T43D3049B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFM.T43D3049B"><span>Source Characterization and <span class="hlt">Seismic</span> Hazard Considerations for Hydraulic Fracture Induced <span class="hlt">Seismicity</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bosman, K.; Viegas, G. F.; Baig, A. M.; Urbancic, T.</p> <p>2015-12-01</p> <p>Large microseismic events (M>0) have been shown to be generated during hydraulic fracture treatments relatively frequently. These events are a concern both from public safety and engineering viewpoints. Recent microseismic monitoring projects in the Horn River Basin have utilized both downhole and surface sensors to <span class="hlt">record</span> events associated with hydraulic fracturing. The resulting hybrid monitoring system has produced a large dataset with two distinct groups of events: large events <span class="hlt">recorded</span> by the surface network (0<M<3), and small events <span class="hlt">recorded</span> only by the downhole sensors (-4<M<0). Large events tend to occur well below the reservoir on pre-existing structures; small events are concentrated at reservoir depth. Differences in behavior have been observed between these two datasets, leading to conclusions of different underlying processes responsible for the <span class="hlt">recorded</span> activity. Both datasets show very low <span class="hlt">seismic</span> efficiency, implying slip weakening and possibly the presence of fluids in the source region. Reservoir events have shear-tensile source mechanisms ranging between tensile opening and tensile closing, and fracture orientations dominated by the rock fabric which are not always optimally oriented to the regional stress field. The observed source characteristics are expected for events driven by increased pore pressure and reduced friction due to lubrication. On average, deep events show higher stress drop, apparent stress, and rupture velocity than reservoir events. This reflects higher confining stresses with depth, and possibly the release of stored energy in the existing zone of weakness. Deep events are dominated by shear failures, but source characteristics are smaller than for naturally occurring tectonic earthquakes of similar magnitude. Most importantly from a <span class="hlt">seismic</span> hazard perspective, large earthquakes associated with hydrofracing have lower stress drops than tectonic earthquakes, and thus produce smaller peak ground acceleration and less damage on</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..1918604B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..1918604B"><span>Site characterization of the national <span class="hlt">seismic</span> network of Italy</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bordoni, Paola; Pacor, Francesca; Cultrera, Giovanna; Casale, Paolo; Cara, Fabrizio; Di Giulio, Giuseppe; Famiani, Daniela; Ladina, Chiara; PIschiutta, Marta; Quintiliani, Matteo</p> <p>2017-04-01</p> <p>The national <span class="hlt">seismic</span> network of Italy (Rete Sismica Nazionale, RSN) run by Istituto Nazionale di Geofisica e Vulcanologia (INGV) consists of more than 400 <span class="hlt">seismic</span> stations connected in real time to the institute data center in order to locate earthquakes for civil defense purposes. A critical issue in the performance of a network is the characterization of site condition at the <span class="hlt">recording</span> stations. Recently INGV has started addressing this subject through the revision of all available geological and geophysical data, the acquisition of new information by means of ad-hoc field measurements and the analysis of <span class="hlt">seismic</span> waveforms. The main effort is towards building a database, integrated with the other INGV infrastructures, designed to archive homogeneous parameters through the <span class="hlt">seismic</span> network useful for a complete site characterization, including housing, geological, seismological and geotechnical features as well as the site class according to the European and Italian building codes. Here we present the ongoing INGV activities.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015EGUGA..17.1996F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015EGUGA..17.1996F"><span>3D Modelling of <span class="hlt">Seismically</span> Active Parts of Underground Faults via <span class="hlt">Seismic</span> Data Mining</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Frantzeskakis, Theofanis; Konstantaras, Anthony</p> <p>2015-04-01</p> <p>, E. and Papathanassiou, G.: 'Aftershock relocation and frequency-size distribution, stress inversion and seismotectonic setting of the 7 August 2013 M=5.4 earthquake in Kallidromon Mountain, central Greece', Tectonophysics, vol. 617, pp. 101-113, 2014 [4] Maravelakis, E., Bilalis, N., Mantzorou, I., Konstantaras, A. and Antoniadis, A.: '3D modelling of the oldest olive tree of the world', International Journal Of Computational Engineering Research, vol. 2 (2), pp. 340-347, 2012 [5] Konstantaras, A., Katsifarakis, E, Maravelakis, E, Skounakis, E, Kokkinos, E. and Karapidakis, E.: 'Intelligent spatial-clustering of <span class="hlt">seismicity</span> in the vicinity of the Hellenic <span class="hlt">seismic</span> arc', Earth Science Research, vol. 1 (2), pp. 1- 10, 2012 [6] Georgoulas, G., Konstantaras, A., Katsifarakis, E., Stylios, <span class="hlt">C</span>., Maravelakis, E and Vachtsevanos, G.: '<span class="hlt">Seismic</span>-mass" density-based algorithm for spatio-temporal clustering', Expert Systems with Applications, vol. 40 (10), pp. 4183-4189, 2013 [7] Konstantaras, A.: 'Classification of Distinct <span class="hlt">Seismic</span> Regions and Regional Temporal Modelling of <span class="hlt">Seismicity</span> in the Vicinity of the Hellenic <span class="hlt">Seismic</span> Arc', Selected Topics in Applied Earth Observations and Remote Sensing, IEEE Journal of', vol. 99, pp. 1-7, 2013</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010EGUGA..1210582V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010EGUGA..1210582V"><span>Intraplate <span class="hlt">seismicity</span> across the Cape Verde swell</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Vales, Dina; Matias, Luís.; Haberland, Christian; Silveira, Graça.; Weber, Michael; Carrilho, Fernando; Dias, Nuno</p> <p>2010-05-01</p> <p>The Cape Verde Archipelago ((15-17°N, 23-26°W) is located within the African plate, about 500km west of Senegal, in the African coast. The islands are located astride the Cape Verde mid-plate topographic swell, one of the largest features of its type in the world's ocean basins. The origin of this Cape Verde swell is still in debate. Previous determinations of the elastic thickness (Te) reveal a normal Te and a modest heat flow anomaly which suggest that the swell cannot be fully explained by uplift due to thermal reheating of the lithosphere by an underlying ‘‘hot spot'' and that other, deep-seated, mantle processes must be involved. The CV-PLUME (An investigation on the geometry and deep signature of the Cape Verde mantle plume) project intends to shape the geometry and deep origin of the Cape Verde mantle plume, via a combined study of <span class="hlt">seismic</span>, magnetic, gravimetric and geochemical observations. Through this study we intend to characterize the structure beneath the archipelago from the surface down to the deep mantle. The core of this 3-year project was a temporary deployment of 39 Very Broad Band seismometers, across all the inhabited islands, to <span class="hlt">recorder</span> local and teleseismic earthquakes. These instruments were operational from November 2007 to September 2008. In this work we report on the preliminary results obtained from the CV-PLUME network on the characterization of the local and regional <span class="hlt">seismicity</span>. To detect the small magnitude <span class="hlt">seismic</span> events the continuous data stream was screened using spectrograms. This proved to be a very robust technique in the face of the high short-period noise <span class="hlt">recorded</span> by many of the stations, particularly during day time. The 10 month observation time showed that the background <span class="hlt">seismic</span> activity in the Archipelago and surrounding area is low, with only a very few events <span class="hlt">recorded</span> by the complete network. However, two clusters of earthquakes were detected close to the Brava Island, one to the NW and a second one, more active</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.S33B0867M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.S33B0867M"><span>Reconstructing the <span class="hlt">Seismic</span> Wavefield using Curvelets and Distributed Acoustic Sensing</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Muir, J. B.; Zhan, Z.</p> <p>2017-12-01</p> <p>Distributed Acoustic Sensing (DAS) offers an opportunity to produce cost effective and uniquely dense images of the surface <span class="hlt">seismic</span> wavefield - DAS also produces extremely large data volumes that require innovative methods of data reduction and <span class="hlt">seismic</span> parameter inversion to handle efficiently. We leverage DAS and the super-Nyquist sampling enabled by compressed sensing of the wavefield in the curvelet domain to produce accurate images of the horizontal velocity within a target region, using only short ( 1-10 minutes) <span class="hlt">records</span> of either active <span class="hlt">seismic</span> sources or ambient <span class="hlt">seismic</span> signals. Once the wavefield has been fully described, modern "tomographic" techniques, such as Helmholtz tomography or Wavefield Gradiometry, can be employed to determine <span class="hlt">seismic</span> parameters of interest such as phase velocity. An additional practical benefit of employing a wavefield reconstruction step is that multiple heterogeneous forms of instrumentation can be naturally combined - therefore in this study we also explore the addition of three component nodal <span class="hlt">seismic</span> data into the reconstructed wavefield. We illustrate these techniques using both synthetic examples and data taken from the Brady Geothermal Field in Nevada during the PoroTomo (U. Wisconsin Madison) experiment of 2016.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19920001515','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19920001515"><span>Martian <span class="hlt">seismicity</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Phillips, Roger J.; Grimm, Robert E.</p> <p>1991-01-01</p> <p>The design and ultimate success of network seismology experiments on Mars depends on the present level of Martian <span class="hlt">seismicity</span>. Volcanic and tectonic landforms observed from imaging experiments show that Mars must have been a <span class="hlt">seismically</span> active planet in the past and there is no reason to discount the notion that Mars is <span class="hlt">seismically</span> active today but at a lower level of activity. Models are explored for present day Mars <span class="hlt">seismicity</span>. Depending on the sensitivity and geometry of a <span class="hlt">seismic</span> network and the attenuation and scattering properties of the interior, it appears that a reasonable number of Martian <span class="hlt">seismic</span> events would be detected over the period of a decade. The thermoelastic cooling mechanism as estimated is surely a lower bound, and a more refined estimate would take into account specifically the regional cooling of Tharsis and lead to a higher frequency of <span class="hlt">seismic</span> events.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014EGUGA..1613010G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014EGUGA..1613010G"><span><span class="hlt">Seismic</span> characterization of the Chelyabinsk meteor's terminal explosion</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>González, Álvaro; Heimann, Sebastian; Wang, Rongjiang; Cesca, Simone; Dahm, Torsten</p> <p>2014-05-01</p> <p>On February 15th, 2013, an exceptionally large meteor in the region of Chelyabinsk, Russia, produced a powerful shock wave which caused unprecedented damage to people and property, the strongest atmospheric infrasound signal ever <span class="hlt">recorded</span>, and remarkable ground motion. Here we describe and model the resulting Rayleigh waves, <span class="hlt">recorded</span> at broadband <span class="hlt">seismic</span> stations at distances from ~230 to ~4,100 km. Our full-waveform modeling uses a seismogram simulation code specifically tailored to consider wave propagation in the atmosphere and solid Earth, and the coupling at the interface between them. An isotropic point-like airburst reproduces very well the available <span class="hlt">seismic</span> observations, without requiring a more complex explanation, such as a moving source. The measured <span class="hlt">seismic</span> shaking was generated by direct coupling of the atmospheric shock wave to the ground, and then it propagated outwards faster than the atmospheric shock wave itself, at up to 3.9 km/s. The best-fitting airburst location (61.22° E, 54.88° N) is SW of Chelyabinsk city, exactly at the terminal part of the meteor's trajectory, just after it experienced a dramatic flare, with apparent brightness larger than the Sun's. We estimated the meteor's ground path from published trajectory data, eyewitness observations, and detailed satellite imagery of the exact location where a major meteorite fragment landed, in the frozen Lake Chebarkul (60.32074° E, 54.95966° N). Fixing the source origin time allowed us calculating that the explosion took place in the stratosphere, at an altitude of 22.5 ± 1.5 km. This value is lower than the reported altitude of peak brightness (about 29.5 km), but more consistent with the observations of shock wave travel times. Such results highlight the importance of terminal energy release down to lower altitude. We analyzed a surveillance video <span class="hlt">recorded</span> inside a factory (61.347° E, 54.902° N) at Korkino, a locality close to the airburst. It shows a time delay of 87.5 seconds</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015EGUGA..17.7430F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015EGUGA..17.7430F"><span>Microseismic monitoring of soft-rock landslide: contribution of a 3D velocity model for the location of <span class="hlt">seismic</span> sources.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Floriane, Provost; Jean-Philippe, Malet; Cécile, Doubre; Julien, Gance; Alessia, Maggi; Agnès, Helmstetter</p> <p>2015-04-01</p> <p>Characterizing the micro-<span class="hlt">seismic</span> activity of landslides is an important parameter for a better understanding of the physical processes controlling landslide behaviour. However, the location of the <span class="hlt">seismic</span> sources on landslides is a challenging task mostly because of (a) the <span class="hlt">recording</span> system geometry, (b) the lack of clear P-wave arrivals and clear wave differentiation, (<span class="hlt">c</span>) the heterogeneous velocities of the ground. The objective of this work is therefore to test whether the integration of a 3D velocity model in probabilistic <span class="hlt">seismic</span> source location codes improves the quality of the determination especially in depth. We studied the clay-rich landslide of Super-Sauze (French Alps). Most of the <span class="hlt">seismic</span> events (rockfalls, slidequakes, tremors...) are generated in the upper part of the landslide near the main scarp. The <span class="hlt">seismic</span> <span class="hlt">recording</span> system is composed of two antennas with four vertical seismometers each located on the east and west sides of the <span class="hlt">seismically</span> active part of the landslide. A refraction <span class="hlt">seismic</span> campaign was conducted in August 2014 and a 3D P-wave model has been estimated using the Quasi-Newton tomography inversion algorithm. The shots of the <span class="hlt">seismic</span> campaign are used as calibration shots to test the performance of the different location methods and to further update the 3D velocity model. Natural <span class="hlt">seismic</span> events are detected with a semi-automatic technique using a frequency threshold. The first arrivals are picked using a kurtosis-based method and compared to the manual picking. Several location methods were finally tested. We compared a non-linear probabilistic method coupled with the 3D P-wave model and a beam-forming method inverted for an apparent velocity. We found that the Quasi-Newton tomography inversion algorithm provides results coherent with the original underlaying topography. The velocity ranges from 500 m.s-1 at the surface to 3000 m.s-1 in the bedrock. For the majority of the calibration shots, the use of a 3D velocity model</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018MS%26E..352a2046S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018MS%26E..352a2046S"><span>Microtremor survey to investigate <span class="hlt">seismic</span> vulnerability around the Seulimum Fault, Aceh Besar-Indonesia</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Simanjuntak, Andrean V. H.; Muksin, Umar; Rahmayani, Febrina</p> <p>2018-05-01</p> <p>The Seulimeum Fault has generated inland earthquake with magnitude larger than M 6.5 that destroyed houses in the Lamteuba and Krueng Raya Villages. Earthquakes along the Seulimeum Fault are mostly right lateral strike-slip characterizing the Fault. The understanding of the <span class="hlt">seismic</span> vulnerability around the highly populated Banda Aceh City and the villages in Aceh Besar is therefore very important since the city, and the villages are very close to the Seulimeum Fault. A microtremor survey has been conducted to investigate <span class="hlt">seismic</span> vulnerability in the area closed to the Seulimeum Fault. The waveforms of the microtremor have been <span class="hlt">recorded</span> in Lamteuba and Kreung Raya villages, Aceh Besar at 20 sites for 7 days from August 14, 2017 with the interval of measurement of 1 km. The waveforms <span class="hlt">recorded</span> for 30 minutes at each site by using one Taurus Seismometer in miniseed format. The data has been analyzing by using Geopsy to obtain the Horizontal-Vertical Spectral Ratio for each site. The <span class="hlt">seismic</span> vulnerability is considered to be high if the value of the Horizontal-Vertical Spectral Ratio is high. The HVSR values are then interpolated to obtain the <span class="hlt">seismic</span> vulnerability map. The preliminary result shows high <span class="hlt">seismic</span> vulnerability in the area around the first site.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007AcGeo..55..191P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007AcGeo..55..191P"><span>Identification of <span class="hlt">seismic</span> anomalies caused by gas saturation on the basis of theoretical P and PS wavefield in the Carpathian Foredeep, SE Poland</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pietsch, Kaja; Marzec, Paweł; Kobylarski, Marcin; Danek, Tomasz; Leśniak, Andrzej; Tatarata, Artur; Gruszczyk, Edward</p> <p>2007-06-01</p> <p>The thin-layer build of the Carpathian Foredeep Miocene formations and large petrophysical parameter variation cause <span class="hlt">seismic</span> images of gas-saturated zones to be ambiguous, and the location of prospection wells on the basis of anomalous <span class="hlt">seismic</span> <span class="hlt">record</span> is risky. A method that assists reservoir interpretation of standard <span class="hlt">recorded</span> <span class="hlt">seismic</span> profiles (P waves) can be a converted wave <span class="hlt">recording</span> (PS waves). This paper presents the results of application of a multicomponent <span class="hlt">seismic</span> survey for the reservoir interpretation over the Chałupki Dębniańskie gas deposit, carried out for the first time in Poland by Geofizyka Kraków Ltd. for the Polish Oil and Gas Company. <span class="hlt">Seismic</span> modeling was applied as the basic research tool, using the SeisMod program based on the finite-difference solution of the acoustic wave equation and equations of motion. Seismogeological models for P waves were developed using Acoustic Logs; S-wave model (<span class="hlt">records</span> only from part of the well) was developed on the basis of theoretical curves calculated by means of the Estymacja program calibrated with average S-velocities, calculated by correlation of <span class="hlt">recorded</span> P and PS wavefields with 1D modeling. The conformity between theoretical and <span class="hlt">recorded</span> wavefields makes it possible to apply the criteria established on the basis of modeling for reservoir interpretation. Direct hydrocarbon indicators (bright spots, phase change, time sag) unambiguously identify gas-prone layers within the ChD-2 prospect. A partial range of the indicators observed in the SW part of the studied profile (bright spot that covers a single, anticlinally bent <span class="hlt">seismic</span> horizon) points to saturation of the horizon. The proposed location is confirmed by criteria determined for converted waves (continuous <span class="hlt">seismic</span> horizons with constant, high amplitude) despite poorer agreement between theoretical and <span class="hlt">recorded</span> wavefields.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70157554','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70157554"><span>Using micro-<span class="hlt">seismicity</span> and <span class="hlt">seismic</span> velocities to map subsurface geologic and hydrologic structure within the Coso geothermal field, California</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Kaven, Joern Ole; Hickman, Stephen H.; Davatzes, Nicholas C.</p> <p>2012-01-01</p> <p>Geothermal reservoirs derive their capacity for fluid and heat transport in large part from faults and fractures. Micro-<span class="hlt">seismicity</span> generated on such faults and fractures can be used to map larger fault structures as well as secondary fractures that add access to hot rock, fluid storage and recharge capacity necessary to have a sustainable geothermal resource. Additionally, inversion of <span class="hlt">seismic</span> velocities from micro-<span class="hlt">seismicity</span> permits imaging of regions subject to the combined effects of fracture density, fluid pressure and steam content, among other factors. We relocate 14 years of <span class="hlt">seismicity</span> (1996-2009) in the Coso geothermal field using differential travel times and simultaneously invert for <span class="hlt">seismic</span> velocities to improve our knowledge of the subsurface geologic and hydrologic structure. We utilize over 60,000 micro-<span class="hlt">seismic</span> events using waveform cross-correlation to augment to expansive catalog of P- and S-wave differential travel times <span class="hlt">recorded</span> at Coso. We further carry out rigorous uncertainty estimation and find that our results are precise to within 10s of meters of relative location error. We find that relocated micro-<span class="hlt">seismicity</span> outlines prominent, through-going faults in the reservoir in some cases. We also find that a significant portion of <span class="hlt">seismicity</span> remains diffuse and does not cluster into more sharply defined major structures. The <span class="hlt">seismic</span> velocity structure reveals heterogeneous distributions of compressional (Vp) and shear (Vs) wave speed, with Vp generally lower in the main field when compared to the east flank and Vs varying more significantly in the shallow portions of the reservoir. The Vp/Vs ratio appears to outline the two main compartments of the reservoir at depths of -0.5 to 1.5 km (relative to sea-level), with a ridge of relatively high Vp/Vs separating the main field from the east flank. In the deeper portion of the reservoir this ridge is less prominent. Our results indicate that high-precision relocations of micro-<span class="hlt">seismicity</span> can provide</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2002EGSGA..27.1536S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2002EGSGA..27.1536S"><span><span class="hlt">Seismic</span> Ecology</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Seleznev, V. S.; Soloviev, V. M.; Emanov, A. F.</p> <p></p> <p>The paper is devoted to researches of influence of <span class="hlt">seismic</span> actions for industrial and civil buildings and people. The <span class="hlt">seismic</span> actions bring influence directly on the people (vibration actions, force shocks at earthquakes) or indirectly through various build- ings and the constructions and can be strong (be felt by people) and weak (be fixed by sensing devices). The great number of work is devoted to influence of violent <span class="hlt">seismic</span> actions (first of all of earthquakes) on people and various constructions. This work is devoted to study weak, but long <span class="hlt">seismic</span> actions on various buildings and people. There is a need to take into account <span class="hlt">seismic</span> oscillations, acting on the territory, at construction of various buildings on urbanized territories. Essential influence, except for violent earthquakes, man-caused <span class="hlt">seismic</span> actions: the explosions, <span class="hlt">seismic</span> noise, emitted by plant facilities and moving transport, radiation from high-rise buildings and constructions under action of a wind, etc. can exert. Materials on increase of man- caused <span class="hlt">seismicity</span> in a number of regions in Russia, which earlier were not <span class="hlt">seismic</span>, are presented in the paper. Along with maps of <span class="hlt">seismic</span> microzoning maps to be built indicating a variation of amplitude spectra of <span class="hlt">seismic</span> noise within day, months, years. The presence of an information about amplitudes and frequencies of oscillations from possible earthquakes and man-caused oscillations in concrete regions allows carry- ing out soundly designing and construction of industrial and civil housing projects. The construction of buildings even in not <span class="hlt">seismically</span> dangerous regions, which have one from resonance frequencies coincident on magnitude to frequency of oscillations, emitted in this place by man-caused objects, can end in failure of these buildings and heaviest consequences for the people. The practical examples of detail of engineering- seismological investigation of large industrial and civil housing projects of Siberia territory (hydro power</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.usgs.gov/of/2004/1243','USGSPUBS'); return false;" href="https://pubs.usgs.gov/of/2004/1243"><span><span class="hlt">Seismic</span> reflection and refraction data acquired in Canada Basin, Northwind Ridge and Northwind Basin, Arctic Ocean in 1988, 1992 and 1993</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Grantz, Arthur; Hart, Patrick E.; May, Steven D.</p> <p>2004-01-01</p> <p><span class="hlt">Seismic</span> reflection and refraction data were collected in generally ice-covered waters of the Canada Basin and the eastern part of the Chukchi Continental Borderland of the Amerasia Basin, Arctic Ocean, during the late summers of 1988, 1992, and 1993. The data were acquired from a Polar class icebreaker, the U.S. Coast Guard Cutter Polar Star, using a <span class="hlt">seismic</span> reflection system designed by the U.S. Geological Survey (USGS). The northernmost data extend to 78? 48' N latitude. In 1988, 155 km of reflection data were acquired with a prototype system consisting of a single 195 cubic inch air gun <span class="hlt">seismic</span> source and a two-channel hydrophone streamer with a 150-m active section. In 1992 and 1993, 500 and 1,900 km, respectively, of <span class="hlt">seismic</span> reflection profile data were acquired with an improved six air gun, 674 to 1303 cubic inch tuned <span class="hlt">seismic</span> source array and the same two-channel streamer. In 1993, a 12-channel streamer with a 150-m active section was used to <span class="hlt">record</span> five of the reflection lines and one line was acquired using a three air gun, 3,000 cubic inch source. All data were <span class="hlt">recorded</span> with a DFS-V digital <span class="hlt">seismic</span> <span class="hlt">recorder</span>. Processed sections feature high quality vertical incidence images to more than 6 km of sub-bottom penetration in the Canada Basin. Refraction data were acquired with U.S. Navy sonobuoys <span class="hlt">recorded</span> simultaneously with the <span class="hlt">seismic</span> reflection profiles. In 1988 eight refraction profiles were <span class="hlt">recorded</span> with the single air gun, and in 1992 and 1993 a total of 47 refraction profiles were <span class="hlt">recorded</span> with the six air gun array. The sonobuoy refraction <span class="hlt">records</span>, with offsets up to 35 km, provide acoustic velocity information to complement the short-offset reflection data. The report includes trackline maps showing the location of the data, as well as both digital data files (SEG-Y) and images of all of the profiles.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.P33D2909N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.P33D2909N"><span>High Resolution Vertical <span class="hlt">Seismic</span> Profile from the Chicxulub IODP/ICDP Expedition 364 Borehole: Wave Speeds and <span class="hlt">Seismic</span> Reflectivity.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Nixon, C.; Kofman, R.; Schmitt, D. R.; Lofi, J.; Gulick, S. P. S.; Christeson, G. L.; Saustrup, S., Sr.; Morgan, J. V.</p> <p>2017-12-01</p> <p>We acquired a closely-spaced vertical <span class="hlt">seismic</span> profile (VSP) in the Chicxulub K-Pg Impact Crater drilling program borehole to calibrate the existing surface <span class="hlt">seismic</span> profiles and provide complementary measurements of in situ <span class="hlt">seismic</span> wave speeds. Downhole <span class="hlt">seismic</span> <span class="hlt">records</span> were obtained at spacings ranging from 1.25 m to 5 m along the borehole from 47.5 m to 1325 mwsf (meters wireline below sea floor) (Fig 1a) using a Sercel SlimwaveTM geophone chain (University of Alberta). The <span class="hlt">seismic</span> source was a 30/30ci Sercel Mini GI airgun (University of Texas), fired a minimum of 5 times per station. <span class="hlt">Seismic</span> data processing used a combination of a commercial processing package (Schlumberger's VISTA) and MatlabTM codes. The VSP displays detailed reflectivity (Fig. 1a) with the strongest reflection seen at 600 mwsf (280 ms one-way time), geologically corresponding to the sharp contact between the post-impact sediments and the target peak ring rock, thus confirming the pre-drilling interpretations of the <span class="hlt">seismic</span> profiles. A two-way time trace extracted from the separated up-going wavefield matches the major reflection both in travel time and character. In the granitic rocks that form the peak ring of the Chicxulub impact crater, we observe P-wave velocities of 4000-4500 m/s which are significantly less than the expected values of granitoids ( 6000 m/s) (Fig. 1b). The VSP measured wave speeds are confirmed against downhole sonic logging and in laboratory velocimetry measurements; these data provide additional evidence that the crustal material displaced by the impact experienced a significant amount of damage. Samples and data provided by IODP. Samples can be requested at http://web.iodp.tamu.edu/sdrm after 19 October 2017. Expedition 364 was jointly funded by ECORD, ICDP, and IODP with contributions and logistical support from the Yucatan State Government and UNAM. The downhole <span class="hlt">seismic</span> chain and wireline system is funded by grants to DRS from the Canada Foundation for Innovation and</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li class="active"><span>22</span></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_22 --> <div id="page_23" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li class="active"><span>23</span></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li><a href="#" onclick='return showDiv("page_25");'>25</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="441"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018E%26ES..140a2101I','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018E%26ES..140a2101I"><span><span class="hlt">Seismic</span> performance for vertical geometric irregularity frame structures</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ismail, R.; Mahmud, N. A.; Ishak, I. S.</p> <p>2018-04-01</p> <p>This research highlights the result of vertical geometric irregularity frame structures. The aid of finite element analysis software, LUSAS was used to analyse <span class="hlt">seismic</span> performance by focusing particularly on type of irregular frame on the differences in height floors and continued in the middle of the building. Malaysia’s building structures were affected once the earthquake took place in the neighbouring country such as Indonesia (Sumatera Island). In Malaysia, concrete is widely used in building construction and limited tension resistance to prevent it. Analysing structural behavior with horizontal and vertical static load is commonly analyses by using the Plane Frame Analysis. The case study of this research is to determine the stress and displacement in the <span class="hlt">seismic</span> response under this type of irregular frame structures. This study is based on seven-storey building of Clinical Training Centre located in Sungai Buloh, Selayang, Selangor. Since the largest earthquake occurs in Acheh, Indonesia on December 26, 2004, the data was <span class="hlt">recorded</span> and used in conducting this research. The result of stress and displacement using IMPlus <span class="hlt">seismic</span> analysis in LUSAS Modeller Software under the <span class="hlt">seismic</span> response of a formwork frame system states that the building is safe to withstand the ground and in good condition under the variation of <span class="hlt">seismic</span> performance.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.P41D2859P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.P41D2859P"><span>A New Moonquake Catalog from Apollo 17 <span class="hlt">Seismic</span> Data II: Lunar Surface Gravimeter: Implications of Expanding the Passive <span class="hlt">Seismic</span> Array</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Phillips, D.; Dimech, J. L.; Weber, R. C.</p> <p>2017-12-01</p> <p>Apollo 17's Lunar Surface Gravimeter (LSG) was deployed on the Moon in 1972, and was originally intended to detect gravitational waves as a confirmation of Einstein's general theory of relativity. Due to a design problem, the instrument did not function as intended. However, remotely-issued reconfiguration commands permitted the instrument to act effectively as a passive seismometer. LSG <span class="hlt">recorded</span> continuously until Sept. 1977, when all surface data <span class="hlt">recording</span> was terminated. Because the instrument did not meet its primary science objective, little effort was made to archive the data. Most of it was eventually lost, with the exception of data spanning the period March 1976 until Sept. 1977, and a recent investigation demonstrated that LSG data do contain moonquake signals (Kawamura et al., 2015). The addition of useable <span class="hlt">seismic</span> data at the Apollo 17 site has important implications for event location schemes, which improve with increasing data coverage. All previous <span class="hlt">seismic</span> event location attempts were limited to the four stations deployed at the Apollo 12, 14, 15, and 16 sites. Apollo 17 extends the functional aperture of the <span class="hlt">seismic</span> array significantly to the east, permitting more accurate moonquake locations and improved probing of the lunar interior. Using the standard location technique of linearized arrival time inversion through a known velocity model, Kawamura et al. (2015) used moonquake signals detected in the LSG data to refine location estimates for 49 deep moonquake clusters, and constrained new locations for five previously un-located clusters. Recent efforts of the Apollo Lunar Surface Experiments Package Data Recovery Focus Group have recovered some of the previously lost LSG data, spanning the time period April 2, 1975 to June 30, 1975. In this study, we expand Kawamura's analysis to the newly recovered data, which contain over 200 known <span class="hlt">seismic</span> signals, including deep moonquakes, shallow moonquakes, and meteorite impacts. We have completed initial</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.S41B0772N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.S41B0772N"><span>Empirical Ground Motion Characterization of Induced <span class="hlt">Seismicity</span> in Alberta and Oklahoma</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Novakovic, M.; Atkinson, G. M.; Assatourians, K.</p> <p>2017-12-01</p> <p>We develop empirical ground-motion prediction equations (GMPEs) for ground motions from induced earthquakes in Alberta and Oklahoma following the stochastic-model-based method of Atkinson et al. (2015 BSSA). The Oklahoma ground-motion database is compiled from over 13,000 small to moderate <span class="hlt">seismic</span> events (M 1 to 5.8) <span class="hlt">recorded</span> at 1600 <span class="hlt">seismic</span> stations, at distances from 1 to 750 km. The Alberta database is compiled from over 200 small to moderate <span class="hlt">seismic</span> events (M 1 to 4.2) <span class="hlt">recorded</span> at 50 regional stations, at distances from 30 to 500 km. A generalized inversion is used to solve for regional source, attenuation and site parameters. The obtained parameters describe the regional attenuation, stress parameter and site amplification. Resolving these parameters allows for the derivation of regionally-calibrated GMPEs that can be used to compare ground motion observations between waste water injection (Oklahoma) and hydraulic fracture induced events (Alberta), and further compare induced observations with ground motions resulting from natural sources (California, NGAWest2). The derived GMPEs have applications for the evaluation of hazards from induced <span class="hlt">seismicity</span> and can be used to track amplitudes across the regions in real time, which is useful for ground-motion-based alerting systems and traffic light protocols.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012GeoJI.190.1607S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012GeoJI.190.1607S"><span>Modelling strong <span class="hlt">seismic</span> ground motion: three-dimensional loading path versus wavefield polarization</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Santisi d'Avila, Maria Paola; Lenti, Luca; Semblat, Jean-François</p> <p>2012-09-01</p> <p><span class="hlt">Seismic</span> waves due to strong earthquakes propagating in surficial soil layers may both reduce soil stiffness and increase the energy dissipation into the soil. To investigate <span class="hlt">seismic</span> wave amplification in such cases, past studies have been devoted to one-directional shear wave propagation in a soil column (1D-propagation) considering one motion component only (1<span class="hlt">C</span>-polarization). Three independent purely 1<span class="hlt">C</span> computations may be performed ('1D-1<span class="hlt">C</span>' approach) and directly superimposed in the case of weak motions (linear behaviour). This research aims at studying local site effects by considering <span class="hlt">seismic</span> wave propagation in a 1-D soil profile accounting for the influence of the 3-D loading path and non-linear hysteretic behaviour of the soil. In the proposed '1D-3<span class="hlt">C</span>' approach, the three components (3<span class="hlt">C</span>-polarization) of the incident wave are simultaneously propagated into a horizontal multilayered soil. A 3-D non-linear constitutive relation for the soil is implemented in the framework of the Finite Element Method in the time domain. The complex rheology of soils is modelled by mean of a multisurface cyclic plasticity model of the Masing-Prandtl-Ishlinskii-Iwan type. The great advantage of this choice is that the only data needed to describe the model is the modulus reduction curve. A parametric study is carried out to characterize the changes in the <span class="hlt">seismic</span> motion of the surficial layers due to both incident wavefield properties and soil non-linearities. The numerical simulations show a <span class="hlt">seismic</span> response depending on several parameters such as polarization of <span class="hlt">seismic</span> waves, material elastic and dynamic properties, as well as on the impedance contrast between layers and frequency content and oscillatory character of the input motion. The 3-D loading path due to the 3<span class="hlt">C</span>-polarization leads to multi-axial stress interaction that reduces soil strength and increases non-linear effects. The non-linear behaviour of the soil may have beneficial or detrimental effects on the <span class="hlt">seismic</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFMNG33B3840T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFMNG33B3840T"><span>Statistical Seismology and Induced <span class="hlt">Seismicity</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tiampo, K. F.; González, P. J.; Kazemian, J.</p> <p>2014-12-01</p> <p>While <span class="hlt">seismicity</span> triggered or induced by natural resources production such as mining or water impoundment in large dams has long been recognized, the recent increase in the unconventional production of oil and gas has been linked to rapid rise in <span class="hlt">seismicity</span> in many places, including central North America (Ellsworth et al., 2012; Ellsworth, 2013). Worldwide, induced events of M~5 have occurred and, although rare, have resulted in both damage and public concern (Horton, 2012; Keranen et al., 2013). In addition, over the past twenty years, the increase in both number and coverage of <span class="hlt">seismic</span> stations has resulted in an unprecedented ability to precisely <span class="hlt">record</span> the magnitude and location of large numbers of small magnitude events. The increase in the number and type of <span class="hlt">seismic</span> sequences available for detailed study has revealed differences in their statistics that previously difficult to quantify. For example, <span class="hlt">seismic</span> swarms that produce significant numbers of foreshocks as well as aftershocks have been observed in different tectonic settings, including California, Iceland, and the East Pacific Rise (McGuire et al., 2005; Shearer, 2012; Kazemian et al., 2014). Similarly, smaller events have been observed prior to larger induced events in several occurrences from energy production. The field of statistical seismology has long focused on the question of triggering and the mechanisms responsible (Stein et al., 1992; Hill et al., 1993; Steacy et al., 2005; Parsons, 2005; Main et al., 2006). For example, in most cases the associated stress perturbations are much smaller than the earthquake stress drop, suggesting an inherent sensitivity to relatively small stress changes (Nalbant et al., 2005). Induced <span class="hlt">seismicity</span> provides the opportunity to investigate triggering and, in particular, the differences between long- and short-range triggering. Here we investigate the statistics of induced <span class="hlt">seismicity</span> sequences from around the world, including central North America and Spain, and</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010AGUFMNS41B1510L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010AGUFMNS41B1510L"><span>Three-Dimensional <span class="hlt">Seismic</span> Image of a Geothermal Prospect: Tinguiririca, Central Andes, Chile</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lira, E.; Comte, D.; Giavelli, A.; Clavero, J. E.; Pineda, G.</p> <p>2010-12-01</p> <p><span class="hlt">Seismic</span> monitoring has been widely used by the oil and gas industry, as a valuable input for the reservoir characterization. This tool has also been used in geothermal productive systems, particularly to understand permeability controls usually associated to shallow crustal fault systems that are <span class="hlt">seismically</span> actives. Faults can be considered either “migration path” or “seals” in Petroleum Systems, depending on their activity story (they are carriers while actives and seals when the activity cease due to diagenetic processes in the fault plain). On the other hand, is well known that <span class="hlt">seismic</span> velocities are strongly related to rock properties, in particular Vp/Vs and VpVs relationship has been successfully used to emphasize the variations in the physical rock properties due to fluid content and porosity. In geothermal systems, P and S-wave velocities are expected to be noticeably affected by massive hydrothermal alteration and/or to the presence of hot water in the fault related fractures of the rocks. In this job, the results of three months of <span class="hlt">seismic</span> monitoring and a <span class="hlt">seismic</span> velocity tomography are presented. Sixteen short period continuous <span class="hlt">recording</span>, three components <span class="hlt">seismic</span> stations were deployed in an area of approximately 20x10 Km2, and a large 8.8 magnitude earthquake took place during the <span class="hlt">recording</span> period. The study area corresponds to the Tinguiririca volcanic complex (70°21''W, 35°48''S), in the high mountain of the Central Andes near the Chile-Argentina border. These preliminary results are complemented with some MT profiles, delineating potentially interesting geothermal features.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011AGUFM.S32A..06R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011AGUFM.S32A..06R"><span>Data-Intensive Discovery Methods for <span class="hlt">Seismic</span> Monitoring</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Richards, P. G.; Schaff, D. P.; Young, C. J.; Slinkard, M.; Heck, S.; Ammon, C. J.; Cleveland, M.</p> <p>2011-12-01</p> <p>For most regions of our planet, earthquakes and explosions are still located one-at-a-time using <span class="hlt">seismic</span> phase picks-a procedure that has not fundamentally changed for more than a century. But methods that recognize and use seismogram archives as a major resource, enabling comparisons of waveforms <span class="hlt">recorded</span> from neighboring events and relocating numerous events relative to each other, have been successfully demonstrated, especially for California, where they have enabled new insights into earthquake physics and Earth structure, and have raised <span class="hlt">seismic</span> monitoring to new levels. We are beginning a series of projects to evaluate such data-intensive methods on ever-larger scales, using cross correlation (CC) to analyze <span class="hlt">seismicity</span> in three different ways: (1) to find repeating earthquakes (whose waveforms are very similar, so the CC value measured over long windows must be high); (2) to measure time differences and amplitude differences to enable precise relocations and relative amplitude studies, of <span class="hlt">seismic</span> events with respect to their neighboring events (then CC can be much lower, yet still give a better estimate of arrival time differences and relative amplitudes, compared to differencing phase picks and magnitudes); and, perhaps most importantly, (3) as a detector, to find new events in current data streams that are similar to events already in the archive, or to add to the number of detections of an already known event. Experience documented by Schaff and Waldhauser (2005) for California and Schaff (2009) for China indicates that the great majority of events in <span class="hlt">seismically</span> active regions generate waveforms that are sufficiently similar to the waveforms of neighboring events to allow CC methods to be used to obtain relative locations. Schaff (2008, 2010) has demonstrated the capability of CC methods to achieve detections, with minimal false alarms, down to more than a magnitude unit below conventional STA/LTA detectors though CC methods are far more computationally</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014E%26PSL.403..432M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014E%26PSL.403..432M"><span>Snap, Crackle, Pop: Dilational fault breccias <span class="hlt">record</span> <span class="hlt">seismic</span> slip below the brittle-plastic transition</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Melosh, Ben L.; Rowe, Christie D.; Smit, Louis; Groenewald, Conrad; Lambert, Christopher W.; Macey, Paul</p> <p>2014-10-01</p> <p>Off-fault dynamic tensile cracks form behind an earthquake rupture front with distinct orientation and spacing. These cracks explode the wall rock and create breccias, which we hypothesize will preserve a unique fingerprint of dynamic rupture. Identification of these characteristic breccias may enable a new tool for identifying paleoseismic slip surfaces in the rock <span class="hlt">record</span>. Using previous experimental and theoretical predictions, we develop a field-based model of dynamic dilational breccia formation. Experimental studies find that secondary tensile fracture networks comprise closely spaced fractures at angles of 70-90° from a slip surface, as well as fractures that branch at angles of ∼ 30 ° from a primary mode I fracture. The Pofadder Shear Zone, in Namibia and South Africa, preserves breccias formed in the brittle-ductile transition zone displaying fracture patterns consistent with those described above. Fracture spacing is approximately two orders of magnitude less than predicted by quasi-static models. Breccias are clast-supported, monomict and can display an abrupt transition from fracture network crackle breccia to mosaic breccia textures. Brecciation occurs by the intersection of off-fault dynamic fractures and wall rock fabric; this is in contrast to previous models of fluid pressure gradient-driven failure ;implosion breccias;. This mechanism tends to form many similar sized clasts with particle size distributions that may not display self-similarity; where self-similarity is observed the distributions have relatively low D-values of 1.47 ± 0.37, similar to other studies of dynamic processes. We measure slip distances at dilational breccia stepovers, estimating earthquake magnitudes between Mw 2.8-5.8 and associated rupture lengths of 0.023-3.3 km. The small calculated rupture dimensions, in combination with our geologic observations, suggest that some earthquakes nucleated within the quartz-plastic transitional zone and potentially <span class="hlt">record</span> deep</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUSM.S52A..06C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUSM.S52A..06C"><span>Historical <span class="hlt">Seismicity</span> of Central Panama</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Camacho, E.</p> <p>2013-05-01</p> <p>Central Panama lies in the Panama microplate, neighboring <span class="hlt">seismically</span> active regions of Costa Rica and Colombia. This region, crossed by the Panama Canal, concentrates most of the population and economic activity of the Republic of Panama. Instrumental observation of earthquakes in Panama began on 1882 by the Compagnie Universelle du Canal Interocéanique de Panama and continued from 1904 to 1977 by the Panama Canal Company. From October 1997 to March 1998 the USGS deployed a temporary digital <span class="hlt">seismic</span> network. Since 2003 this region is monitored by a digital <span class="hlt">seismic</span> network operated by the Panama Canal Authority and I complemented by the broad band stations of the University of Panama <span class="hlt">seismic</span> network. The <span class="hlt">seismicity</span> in this region is very diffuse and the few events which are <span class="hlt">recorded</span> have magnitudes less than 3.0. Historical archives and antique newspapers from Spain, Colombia, Panama and the United Sates have been searched looking for historical earthquake information which could provide a better estimate of the <span class="hlt">seismicity</span> in this region. We find that Panama City has been shaken by two destructive earthquakes in historical times. One by a local fault (i.e. Pedro Miguel fault) on May 2, 1621 (I=Vlll MM), and a subduction event from the North Panama Deformed Belt (NPDB) on September 7, 1882 (I=Vll MM). To test these findings two earthquakes scenarios were generated, using SELENA, for Panama City Old Quarter. Panama City was rebuilt on January 21, 1673, on a rocky point facing the Pacific Ocean after the sack by pirate Morgan on January 28, 1671. The pattern of damage to calicanto (unreinforced colonial masonry) and wood structures for a crustal local event are higher than those for an event from the NPDB and seem to confirm that the city has not been shaken by a major local event since May 2, 1621 and a subduction event since September 7, 1882</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015NHESS..15.1265H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015NHESS..15.1265H"><span>Dynamics of the Oso-Steelhead landslide from broadband <span class="hlt">seismic</span> analysis</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hibert, C.; Stark, C. P.; Ekström, G.</p> <p>2015-06-01</p> <p>We carry out a combined analysis of the short- and long-period <span class="hlt">seismic</span> signals generated by the devastating Oso-Steelhead landslide that occurred on 22 March 2014. The <span class="hlt">seismic</span> <span class="hlt">records</span> show that the Oso-Steelhead landslide was not a single slope failure, but a succession of multiple failures distinguished by two major collapses that occurred approximately 3 min apart. The first generated long-period surface waves that were <span class="hlt">recorded</span> at several proximal stations. We invert these long-period signals for the forces acting at the source, and obtain estimates of the first failure runout and kinematics, as well as its mass after calibration against the mass-centre displacement estimated from remote-sensing imagery. Short-period analysis of both events suggests that the source dynamics of the second event is more complex than the first. No distinct long-period surface waves were <span class="hlt">recorded</span> for the second failure, which prevents inversion for its source parameters. However, by comparing the <span class="hlt">seismic</span> energy of the short-period waves generated by both events we are able to estimate the volume of the second. Our analysis suggests that the volume of the second failure is about 15-30% of the total landslide volume, giving a total volume mobilized by the two events between 7 × 106 and 10 × 106 m3, in agreement with estimates from ground observations and lidar mapping.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015EGUGA..17.3354M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015EGUGA..17.3354M"><span>An Open Hardware <span class="hlt">seismic</span> data <span class="hlt">recorder</span> - a solid basis for citizen science</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mertl, Stefan</p> <p>2015-04-01</p> <p>"Ruwai" is a 24-Bit Open Hardware <span class="hlt">seismic</span> data <span class="hlt">recorder</span>. It is built up of four stackable printed circuit boards fitting the Arduino Mega 2560 microcontroller prototyping platform. An interface to the BeagleBone Black single-board computer enables extensive data storage, -processing and networking capabilities. The four printed circuit boards provide a uBlox Lea-6T GPS module and real-time clock (GPS Timing shield), an Texas Instruments ADS1274 24-Bit analog to digital converter (ADC main shield), an analog input section with a Texas Instruments PGA281 programmable gain amplifier and an analog anti-aliasing filter (ADC analog interface pga) and the power conditioning based on 9-36V DC input (power supply shield). The Arduino Mega 2560 is used for controlling the hardware components, timestamping sampled data using the GPS timing information and transmitting the data to the BeagleBone Black single-board computer. The BeagleBone Black provides local data storage, wireless mesh networking using the optimized link state routing daemon and differential GNSS positioning using the RTKLIB software. The complete hardware and software is published under free software - or open hardware licenses and only free software (e.g. KiCad) was used for the development to facilitate the reusability of the design and increases the sustainability of the project. "Ruwai" was developed within the framework of the "Community Environmental Observation Network (CEON)" (http://www.mertl-research.at/ceon/) which was supported by the Internet Foundation Austria (IPA) within the NetIdee 2013 call.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFM.S33A2750H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFM.S33A2750H"><span>How a Country-Wide Seismological Network Can Improve Understanding of <span class="hlt">Seismicity</span> and <span class="hlt">Seismic</span> Hazard -- The Example of Bhutan</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hetényi, G.; Diehl, T.; Singer, J.; Kissling, E. H.; Clinton, J. F.; Wiemer, S.</p> <p>2015-12-01</p> <p>The Eastern Himalayas are home to a seemingly complex seismo-tectonic evolution. The rate of instrumental <span class="hlt">seismicity</span> is lower than the average along the orogen, there is no <span class="hlt">record</span> of large historical events, but both paleoseismology and GPS studies point to potentially large (M>8) earthquakes. Due to the lack of a permanent <span class="hlt">seismic</span> monitoring system in the area, our current level of understanding is inappropriate to create a reliable quantitative <span class="hlt">seismic</span> hazard model for the region. Existing maps are based on questionable hypotheses and show major inconsistencies when compared to each other. Here we present results on national and regional scales from a 38-station broadband seismological network we operated for almost 2 years in the Kingdom of Bhutan. A thorough, state-of-the-art analysis of local and regional earthquakes builds a comprehensive catalogue that reveals significantly (2-to-3 orders of magnitude) more events than detected from global networks. The seismotectonic analysis reveals new patterns of <span class="hlt">seismic</span> activity as well as striking differences over relatively short distances within the Himalayas, only partly explained by surface observations such as geology. We compare a priori and a posteriori (BMC) magnitude of completeness maps and show that our network was able to detect all felt events during its operation. Some of these events could be felt at surprisingly large distances. Based on our experiment and experience, we draft the pillars on which a permanent seismological observatory for Bhutan could be constructed. Such a continuous monitoring system of <span class="hlt">seismic</span> activity could then lead to a reliable quantitative <span class="hlt">seismic</span> hazard model for Bhutan and surrounding regions, and serve as a base to improve building codes and general preparedness.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015EGUGA..1711140S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015EGUGA..1711140S"><span>Geochemical variations during the 2012 Emilia <span class="hlt">seismic</span> sequence</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sciarra, Alessandra; Cantucci, Barbara; Galli, Gianfranco; Cinti, Daniele; Pizzino, Luca</p> <p>2015-04-01</p> <p>Several geochemical surveys (soil gas and shallow water) were performed in the Modena province (Massa Finalese, Finale Emilia, Medolla and S. Felice sul Panaro), during 2006-2014 period. In May-June 2012, a <span class="hlt">seismic</span> sequence (main shocks of ML 5.9 and 5.8) was occurred closely to the investigated area. In this area 300 CO2 and CH4 fluxes measurements, 150 soil gas concentrations (He, H2, CO2, CH4 and <span class="hlt">C</span>2H6), 30 shallow waters and their isotopic analyses (δ13<span class="hlt">C</span>- CH4, δD- CH4 and δ13<span class="hlt">C</span>- CO2) were performed in April-May 2006, October and December 2008, repeated in May and September 2012, June 2013 and July 2014 afterwards the 2012 Emilia <span class="hlt">seismic</span> sequences. Chemical composition of soil gas are dominated by CH4 in the southern part by CO2 in the northern part. Very anomalous fluxes and concentrations are <span class="hlt">recorded</span> in spot areas; elsewhere CO2 and CH4 values are very low, within the typical range of vegetative and of organic exhalation of the cultivated soil. After the <span class="hlt">seismic</span> sequence the CH4 and CO2 fluxes are increased of one order of magnitude in the spotty areas, whereas in the surrounding area the values are within the background. On the contrary, CH4 concentration decrease (40%v/v in the 2012 surveys) and CO2 concentration increase until to 12.7%v/v (2013 survey). Isotopic gas analysis were carried out only on samples with anomalous values. Pre-<span class="hlt">seismic</span> data hint a thermogenic origin of CH4 probably linked to leakage from a deep source in the Medolla area. Conversely, 2012/2013 isotopic data indicate a typical biogenic origin (i.e. microbial hydrocarbon production) of the CH4, as recognized elsewhere in the Po Plain and surroundings. The δ13<span class="hlt">C</span>-CO2 value suggests a prevalent shallow origin of CO2 (i.e. organic and/or soil-derived) probably related to anaerobic oxidation of heavy hydrocarbons. Water samples, collected from domestic, industrial and hydrocarbons exploration wells, allowed us to recognize different families of waters. Waters are meteoric in origin and</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.S31B0811F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.S31B0811F"><span>A <span class="hlt">seismic</span> hazard overview of the Mitidja Basin (Northern Algeria)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Fontiela, J. F.; Borges, J.; Ouyed, M.; Bezzeghoud, M.; Idres, M.; Caldeira, B.; Boughacha, M. S.; Carvalho, J.; Samai, S.; Aissa, S.; Benfadda, A.; Chimouni, R.; Yalaoui, R.; Dias, R.</p> <p>2017-12-01</p> <p>The Mitidja Basin (MB) is located in N Algeria and it is filled by quaternary sediments with a length of 100 km on the EW direction and around 20 km width. The S and N limites comprise the Boumerdes-Larbaa-Blida, and the Thenia-Sahel active fault system, respectively. Both fault systems are of the reverse type with opposed dips and accommodate a general slip rate of ˜4 mm/year. In the basin occurred earthquakes that caused severe damage and losses such as the ones of Algiers (1365, Io=X; 1716, Io=X) and the Bourmedes earthquake (Mw 6.9; May 2003) that affected the area of Zemmouri and caused 2.271 deaths. The event was caused by the reactivation of the MB boundary faults. The earthquake generated a max uplift of 0.8m along the coast and a horizontal max. slip of 0.24m.Recent studies show that the Boumerdes earthquake overloaded the adjacent faults system with a stress increase between 0.4 and 1.5 bar. The stress change recommends a detailed study of mentioned faults system due to the increase of the <span class="hlt">seismic</span> hazard. The high seismogenic potential of the fault system bordering the MB, increases the vulnerability of densely populated areas of Algiers and the amplification effect caused by the basin are the motivation of this project that will focus on the evaluation of the <span class="hlt">seismic</span> hazard of the region. To achieve <span class="hlt">seismic</span> hazard assessment on the MB, through realistic predictions of strong ground motion, caused by moderate and large earthquakes, it is important 1) develop a detailed 3D velocity/structure model of the MB that includes geological constraints, <span class="hlt">seismic</span> reflection data acquired on wells, refraction velocities and <span class="hlt">seismic</span> noise data, and determination of the attenuation laws based on instrumental <span class="hlt">records</span>; 2) evaluate the <span class="hlt">seismic</span> potential and parameters of the main active faults of the MB; 3) develop numerical methods (deterministic and stochastic) to simulate strong ground motions produced by extended <span class="hlt">seismic</span> sources. To acquire <span class="hlt">seismic</span> noise were used</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007AGUFM.U23C1448A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007AGUFM.U23C1448A"><span>50 years of Global <span class="hlt">Seismic</span> Observations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Anderson, K. R.; Butler, R.; Berger, J.; Davis, P.; Derr, J.; Gee, L.; Hutt, C. R.; Leith, W. S.; Park, J. J.</p> <p>2007-12-01</p> <p>Seismological <span class="hlt">recordings</span> have been made on Earth for hundreds of years in some form or another, however, global monitoring of earthquakes only began in the 1890's when John Milne created 40 <span class="hlt">seismic</span> observatories to measure the waves from these events. Shortly after the International Geophysical Year (IGY), a concerted effort was made to establish and maintain a more modern standardized <span class="hlt">seismic</span> network on the global scale. In the early 1960's, the World-Wide Standardized Seismograph Network (WWSSN) was established through funding from the Advanced Research Projects Agency (ARPA) and was installed and maintained by the USGS's Albuquerque Seismological Laboratory (then a part of the US Coast and Geodetic Survey). This network of identical <span class="hlt">seismic</span> instruments consisted of 120 stations in 60 countries. Although the network was motivated by nuclear test monitoring, the WWSSN facilitated numerous advances in observational seismology. From the IGY to the present, the network has been upgraded (High-Gain Long-Period Seismograph Network, <span class="hlt">Seismic</span> Research Observatories, Digital WWSSN, Global Telemetered Seismograph Network, etc.) and expanded (International Deployment of Accelerometers, US National <span class="hlt">Seismic</span> Network, China Digital Seismograph Network, Joint <span class="hlt">Seismic</span> Project, etc.), bringing the modern day Global Seismographic Network (GSN) to a current state of approximately 150 stations. The GSN consists of state-of-the-art very broadband <span class="hlt">seismic</span> transducers, continuous power and communications, and ancillary sensors including geodetic, geomagnetic, microbarographic, meteorological and other related instrumentation. Beyond the GSN, the system of global network observatories includes contributions from other international partners (e.g., GEOSCOPE, GEOFON, MEDNET, F-Net, CTBTO), forming an even larger backbone of permanent seismological observatories as a part of the International Federation of Digital Seismograph Networks. 50 years of <span class="hlt">seismic</span> network operations have provided</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFM.S41B4466P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFM.S41B4466P"><span>Small Arrays for <span class="hlt">Seismic</span> Intruder Detections: A Simulation Based Experiment</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pitarka, A.</p> <p>2014-12-01</p> <p><span class="hlt">Seismic</span> sensors such as geophones and fiber optic have been increasingly recognized as promising technologies for intelligence surveillance, including intruder detection and perimeter defense systems. Geophone arrays have the capability to provide cost effective intruder detection in protecting assets with large perimeters. A <span class="hlt">seismic</span> intruder detection system uses one or multiple arrays of geophones design to <span class="hlt">record</span> <span class="hlt">seismic</span> signals from footsteps and ground vehicles. Using a series of real-time signal processing algorithms the system detects, classify and monitors the intruder's movement. We have carried out numerical experiments to demonstrate the capability of a <span class="hlt">seismic</span> array to detect moving targets that generate <span class="hlt">seismic</span> signals. The <span class="hlt">seismic</span> source is modeled as a vertical force acting on the ground that generates continuous impulsive <span class="hlt">seismic</span> signals with different predominant frequencies. Frequency-wave number analysis of the synthetic array data was used to demonstrate the array's capability at accurately determining intruder's movement direction. The performance of the array was also analyzed in detecting two or more objects moving at the same time. One of the drawbacks of using a single array system is its inefficiency at detecting <span class="hlt">seismic</span> signals deflected by large underground objects. We will show simulation results of the effect of an underground concrete block at shielding the <span class="hlt">seismic</span> signal coming from an intruder. Based on simulations we found that multiple small arrays can greatly improve the system's detection capability in the presence of underground structures. This work was performed under the auspices of the U.S. Department of Energy by Lawrence Livermore National Laboratory under Contract DE-AC52-07NA27344</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUFM.S43A2475L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUFM.S43A2475L"><span>The Great Maule earthquake: <span class="hlt">seismicity</span> prior to and after the main shock from amphibious <span class="hlt">seismic</span> networks</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lieser, K.; Arroyo, I. G.; Grevemeyer, I.; Flueh, E. R.; Lange, D.; Tilmann, F. J.</p> <p>2013-12-01</p> <p>The Chilean subduction zone is among the <span class="hlt">seismically</span> most active plate boundaries in the world and its coastal ranges suffer from a magnitude 8 or larger megathrust earthquake every 10-20 years. The Constitución-Concepción or Maule segment in central Chile between ~35.5°S and 37°S was considered to be a mature <span class="hlt">seismic</span> gap, rupturing last in 1835 and being <span class="hlt">seismically</span> quiet without any magnitude 4.5 or larger earthquakes reported in global catalogues. It is located to the north of the nucleation area of the 1960 magnitude 9.5 Valdivia earthquake and to the south of the 1928 magnitude 8 Talca earthquake. On 27 February 2010 this segment ruptured in a Mw=8.8 earthquake, nucleating near 36°S and affecting a 500-600 km long segment of the margin between 34°S and 38.5°S. Aftershocks occurred along a roughly 600 km long portion of the central Chilean margin, most of them offshore. Therefore, a network of 30 ocean-bottom-seismometers was deployed in the northern portion of the rupture area for a three month period, <span class="hlt">recording</span> local offshore aftershocks between 20 September 2010 and 25 December 2010. In addition, data of a network consisting of 33 landstations of the GeoForschungsZentrum Potsdam were included into the network, providing an ideal coverage of both the rupture plane and areas affected by post-<span class="hlt">seismic</span> slip as deduced from geodetic data. Aftershock locations are based on automatically detected P wave onsets and a 2.5D velocity model of the combined on- and offshore network. Aftershock <span class="hlt">seismicity</span> analysis in the northern part of the survey area reveals a well resolved <span class="hlt">seismically</span> active splay fault in the accretionary prism of the Chilean forearc. Our findings imply that in the northernmost part of the rupture zone, co-<span class="hlt">seismic</span> slip most likely propagated along the splay fault and not the subduction thrust fault. In addition, the updip limit of aftershocks along the plate interface can be verified to about 40 km landwards from the deformation front. Prior to</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..19.5937B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..19.5937B"><span>Orienting Ocean Bottom <span class="hlt">Seismic</span> Sensors from Ship Noise Polarization Analysis</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Barruol, Guilhem; Dreo, Richard; Fontaine, Fabrice R.; Scholz, John R.; Sigloch, Karin; Geay, Bruno; Bouillon, Alexandre</p> <p>2017-04-01</p> <p>For the RHUM-RUM project (Réunion Hotspot and Upper Mantle - Réunions Unterer Mantel, www.rhum-rum.net), a network of 57 ocean-bottom seismometers (OBS) was installed on the ocean floor around La Réunion Island in the SW Indian Ocean. Part of the network happened to be located beneath a route of heavy ship traffic connecting SE-Asia and the South-Atlantic region. We analysed the ship noise <span class="hlt">recorded</span> on the OBS and show that it can be used for determining the horizontal orientations of the <span class="hlt">seismic</span> instruments as they were <span class="hlt">recording</span> on the ocean floor. The OBS, provided by the German DEPAS and the French INSU OBS national pools, were equipped with wide-band or broad-band three-components <span class="hlt">seismic</span> and hydro-acoustic sensors. They were deployed in Nov. 2012 by R/V Marion Dufresne and recovered by R/V Meteor one year later. Depending on the configuration, the OBS <span class="hlt">recorded</span> for 8 to 13 months. By combining the trajectories of passing ships - provided by AIS (Automatic Identification system) GPS data - with our geophysical data <span class="hlt">recorded</span> on the ocean floor, we show that both hydro-acoustic and <span class="hlt">seismic</span> spectral analyses exhibit clear signals associated with vessels between 1 and 50 Hz, in the high-frequency range of our instruments. Large cargo vessels are detected several hours before and after their closest point of approach (CPA) and show clear Doppler effects which put quantitative constraints on their distances and speeds. By analysing the continuous noise polarization on the three <span class="hlt">seismic</span> components, we show that the polarization of the noise emitted by ships passing in the neighbourhood of an ocean-bottom seismometer can be used for retrieving the orientation of the OBS horizontal components on the ocean floor with respect to the geographic reference frame. We find good agreement between OBS orientations thus calculated from ship noise and the OBS orientations determined independently from teleseismic body and surface wave polarization methods (Scholz et al., GJI</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009AGUFM.U51C0028W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009AGUFM.U51C0028W"><span>EMERALD: Coping with the Explosion of <span class="hlt">Seismic</span> Data</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>West, J. D.; Fouch, M. J.; Arrowsmith, R.</p> <p>2009-12-01</p> <p>, extensible, standalone database server system based on the open-source PostgreSQL database engine. The system is designed for fast and easy processing of <span class="hlt">seismic</span> datasets, and provides the necessary tools to manage very large datasets and all associated metadata. EMERALD provides methods for efficient preprocessing of <span class="hlt">seismic</span> <span class="hlt">records</span>; large <span class="hlt">record</span> sets can be easily and quickly searched, reviewed, revised, reprocessed, and exported. EMERALD can retrieve and store station metadata and alert the user to metadata changes. The system provides many methods for visualizing data, analyzing dataset statistics, and tracking the processing history of individual datasets. EMERALD allows development and sharing of visualization and processing methods using any of 12 programming languages. EMERALD is designed to integrate existing software tools; the system provides wrapper functionality for existing widely-used programs such as GMT, SOD, and TauP. Users can interact with EMERALD via a web browser interface, or they can directly access their data from a variety of database-enabled external tools. Data can be imported and exported from the system in a variety of file formats, or can be directly requested and downloaded from the IRIS DMC from within EMERALD.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JGRB..122.3916P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JGRB..122.3916P"><span>Accurate estimation of <span class="hlt">seismic</span> source parameters of induced <span class="hlt">seismicity</span> by a combined approach of generalized inversion and genetic algorithm: Application to The Geysers geothermal area, California</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Picozzi, M.; Oth, A.; Parolai, S.; Bindi, D.; De Landro, G.; Amoroso, O.</p> <p>2017-05-01</p> <p>The accurate determination of stress drop, <span class="hlt">seismic</span> efficiency, and how source parameters scale with earthquake size is an important issue for <span class="hlt">seismic</span> hazard assessment of induced <span class="hlt">seismicity</span>. We propose an improved nonparametric, data-driven strategy suitable for monitoring induced <span class="hlt">seismicity</span>, which combines the generalized inversion technique together with genetic algorithms. In the first step of the analysis the generalized inversion technique allows for an effective correction of waveforms for attenuation and site contributions. Then, the retrieved source spectra are inverted by a nonlinear sensitivity-driven inversion scheme that allows accurate estimation of source parameters. We therefore investigate the earthquake source characteristics of 633 induced earthquakes (Mw 2-3.8) <span class="hlt">recorded</span> at The Geysers geothermal field (California) by a dense <span class="hlt">seismic</span> network (i.e., 32 stations, more than 17.000 velocity <span class="hlt">records</span>). We find a nonself-similar behavior, empirical source spectra that require an ωγ source model with γ > 2 to be well fit and small radiation efficiency ηSW. All these findings suggest different dynamic rupture processes for smaller and larger earthquakes and that the proportion of high-frequency energy radiation and the amount of energy required to overcome the friction or for the creation of new fractures surface changes with earthquake size. Furthermore, we observe also two distinct families of events with peculiar source parameters that in one case suggests the reactivation of deep structures linked to the regional tectonics, while in the other supports the idea of an important role of steeply dipping faults in the fluid pressure diffusion.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li class="active"><span>23</span></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li><a href="#" onclick='return showDiv("page_25");'>25</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_23 --> <div id="page_24" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li class="active"><span>24</span></li> <li><a href="#" onclick='return showDiv("page_25");'>25</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="461"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.T51D0516B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.T51D0516B"><span>Gravity and <span class="hlt">Seismic</span> Investigations of the Northern Rio Grande Rift Area, New Mexico</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Braile, L. W.; Deepak, A.; Helprin, O.; Kondas, S.; Maguire, H.; McCallister, B.; Orubu, A.; Rijfkogel, L.; Schumann, H.; Vannette, M.; Wanpiyarat, N.; Carchedi, C.; Ferguson, J. F.; McPhee, D.; Biehler, S.; Ralston, M. D.; Baldridge, W. S.</p> <p>2017-12-01</p> <p>Participants in the Summer of Applied Geophysical Experience (SAGE, a research and education program in applied geophysics for undergraduate and graduate students) program have studied the northern Rio Grande rift (RGR) area of New Mexico for the past thirty-five years. In recent years, the SAGE program has focused on the western edge of the Española basin and the transition into the Santo Domingo basin and the Valles caldera. During this time, we have collected about 50 km of <span class="hlt">seismic</span> reflection and refraction data along approximately East-West profiles using a 120 channel data acquisition system with a 20 m station interval and a Vibroseis source. We also have access to several energy-industry <span class="hlt">seismic</span> reflection <span class="hlt">record</span> sections from the 1970s in the study area. During SAGE 2017, new gravity measurements north of the Jemez Mountains and a <span class="hlt">seismic</span> reflection profile (Rio de Truchas Profile) in the Valarde graben adjacent to the eastern boundary of the RGR have added new constraints to a west-to-east transect in area of the northern RGR. The <span class="hlt">recorded</span> near-vertical and wide-angle <span class="hlt">seismic</span> refection data were processed to produce a CMP (common midpoint) stacked <span class="hlt">record</span> section. Bandpass filtering, muting, deconvolution, and F-K velocity filtering were found to be effective in enhancing the <span class="hlt">seismic</span> reflections. Modeling and interpretation of the northern RGR west-to-east geophysical profile indicates that the sedimentary rock fill in the Velarde graben is at least 3 km near the center of the graben. Gravity modeling also suggests the presence of a high-density intrusion at the top of the crystalline basement in an area to the north and west of Abiquiu, NM.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26289598','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26289598"><span><span class="hlt">Seismic</span> monitoring in the oceans by autonomous floats.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Sukhovich, Alexey; Bonnieux, Sébastien; Hello, Yann; Irisson, Jean-Olivier; Simons, Frederik J; Nolet, Guust</p> <p>2015-08-20</p> <p>Our understanding of the internal dynamics of the Earth is largely based on images of <span class="hlt">seismic</span> velocity variations in the mantle obtained with global tomography. However, our ability to image the mantle is severely hampered by a lack of <span class="hlt">seismic</span> data collected in marine areas. Here we report observations made under different noise conditions (in the Mediterranean Sea, the Indian and Pacific Oceans) by a submarine floating seismograph, and show that such floats are able to fill the oceanic data gap. Depending on the ambient noise level, the floats can <span class="hlt">record</span> between 35 and 63% of distant earthquakes with a moment magnitude M≥6.5. Even magnitudes <6.0 can be successfully observed under favourable noise conditions. The serendipitous <span class="hlt">recording</span> of an earthquake swarm near the Indian Ocean triple junction enabled us to establish a threshold magnitude between 2.7 and 3.4 for local earthquakes in the noisiest of the three environments.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4560755','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4560755"><span><span class="hlt">Seismic</span> monitoring in the oceans by autonomous floats</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Sukhovich, Alexey; Bonnieux, Sébastien; Hello, Yann; Irisson, Jean-Olivier; Simons, Frederik J.; Nolet, Guust</p> <p>2015-01-01</p> <p>Our understanding of the internal dynamics of the Earth is largely based on images of <span class="hlt">seismic</span> velocity variations in the mantle obtained with global tomography. However, our ability to image the mantle is severely hampered by a lack of <span class="hlt">seismic</span> data collected in marine areas. Here we report observations made under different noise conditions (in the Mediterranean Sea, the Indian and Pacific Oceans) by a submarine floating seismograph, and show that such floats are able to fill the oceanic data gap. Depending on the ambient noise level, the floats can <span class="hlt">record</span> between 35 and 63% of distant earthquakes with a moment magnitude M≥6.5. Even magnitudes <6.0 can be successfully observed under favourable noise conditions. The serendipitous <span class="hlt">recording</span> of an earthquake swarm near the Indian Ocean triple junction enabled us to establish a threshold magnitude between 2.7 and 3.4 for local earthquakes in the noisiest of the three environments. PMID:26289598</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2001AGUFM.T31A0837S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2001AGUFM.T31A0837S"><span>The Crustal Structure and <span class="hlt">Seismicity</span> of Eastern Venezuela</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Schmitz, M.; Martins, A.; Sobiesiak, M.; Alvarado, L.; Vasquez, R.</p> <p>2001-12-01</p> <p>Eastern Venezuela is characterized by a moderate to high <span class="hlt">seismicity</span>, evidenced recently by the 1997 Cariaco earthquake located on the El Pilar Fault, a right lateral strike slip fault which marks the plate boundary between the Caribbean and South-American plates in this region. Recently, the <span class="hlt">seismic</span> activity seems to migrate towards the zone of subduction of the Lesser Antilles in the northeast, where a mb 6.0 earthquake occurred in October 2000 at 120 km of depth. Periodical changes in the <span class="hlt">seismic</span> activity are related to the interaction of the stress fields of the strike-slip and the subduction regimes. The <span class="hlt">seismic</span> activity decreases rapidly towards to the south with some disperse events on the northern edge of the Guayana Shield, related to the Guri fault system. The crustal models used in the region are derived from the information generated by the national seismological network since 1982 and by microseismicity studies in northeastern Venezuela, coinciding in a crustal thickness of about 35 km in depth. Results of <span class="hlt">seismic</span> refraction measurements for the region were obtained during field campains in 1998 (ECOGUAY) for the Guayana Shield and the Cariaco sedimentary basin and in 2001 (ECCO) for the Oriental Basin. The total crustal thickness decreases from about 45 km on the northern edge of the Guayana Shield to some 36 km close to El Tigre in the center of the Oriental Basin. The average crustal velocity decreases in the same sense from 6.5 to 5.8 km/s. In the Cariaco sedimentary basin a young sedimentary cover of 1 km thickness with a <span class="hlt">seismic</span> velocity of 2 km/s was derived. Towards the northern limit of the South-American plate, no deep <span class="hlt">seismic</span> refraction data are available up to now. The improvement of the crustal models used in that region would constitute a step forward in the analysis of the <span class="hlt">seismic</span> hazard. <span class="hlt">Seismic</span> refraction studies funded by CONICIT S1-97002996 and S1-2000000685 projects and PDVSA (additional drilling and blasting), <span class="hlt">recording</span> equipment</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.usgs.gov/of/1980/0369/ofr1980369.pdf','USGSPUBS'); return false;" href="https://pubs.usgs.gov/of/1980/0369/ofr1980369.pdf"><span><span class="hlt">Seismic</span>-reflection data on the eastern U.S. continental shelf acquired by M. V. L'OLONNOIS as part of the Atlantic Margin Coring Project (AMCOR) of the U.S. Geological Survey, July-September 1976</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Robb, James M.</p> <p>1980-01-01</p> <p>In 1976 the U.S. Geological Survey undertook a program to sample the eastern United States Shelf for stratigraphic information by drilling a set of core holes. Results of this Atlantic Margin Coring Program (AMCOR) have been reported by Hathaway and others. Sites were chosen from <span class="hlt">seismic</span>-reflection data and were reviewed by a safety panel to minimize the risk of penetrating any hydrocarbon accumulation which might lead to environmental contamination.The M-V-L'OLONNOIS, the service ship for the drilling operation, was fitted with <span class="hlt">seismic</span>-reflection profiling equipment (listed below), to run <span class="hlt">seismic</span>-reflection profiles before drilling began on each hole. This provided additional assurance that no closed structures would be penetrated and allowed minor adjustment with the site selection. A total of 491 km of high-resolution <span class="hlt">seismic</span> profiles was collected on 22 sites.Equipment used (specifics for each site noted on <span class="hlt">records</span>): Bolt Air Guns 1-40 cubic inch chambers EPC <span class="hlt">Recorder</span> Teledyne Minisparker (last two sites) Navigation used two Internav 101 Loran-<span class="hlt">C</span> receivers.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/961550','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/961550"><span>HANFORD DOUBLE SHELL TANK (DST) THERMAL & <span class="hlt">SEISMIC</span> PROJECT <span class="hlt">SEISMIC</span> ANALYSIS IN SUPPORT OF INCREASED LIQUID LEVEL IN 241-AP TANK FARMS</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>MACKEY TC; ABBOTT FG; CARPENTER BG</p> <p>2007-02-16</p> <p>The overall scope of the project is to complete an up-to-date comprehensive analysis of <span class="hlt">record</span> of the DST System at Hanford. The "Double-Shell Tank (DST) Integrity Project - DST Thermal and <span class="hlt">Seismic</span> Project" is in support of Tri-Party Agreement Milestone M-48-14.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EGUGA..1810134A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EGUGA..1810134A"><span>Structure of Suasselkä Postglacial Fault in northern Finland obtained by analysis of ambient <span class="hlt">seismic</span> noise</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Afonin, Nikita; Kozlovskaya, Elena</p> <p>2016-04-01</p> <p>Understanding inner structure of seismogenic faults and their ability to reactivate is particularly important in investigating the continental intraplate <span class="hlt">seismicity</span> regime. In our study we address this problem using analysis of ambient <span class="hlt">seismic</span> noise <span class="hlt">recorded</span> by the temporary DAFNE array in northern Fennoscandian Shield. The main purpose of the DAFNE/FINLAND passive <span class="hlt">seismic</span> array experiment was to characterize the present-day <span class="hlt">seismicity</span> of the Suasselkä post-glacial fault (SPGF) that was proposed as one potential target for the DAFNE (Drilling Active Faults in Northern Europe) project. The DAFNE/FINLAND array comprised the area of about 20 to 100 km and consisted of 8 short-period and 4 broad-band 3-component autonomous <span class="hlt">seismic</span> stations installed in the close vicinity of the fault area. The array <span class="hlt">recorded</span> continuous <span class="hlt">seismic</span> data during September, 2011-May, 2013. <span class="hlt">Recordings</span> of the array have being analyzed in order to identify and locate natural earthquakes from the fault area and to discriminate them from the blasts in the Kittilä Gold Mine. As a result, we found several dozens of natural <span class="hlt">seismic</span> events originating from the fault area, which proves that the fault is still <span class="hlt">seismically</span> active. In order to study the inner structure of the SPGF we use cross-correlation of ambient <span class="hlt">seismic</span> noise <span class="hlt">recorded</span> by the array. Analysis of azimuthal distribution of noise sources demonstrated that that during the time interval under consideration the distribution of noise sources is close to the uniform one. The continuous data were processed in several steps including single station data analysis, instrument response removal and time-domain stacking. The data were used to estimate empirical Green's functions between pairs of stations in the frequency band of 0.1-1 Hz and to calculate correspondent surface wave dispersion curves. After that S-wave velocity models were obtained as a result of dispersion curves inversion using Geopsy software. The results suggest that the area of</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014EGUGA..16.9754R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014EGUGA..16.9754R"><span>Detailed <span class="hlt">seismicity</span> analysis in the SE of Romania (Dobrogea region)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Rogozea, Maria; Radulian, Mircea; Ghica, Daniela; Popa, Mihaela</p> <p>2014-05-01</p> <p>The purpose of this paper is to analyze the <span class="hlt">seismicity</span> in the south-eastern part of Romania, in the Dobrogea region (namely the Predobrogean Depression and Black Sea area). Predobrogean Depression is the name attributed to the structures belonging to the Scythian Platform. The <span class="hlt">seismic</span> activity is moderate with most significant earthquakes at the boundary between the North Dobrogea Orogen and Scythian Platform (Sf. Gheorghe fault). The largest magnitude event was <span class="hlt">recorded</span> in 02.11.1871 (Mw = 5.3). Other events with magnitude above 4 were observed close to Tulcea city (13.11.1981, Mw = 5.1, 03.09.204, Mw =5.1) and Galati city (11.09.1980, Mw = 4.2). Recently, an earthquake swarm of 406 events extended over two months and a half (23 September - 5 December 2013) was produced in the Galati area (maximum magnitude 3.9). The deformation field has an extensional regime, as resulted from fault plane solutions and geotectonic investigations. The maximum expected magnitude in this area is estimated at Mw = 5.5. The <span class="hlt">seismic</span> activity in the Black Sea area, close to Romania seashore and north-east Bulgarian seashore, concentrates along Shabla fault system. Large shocks (magnitude above 7) are reported here at intervals of a few centuries. The most recent major shock was <span class="hlt">recorded</span> on 31 January 1901 (Mw = 7.2) in Shabla region, Bulgaria. To characterize <span class="hlt">seismicity</span> parameters, the Romanian catalogue of the National Institute of Earth Physics was used as a basic input. The catalogue was revised as concerns historical information by reanalyzing macroseismic data and for the recent events, by applying up-to-date tools to relocate and re-parametrize the <span class="hlt">seismic</span> sources.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012PhRvE..86a1107Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012PhRvE..86a1107Z"><span>Scaling of <span class="hlt">seismic</span> memory with earthquake size</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zheng, Zeyu; Yamasaki, Kazuko; Tenenbaum, Joel; Podobnik, Boris; Tamura, Yoshiyasu; Stanley, H. Eugene</p> <p>2012-07-01</p> <p>It has been observed that discrete earthquake events possess memory, i.e., that events occurring in a particular location are dependent on the history of that location. We conduct an analysis to see whether continuous real-time data also display a similar memory and, if so, whether such autocorrelations depend on the size of earthquakes within close spatiotemporal proximity. We analyze the <span class="hlt">seismic</span> wave form database <span class="hlt">recorded</span> by 64 stations in Japan, including the 2011 “Great East Japan Earthquake,” one of the five most powerful earthquakes ever <span class="hlt">recorded</span>, which resulted in a tsunami and devastating nuclear accidents. We explore the question of <span class="hlt">seismic</span> memory through use of mean conditional intervals and detrended fluctuation analysis (DFA). We find that the wave form sign series show power-law anticorrelations while the interval series show power-law correlations. We find size dependence in earthquake autocorrelations: as the earthquake size increases, both of these correlation behaviors strengthen. We also find that the DFA scaling exponent α has no dependence on the earthquake hypocenter depth or epicentral distance.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70133685','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70133685"><span>Pulling the rug out from under California: <span class="hlt">Seismic</span> images of the Mendocino Triple Junction region</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Tréhu, Anne M.</p> <p>1995-01-01</p> <p>In 1993 and 1994 a network of large-aperture <span class="hlt">seismic</span> profiles was collected to image the crustal and upper-mantle structure beneath northern California and the adjacent continental margin. The data include approximately 650 km of onshore <span class="hlt">seismic</span> refraction/reflection data, 2000 km of off-shore multichannel <span class="hlt">seismic</span> (MCS) reflection data, and simultaneous onshore and offshore <span class="hlt">recording</span> of the MCS airgun source to yield large-aperture data. Scientists from more than 12 institutions were involved in data acquisition.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009EGUGA..11.4462B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009EGUGA..11.4462B"><span>Reassessment of the <span class="hlt">Seismicity</span> and <span class="hlt">seismic</span> hazards of Libya</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ben Suleman, A.; Elmeladi, A.</p> <p>2009-04-01</p> <p>The tectonic evolution of Libya, located at the northern extreme of the African continent, has yielded a complex crustal structure that is composed of a series of basins and uplifts. The present day deformation of Libya is the result of the Eurasia-Africa continental collision. At the end of the year 2005, The Libyan National Seismological Network was established to monitor local, regional and teleseismic activities, as well as to provide high quality data for research projects both locally and on the regional and global scale. This study aims to discuss the <span class="hlt">seismicity</span> of Libya by using the new data from the Libyan national seismological network and to focus on the <span class="hlt">seismic</span> hazards. At first glance the <span class="hlt">seismic</span> activity map shows dominant trends of <span class="hlt">seismicity</span> with most of the <span class="hlt">seismic</span> activity concentrated along the northern coastal areas. Four major <span class="hlt">seismic</span> trends were quite noticeable. A first trend is a NW-SE direction coinciding with the eastern boarder of the Hun Graben. A second trend is also a NW-SE direction in the offshore area and might be a continuation of this trend. The other two trends were located in the western Gulf of Sirt and Cyrenaica platform. The rest of <span class="hlt">seismicity</span> is diffuse either offshore or in land, with no good correlation with well-mapped faults. Detailed investigations of the Libyan <span class="hlt">seismicity</span> indicates that the Libya has experienced earthquakes of varying magnitudes and that there is definitely a certain amount of <span class="hlt">seismic</span> risk involved in engineering projects, particularly in the northern regions. Detailed investigation of the distribution of the Libyan earthquakes in space and time along with all other geological considerations suggested the classification of the country into four <span class="hlt">seismic</span> zones with the Hun graben zone being the most <span class="hlt">seismically</span> active zone.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010AGUFM.S21C2075M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010AGUFM.S21C2075M"><span>How <span class="hlt">seismic</span> waves can be used to understand and constrain landslide dynamics</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mangeney, A.; Favreau, P.; Moretti, L.; Lucas, A.; Le Friant, A.; Bouchut, F.</p> <p>2010-12-01</p> <p>Gravitational instabilities such as debris flows, landslide or avalanches play a key role in erosion processes on the Earth’s surface and represent one of the major natural hazard threatening life and property in mountainous, volcanic, <span class="hlt">seismic</span> and coastal areas. Despite the great amount of experimental, numerical and field studies, the understanding of landslide dynamics is still an open question. In particular, there is no consensus to explain the high mobility of natural avalanches. Field measurements relevant to the dynamics of natural landslides are scarce. This is due to their unpredictability and destructive power and prevents detailed investigation of the mechanical properties of the flowing material. Recent studies have shown that the <span class="hlt">seismic</span> signal generated by landslides provides a unique way to detect gravitational instabilities and to get information on their dynamics and geometrical characteristics. In particular, Favreau et al. [2009] show that simulation of landslides and generated <span class="hlt">seismic</span> waves reproduce the main features of the <span class="hlt">recorded</span> low frequency <span class="hlt">seismic</span> signal, making it possible to discriminate between possible alternative scenarios for flow dynamics and to provide first estimates of the rheological parameters. We propose here to go further in this direction by investigating the following key questions: What is the effect of the topography and of the landslide volume on the generated <span class="hlt">seismic</span> signal? What is the sensitivity of the generated <span class="hlt">seismic</span> signal to the mechanical behavior of the landslide? At what distance and frequency is the point source approximation correct? To address these issues, numerical simulation of two well constrained landslides has been performed: the 2.5 Mm3 Thurwieser landslide that occurred in Italy in 2004 and the 60 Mm3 Boxing Day debris avalanche that occurred in Montserrat in 1997 during the volcanic eruption. For both landslides, simulation shows the major role of topography curvature on the generated <span class="hlt">seismic</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70034932','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70034932"><span>Enhancement of long period components of <span class="hlt">recorded</span> and synthetic ground motions using InSAR</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Abell, J.A.; Carlos de la Llera, J.; Wicks, C.W.</p> <p>2011-01-01</p> <p>Tall buildings and flexible structures require a better characterization of long period ground motion spectra than the one provided by current <span class="hlt">seismic</span> building codes. Motivated by that, a methodology is proposed and tested to improve <span class="hlt">recorded</span> and synthetic ground motions which are consistent with the observed co-<span class="hlt">seismic</span> displacement field obtained from interferometric synthetic aperture radar (InSAR) analysis of image data for the Tocopilla 2007 earthquake (Mw=7.7) in Northern Chile. A methodology is proposed to correct the observed motions such that, after double integration, they are coherent with the local value of the residual displacement. Synthetic <span class="hlt">records</span> are generated by using a stochastic finite-fault model coupled with a long period pulse to capture the long period fling effect. It is observed that the proposed co-<span class="hlt">seismic</span> correction yields <span class="hlt">records</span> with more accurate long-period spectral components as compared with regular correction schemes such as acausal filtering. These signals provide an estimate for the velocity and displacement spectra, which are essential for tall-building design. Furthermore, hints are provided as to the shape of long-period spectra for <span class="hlt">seismic</span> zones prone to large co-<span class="hlt">seismic</span> displacements such as the Nazca-South American zone. ?? 2011 Elsevier Ltd.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/869911','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/869911"><span><span class="hlt">Seismic</span> switch for strong motion measurement</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Harben, Philip E.; Rodgers, Peter W.; Ewert, Daniel W.</p> <p>1995-01-01</p> <p>A <span class="hlt">seismic</span> switching device that has an input signal from an existing microseismic station seismometer and a signal from a strong motion measuring instrument. The <span class="hlt">seismic</span> switch monitors the signal level of the strong motion instrument and passes the seismometer signal to the station data telemetry and <span class="hlt">recording</span> systems. When the strong motion instrument signal level exceeds a user set threshold level, the seismometer signal is switched out and the strong motion signal is passed to the telemetry system. The amount of time the strong motion signal is passed before switching back to the seismometer signal is user controlled between 1 and 15 seconds. If the threshold level is exceeded during a switch time period, the length of time is extended from that instant by one user set time period.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/63436','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/biblio/63436"><span><span class="hlt">Seismic</span> switch for strong motion measurement</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Harben, P.E.; Rodgers, P.W.; Ewert, D.W.</p> <p>1995-05-30</p> <p>A <span class="hlt">seismic</span> switching device is described that has an input signal from an existing microseismic station seismometer and a signal from a strong motion measuring instrument. The <span class="hlt">seismic</span> switch monitors the signal level of the strong motion instrument and passes the seismometer signal to the station data telemetry and <span class="hlt">recording</span> systems. When the strong motion instrument signal level exceeds a user set threshold level, the seismometer signal is switched out and the strong motion signal is passed to the telemetry system. The amount of time the strong motion signal is passed before switching back to the seismometer signal is user controlled between 1 and 15 seconds. If the threshold level is exceeded during a switch time period, the length of time is extended from that instant by one user set time period. 11 figs.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFM.S43B2787B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFM.S43B2787B"><span>A Framework for the Validation of Probabilistic <span class="hlt">Seismic</span> Hazard Analysis Maps Using Strong Ground Motion Data</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bydlon, S. A.; Beroza, G. C.</p> <p>2015-12-01</p> <p>Recent debate on the efficacy of Probabilistic <span class="hlt">Seismic</span> Hazard Analysis (PSHA), and the utility of hazard maps (i.e. Stein et al., 2011; Hanks et al., 2012), has prompted a need for validation of such maps using <span class="hlt">recorded</span> strong ground motion data. Unfortunately, strong motion <span class="hlt">records</span> are limited spatially and temporally relative to the area and time windows hazard maps encompass. We develop a framework to test the predictive powers of PSHA maps that is flexible with respect to a map's specified probability of exceedance and time window, and the strong motion receiver coverage. Using a combination of <span class="hlt">recorded</span> and interpolated strong motion <span class="hlt">records</span> produced through the ShakeMap environment, we compile a <span class="hlt">record</span> of ground motion intensity measures for California from 2002-present. We use this information to perform an area-based test of California PSHA maps inspired by the work of Ward (1995). Though this framework is flexible in that it can be applied to <span class="hlt">seismically</span> active areas where ShakeMap-like ground shaking interpolations have or can be produced, this testing procedure is limited by the relatively short lifetime of strong motion <span class="hlt">recordings</span> and by the desire to only test with data collected after the development of the PSHA map under scrutiny. To account for this, we use the assumption that PSHA maps are time independent to adapt the testing procedure for periods of <span class="hlt">recorded</span> data shorter than the lifetime of a map. We note that accuracy of this testing procedure will only improve as more data is collected, or as the time-horizon of interest is reduced, as has been proposed for maps of areas experiencing induced <span class="hlt">seismicity</span>. We believe that this procedure can be used to determine whether PSHA maps are accurately portraying <span class="hlt">seismic</span> hazard and whether discrepancies are localized or systemic.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFM.S13B2803P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFM.S13B2803P"><span>Induced <span class="hlt">Seismicity</span> from different sources in Italy: how to interpret it?</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pastori, M.; De Gori, P.; Piccinini, D.; Bagh, S.; Improta, L.; Chiarabba, C.</p> <p>2015-12-01</p> <p>Typically the term "induced <span class="hlt">seismicity</span>" is used to refer minor earthquakes and tremors caused by human activities that alter the stresses and strains on the Earth's crust. In the last years, the interest in the induced <span class="hlt">seismicity</span> related to fluids (oil and gas, and geothermal resources) extraction or injection is increased, because it is believed to be responsible to enucleate earthquakes. Possible sources of induced <span class="hlt">seismicity</span> are not only represented by the oil and gas production but also, i.e., by changes in the water level of artificial lakes. The aim of this work is to show results from two different sources, wastewater injection and changes in the water level of an artificial reservoir (Pertusillo lake), that can produce induced earthquakes observed in the Val d'Agri basin (Italy) and to compare them with variation in crustal elastic parameters. Val d'Agri basin in the Apennines extensional belt hosts the largest oilfield in onshore Europe and is bordered by NW-SE ­trending fault systems. Most of the <span class="hlt">recorded</span> <span class="hlt">seismicity</span> seems to be related to these structures. We correlated the <span class="hlt">seismicity</span> rate, injection curves and changes in water levels with temporal variations of Vp/Vs and anisotropic parameters of the crustal reservoirs and in the nearby area. We analysed about 983 high-quality <span class="hlt">recordings</span> occurred from 2002 to 2014 in Val d'Agri basin from temporary and permanent network held by INGV and ENI corporate. 3D high-precision locations and manual-revised P- and S-picking are used to estimate anisotropic parameters (delay time and fast direction polarization) and Vp/Vs ratio. <span class="hlt">Seismicity</span> is mainly located in two areas: in the SW of the Pertusillo Lake, and near the Eni Oil field (SW and NE of the Val d'Agri basin respectively). Our correlations well recognize the <span class="hlt">seismicity</span> diffusion process, caused by both water injection and water level changes; these findings could help to model the active and pre-existing faults failure behaviour.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012AGUFM.C23B0655C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012AGUFM.C23B0655C"><span><span class="hlt">Seismic</span> Response of the Greenland Ice-sheet over Several Melt Seasons near Draining Supraglacial Lakes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Carmichael, J. D.; Joughin, I. R.; Behn, M. D.; Das, S. B.; Lizarralde, D.</p> <p>2012-12-01</p> <p>We present <span class="hlt">seismic</span> observations assembled from 3+ years of melt season measurements collected near seasonally-draining supraglacial lakes on the Greenland Ice-sheet (68.7311,-49.5925). On transient time scales (< 1 day), these data include a <span class="hlt">record</span> of <span class="hlt">seismic</span> response coincident with at least three documented lake drainage events. During a particular event, drainage is preceded by two hours of impulsive high-energy <span class="hlt">seismic</span> signals, followed by the onset of continuous broadband signals (2-50Hz) that we interpret as surface-to-bed meltwater transfer. This drainage is followed additional transient icequakes similar in timing and energy to the precursory activity. Over a seasonal time scale (> 1 month), our data <span class="hlt">records</span> a transition in <span class="hlt">seismicity</span> between two distinct modes, with one mode characterized by relative quiescence, and the other mode characterized by uniform energy that is observed network-wide as a continuous, repetitive signal. The transition between modes is abrupt (~ 2 hours) and is observed using multiple <span class="hlt">seismic</span> discriminants. We interpret this rapid transition as reflecting the evolution of the morphology of a basal drainage system as it responds to melt input. This interpretation is tested against additional geophysical observations that include temperature-based melt models, satellite imagery, and GPS measurements. Finally, we outline and advocate a routine for monitoring icesheet <span class="hlt">seismicity</span> with a focus on distinguishing surface from basal sources.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/21148929-seismic-behavior-retrofit-concrete-columns-old-buildings-reinforced-plain-bars','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/21148929-seismic-behavior-retrofit-concrete-columns-old-buildings-reinforced-plain-bars"><span><span class="hlt">Seismic</span> Behavior and Retrofit of Concrete Columns of Old R.<span class="hlt">C</span>. Buildings Reinforced With Plain Bars</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Marefat, M. S.; Arani, K. Karbasi; Shirazi, S. M. Hassanzadeh</p> <p>2008-07-08</p> <p><span class="hlt">Seismic</span> rehabilitation of old buildings has been a major challenge in recent years. The first step in <span class="hlt">seismic</span> rehabilitation is evaluation of the existing capacity and the <span class="hlt">seismic</span> behaviour. For investigation of the <span class="hlt">seismic</span> behaviour of RC members of a real old building in Iran which has been designed and constructed by European engineers in 1940, three half-scale column specimens reinforced with plain bars have been tested. The tests indicate significant differences between the responses of specimens reinforced by plain bars relative to those reinforced by deformed bars. A regular pattern of cracking and a relatively brittle behaviour was observedmore » while a relatively large residual strength appeared after sudden drop of initial strength and stiffness due to slip of longitudinal bars.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010AGUFM.S43B2061S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010AGUFM.S43B2061S"><span>Limitation and applicability of microtremor <span class="hlt">records</span> for site-response estimation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Song, G.; Kang, T.; Park, S.</p> <p>2010-12-01</p> <p>Site effects are the modifications of <span class="hlt">seismic</span> motions which are traveling through near-surface materials. The impedance contrast between the topmost layer and bedrock may significantly amplify ground motions and augment their durations. Inelastic behavior of the geological media such as highly fractured/weathered rocks and unconsolidated sediments may absorb <span class="hlt">seismic</span> energy, and thus damp the resulting ground motions. It is inherently most desirable to evaluate the site effects using <span class="hlt">seismic</span> <span class="hlt">records</span> from large earthquakes. If there are only small events that will be <span class="hlt">recorded</span> by several seismograph stations, it becomes difficult to evaluate site effects using earthquake data. Recently a number of studies pay attention to microtremor <span class="hlt">records</span> to assess site effects. The main reason of such efforts is that measurements are relatively easy regardless of site condition and cost-effective without necessity of waiting for earthquakes or of using active sources. Especially microtremor measurements are exclusively a useful option to assess site effects, and thus <span class="hlt">seismic</span> microzonation, in the urban area and/or region of low to moderate <span class="hlt">seismicity</span>. Spectral ratios of horizontal components to vertical component (HVSR) of microtremor <span class="hlt">records</span> have been popular for estimation of site resonant frequency. Although some studies have shown that the amplitude of spectral ratios is an indicator of site amplification relative to bedrock motion, there are still debates on it. This discrepancy may originate from the deficiency of our understanding on the nature of microtremor. Therefore, it is important to understand the limitation and applicability of microtremor <span class="hlt">records</span> for site-effect assessments. The focus on this problem is how microtremor responses on the subsurface structures and their physical properties, and how parameters deduced from microtremor analyses are related to site responses during earthquake ground motions. In order to investigate how these issues have a practical</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li class="active"><span>24</span></li> <li><a href="#" onclick='return showDiv("page_25");'>25</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_24 --> <div id="page_25" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li class="active"><span>25</span></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="481"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016JGRB..121.6009K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016JGRB..121.6009K"><span>Validating induced <span class="hlt">seismicity</span> forecast models—Induced <span class="hlt">Seismicity</span> Test Bench</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Király-Proag, Eszter; Zechar, J. Douglas; Gischig, Valentin; Wiemer, Stefan; Karvounis, Dimitrios; Doetsch, Joseph</p> <p>2016-08-01</p> <p>Induced earthquakes often accompany fluid injection, and the <span class="hlt">seismic</span> hazard they pose threatens various underground engineering projects. Models to monitor and control induced <span class="hlt">seismic</span> hazard with traffic light systems should be probabilistic, forward-looking, and updated as new data arrive. In this study, we propose an Induced <span class="hlt">Seismicity</span> Test Bench to test and rank such models; this test bench can be used for model development, model selection, and ensemble model building. We apply the test bench to data from the Basel 2006 and Soultz-sous-Forêts 2004 geothermal stimulation projects, and we assess forecasts from two models: Shapiro and Smoothed <span class="hlt">Seismicity</span> (SaSS) and Hydraulics and <span class="hlt">Seismics</span> (HySei). These models incorporate a different mix of physics-based elements and stochastic representation of the induced sequences. Our results show that neither model is fully superior to the other. Generally, HySei forecasts the <span class="hlt">seismicity</span> rate better after shut-in but is only mediocre at forecasting the spatial distribution. On the other hand, SaSS forecasts the spatial distribution better and gives better <span class="hlt">seismicity</span> rate estimates before shut-in. The shut-in phase is a difficult moment for both models in both reservoirs: the models tend to underpredict the <span class="hlt">seismicity</span> rate around, and shortly after, shut-in.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUFMNH24A..06L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUFMNH24A..06L"><span>Toward predicting clay landslide with ambient <span class="hlt">seismic</span> noise</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Larose, E. F.; Mainsant, G.; Carriere, S.; Chambon, G.; Michoud, C.; Jongmans, D.; Jaboyedoff, M.</p> <p>2013-12-01</p> <p>Clay-rich pose critical problems in risk management worldwide. The most widely proposed mechanism leading to such flow-like movements is the increase in water pore pressure in the sliding mass, generating partial or complete liquefaction. This solid-to-liquid transition results in a dramatic reduction of mechanical rigidity, which could be detected by monitoring shear wave velocity variations, The ambient <span class="hlt">seismic</span> noise correlation technique has been applied to measure the variation in the <span class="hlt">seismic</span> surface wave velocity in the Pont Bourquin landslide (Swiss Alps). This small but active composite earthslide-earthflow was equipped with continuously <span class="hlt">recording</span> <span class="hlt">seismic</span> sensors during spring and summer 2010, and then again from fall 2011 on. An earthslide of a few thousand cubic meters was triggered in mid-August 2010, after a rainy period. This article shows that the <span class="hlt">seismic</span> velocity of the sliding material, measured from daily noise correlograms, decreased continuously and rapidly for several days prior to the catastrophic event. From a spectral analysis of the velocity decrease, it was possible to determine the location of the change at the base of the sliding layer. These results are confirmed by analogous small-scale experiments in the laboratory. These results demonstrate that ambient <span class="hlt">seismic</span> noise can be used to detect rigidity variations before failure and could potentially be used to predict landslides.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.S53B0695M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.S53B0695M"><span>High-resolution <span class="hlt">seismicity</span> catalog of Italian peninsula in the period 1981-2015</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Michele, M.; Latorre, D.; Castello, B.; Di Stefano, R.; Chiaraluce, L.</p> <p>2017-12-01</p> <p>In order to provide an updated reference catalog of Italian <span class="hlt">seismicity</span>, the absolute location of the last 35 years (1981-2015) of <span class="hlt">seismic</span> activity was computed with a three-dimensional VP and VS velocity model covering the whole Italian territory. The NonLinLoc code (Lomax et al., 2000), which is based on a probabilistic approach, was used to provide a complete and robust description of the uncertainties associated to the locations corresponding to the hypocentral solutions with the highest probability density. Moreover, the code using a finite difference approximation of the eikonal equation (Podvin and Lecomte, 1991), allows to manage very contrasted velocity models in the arrival time computation. To optimize the earthquakes location, we included the station corrections in the inverse problem. For each year, the number of available earthquakes depends on both the network detection capability and the occurrence of major <span class="hlt">seismic</span> sequences. The starting earthquakes catalog was based on 2.6 million P and 1.9 million S arrival time picks for 278.607 selected earthquakes, <span class="hlt">recorded</span> at least by 3 <span class="hlt">seismic</span> stations of the Italian <span class="hlt">seismic</span> network. The new catalog compared to the previous ones consisting of hypocentral locations retrieved with linearized location methods, shows a very good improvement as testified by the location parameters assessing the quality of the solution (i.e., RMS, azimuthal gap, formal error on horizontal and vertical components). In addition, we used the distance between the expected and the maximum likelihood hypocenter location to establish the unimodal (high-resolved location) or multimodal (poor-resolved location) character of the probability distribution. We used these parameters to classify the resulting locations in four classes (A, B, <span class="hlt">C</span> and D) considering the simultaneous goodness of the previous parameters. The upper classes (A and B) include the 65% of the relocated earthquake, while the lowest class (D) only includes the 7% of the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JGRB..122.6569B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JGRB..122.6569B"><span>Evaluating the effectiveness of induced <span class="hlt">seismicity</span> mitigation: Numerical modeling of wastewater injection near Greeley, Colorado</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Brown, Megan R. M.; Ge, Shemin; Sheehan, Anne F.; Nakai, Jenny S.</p> <p>2017-08-01</p> <p>Mitigation of injection-induced <span class="hlt">seismicity</span> in Greeley, Colorado, is based largely on proximity of wastewater disposal wells to <span class="hlt">seismicity</span> and consists of cementation of the bottom of wells to eliminate connection between the disposal interval and crystalline basement. Brief injection rate reductions followed felt events, but injection rates returned to high levels, >250,000 barrels/month, within 6 months. While brief rate reduction reduces <span class="hlt">seismicity</span> in the short term, overall <span class="hlt">seismicity</span> is not reduced. We examine contributions to pore pressure change by injection from 22 wells within 30 km of the center of <span class="hlt">seismicity</span>. The combined injection rate of seven disposal wells within 15 km of the <span class="hlt">seismicity</span> (Greeley Wells) is correlated with the <span class="hlt">seismicity</span> rate. We find that injection from NGL-<span class="hlt">C</span>4A, the well previously suspected as the likely cause of the induced <span class="hlt">seismicity</span>, is responsible for 28% of pore pressure increase. The other six Greeley Wells contribute 28% of pore pressure increase, and the 15 Far-field Wells between 15 and 30 km from the <span class="hlt">seismicity</span> contribute 44% of pore pressure increase. Modeling results show that NGL-<span class="hlt">C</span>4A plays the largest role in increased pore pressure but shows that the six other Greeley Wells have approximately the same influence as NGL-<span class="hlt">C</span>4A. Furthermore, the 15 Far-field Wells have significant influence on pore pressure near the <span class="hlt">seismicity</span>. Since the main mitigation action of cementing the bottom of wells has not decreased <span class="hlt">seismicity</span>, mitigation based on reduced injection rates and spacing wells farther apart would likely have a higher potential for success.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JAESc.145...37Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JAESc.145...37Z"><span><span class="hlt">Seismic</span> probing of continental subduction zones</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhao, Liang; Xu, Xiaobing; Malusà, Marco G.</p> <p>2017-09-01</p> <p>High-resolution images of Earth's interior provide pivotal information for the understanding of a range of geodynamic processes, including continental subduction and exhumation of ultrahigh-pressure (UHP) metamorphic rocks. Here we present a synthesis of available global <span class="hlt">seismic</span> observations on continental subduction zones, and selected examples of <span class="hlt">seismic</span> probing from the European Alps, the Himalaya-Tibet and the Qinling-Dabie orogenic belts. Our synthesis and examples show that slabs recognized beneath exhumed continental UHP terranes generally have shallow dip angles (<45°) at depths <100 km, to become much steeper at depths >100 km. Slabs underlined by a clear high velocity anomaly from Earth's surface to the mantle are generally Cenozoic in age. Some of these slabs are continuous, whereas other continental subduction zones are located above discontinuous high velocity anomalies possibly suggesting slab breakoff. The density of <span class="hlt">seismic</span> stations and the quality of <span class="hlt">recordings</span> are of primary importance to get high-resolution images of the upper mantle to be used as a starting point to provide reliable geodynamic interpretations. In some cases, areas previously indicated as possible site of slab breakoff, such as the European Alps, have been later proven to be located above a continuous slab by using higher quality travel time data from denser <span class="hlt">seismic</span> arrays. Discriminating between oceanic and continental slabs can be challenging, but valuable information can be provided by combining teleseismic tomography and receiver function analysis. The upper mantle beneath most continental UHP terranes generally shows complex <span class="hlt">seismic</span> anisotropy patterns that are potentially preserved even in pre-Cenozoic subduction zones. These patterns can be used to provide information on continental slabs that are no longer highlighted by a clear high-velocity anomaly.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMNS31A1939B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMNS31A1939B"><span>Instrument Correction and Dynamic Site Profile Validation at the Central United States <span class="hlt">Seismic</span> Observatory, New Madrid <span class="hlt">Seismic</span> Zone</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Brengman, C.; Woolery, E. W.; Wang, Z.; Carpenter, S.</p> <p>2016-12-01</p> <p>The Central United States <span class="hlt">Seismic</span> Observatory (CUSSO) is a vertical <span class="hlt">seismic</span> array located in southwestern Kentucky within the New Madrid <span class="hlt">seismic</span> zone. It is intended to describe the effects of local geology, including thick sediment overburden, on <span class="hlt">seismic</span>-wave propagation, particularly strong-motion. The three-borehole array at CUSSO is composed of <span class="hlt">seismic</span> sensors placed on the surface, and in the bedrock at various depths within the 585 m thick sediment overburden. The array's deep borehole provided a unique opportunity in the northern Mississippi embayment for the direct geological description and geophysical measurement of the complete late Cretaceous-Quaternary sediment column. A seven layer, intra-sediment velocity model is interpreted from the complex, inhomogeneous stratigraphy. The S- and P-wave sediment velocities range between 160 and 875 m/s and between 1000 and 2300 m/s, respectively, with bedrock velocities of 1452 and 3775 m/s, respectively. Cross-correlation and direct comparisons were used to filter out the instrument response and determine the instrument orientation, making CUSSO data ready for analysis, and making CUSSO a viable calibration site for other free-field sensors in the area. The corrected bedrock motions were numerically propagated through the CUSSO soil profile (transfer function) and compared, in terms of both peak acceleration and amplitude spectra, to the <span class="hlt">recorded</span> surface observations. Initial observations reveal a complex spectral mix of amplification and de-amplification across the array, indicating the site effect in this deep sediment setting is not simply generated by the shallowest layers.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFM.S51D2741O','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFM.S51D2741O"><span>Updating Hawaii <span class="hlt">Seismicity</span> Catalogs with Systematic Relocations and Subspace Detectors</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Okubo, P.; Benz, H.; Matoza, R. S.; Thelen, W. A.</p> <p>2015-12-01</p> <p>We continue the systematic relocation of <span class="hlt">seismicity</span> <span class="hlt">recorded</span> in Hawai`i by the United States Geological Survey's (USGS) Hawaiian Volcano Observatory (HVO), with interests in adding to the products derived from the relocated <span class="hlt">seismicity</span> catalogs published by Matoza et al., (2013, 2014). Another goal of this effort is updating the systematically relocated HVO catalog since 2009, when earthquake cataloging at HVO was migrated to the USGS Advanced National <span class="hlt">Seismic</span> System Quake Management Software (AQMS) systems. To complement the relocation analyses of the catalogs generated from traditional STA/LTA event-triggered and analyst-reviewed approaches, we are also experimenting with subspace detection of events at Kilauea as a means to augment AQMS procedures for cataloging <span class="hlt">seismicity</span> to lower magnitudes and during episodes of elevated volcanic activity. Our earlier catalog relocations have demonstrated the ability to define correlated or repeating families of earthquakes and provide more detailed definition of seismogenic structures, as well as the capability for improved automatic identification of diverse volcanic <span class="hlt">seismic</span> sources. Subspace detectors have been successfully applied to cataloging <span class="hlt">seismicity</span> in situations of low <span class="hlt">seismic</span> signal-to-noise and have significantly increased catalog sensitivity to lower magnitude thresholds. We anticipate similar improvements using event subspace detections and cataloging of volcanic <span class="hlt">seismicity</span> that include improved discrimination among not only evolving earthquake sequences but also diverse volcanic <span class="hlt">seismic</span> source processes. Matoza et al., 2013, Systematic relocation of <span class="hlt">seismicity</span> on Hawai`i Island from 1992 to 2009 using waveform cross correlation and cluster analysis, J. Geophys. Res., 118, 2275-2288, doi:10.1002/jgrb.580189 Matoza et al., 2014, High-precision relocation of long-period events beneath the summit region of Kīlauea Volcano, Hawai`i, from 1986 to 2009, Geophys. Res. Lett., 41, 3413-3421, doi:10.1002/2014GL059819</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.S12B..07M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.S12B..07M"><span><span class="hlt">Seismic</span> Interferometry at a Large, Dense Array: Capturing the Wavefield at the Source Physics Experiment</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Matzel, E.; Mellors, R. J.; Magana-Zook, S. A.</p> <p>2016-12-01</p> <p><span class="hlt">Seismic</span> interferometry is based on the observation that the Earth's background wavefield includes coherent energy, which can be recovered by observing over long time periods, allowing the incoherent energy to cancel out. The cross correlation of the energy <span class="hlt">recorded</span> at a pair of stations results in an estimate of the Green's Function (GF) and is equivalent to the <span class="hlt">record</span> of a simple source located at one of the stations as <span class="hlt">recorded</span> by the other. This allows high resolution imagery beneath dense <span class="hlt">seismic</span> networks even in areas of low <span class="hlt">seismicity</span>. The power of these inter-station techniques increases rapidly as the number of seismometers in a network increases. For large networks the number of correlations computed can run into the millions and this becomes a "big-data" problem where data-management dominates the efficiency of the computations. In this study, we use several methods of <span class="hlt">seismic</span> interferometry to obtain highly detailed images at the site of the Source Physics Experiment (SPE). The objective of SPE is to obtain a physics-based understanding of how <span class="hlt">seismic</span> waves are created at and scattered near the source. In 2015, a temporary deployment of 1,000 closely spaced geophones was added to the main network of instruments at the site. We focus on three interferometric techniques: Shot interferometry (SI) uses the SPE shots as rich sources of high frequency, high signal energy. Coda interferometry (CI) isolates the energy from the scattered wavefield of distant earthquakes. Ambient noise correlation (ANC) uses the energy of the ambient background field. In each case, the data <span class="hlt">recorded</span> at one seismometer are correlated with the data <span class="hlt">recorded</span> at another to obtain an estimate of the GF between the two. The large network of mixed geophone and broadband instruments at the SPE allows us to calculate over 500,000 GFs, which we use to characterize the site and measure the localized wavefield. This work performed under the auspices of the U.S. Department of Energy by</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009GeoJI.178.1493L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009GeoJI.178.1493L"><span>Chaotic system detection of weak <span class="hlt">seismic</span> signals</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Li, Y.; Yang, B. J.; Badal, J.; Zhao, X. P.; Lin, H. B.; Li, R. L.</p> <p>2009-09-01</p> <p>When the signal-to-noise (S/N) ratio is less than -3 dB or even 0 dB, <span class="hlt">seismic</span> events are generally difficult to identify from a common shot <span class="hlt">record</span>. To overcome this type of problem we present a method to detect weak <span class="hlt">seismic</span> signals based on the oscillations described by a chaotic dynamic system in phase space. The basic idea is that a non-linear chaotic oscillator is strongly immune to noise. Such a dynamic system is less influenced by noise, but it is more sensitive to periodic signals, changing from a chaotic state to a large-scale periodic phase state when excited by a weak signal. With the purpose of checking the possible contamination of the signal by noise, we have performed a numerical experiment with an oscillator controlled by the Duffing-Holmes equation, taking a distorted Ricker wavelet sequence as input signal. In doing so, we prove that the oscillator system is able to reach a large-scale periodic phase state in a strong noise environment. In the case of a common shot <span class="hlt">record</span> with low S/N ratio, the onsets reflected from a same interface are similar to one other and can be put on a single trace with a common reference time and the periodicity of the so-generated signal follows as a consequence of moveout at a particular scanning velocity. This operation, which is called `horizontal dynamic correction' and leads to a nearly periodic signal, is implemented on synthetic wavelet sequences taking various sampling arrival times and scanning velocities. Thereafter, two tests, both in a noisy ambient of -3.7 dB, are done using a chaotic oscillator: the first demonstrates the capability of the method to really detect a weak <span class="hlt">seismic</span> signal; the second takes care of the fundamental weakness of the dynamic correction coming from the use of a particular scanning velocity, which is investigated from the effect caused by near-surface lateral velocity variation on the periodicity of the reconstructed <span class="hlt">seismic</span> signal. Finally, we have developed an application of the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.S13C0679K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.S13C0679K"><span>Comparison of <span class="hlt">Seismic</span> Sources and Frequencies in West Texas</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kaip, G.; Harder, S. H.; Karplus, M. S.</p> <p>2017-12-01</p> <p>During October 2017 the <span class="hlt">Seismic</span> Source Facility (SSF) located at the University of Texas at El Paso (UTEP) Department of Geological Sciences collected <span class="hlt">seismic</span> data at SSF test facility located near Fabens, TX. The project objective was to compare source amplitudes and frequencies of various <span class="hlt">seismic</span> sources available through the SSF. Selecting the appropriate <span class="hlt">seismic</span> source is important to reach geological objectives. We compare <span class="hlt">seismic</span> sources between explosive sources (pentolite and shotgun) and mechanical sources (accelerated weight drop and hammer on plate), focusing on amplitude and frequency. All sources were tested in same geologic environment. Although this is not an ideal geologic formation for source coupling, it does allow an "apples to apples" comparison. Twenty Reftek RT125A <span class="hlt">seismic</span> <span class="hlt">recorders</span> with 4.5 Hz geophones were laid out in a line with 3m station separation. Mechanical sources were tested first to minimize changes in the subsurface related to explosive sources Explosive sources, while yielding higher amplitudes, have lower frequency content. The explosions exhibit a higher signal-to-noise ratio, allowing us to recognize <span class="hlt">seismic</span> energy deeper and farther from the source. Mechanical sources yield higher frequencies allowing better resolution at shallower depths, but have a lower signal-to-noise ratio and lower amplitudes, even with source stacking. We analyze the details of the shot spectra from the different types of sources. A combination of source types can improve data resolution and amplitude, thereby improving imaging potential. However, cost, logistics, and complexities also have a large influence on source selection.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015EGUGA..17.1460B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015EGUGA..17.1460B"><span>Time-lapse CO2 monitoring using ambient-noise <span class="hlt">seismic</span> interferometry: a feasibility study from Ketzin, Germany</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Boullenger, Boris; Verdel, Arie; Paap, Bob; Thorbecke, Jan; Draganov, Deyan</p> <p>2015-04-01</p> <p><span class="hlt">Seismic</span> interferometry applied to ambient-noise measurements allows retrieval of the Green's function between two <span class="hlt">seismic</span> receivers, by cross-correlating their <span class="hlt">recordings</span>, as if from a source at one of the receivers. We propose to use ambient-noise <span class="hlt">seismic</span> interferometry (ANSI) to retrieve reflection data. The time-lapse differences between different vintages of the retrieved data may help characterize property changes within a geologic reservoir with varying CO2 saturation. We test the feasibility of this time-lapse passive <span class="hlt">seismic</span> method with numerical experiments based on the CO2-storage site of Ketzin, Germany. Ambient-noise <span class="hlt">recordings</span> from Ketzin exhibit significant passive body-wave energy (from natural tremors or induced <span class="hlt">seismicity</span> in the vicinity of the reservoir), which is advantageous to retrieve reflections with ANSI. The ANSI numerical experiments aim to understand what the requirements are for the <span class="hlt">recorded</span> body-wave noise to retrieve the time-lapse reflection signal caused by an increase of CO2 saturation in the reservoir. For this purpose, we design two velocity scenarios at Ketzin: a base scenario before the injection of CO2, and a repeat scenario corresponding to a P-wave velocity decline in the reservoir by 20 percent. For both scenarios, we simulate passive <span class="hlt">seismic</span> experiments of body-wave noise <span class="hlt">recordings</span> that may take several days or months to <span class="hlt">record</span> in the field. The passive <span class="hlt">recordings</span> are obtained by modelling global (direct wave, internal and surface multiples) transmission responses from band-limited subsurface noise sources, randomly triggered in space and time. The time-lapse reflection signal is obtained by taking the differences between the base and the repeat retrieved reflection data (virtual common-shot gathers). We found that the time-lapse signal is still recovered with ANSI even if the base and repeat retrieved reflection data are partially polluted with artifacts. This means that uneven illumination of the array does not</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017SolE....8..531A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017SolE....8..531A"><span>Structure of the Suasselkä postglacial fault in northern Finland obtained by analysis of local events and ambient <span class="hlt">seismic</span> noise</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Afonin, Nikita; Kozlovskaya, Elena; Kukkonen, Ilmo; Dafne/Finland Working Group</p> <p>2017-04-01</p> <p>Understanding the inner structure of seismogenic faults and their ability to reactivate is particularly important in investigating the continental intraplate <span class="hlt">seismicity</span> regime. In our study we address this problem using analysis of local <span class="hlt">seismic</span> events and ambient <span class="hlt">seismic</span> noise <span class="hlt">recorded</span> by the temporary DAFNE array in the northern Fennoscandian Shield. The main purpose of the DAFNE/FINLAND passive <span class="hlt">seismic</span> array experiment was to characterize the present-day <span class="hlt">seismicity</span> of the Suasselkä postglacial fault (SPGF), which was proposed as one potential target for the DAFNE (Drilling Active Faults in Northern Europe) project. The DAFNE/FINLAND array comprised an area of about 20 to 100 km and consisted of eight short-period and four broadband three-component autonomous <span class="hlt">seismic</span> stations installed in the close vicinity of the fault area. The array <span class="hlt">recorded</span> continuous <span class="hlt">seismic</span> data during September 2011-May 2013. <span class="hlt">Recordings</span> of the array have being analysed in order to identify and locate natural earthquakes from the fault area and to discriminate them from the blasts in the Kittilä gold mine. As a result, we found a number of natural <span class="hlt">seismic</span> events originating from the fault area, which proves that the fault is still <span class="hlt">seismically</span> active. In order to study the inner structure of the SPGF we use cross-correlation of ambient <span class="hlt">seismic</span> noise <span class="hlt">recorded</span> by the array. Analysis of azimuthal distribution of noise sources demonstrated that during the time interval under consideration the distribution of noise sources is close to the uniform one. The continuous data were processed in several steps including single-station data analysis, instrument response removal and time-domain stacking. The data were used to estimate empirical Green's functions between pairs of stations in the frequency band of 0.1-1 Hz and to calculate corresponding surface wave dispersion curves. The S-wave velocity models were obtained as a result of dispersion curve inversion. The results suggest that the area of</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..1911233U','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..1911233U"><span>A Trial for Detecting the Temporal Variation in <span class="hlt">Seismic</span> Velocity Accompanied by a Slow Slip Event using <span class="hlt">Seismic</span> Interferometry of Ambient Noise</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Uemura, Miyuu; Ito, Yoshihiro; Ohta, Kazuaki; Hino, Ryota; Shinohara, Masanao</p> <p>2017-04-01</p> <p><span class="hlt">Seismic</span> interferometry is one of the most effective techniques to detect temporal variations in <span class="hlt">seismic</span> velocity before or after a large earthquake. Some previous studies have been reported on <span class="hlt">seismic</span> velocity reduction due to the occurrence of large earthquakes (e.g., Wegler et al., 2009; Yamada et al., 2010) as well as preceding them (e.g., Lockner et al., 1977; Yoshimitsu et al., 2009). However, there have only been a few studies thus far which attempt to detect <span class="hlt">seismic</span> velocity changes associated with slow slip events (SSEs). In this study, we focus on applying <span class="hlt">seismic</span> interferometry to ambient noise data from ocean bottom seismometers (OBSs) deployed near a subduction zone. Between the end of January 2011 and the largest foreshock occurring on March 9th that precedes the March 11, 2011 Tohoku-Oki earthquake, SSEs and low-frequency tremors were detected offshore Miyagi Prefecture (Ito et al., 2013, 2015; Katakami et al., 2016). We applied our <span class="hlt">seismic</span> interferometry analysis using ambient noise to <span class="hlt">recordings</span> from 17 OBS stations that were installed in the vicinity of the 2011 Tohoku-Oki earthquake source region, and only considered the <span class="hlt">recordings</span> from before that major earthquake. All the OBSs are short-period seismometers with three components which have an eigenfrequency of 4.5 Hz. These OBSs were deployed offshore Miyagi Prefecture between November 2010 and April 2011. Before proceeding with the <span class="hlt">seismic</span> interferometry analysis, we needed to estimate the two horizontal components of the original deployment orientation for 13 OBSs in (we could not estimate them for 4 OBSs). To obtain the OBS orientation, we used particle orbits of some direct P waves from selected tectonic earthquakes, in order to extract one vertical and two horizontal components. Then, the <span class="hlt">seismic</span> interferometry analysis consisted of the following steps. First, we applied a band-pass filter of 0.25-2.0 Hz and one-bit technique to the ambient noise signal. Second, we calculated auto</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016DPS....4851312J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016DPS....4851312J"><span>Recent Impacts on Mars: Cluster Properties and <span class="hlt">Seismic</span> Signal Predictions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Justine Daubar, Ingrid; Schmerr, Nicholas; Banks, Maria; Marusiak, Angela; Golombek, Matthew P.</p> <p>2016-10-01</p> <p>Impacts are a key source of <span class="hlt">seismic</span> waves that are a primary constraint on the formation, evolution, and dynamics of planetary objects. Geophysical missions such as InSight (Banerdt et al., 2013) will monitor <span class="hlt">seismic</span> signals from internal and external sources. New martian craters have been identified in orbital images (Malin et al., 2006; Daubar et al., 2013). <span class="hlt">Seismically</span> detecting such impacts and subsequently imaging the resulting craters will provide extremely accurate epicenters and source crater sizes, enabling calibration of <span class="hlt">seismic</span> velocities, the efficiency of impact-<span class="hlt">seismic</span> coupling, and retrieval of detailed regional and local internal structure.To investigate recent impact-induced <span class="hlt">seismicity</span> on Mars, we have assessed ~100 new, dated impact sites. In approximately half of new impacts, the bolide partially disintegrates in the atmosphere, forming multiple craters in a cluster. We incorporate the resulting, more complex, <span class="hlt">seismic</span> effects in our model. To characterize the variation between sites, we focus on clustered impacts. We report statistics of craters within clusters: diameters, morphometry indicating subsurface layering, strewn-field azimuths indicating impact direction, and dispersion within clusters indicating combined effects of bolide strength and elevation of breakup.Measured parameters are converted to <span class="hlt">seismic</span> predictions for impact sources using a scaling law relating crater diameter to the momentum and source duration, calibrated for impacts <span class="hlt">recorded</span> by Apollo (Lognonne et al., 2009). We use plausible ranges for target properties, bolide densities, and impact velocities to bound the <span class="hlt">seismic</span> moment. The expected <span class="hlt">seismic</span> sources are modeled in the near field using a 3-D wave propagation code (Petersson et al., 2010) and in the far field using a 1-D wave propagation code (Friederich et al., 1995), for a martian <span class="hlt">seismic</span> model. Thus we calculate the amplitudes of <span class="hlt">seismic</span> phases at varying distances, which can be used to evaluate the detectability</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26173557','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26173557"><span><span class="hlt">Seismic</span> footprints of shallow dyke propagation at Etna, Italy.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Falsaperla, Susanna; Neri, Marco</p> <p>2015-07-15</p> <p>One of the key issues in forecasting volcanic eruptions is to detect signals that can track the propagation of dykes towards the surface. Continuous monitoring of active volcanoes helps significantly in achieving this goal. The <span class="hlt">seismic</span> data presented here are unique, as they document surface faulting processes close (tens to a few hundred meters) to their source, namely the dyke tip. They originated nearby - and under - a <span class="hlt">seismic</span> station that was subsequently destroyed by lava flows during eruptive activity at Etna volcano, Italy, in 2013. On February 20, a ~600 m-long and ~120 m wide NW-SE fracture field opened at an altitude between 2750 and 2900 m. The consequent rock dislocation caused the station to tilt and offset the <span class="hlt">seismic</span> signal temporarily. Data acquisition continued until the arrival of the lava flow that led to the breakdown of the transmission system. Shallow ground fracturing and repeated low-frequency oscillations occurred during two stages in which the <span class="hlt">seismic</span> signal underwent a maximum offset ~2.57 × 10(4) nm/s. Bridging instrumental <span class="hlt">recordings</span>, fieldwork and conceptual modelling, these data are interpreted as the <span class="hlt">seismic</span> footprints of a magmatic dyke intrusion that moved at speed ~0.02 m/s (first stage) and 0.46 m/s (second stage).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.usgs.gov/of/2006/1231/','USGSPUBS'); return false;" href="https://pubs.usgs.gov/of/2006/1231/"><span>Hawaiian Volcano Observatory <span class="hlt">seismic</span> data, January to December 2005</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Nakata, Jennifer S.</p> <p>2006-01-01</p> <p>The Hawaiian Volcano Observatory (HVO) summary presents <span class="hlt">seismic</span> data gathered during the year. The <span class="hlt">seismic</span> summary is offered without interpretation as a source of preliminary data. It is complete in the sense that most data for events of M-1.5 routinely gathered by the Observatory are included. The HVO summaries have been published in various forms since 1956. Summaries prior to 1974 were issued quarterly, but cost, convenience of preparation and distribution, and the large quantities of data dictated an annual publication beginning with Summary 74 for the year 1974. Summary 86 (the introduction of CUSP at HVO) includes a description of the <span class="hlt">seismic</span> instrumentation, calibration, and processing used in recent years. Beginning with 2004, summaries will simply be identified by the year, rather than Summary number. The present summary includes background information on the <span class="hlt">seismic</span> network and processing to allow use of the data and to provide an understanding of how they were gathered. A report by Klein and Koyanagi (1980) tabulates instrumentation, calibration, and <span class="hlt">recording</span> history of each <span class="hlt">seismic</span> station in the network. It is designed as a reference for users of seismograms and phase data and includes and augments the information in the station table in this summary.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.usgs.gov/of/2007/1073/','USGSPUBS'); return false;" href="https://pubs.usgs.gov/of/2007/1073/"><span>Hawaiian Volcano Observatory <span class="hlt">Seismic</span> Data, January to December 2006</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Nakata, Jennifer</p> <p>2007-01-01</p> <p>Introduction The Hawaiian Volcano Observatory (HVO) summary presents <span class="hlt">seismic</span> data gathered during the year. The <span class="hlt">seismic</span> summary is offered without interpretation as a source of preliminary data. It is complete in the sense that most data for events of M>1.5 routinely gathered by the Observatory are included. The HVO summaries have been published in various forms since 1956. Summaries prior to 1974 were issued quarterly, but cost, convenience of preparation and distribution, and the large quantities of data dictated an annual publication beginning with Summary 74 for the year 1974. Summary 86 (the introduction of CUSP at HVO) includes a description of the <span class="hlt">seismic</span> instrumentation, calibration, and processing used in recent years. Beginning with 2004, summaries are simply identified by the year, rather than Summary number. The present summary includes background information on the <span class="hlt">seismic</span> network and processing to allow use of the data and to provide an understanding of how they were gathered. A report by Klein and Koyanagi (1980) tabulates instrumentation, calibration, and <span class="hlt">recording</span> history of each <span class="hlt">seismic</span> station in the network. It is designed as a reference for users of seismograms and phase data and includes and augments the information in the station table in this summary.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2010-title6-vol1/pdf/CFR-2010-title6-vol1-part5-appC.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title6-vol1/pdf/CFR-2010-title6-vol1-part5-appC.pdf"><span>6 CFR Appendix <span class="hlt">C</span> to Part 5 - DHS Systems of <span class="hlt">Records</span> Exempt From the Privacy Act</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2010&page.go=Go">Code of Federal Regulations, 2010 CFR</a></p> <p></p> <p>2010-01-01</p> <p>... DISCLOSURE OF <span class="hlt">RECORDS</span> AND INFORMATION Pt. 5, App. <span class="hlt">C</span> Appendix <span class="hlt">C</span> to Part 5—DHS Systems of <span class="hlt">Records</span> Exempt From... Homeland Security (DHS) Freedom of Information Act (FOIA) and Privacy Act (PA) <span class="hlt">Record</span> System allows the DHS... information contained in other systems of <span class="hlt">records</span> subject to such exemptions pursuant to 5 U.S.<span class="hlt">C</span>. 552a(j)(2...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.S13C0676L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.S13C0676L"><span>Amplification Factors for Spectral Acceleration Using Borehole <span class="hlt">Seismic</span> Array in Taiwan</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lai, T. S.; Yih-Min, W.; Chao, W. A.; Chang, C. H.</p> <p>2017-12-01</p> <p>In order to reduce the noise from surface to get the high-quality <span class="hlt">seismic</span> <span class="hlt">recordings</span>, there are 54 borehole <span class="hlt">seismic</span> arrays have been installed in Taiwan deployed by Central Weather Bureau (CWB) until the end of 2016. Each array includes two force balance accelerometers, one at the surface and other inside the borehole, as well as one broadband seismometer inside the borehole. The downhole instruments are placed at a depth between 120 and 400 m. The background noise level are lower at the borehole stations, but the amplitudes <span class="hlt">recorded</span> by borehole stations are smaller than surface stations for the same earthquake due to the different geology conditions. Therefore, the earthquake magnitude estimated by borehole station is smaller than surface station. So far, CWB only use the surface stations in the magnitude determination due to this situation. In this study, we investigate the site effects between surface and downhole for borehole <span class="hlt">seismic</span> arrays. Using the spectral ratio derived by the two-station spectral method as the transfer function, simulated the waveform <span class="hlt">recorded</span> by borehole stations to the surface stations. In the future, through the transfer function, the borehole stations will be included in the estimation of earthquake magnitude and the results of amplification factors can provide the information of near-surface site effects for the ground motion simulation applications.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009AIPC.1118...58S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009AIPC.1118...58S"><span>Seismo-Electromagnetic Emissions Related to <span class="hlt">Seismic</span> Waves can Trigger TLEs</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sorokin, Leonid V.</p> <p>2009-04-01</p> <p>This paper deals with the rare high intensity electromagnetic pulses associated with earthquakes, whose spectrum signature differs from that of atmospherics produced by lightning discharges. On the basis of actual data <span class="hlt">records</span>, cases of the generation of anomalous seismo-electromagnetic emissions are described. These natural sub-millisecond electromagnetic pulses were associated with the passage of <span class="hlt">seismic</span> waves from earthquakes to Moscow, the place where the electromagnetic field observations were made. Space-time coupling has been revealed between exact <span class="hlt">seismic</span> waves from the earthquakes, lightning triggering and Transient Luminous Events triggering.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li class="active"><span>25</span></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_25 --> <div class="footer-extlink text-muted" style="margin-bottom:1rem; text-align:center;">Some links on this page may take you to non-federal websites. 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