Sample records for observations captured solar

  1. Dynamics of Coronal Structures Captured During the 2012 and 2013 Total Solar Eclipses

    NASA Astrophysics Data System (ADS)

    Alzate, N.; Habbal, S. R.; Druckmuller, M.

    2017-12-01

    White light eclipse images taken during total solar eclipses provide a very high dynamic range spanning tens of solar radii starting from the solar surface. They capture the instantaneous state of the corona, including dynamic events. We present observations of the 2012 November 13 and 2013 November 3 total solar eclipses, taken by Constantinos Emmanouilidis, in which we captured high latitude tethered prominences accompanied by CMEs, as well as several `atypical' large scale structures, spanning a few solar radii above the solar surface. By complementing the eclipse observations with co-temporaneous SDO/AIA, STEREO/EUVI and SOHO/LASCO observations, we show how the shape of the atypical structures outlines the shape of faint CME shock fronts, driven by flaring activities. The tethered prominences were imaged from their anchor at the solar surface out to several solar radii. The SDO/AIA 30.4, 17.1 and 19.3 nm emission clearly show how a direct link between the cool (104 - 105 K) filamentary emission from prominence material, and the filamentary structures emitting at coronal temperatures (> 106 K), is unmistakably present. The observed survival of these tethered systems out to the field of view of LASCO C3, establishes the likely origin of counter-streaming electrons associated with CMEs observed in interplanetary space (ICMEs). They also provide new insights for CME-initiation models associated with prominence eruptions. Our work highlights the uniqueness of eclipse observations in identifying the impact of transit events on large-scale coronal structures.

  2. Solar wind alpha particle capture at Mars and Venus

    NASA Astrophysics Data System (ADS)

    Stenberg, Gabriella; Barabash, Stas; Nilsson, Hans; Fedorov, A.; Brain, David; André, Mats

    Helium is detected in the atmospheres of both Mars and Venus. It is believed that radioactive decay of uranium and thorium in the interior of the planets' is not sufficient to account for the abundance of helium observed. Alpha particles in the solar wind are suggested to be an additional source of helium, especially at Mars. Recent hybrid simulations show that as much as 30We use ion data from the ASPERA-3 and ASPERA-4 instruments on Mars and Venus Express to estimate how efficient solar wind alpha particles are captured in the atmospheres of the two planets.

  3. Solar Eclipse Video Captured by STEREO-B

    NASA Technical Reports Server (NTRS)

    2007-01-01

    No human has ever witnessed a solar eclipse quite like the one captured on this video. The NASA STEREO-B spacecraft, managed by the Goddard Space Center, was about a million miles from Earth , February 25, 2007, when it photographed the Moon passing in front of the sun. The resulting movie looks like it came from an alien solar system. The fantastically-colored star is our own sun as STEREO sees it in four wavelengths of extreme ultraviolet light. The black disk is the Moon. When we observe a lunar transit from Earth, the Moon appears to be the same size as the sun, a coincidence that produces intoxicatingly beautiful solar eclipses. The silhouette STEREO-B saw, on the other hand, was only a fraction of the Sun. The Moon seems small because of the STEREO-B location. The spacecraft circles the sun in an Earth-like orbit, but it lags behind Earth by one million miles. This means STEREO-B is 4.4 times further from the Moon than we are, and so the Moon looks 4.4 times smaller. This version of the STEREO-B eclipse movie is a composite of data from the coronagraph and extreme ultraviolet imager of the spacecraft. STEREO-B has a sister ship named STEREO-A. Both are on a mission to study the sun. While STEREO-B lags behind Earth, STEREO-A orbits one million miles ahead ('B' for behind, 'A' for ahead). The gap is deliberate as it allows the two spacecraft to capture offset views of the sun. Researchers can then combine the images to produce 3D stereo movies of solar storms. The two spacecraft were launched in Oct. 2006 and reached their stations on either side of Earth in January 2007.

  4. NASA’s Solar Dynamics Observatory Captured Trio of Solar Flares April 2-3

    NASA Image and Video Library

    2017-12-08

    The sun emitted a trio of mid-level solar flares on April 2-3, 2017. The first peaked at 4:02 a.m. EDT on April 2, the second peaked at 4:33 p.m. EDT on April 2, and the third peaked at 10:29 a.m. EDT on April 3. NASA’s Solar Dynamics Observatory, which watches the sun constantly, captured images of the three events. Solar flares are powerful bursts of radiation. Harmful radiation from a flare cannot pass through Earth's atmosphere to physically affect humans on the ground, however — when intense enough — they can disturb the atmosphere in the layer where GPS and communications signals travel. Learn more: go.nasa.gov/2oQVFju Caption: NASA's Solar Dynamics Observatory captured this image of a solar flare peaking at 10:29 a.m. EDT on April 3, 2017, as seen in the bright flash near the sun’s upper right edge. The image shows a subset of extreme ultraviolet light that highlights the extremely hot material in flares and which is typically colorized in teal. Credits: NASA/SDO NASA image use policy. NASA Goddard Space Flight Center enables NASA’s mission through four scientific endeavors: Earth Science, Heliophysics, Solar System Exploration, and Astrophysics. Goddard plays a leading role in NASA’s accomplishments by contributing compelling scientific knowledge to advance the Agency’s mission. Follow us on Twitter Like us on Facebook Find us on Instagram

  5. High-Order Shock-Capturing Methods for Modeling Dynamics of the Solar Atmosphere

    NASA Technical Reports Server (NTRS)

    Bryson, Steve; Kosovichev, Alexander; Levy, Doron

    2004-01-01

    We use one-dimensional high-order central shock capturing numerical methods to study the response of various model solar atmospheres to forcing at the solar surface. The dynamics of the atmosphere is modeled with the Euler equations in a variable-sized flux tube in the presence of gravity. We study dynamics of the atmosphere suggestive of spicule formation and coronal oscillations. These studies are performed on observationally-derived model atmospheres above the quiet sun and above sunspots. To perform these simulations, we provide a new extension of existing second- and third- order shock-capturing methods to irregular grids. We also solve the problem of numerically maintaining initial hydrostatic balance via the introduction of new variables in the model equations and a careful initialization mechanism. We find several striking results: all model atmospheres respond to a single impulsive perturbation with several strong shock waves consistent with the rebound-shock model. These shock waves lift material and the transition region well into the initial corona, and the sensitivity of this lift to the initial impulse depends non-linearly on the details of the atmosphere model. We also reproduce an observed 3-minute coronal oscillation above sunspots compared to 5-minute oscillations above the quiet sun.

  6. The Unique Scientific Assets of Multi-Wavelength Total Solar Eclipse Observations

    NASA Astrophysics Data System (ADS)

    Habbal, S. R.; Druckmuller, M.; Ding, A.

    2017-12-01

    Total solar eclipses continue to yield new discoveries regarding the dynamics and thermodynamics of the corona, due to the radial span of the field of view available during totality, starting from the solar surface out to several solar radii, and due to the diagnostic potential provided by coronal emission lines. Scientific highlights from past eclipse observations as well as from the 21 August 2017 eclipse, now spanning a solar cycle, will be presented. These include white light and spectral line imaging as well as imaging spectrometry. Emphasis will be placed on the unique insights into the origin of dynamic structures captured in eclipse images, and the temperature distribution in the corona derived from these eclipse observations. Implications of these results for the general problem of coronal heating, as well as for the next generation of space instrumentation will be discussed.

  7. Atmospheric Mining in the Outer Solar System: Resource Capturing, Storage, and Utilization

    NASA Technical Reports Server (NTRS)

    Palaszewski, Bryan

    2012-01-01

    Atmospheric mining in the outer solar system has been investigated as a means of fuel production for high energy propulsion and power. Fusion fuels such as Helium 3 (3He) and hydrogen can be wrested from the atmospheres of Uranus and Neptune and either returned to Earth or used in-situ for energy production. Helium 3 and hydrogen (deuterium, etc.) were the primary gases of interest with hydrogen being the primary propellant for nuclear thermal solid core and gas core rocket-based atmospheric flight. A series of analyses were undertaken to investigate resource capturing aspects of atmospheric mining in the outer solar system. This included the gas capturing rate for hydrogen helium 4 and helium 3, storage options, and different methods of direct use of the captured gases. Additional supporting analyses were conducted to illuminate vehicle sizing and orbital transportation issues.

  8. Atmospheric Mining in the Outer Solar System: Resource Capturing, Storage, and Utilization

    NASA Technical Reports Server (NTRS)

    Palaszewski, Bryan

    2014-01-01

    Atmospheric mining in the outer solar system has been investigated as a means of fuel production for high energy propulsion and power. Fusion fuels such as helium 3 and hydrogen can be wrested from the atmospheres of Uranus and Neptune and either returned to Earth or used in-situ for energy production. Helium 3 and hydrogen (deuterium, etc.) were the primary gases of interest with hydrogen being the primary propellant for nuclear thermal solid core and gas core rocket-based atmospheric flight. A series of analyses were undertaken to investigate resource capturing aspects of atmospheric mining in the outer solar system. This included the gas capturing rate for hydrogen helium 4 and helium 3, storage options, and different methods of direct use of the captured gases. Additional supporting analyses were conducted to illuminate vehicle sizing and orbital transportation issues.

  9. Analysis of daylight performance of solar light pipes influenced by size and shape of sunlight captures

    NASA Astrophysics Data System (ADS)

    Wu, Yanpeng; Jin, Rendong; Zhang, Wenming; Liu, Li; Zou, Dachao

    2009-11-01

    Experimental investigations on three different sunlight captures with diameter 150mm, 212mm, 300mm were carried out under different conditions such as sunny conditions, cloudy conditions and overcast conditions and the two different size solar light pipes with diameter 360mm and 160mm under sunny conditions. The illuminance in the middle of the sunlight capture have relationship with its size, but not linear. To improve the efficiency of the solar light pipes, the structure and the performance of the sunlight capture must be enhanced. For example, University of Science and Technology Beijing Gymnasium, Beijing 2008 Olympic events of Judo and Taekwondo, 148 solar light pipes were installed with the diameter 530mm for each light pipe. Two sunlight captures with different shape were installed and tested. From the measuring results of the illuminance on the work plane of the gymnasium, the improvement sunlight captures have better effects with the size of augmenting and the machining of the internal surface at the same time, so that the refraction increased and the efficiency of solar light pipes improved. The better effects of supplementary lighting for the gymnasium have been achieved.

  10. The solar maximum satellite capture cell: Impact features and orbital debris and micrometeoritic projectile materials

    NASA Technical Reports Server (NTRS)

    Mckay, D. S.; Rietmeijer, F. J. M.; Schramm, L. S.; Barrett, R. A.; Zook, H. A.; Blanford, G. E.

    1986-01-01

    The physical properties of impact features observed in the Solar Max main electronics box (MEB) thermal blanket generally suggest an origin by hypervelocity impact. The chemistry of micrometeorite material suggests that a wide variety of projectile materials have survived impact with retention of varying degrees of pristinity. Impact features that contain only spacecraft paint particles are on average smaller than impact features caused by micrometeorite impacts. In case both types of materials co-occur, it is belevied that the impact feature, generally a penetration hole, was caused by a micrometeorite projectile. The typically smaller paint particles were able to penetrate though the hole in the first layer and deposit in the spray pattern on the second layer. It is suggested that paint particles have arrived with a wide range of velocities relative to the Solar Max satellite. Orbiting paint particles are an important fraction of materials in the near-Earth environment. In general, the data from the Solar Max studies are a good calibration for the design of capture cells to be flown in space and on board Space Station. The data also suggest that development of multiple layer capture cells in which the projectile may retain a large degree of pristinity is a feasible goal.

  11. Solar Observations with ALMA

    NASA Astrophysics Data System (ADS)

    Wedemeyer, Sven

    2018-04-01

    The continuum intensity at millimeter wavelengths can serve as an essentially linear thermometer of the plasma in a thin layer in the atmosphere of the Sun, whereas the polarisation of the received radiation is a measure for the longitudinal magnetic field component in the same layer. The enormous leap in terms of spatial resolution with the Atacama Large Millimeter/submillimeter Array (ALMA) now makes it possible to observe the intricate fine-structure of the solar atmosphere at sufficiently high spatial, temporal, and spectral resolution, thus enabling studies of a wide range of scientific topics in solar physics that had been inaccessible at millimeter wavelengths before. The radiation observed by ALMA originates mostly from the chromosphere - a complex and dynamic layer between the photosphere and corona, which plays a crucial role in the transport of energy and matter and, ultimately, the heating of the outer solar atmosphere. ALMA observations of the solar chromosphere, which are offered as a regular capability since 2016, therefore have the potential to make important contributions towards the solution of fundamental questions in solar physics with implications for our understanding of stars in general. In this presentation, I will give a short description of ALMA's solar observing mode, it challenges and opportunities, and selected science cases in combination with numerical simulations and coordinated observations at other wavelengths. ALMA's scientific potential for studying the dynamic small-scale pattern of the solar chromosphere is illustrated with first results from Cycle 4.

  12. Long-term solar-terrestrial observations

    NASA Technical Reports Server (NTRS)

    1988-01-01

    The results of an 18-month study of the requirements for long-term monitoring and archiving of solar-terrestrial data is presented. The value of long-term solar-terrestrial observations is discussed together with parameters, associated measurements, and observational problem areas in each of the solar-terrestrial links (the sun, the interplanetary medium, the magnetosphere, and the thermosphere-ionosphere). Some recommendations are offered for coordinated planning for long-term solar-terrestrial observations.

  13. Bayesian Analysis Of HMI Solar Image Observables And Comparison To TSI Variations And MWO Image Observables

    NASA Astrophysics Data System (ADS)

    Parker, D. G.; Ulrich, R. K.; Beck, J.

    2014-12-01

    We have previously applied the Bayesian automatic classification system AutoClass to solar magnetogram and intensity images from the 150 Foot Solar Tower at Mount Wilson to identify classes of solar surface features associated with variations in total solar irradiance (TSI) and, using those identifications, modeled TSI time series with improved accuracy (r > 0.96). (Ulrich, et al, 2010) AutoClass identifies classes by a two-step process in which it: (1) finds, without human supervision, a set of class definitions based on specified attributes of a sample of the image data pixels, such as magnetic field and intensity in the case of MWO images, and (2) applies the class definitions thus found to new data sets to identify automatically in them the classes found in the sample set. HMI high resolution images capture four observables-magnetic field, continuum intensity, line depth and line width-in contrast to MWO's two observables-magnetic field and intensity. In this study, we apply AutoClass to the HMI observables for images from May, 2010 to June, 2014 to identify solar surface feature classes. We use contemporaneous TSI measurements to determine whether and how variations in the HMI classes are related to TSI variations and compare the characteristic statistics of the HMI classes to those found from MWO images. We also attempt to derive scale factors between the HMI and MWO magnetic and intensity observables. The ability to categorize automatically surface features in the HMI images holds out the promise of consistent, relatively quick and manageable analysis of the large quantity of data available in these images. Given that the classes found in MWO images using AutoClass have been found to improve modeling of TSI, application of AutoClass to the more complex HMI images should enhance understanding of the physical processes at work in solar surface features and their implications for the solar-terrestrial environment. Ulrich, R.K., Parker, D, Bertello, L. and

  14. NASA's SDO Observes an X-class Solar Flare

    NASA Image and Video Library

    2017-12-08

    The sun emitted a significant solar flare, peaking at 1:01 a.m. EDT on Oct. 19, 2014. NASA's Solar Dynamics Observatory, which is always observing the sun, captured an image of the event. Solar flares are powerful bursts of radiation. Harmful radiation from a flare cannot pass through Earth's atmosphere to physically affect humans on the ground, however -- when intense enough -- they can disturb the atmosphere in the layer where GPS and communications signals travel. To see how this event may affect Earth, please visit NOAA's Space Weather Prediction Center at spaceweather.gov, the U.S. government's official source for space weather forecasts, alerts, watches and warnings. This flare is classified as an X1.1-class flare. X-class denotes the most intense flares, while the number provides more information about its strength. An X2 is twice as intense as an X1, an X3 is three times as intense, etc. Credit: NASA/SDO NASA image use policy. NASA Goddard Space Flight Center enables NASA’s mission through four scientific endeavors: Earth Science, Heliophysics, Solar System Exploration, and Astrophysics. Goddard plays a leading role in NASA’s accomplishments by contributing compelling scientific knowledge to advance the Agency’s mission. Follow us on Twitter Like us on Facebook Find us on Instagram

  15. Ion Acceleration in Solar Flares Determined by Solar Neutron Observations

    NASA Astrophysics Data System (ADS)

    Watanabe, K.; Solar Neutron Observation Group

    2013-05-01

    Large amounts of particles can be accelerated to relativistic energy in association with solar flares and/or accompanying phenomena (e.g., CME-driven shocks), and they sometimes reach very near the Earth and penetrate the Earth's atmosphere. These particles are observed by ground-based detectors (e.g., neutron monitors) as Ground Level Enhancements (GLEs). Some of the GLEs originate from high energy solar neutrons which are produced in association with solar flares. These neutrons are also observed by ground-based neutron monitors and solar neutron telescopes. Recently, some of the solar neutron detectors have also been operating in space. By observing these solar neutrons, we can obtain information about ion acceleration in solar flares. Such neutrons were observed in association with some X-class flares in solar cycle 23, and sometimes they were observed by two different types of detectors. For example, on 2005 September 7, large solar neutron signals were observed by the neutron monitor at Mt. Chacaltaya in Bolivia and Mexico City, and by the solar neutron telescopes at Chacaltaya and Mt. Sierra Negra in Mexico in association with an X17.0 flare. The neutron signal continued for more than 20 minutes with high statistical significance. Intense gamma-ray emission was also registered by INTEGRAL, and by RHESSI during the decay phase. We analyzed these data using the solar-flare magnetic-loop transport and interaction model of Hua et al. (2002), and found that the model could successfully fit the data with intermediate values of loop magnetic convergence and pitch angle scattering parameters. These results indicate that solar neutrons were produced at the same time as the gamma-ray line emission and that ions were continuously accelerated at the emission site. In this paper, we introduce some of the solar neutron observations in solar cycle 23, and discuss the tendencies of the physical parameters of solar neutron GLEs, and the energy spectrum and population of the

  16. Hybrid photosynthesis-powering biocatalysts with solar energy captured by inorganic devices.

    PubMed

    Zhang, Tian; Tremblay, Pier-Luc

    2017-01-01

    The biological reduction of CO 2 driven by sunlight via photosynthesis is a crucial process for life on earth. However, the conversion efficiency of solar energy to biomass by natural photosynthesis is low. This translates in bioproduction processes relying on natural photosynthesis that are inefficient energetically. Recently, hybrid photosynthetic technologies with the potential of significantly increasing the efficiency of solar energy conversion to products have been developed. In these systems, the reduction of CO 2 into biofuels or other chemicals of interest by biocatalysts is driven by solar energy captured with inorganic devices such as photovoltaic cells or photoelectrodes. Here, we explore hybrid photosynthesis and examine the strategies being deployed to improve this biotechnology.

  17. COMPTEL solar flare observations

    NASA Technical Reports Server (NTRS)

    Ryan, J. M.; Aarts, H.; Bennett, K.; Debrunner, H.; Devries, C.; Denherder, J. W.; Eymann, G.; Forrest, D. J.; Diehl, R.; Hermsen, W.

    1992-01-01

    COMPTEL as part of a solar target of opportunity campaign observed the sun during the period of high solar activity from 7-15 Jun. 1991. Major flares were observed on 9 and 11 Jun. Although both flares were large GOES events (greater than or = X10), they were not extraordinary in terms of gamma-ray emission. Only the decay phase of the 15 Jun. flare was observed by COMPTEL. We report the preliminary analysis of data from these flares, including the first spectroscopic measurement of solar flare neutrons. The deuterium formation line at 2.223 MeV was present in both events and for at least the 9 Jun. event, was comparable to the flux in the nuclear line region of 4-8 MeV, consistent with Solar-Maximum Mission (SSM) Observations. A clear neutron signal was present in the flare of 9 Jun. with the spectrum extending up to 80 MeV and consistent in time with the emission of gamma-rays, confirming the utility of COMPTEL in measuring the solar neutron flux at low energies. The neutron flux below 100 MeV appears to be lower than that of the 3 Jun. 1982 flare by more than an order of magnitude. The neutron signal of the 11 Jun. event is under study. Severe dead time effects resulting from the intense thermal x-rays require significant corrections to the measured flux which increase the magnitude of the associated systematic uncertainties.

  18. Efficient solar-driven synthesis, carbon capture, and desalinization, STEP: solar thermal electrochemical production of fuels, metals, bleach.

    PubMed

    Licht, S

    2011-12-15

    STEP (solar thermal electrochemical production) theory is derived and experimentally verified for the electrosynthesis of energetic molecules at solar energy efficiency greater than any photovoltaic conversion efficiency. In STEP the efficient formation of metals, fuels, chlorine, and carbon capture is driven by solar thermal heated endothermic electrolyses of concentrated reactants occuring at a voltage below that of the room temperature energy stored in the products. One example is CO(2) , which is reduced to either fuels or storable carbon at a solar efficiency of over 50% due to a synergy of efficient solar thermal absorption and electrochemical conversion at high temperature and reactant concentration. CO(2) -free production of iron by STEP, from iron ore, occurs via Fe(III) in molten carbonate. Water is efficiently split to hydrogen by molten hydroxide electrolysis, and chlorine, sodium, and magnesium from molten chlorides. A pathway is provided for the STEP decrease of atmospheric carbon dioxide levels to pre-industial age levels in 10 years. Copyright © 2011 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim.

  19. Solar Eclipses Observed from Antarctica

    NASA Astrophysics Data System (ADS)

    Pasachoff, Jay M.

    2013-01-01

    Aspects of the solar corona are still best observed during totality of solar eclipses, and other high-resolution observations of coronal active regions can be observed with radio telescopes by differentiation of occultation observations, as we did with the Jansky Very Large Array for the annular solar eclipse of 2012 May 20 in the US. Totality crossing Antarctica included the eclipse of 2003 November 23, and will next occur on 2021 December 4; annularity crossing Antarctica included the eclipse of 2008 February 7, and will next occur on 2014 April 29. Partial phases as high as 87% coverage were visible and were imaged in Antarctica on 2011 November 25, and in addition to partial phases of the total and annular eclipses listed above, partial phases were visible in Antarctica on 2001 July 2011, 2002 December 4, 2004 April 19, 2006 September 22, 2007 September 11, and 2009 January 26, and will be visible on 2015 September 13, 2016 September 1, 2017 February 26, 2018 February 15, and 2020 December 14. On behalf of the Working Group on Solar Eclipses of the IAU, the poster showed the solar eclipses visible from Antarctica and this article shows a subset (see www.eclipses.info for the full set). A variety of investigations of the Sun and of the response of the terrestrial atmosphere and ionosphere to the abrupt solar cutoff can be carried out at the future eclipses, making the Antarctic observations scientifically useful.

  20. Solar Neutrinos

    DOE R&D Accomplishments Database

    Davis, R. Jr.; Harmer, D. S.

    1964-12-01

    The prospect of studying the solar energy generation process directly by observing the solar neutrino radiation has been discussed for many years. The main difficulty with this approach is that the sun emits predominantly low energy neutrinos, and detectors for observing low fluxes of low energy neutrinos have not been developed. However, experimental techniques have been developed for observing neutrinos, and one can foresee that in the near future these techniques will be improved sufficiently in sensitivity to observe solar neutrinos. At the present several experiments are being designed and hopefully will be operating in the next year or so. We will discuss an experiment based upon a neutrino capture reaction that is the inverse of the electron-capture radioactive decay of argon-37. The method depends upon exposing a large volume of a chlorine compound, removing the radioactive argon-37 and observing the characteristic decay in a small low-level counter.

  1. Development of gridded solar radiation data over Belgium based on Meteosat and in-situ observations

    NASA Astrophysics Data System (ADS)

    Journée, Michel; Vanderveken, Gilles; Bertrand, Cédric

    2013-04-01

    Knowledge on solar resources is highly important for all forms of solar energy applications. With the recent development in solar-based technologies national meteorological services are faced with increasing demands for high-quality and reliable site-time specific solar resource information. Traditionally, solar radiation is observed by means of networks of meteorological stations. Costs for installation and maintenance of such networks are very high and national networks comprise only few stations. Consequently the availability of ground-based solar radiation measurements has proven to be spatially and temporally inadequate for many applications. To overcome such a limitation, a major effort has been undertaken at the Royal Meteorological Institute of Belgium (RMI) to provide the solar energy industry, the electricity sector, governments, and renewable energy organizations and institutions with the most suitable and accurate information on the solar radiation resources at the Earth's surface over the Belgian territory. Only space-based observations can deliver a global coverage of the solar irradiation impinging on horizontal surface at the ground level. Because only geostationary data allow to capture the diurnal cycle of the solar irradiance at the Earth's surface, a method that combines information from Meteosat Second Generation satellites and ground-measurement has been implemented at RMI to generate high resolution solar products over Belgium on an operational basis. Besides these new products, the annual and seasonal variability of solar energy resource was evaluated, solar radiation climate zones were defined and the recent trend in solar radiation was characterized.

  2. Chandra Observations of the Solar System

    NASA Astrophysics Data System (ADS)

    Lisse, Carey

    2014-11-01

    Many solar system objects are now known to emit X-rays due to charge-exchange between highly charged solar wind (SW) minor ions and neutrals in their extended atmospheres, including Earth, Venus, Mars, Jupiter, and the heliosphere, with total power outputs on the MW - GW scale. (Currently only upper limits exist for Saturn and Pluto.) Chandra observations of their morphology, spectra, and time dependence provide important information about the neutral atmosphere structure and the SW flux and charge state. Chandra observations of solar x-ray scattering from Earth, Venus, Mars, Jupiter, Saturn, and the Moon have also provided important clues for the scattering material and the solar radiation field at the body. We present here a 15 year summary of Chandra's solar system observations.

  3. Perception of Solar Eclipses Captured by Art Explains How Imaging Misrepresented the Source of the Solar Wind

    PubMed Central

    2015-01-01

    The visible corona revealed by the natural phenomenon of solar eclipses has been studied for 150 years. A turning point has been the discovery that the true spatial distribution of coronal brightness can neither be seen nor imaged on account of its unprecedented dynamic range. Howard Russell Butler (1856–1934), the painter of solar eclipses in the early 20th century, possessed the extraordinary skill of painting from memory what he saw for only a brief time. His remarkable but forgotten eclipse paintings are, therefore, ideal for capturing and representing best the perceptual experience of the visible corona. Explained here is how by bridging the eras of visual (late 19th century) and imaging investigations (since the latter half of the 20th century), Butler’s paintings reveal why white-light images misled researching and understanding the Sun’s atmosphere, the solar wind. The closure in understanding solar eclipses through the convergence of perception, art, imaging, science and the history of science promises to enrich the experience of viewing and photographing the first solar eclipse of the 21st century in the United States on 21st August 2017. PMID:27551356

  4. Perception of Solar Eclipses Captured by Art Explains How Imaging Misrepresented the Source of the Solar Wind.

    PubMed

    Woo, Richard

    2015-12-01

    The visible corona revealed by the natural phenomenon of solar eclipses has been studied for 150 years. A turning point has been the discovery that the true spatial distribution of coronal brightness can neither be seen nor imaged on account of its unprecedented dynamic range. Howard Russell Butler (1856-1934), the painter of solar eclipses in the early 20th century, possessed the extraordinary skill of painting from memory what he saw for only a brief time. His remarkable but forgotten eclipse paintings are, therefore, ideal for capturing and representing best the perceptual experience of the visible corona. Explained here is how by bridging the eras of visual (late 19th century) and imaging investigations (since the latter half of the 20th century), Butler's paintings reveal why white-light images misled researching and understanding the Sun's atmosphere, the solar wind. The closure in understanding solar eclipses through the convergence of perception, art, imaging, science and the history of science promises to enrich the experience of viewing and photographing the first solar eclipse of the 21st century in the United States on 21st August 2017.

  5. Observations of the Dynamics and Thermodynamics of the Corona during the 21 August 2017 Total Solar Eclipse

    NASA Astrophysics Data System (ADS)

    Habbal, Shadia Rifai; Ding, Adalbert; Druckmuller, Miloslav; Solar Wind Sherpas

    2018-01-01

    The visible wavelength range, encompassing forbidden coronal emission lines, offers unique diagnostic tools for exploring the physics of the solar corona, such as its chemical composition and the dynamics of its major and minor constituents. These tools are best exploited during total solar eclipses, when the field of view spans several solar radii, starting from the solar surface. This spatial span is currently untenable from any observing platform. Imaging and spectroscopic eclipse observations, including the 2017 August 21 event, are shown to be the first to yield the temperature distribution in the corona as a function of solar cycle. They are also the first to lead to the discovery of cool prominence material at less than 10,000 to 50,000 K, within more than a radius above the solar surface, streaming away from the Sun, while maintaining its compositional identity. These data underscore the importance of capturing emission from coronal forbidden lines with the next generation space-based instrumentation to address the general problem of coronal heating.

  6. Terahertz photometers to observe solar flares from space (SOLAR-T project)

    NASA Astrophysics Data System (ADS)

    Kaufmann, Pierre; Raulin, Jean-Pierre

    The space experiment SOLAR-T designed to observe solar flares at THz frequencies was completed. We present the concept, fabrication and performance of a double THz photometers system. An innovative optical setup allows observations of the full solar disk and the detection of small burst transients at the same time. It is the first detecting system conceived to observe solar flare THz emissions on board of stratospheric balloons. The system has been integrated to data acquisition and telemetry modules for this application. SOLAR-T uses two Golay cell detectors preceded by low-pass filters made of rough surface primary mirrors and membranes, 3 and 7 THz band-pass filters, and choppers. Its photometers can detect small solar bursts (tens of solar flux units) with sub second time resolution. One artificial Sun setup was developed to simulate actual observations. Tests comprised the whole system performance, on ambient and low pressure and temperature conditions. It is intended to provide data on the still unrevealed spectral shape of the mysterious THz solar flares emissions. The experiment is planned to be on board of two long-duration stratospheric balloon flights over Antarctica and Russia in 2014-2016. The SOLAR-T development, fabrication and tests has been accomplished by engineering and research teams from Mackenzie, Unicamp and Bernard Lyot Solar Observatory; Propertech Ltda.; Neuron Ltda.; and Samsung, Brazil; Tydex LCC, Russia; CONICET, Argentina; the stratospheric balloon missions will be carried in cooperation with teams from University of California, Berkeley, USA (flight over Antarctica), and Lebedev Physical Institute, Moscow, Russia (flight over Russia).

  7. Solar System Observations with JWST

    NASA Technical Reports Server (NTRS)

    Norwood, James; Hammel, Heidi; Milam, Stefanie; Stansberry, John; Lunine, Jonathan; Chanover, Nancy; Hines, Dean; Sonneborn, George; Tiscareno, Matthew; Brown, Michael; hide

    2014-01-01

    The James Webb Space Telescope will enable a wealth of new scientific investigations in the near- and mid- infrared, with sensitivity and spatial-spectral resolution greatly surpassing its predecessors. In this paper, we focus upon Solar System science facilitated by JWST, discussing the most current information available concerning JWST instrument properties and observing techniques relevant to planetary science. We also present numerous example observing scenarios for a wide variety of Solar System targets to illustrate the potential of JWST science to the Solar System community. This paper updates and supersedes the Solar System white paper published by the JWST Project in 2010 (Lunine et al., 2010). It is based both on that paper and on a workshop held at the annual meeting of the Division for Planetary Sciences in Reno, NV in 2012.

  8. On the Performance of Multi-Instrument Solar Flare Observations During Solar Cycle 24

    NASA Astrophysics Data System (ADS)

    Milligan, Ryan O.; Ireland, Jack

    2018-02-01

    The current fleet of space-based solar observatories offers us a wealth of opportunities to study solar flares over a range of wavelengths. Significant advances in our understanding of flare physics often come from coordinated observations between multiple instruments. Consequently, considerable efforts have been, and continue to be, made to coordinate observations among instruments ( e.g. through the Max Millennium Program of Solar Flare Research). However, there has been no study to date that quantifies how many flares have been observed by combinations of various instruments. Here we describe a technique that retrospectively searches archival databases for flares jointly observed by the Ramaty High Energy Solar Spectroscopic Imager (RHESSI), Solar Dynamics Observatory (SDO)/ EUV Variability Experiment (EVE - Multiple EUV Grating Spectrograph (MEGS)-A and -B, Hinode/( EUV Imaging Spectrometer, Solar Optical Telescope, and X-Ray Telescope), and Interface Region Imaging Spectrograph (IRIS). Out of the 6953 flares of GOES magnitude C1 or greater that we consider over the 6.5 years after the launch of SDO, 40 have been observed by 6 or more instruments simultaneously. Using each instrument's individual rate of success in observing flares, we show that the numbers of flares co-observed by 3 or more instruments are higher than the number expected under the assumption that the instruments operated independently of one another. In particular, the number of flares observed by larger numbers of instruments is much higher than expected. Our study illustrates that these missions often acted in cooperation, or at least had aligned goals. We also provide details on an interactive widget ( Solar Flare Finder), now available in SSWIDL, which allows a user to search for flaring events that have been observed by a chosen set of instruments. This provides access to a broader range of events in order to answer specific science questions. The difficulty in scheduling coordinated

  9. Hinode Satellite Captures Total Solar Eclipse Video Aug. 21

    NASA Image and Video Library

    2017-08-21

    The Japan Aerospace Exploration Agency, the National Astronomical Observatory of Japan and NASA released this video of Aug. 21 total solar eclipse taken by the X-ray telescope aboard the Hinode joint solar observation satellite as it orbited high above the Pacific Ocean.

  10. Observations of an Eruptive Solar Flare in the Extended EUV Solar Corona

    NASA Astrophysics Data System (ADS)

    Seaton, Daniel B.; Darnel, Jonathan M.

    2018-01-01

    We present observations of a powerful solar eruption, accompanied by an X8.2 solar flare, from NOAA Active Region 12673 on 2017 September 10 by the Solar Ultraviolet Imager (SUVI) on the GOES-16 spacecraft. SUVI is noteworthy for its relatively large field of view, which allows it to image solar phenomena to heights approaching 2 solar radii. These observations include the detection of an apparent current sheet associated with magnetic reconnection in the wake of the eruption, and evidence of an extreme-ultraviolet wave at some of the largest heights ever reported. We discuss the acceleration of the nascent coronal mass ejection to approximately 2000 km s‑1 at about 1.5 solar radii. We compare these observations with models of eruptions and eruption-related phenomena. We also describe the SUVI data and discuss how the scientific community can access SUVI observations of the event.

  11. Solar Electric Propulsion Triple-Satellite-Aided Capture With Mars Flyby

    NASA Astrophysics Data System (ADS)

    Patrick, Sean

    Triple-Satellite-aided-capture sequences use gravity-assists at three of Jupiter's four massive Galilean moons to reduce the DeltaV required to enter into Jupiter orbit. A triple-satellite-aided capture at Callisto, Ganymede, and Io is proposed to capture a SEP spacecraft into Jupiter orbit from an interplanetary Earth-Jupiter trajectory that employs low-thrust maneuvers. The principal advantage of this method is that it combines the ISP efficiency of ion propulsion with nearly impulsive but propellant-free gravity assists. For this thesis, two main chapters are devoted to the exploration of low-thrust triple-flyby capture trajectories. Specifically, the design and optimization of these trajectories are explored heavily. The first chapter explores the design of two solar electric propulsion (SEP), low-thrust trajectories developed using the JPL's MALTO software. The two trajectories combined represent a full Earth to Jupiter capture split into a heliocentric Earth to Jupiter Sphere of Influence (SOI) trajectory and a Joviocentric capture trajectory. The Joviocentric trajectory makes use of gravity assist flybys of Callisto, Ganymede, and Io to capture into Jupiter orbit with a period of 106.3 days. Following this, in chapter two, three more SEP low-thrust trajectories were developed based upon those in chapter one. These trajectories, devised using the high-fidelity Mystic software, also developed by JPL, improve upon the original trajectories developed in chapter one. Here, the developed trajectories are each three separate, full Earth to Jupiter capture orbits. As in chapter one, a Mars gravity assist is used to augment the heliocentric trajectories. Gravity-assist flybys of Callisto, Ganymede, and Io or Europa are used to capture into Jupiter Orbit. With between 89.8 and 137.2-day periods, the orbits developed in chapters one and two are shorter than most Jupiter capture orbits achieved using low-thrust propulsion techniques. Finally, chapter 3 presents an

  12. Asteroseismology - The impact of solar space observations

    NASA Technical Reports Server (NTRS)

    Hudson, H. S.

    1993-01-01

    Observations from space relevant to solar global properties (oscillations, magnetic activity, etc.) are helpful both scientifically and technically in preparing for stellar observations. This paper summarizes the results from the main previous experiments (ACRIM, SOUP, and IPHIR), and also gives an initial technical report from the SXT instrument on board Yohkoh, launched in August 1991. The solar observations to date demonstrate the existence of several mechanisms for low-level variability: spots, faculae, the photospheric network, granulation, and p-mode oscillations. The observations of oscillations have been particularly helpful in setting limits on solar interior rotation. In addition to the solar processes, stars of other types may have different mechanisms of variability. These may include the analogs of coronal holes or solar flares, modes of oscillation not detected in the sun, collisions with small bodies, duplicity, and probably mechanisms not invented yet but related in interesting ways to stellar convection and magnetism.

  13. How well do satellite observations and models capture diurnal variation in aerosols over the Korean Peninsula?

    NASA Astrophysics Data System (ADS)

    Hyer, E. J.; Xian, P.; Campbell, J. R.

    2016-12-01

    Aerosol sources, sinks, and transport processes have important variations over the diurnal cycle. Advances in geostationary satellite observation have made it possible to retrieve aerosol properties over a larger fraction of the diurnal cycle in many areas. However, the conditions for retrieval of aerosol from space also have systematic diurnal variation, which must be considered when interpreting satellite data. We used surface PM2.5 observations from the Korean National Institute for Environmental Research, together with the dense network of AERONET sun photometers deployed in Korea for the KORUS-AQ mission in spring 2016, to examine diurnal variations in aerosol conditions and quantify the effect of systematic diurnal processes on daily integrated aerosol quantities of forcing and PM2.5 24-hour exposure. Time-resolved observations of aerosols from in situ data were compared to polar and geostationary satellite observations to evaluate these questions: 1) How well is diurnal variation observed in situ captured by satellite products? 2) Do the satellite products show evidence of systematic biases related to diurnally varying observing conditions? 3) What is the implication of diurnal variation for aerosol forcing estimates based on observations near solar noon? The diurnal variation diagnosed from observations was also compared to the output of the Navy Aerosol Analysis and Prediction System (NAAPS), to examine the ability of this model to capture aerosol diurnal variation. Finally, we discuss the implications of the observed diurnal variation for assimilation of aerosol observations into forecast models.

  14. Hinode: A Decade of Success in Capturing Solar Activity

    NASA Technical Reports Server (NTRS)

    Savage, S.; Elrod, S.; Deluca, E.; Doschek, G.; Tarbell, T.

    2017-01-01

    As the present solar cycle passes into its minimum phase, the Hinode mission marks its tenth year of investigating solar activity. Hinode's decade of successful observations have provided us with immeasurable insight into the solar processes that invoke space weather and thereby affect the interplanetary environment in which we reside. The mission's complementary suite of instruments allows us to probe transient, high energy events alongside long-term, cycle-dependent phenomena from magnetic fields at the Sun's surface out to highly thermalized coronal plasma enveloping active regions (ARs). These rich data sets have already changed the face of solar physics and will continue to provoke exciting research as new observational paradigms are pursued. Hinode was launched as part of the Science Mission Directorate's (SMD) Solar Terrestrial Probes Program in 2006. It is a sophisticated spacecraft equipped with a Solar Optical Telescope (SOT), an Extreme-ultraviolet Imaging Spectrometer (EIS), and an X-Ray Telescope (XRT) (see x 4). With high resolution and sensitivity, Hinode serves as a microscope for the Sun, providing us with unique capabilities for observing magnetic fields near the smallest scales achievable, while also rendering full-Sun coronal context in the highest thermal regimes. The 2014 NASA SMD strategic goals objective to "Understand the Sun and its interactions with the Earth and the solar system, including space weather" forms the basis of three underlying Heliophysics Science Goals. While Hinode relates to all three, the observatory primarily addresses: Explore the physical processes in the space environment from the Sun to the Earth and through the solar system. Within the NASA National Research Council (NRC) Decadal Survey Priorities, Hinode targets: (a) Determine the origins of the Sun's activity and predict the variations of the space environment and (d) Discover and characterize fundamental processes that occur both within the heliosphere and

  15. High-spectral resolution solar microwave observations

    NASA Technical Reports Server (NTRS)

    Hurford, G. J.

    1986-01-01

    The application of high-spectral resolution microwave observations to the study of solar activity is discussed with particular emphasis on the frequency dependence of microwave emission from solar active regions. A shell model of gyroresonance emission from active regions is described which suggest that high-spectral resolution, spatially-resolved observations can provide quantitative information about the magnetic field distribution at the base of the corona. Corresponding observations of a single sunspot with the Owens Valley frequency-agile interferometer at 56 frequencies between 1.2 and 14 Ghs are presented. The overall form of the observed size and brightness temperature spectra was consistent with expectations based on the shell model, although there were differences of potential physical significance. The merits and weaknesses of microwave spectroscopy as a technique for measuring magnetic fields in the solar corona are briefly discussed.

  16. SOLAR-ISS: A new reference spectrum based on SOLAR/SOLSPEC observations

    NASA Astrophysics Data System (ADS)

    Meftah, M.; Damé, L.; Bolsée, D.; Hauchecorne, A.; Pereira, N.; Sluse, D.; Cessateur, G.; Irbah, A.; Bureau, J.; Weber, M.; Bramstedt, K.; Hilbig, T.; Thiéblemont, R.; Marchand, M.; Lefèvre, F.; Sarkissian, A.; Bekki, S.

    2018-03-01

    Context. Since April 5, 2008 and up to February 15, 2017, the SOLar SPECtrometer (SOLSPEC) instrument of the SOLAR payload on board the International Space Station (ISS) has performed accurate measurements of solar spectral irradiance (SSI) from the middle ultraviolet to the infrared (165 to 3088 nm). These measurements are of primary importance for a better understanding of solar physics and the impact of solar variability on climate. In particular, a new reference solar spectrum (SOLAR-ISS) is established in April 2008 during the solar minima of cycles 23-24 thanks to revised engineering corrections, improved calibrations, and advanced procedures to account for thermal and aging corrections of the SOLAR/SOLSPEC instrument. Aims: The main objective of this article is to present a new high-resolution solar spectrum with a mean absolute uncertainty of 1.26% at 1σ from 165 to 3000 nm. This solar spectrum is based on solar observations of the SOLAR/SOLSPEC space-based instrument. Methods: The SOLAR/SOLSPEC instrument consists of three separate double monochromators that use concave holographic gratings to cover the middle ultraviolet (UV), visible (VIS), and infrared (IR) domains. Our best ultraviolet, visible, and infrared spectra are merged into a single absolute solar spectrum covering the 165-3000 nm domain. The resulting solar spectrum has a spectral resolution varying between 0.6 and 9.5 nm in the 165-3000 nm wavelength range. We build a new solar reference spectrum (SOLAR-ISS) by constraining existing high-resolution spectra to SOLAR/SOLSPEC observed spectrum. For that purpose, we account for the difference of resolution between the two spectra using the SOLAR/SOLSPEC instrumental slit functions. Results: Using SOLAR/SOLSPEC data, a new solar spectrum covering the 165-3000 nm wavelength range is built and is representative of the 2008 solar minimum. It has a resolution better than 0.1 nm below 1000 nm and 1 nm in the 1000-3000 nm wavelength range. The new

  17. Solar wind charge exchange in laboratory - Observation of forbidden X-ray transitions

    NASA Astrophysics Data System (ADS)

    Numadate, Naoki; Shimaya, Hirofumi; Ishida, Takuya; Okada, Kunihiro; Nakamura, Nobuyuki; Tanuma, Hajime

    2017-10-01

    We have reproduced solar wind charge exchange collisions of hydrogen-like O7+ ions with He gas at collision energies of 42 keV in the laboratory and observed the forbidden transition of 1s21S0 -1s2s 3S1 in helium-like O6+ ions produced by single electron capture. The measured soft X-ray spectrum had a peak at 560 eV which corresponds to the energy of the forbidden 1s21S0 -1s2s 3S1 transition in the O6+ ion, and a reasonable energy difference between peak positions of the forbidden and resonance lines was found, which ensured that we succeeded in observing the forbidden transition of O6+ ions. The dominant electron capture level in the collision of O7+ ions with He can be estimated to be a principal quantum number n = 4 by the classical over barrier model and the two-center atomic orbital close coupling method. After the charge exchange, the population of the 1s2s state becomes large due to cascade transitions from the higher excited states, so the long-lived forbidden transition to the 1s21S0 ground state is one of main features observed in the charge exchange spectra.

  18. Capabilities of GRO/OSSE for observing solar flares

    NASA Technical Reports Server (NTRS)

    Kurfess, J. D.; Johnson, W. N.; Share, G. H.; Hulburt, E. O.; Matz, S. M.; Murphy, R. J.

    1989-01-01

    The launch of the Gamma Ray Observatory (GRO) near solar maximum makes solar flare studies early in the mission particularly advantageous. The Oriented Scintillation Spectrometer Experiment (OSSE) on GRO, covering the energy range 0.05 to 150 MeV, has some significant advantages over the previous generation of satellite-borne gamma-ray detectors for solar observations. The OSSE detectors will have about 10 times the effective area of the Gamma-Ray Spectrometer (GRS) on Solar Maximum Mission (SMM) for both photons and high-energy neutrons. The OSSE also has the added capability of distinguishing between high-energy neutrons and photons directly. The OSSE spectral accumulation time (approx. 4s) is four times faster than that of the SMM/GRS; much better time resolution is available in selected energy ranges. These characteristics will allow the investigation of particle acceleration in flares based on the evolution of the continuum and nuclear line components of flare spectra, nuclear emission in small flares, the anisotropy of continuum emission in small flares, and the relative intensities of different nuclear lines. The OSSE observational program will be devoted primarily to non-solar sources. Therefore, solar observations require planning and special configurations. The instrumental and operational characteristics of OSSE are discussed in the context of undertaking solar observations. The opportunities for guest investigators to participate in solar flare studies with OSSE is also presented.

  19. High Resolution Observations of Solar Quiescent Prominences with the Hinode Solar Optical Telescope: an Open Challenge to 21st Century Ground-based Solar Telescopes (Invited)

    NASA Astrophysics Data System (ADS)

    Berger, T. E.

    2009-12-01

    The Solar Optical Telescope (SOT) on the Japanese Hinode satellite is a 0.5-meter diameter Gregorian solar telescope in a 600 km Sun-synchronous orbit. The telescope achieves diffraction-limited imaging with no atmospheric seeing in a wavelength range from 380 nm to 660 nm. Using both the Broadband Filter Imager (BFI) Ca II H-line channel at 389.6 nm and the tunable Narrowband Filter Imager (NFI) H-alpha channel at 656.3 nm we have observed many quiescent solar prominences since the satellite launch in September 2006. The excellent optical quality and low scattering of the SOT telescope combined with the lack of atmospheric scattering and seeing enables us to capture multi-hour diffraction-limited movies of quiescent prominences above the limb that achieve 200 km spatial resolution and 15--30 second temporal resolution. These SOT observations have led to the discovery of new flows in the solar outer atmosphere in the form of buoyant small-scale (2--6 Mm) plumes and large-scale (10--50 Mm) "bubbles" or arches that originate below quiescent prominences and rise with speeds of 10--30 km/sec to heights of 10--30+ Mm above the solar limb. In this talk we review the kinematic properties of these new flows in combination with the long-observed filamentary downflows to show that quisecent prominences are not magnetostatic structures "suspended against gravity" but are rather entirely dynamic structures in which mass is continually drained in the downflows while being resupplied largely by condensation from the coronal cavity above and episodic buoyant flows from below. The Hinode/SOT instrument has definitively shown the value of flying high-resolution visible-light solar telescopes in space by acheiving in its first six months what had been a long-standing goal of ground-based solar prominence research for the past 50 years. However many key quiescent prominence characteristics cannot be measured by the limited instrumentation on the Hinode satellite. Primary among these

  20. LOFAR observations of the quiet solar corona

    NASA Astrophysics Data System (ADS)

    Vocks, C.; Mann, G.; Breitling, F.; Bisi, M. M.; Dąbrowski, B.; Fallows, R.; Gallagher, P. T.; Krankowski, A.; Magdalenić, J.; Marqué, C.; Morosan, D.; Rucker, H.

    2018-06-01

    Context. The quiet solar corona emits meter-wave thermal bremsstrahlung. Coronal radio emission can only propagate above that radius, Rω, where the local plasma frequency equals the observing frequency. The radio interferometer LOw Frequency ARray (LOFAR) observes in its low band (10-90 MHz) solar radio emission originating from the middle and upper corona. Aims: We present the first solar aperture synthesis imaging observations in the low band of LOFAR in 12 frequencies each separated by 5 MHz. From each of these radio maps we infer Rω, and a scale height temperature, T. These results can be combined into coronal density and temperature profiles. Methods: We derived radial intensity profiles from the radio images. We focus on polar directions with simpler, radial magnetic field structure. Intensity profiles were modeled by ray-tracing simulations, following wave paths through the refractive solar corona, and including free-free emission and absorption. We fitted model profiles to observations with Rω and T as fitting parameters. Results: In the low corona, Rω < 1.5 solar radii, we find high scale height temperatures up to 2.2 × 106 K, much more than the brightness temperatures usually found there. But if all Rω values are combined into a density profile, this profile can be fitted by a hydrostatic model with the same temperature, thereby confirming this with two independent methods. The density profile deviates from the hydrostatic model above 1.5 solar radii, indicating the transition into the solar wind. Conclusions: These results demonstrate what information can be gleaned from solar low-frequency radio images. The scale height temperatures we find are not only higher than brightness temperatures, but also than temperatures derived from coronograph or extreme ultraviolet (EUV) data. Future observations will provide continuous frequency coverage. This continuous coverage eliminates the need for local hydrostatic density models in the data analysis and

  1. The Trojan-Hilda-KBO connection: An observational test of solar system evolution models

    NASA Astrophysics Data System (ADS)

    Wong, Ian; Brown, Michael

    2017-10-01

    Over the past few decades, many theories have been devised to explain the observed solar system architecture. The current paradigm posits that a significant reorganization of the outer Solar System occurred after the end of planet formation. Specifically, it is hypothesized that Jupiter and Saturn crossed a mutual mean motion resonance, leading to a chaotic expansion of the ice giants’ orbits that disrupted the large population of planetesimals situated further out. While the majority of these bodies were ejected from the Solar System, a fraction of them were retained as the present-day Kuiper Belt, while others were scattered inward and captured into resonances with Jupiter to become the Trojans and Hildas. Dynamical instability models invariably predict that Trojans, Hildas, and Kuiper Belt objects (KBOs) were sourced from the same primordial body of outer solar system planetesimals. Therefore, comparison of these minor body populations serves as one of the few available observational tests of our present understanding of solar system evolution.We present the results of a series of studies aimed at synthesizing a detailed picture of Trojans and related asteroid populations. By combining analyses of archival data with new photometric surveys, we have derived the first debiased color distributions of Trojans and KBOs and extended/refined our knowledge of their respective size distributions. In addition, we have explored the peculiar color bimodality attested in the Trojans, Hildas, and KBOs, which indicates the presence of two sub-populations. As part of our continuing efforts to characterize the surface composition of these bodies, we have also obtained new near-infrared spectra of Hildas for comparison with previously published spectra of Trojans covering the same wavelength region. We have utilized the full body of observations to formulate hypotheses regarding the formation, composition, and dynamical/chemical evolution of the primordial outer solar system

  2. The Trojan-Hilda-KBO connection: An observational test of solar system evolution models

    NASA Astrophysics Data System (ADS)

    Wong, I.; Brown, M. E.

    2017-12-01

    Over the past few decades, many theories have been devised to explain the observed solar system architecture. The current paradigm posits that a significant reorganization of the outer Solar System occurred after the end of planet formation. Specifically, it is hypothesized that Jupiter and Saturn crossed a mutual mean motion resonance, leading to a chaotic expansion of the ice giants' orbits that disrupted the large population of planetesimals situated further out. While the majority of these bodies were ejected from the Solar System, a fraction of them were retained as the present-day Kuiper Belt, while others were scattered inward and captured into resonances with Jupiter to become the Trojans and Hildas. Dynamical instability models invariably predict that Trojans, Hildas, and Kuiper Belt objects (KBOs) were sourced from the same primordial body of outer solar system planetesimals. Therefore, comparison of these minor body populations serves as one of the few available observational tests of our present understanding of solar system evolution. We present the results of a series of studies aimed at synthesizing a detailed picture of Trojans and related asteroid populations. By combining analyses of archival data with new photometric surveys, we have derived the first debiased color distributions of Trojans and KBOs and extended/refined our knowledge of their respective size distributions. In addition, we have explored the peculiar color bimodality attested in the Trojans, Hildas, and KBOs, which indicates the presence of two sub-populations. As part of our continuing efforts to characterize the surface composition of these bodies, we have also obtained new near-infrared spectra of Hildas for comparison with previously published spectra of Trojans covering the same wavelength region. We have utilized the full body of observations to formulate hypotheses regarding the formation, composition, and dynamical/chemical evolution of the primordial outer solar system

  3. Capture of irregular satellites at Jupiter

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

    Nesvorný, David; Vokrouhlický, David; Deienno, Rogerio

    The irregular satellites of outer planets are thought to have been captured from heliocentric orbits. The exact nature of the capture process, however, remains uncertain. We examine the possibility that irregular satellites were captured from the planetesimal disk during the early solar system instability when encounters between the outer planets occurred. Nesvorný et al. already showed that the irregular satellites of Saturn, Uranus, and Neptune were plausibly captured during planetary encounters. Here we find that the current instability models present favorable conditions for capture of irregular satellites at Jupiter as well, mainly because Jupiter undergoes a phase of close encountersmore » with an ice giant. We show that the orbital distribution of bodies captured during planetary encounters provides a good match to the observed distribution of irregular satellites at Jupiter. The capture efficiency for each particle in the original transplanetary disk is found to be (1.3-3.6) × 10{sup –8}. This is roughly enough to explain the observed population of jovian irregular moons. We also confirm Nesvorný et al.'s results for the irregular satellites of Saturn, Uranus, and Neptune.« less

  4. Observed solar near UV variability: A contribution to variations of the solar constant

    NASA Technical Reports Server (NTRS)

    London, Julius; Pap, Judit; Rottman, Gary J.

    1989-01-01

    Continuous Measurements of the Solar UV have been made by an instrument on the Solar Mesosphere Explorer (SME) since October 1981. The results for the wavelength interval 200 to 300 nm show an irradiance decrease to a minimum in early 1987 and a subsequent increase to mid-April 1989. The observed UV changes during part of solar cycles 21 to 22 represent approx. 35 percent (during the decreasing phase) and 25 percent (during the increasing phase) of the observed variations of the solar constant for the same time period as the SME measurements.

  5. Solar Observations on Magneto-Convection

    DTIC Science & Technology

    1989-05-31

    Technical Library National Solar Observatory Sunspot, NM 88349 Karl - Schwarzschild -Strasse 1 8046 Garching bei Mundhen Solar Observations On Magneto...Schmidt, Hermann-Ulrich Schmidt, Hans-Christoph Thomas (eds.) Max-Planck-Institut fir Physik und Astrophysik Institut fiur Astrophysik Karl ... Schwarzschild -St-. 1 D-8046 Garching, FklG 14TIS CRiA.&l DTIC TA. U~Jar,iou8:ed B ......... ... Distribution I -- Availability COcý----- Avail and or Dist special

  6. Spacecraft observations of the solar wind composition

    NASA Technical Reports Server (NTRS)

    Bame, S. J.

    1972-01-01

    Solar wind composition studies by means of plasma analyzers carried on various spacecraft are reviewed. The average ratio of helium to hydrogen over the solar cycle is close to 0.045; values as low as 0.0025 and as high as 0.25 have been observed. High values have been observed following solar flares and interplanetary shock waves when the flare gas driving the shock arrives at the spacecraft. Ions of He-3(+2), O-16(+6), and O-16(+7) have been observed with Vela 3 electrostatic analyzers. Further measurements with Vela 5 analyzers have shown the presence of N-14(+6), Si-28(+7) to Si-28(+9) and Fe-56(+7) to Fe-56(+12) ions. The relative abundance of oxygen, silicon, and iron in the solar wind of July 6, 1969, was 1.00, 0.21, and 0.17, which is very similar to reported values for the corona. The ratio of helium to oxygen is variable; the average value of He/O is close to 100, but values between 30 and 400 have been observed.

  7. Direct observations of low-energy solar electrons associated with a type 3 solar radio burst

    NASA Technical Reports Server (NTRS)

    Frank, L. A.; Gurnett, D. A.

    1972-01-01

    On 6 April 1971 a solar X-ray flare and a type 3 solar radio noise burst were observed with instrumentation on the eccentric-orbiting satellite IMP 6. The type 3 solar radio noise burst was detected down to a frequency of 31 kHz. A highly anisotropic packet of low-energy solar electron intensities arrived at the satellite approximately 6000 seconds after the onset of the solar flare. This packet of solar electron intensities was observed for 4200 seconds. Maximum differential intensities of the solar electrons were in the energy range of one to several keV. The frequency drift rate of the type 3 radio noise at frequencies below 178 kHz also indicated an average particle speed corresponding to that of a 3-keV electron. The simultaneous observations of these solar electron intensities and of the type 3 solar radio burst are presented, and their interrelationships are explored.

  8. Determination of variations of the solar radius from solar eclipse observations

    NASA Technical Reports Server (NTRS)

    Sofia, S.; Dunham, D. W.; Fiala, A. D.

    1980-01-01

    This paper describes the method to determine the solar radius and its variations from observations made during total solar eclipses. In particular, the procedure to correct the spherical moon predictions for the effects of lunar mountains and valleys on the width and location of the path of totality is addressed in detail. The errors affecting this technique are addressed, a summary of the results of its application to three solar eclipses are presented, and the implications of the results on the constancy of the solar constant are described.

  9. Observational capabilities of solar satellite "Coronas-Photon"

    NASA Astrophysics Data System (ADS)

    Kotov, Yu.

    Coronas-Photon mission is the third satellite of the Russian Coronas program on solar activity observation The main goal of the Coronas-Photon is the study of solar hard electromagnetic radiation in the wide energy range from UV up to high energy gamma-radiation sim 2000MeV Scientific payload for solar radiation observation consists of three type of instruments 1 monitors Natalya-2M Konus-RF RT-2 Penguin-M BRM Phoka Sphin-X Sokol for spectral and timing measurements of full solar disk radiation with timing in flare burst mode up to one msec Instruments Natalya-2M Konus-RF RT-2 will cover the wide energy range of hard X-rays and soft Gamma rays 15keV to 2000MeV and will together constitute the largest area detectors ever used for solar observations Detectors of gamma-ray monitors are based on structured inorganic scintillators with energy resolution sim 5 for nuclear gamma-line band to 35 for GeV-band PSD analysis is used for gamma neutron separation for solar neutron registration T 30MeV Penguin-M has capability to measure linear polarization of hard X-rays using azimuth are measured by Compton scattering asymmetry in case of polarization of an incident flux For X-ray and EUV monitors the scintillation phoswich detectors gas proportional counter CZT assembly and Filter-covered Si-diodes are used 2 Telescope-spectrometer TESIS for imaging solar spectroscopy in X-rays with angular resolution up to 1 in three spectral lines and RT-2 CZT assembly of CZT

  10. Long-term evolution of Oort Cloud comets: capture of comets

    NASA Astrophysics Data System (ADS)

    Nurmi, P.; Valtonen, M. J.; Zheng, J. Q.; Rickman, H.

    2002-07-01

    We test different possibilities for the origin of short-period comets captured from the Oort Cloud. We use an efficient Monte Carlo simulation method that takes into account non-gravitational forces, Galactic perturbations, observational selection effects, physical evolution and tidal splittings of comets. We confirm previous results and conclude that the Jupiter family comets cannot originate in the spherically distributed Oort Cloud, since there is no physically possible model of how these comets can be captured from the Oort Cloud flux and produce the observed inclination and Tisserand constant distributions. The extended model of the Oort Cloud predicted by the planetesimal theory consisting of a non-randomly distributed inner core and a classical Oort Cloud also cannot explain the observed distributions of Jupiter family comets. The number of comets captured from the outer region of the Solar system are too high compared with the observations if the inclination distribution of Jupiter family comets is matched with the observed distribution. It is very likely that the Halley-type comets are captured mainly from the classical Oort Cloud, since the distributions in inclination and Tisserand value can be fitted to the observed distributions with very high confidence. Also the expected number of comets is in agreement with the observations when physical evolution of the comets is included. However, the solution is not unique, and other more complicated models can also explain the observed properties of Halley-type comets. The existence of Jupiter family comets can be explained only if they are captured from the extended disc of comets with semimajor axes of the comets a<5000au. The original flattened distribution of comets is conserved as the cometary orbits evolve from the outer Solar system era to the observed region.

  11. Capturing the Sun: A Roadmap for Navigating Data-Access Challenges and Auto-Populating Solar Home Sales Listings

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

    Stukel, Laura; Hoen, Ben; Adomatis, Sandra

    Capturing the Sun: A Roadmap for Navigating Data-Access Challenges and Auto-Populating Solar Home Sales Listings supports a vision of solar photovoltaic (PV) advocates and real estate advocates evolving together to make information about solar homes more accessible to home buyers and sellers and to simplify the process when these homes are resold. The Roadmap is based on a concept in the real estate industry known as automatic population of fields. Auto-population (also called auto-pop in the industry) is the technology that allows data aggregated by an outside industry to be matched automatically with home sale listings in a multiple listingmore » service (MLS).« less

  12. Forecast of solar wind parameters according to STOP magnetograph observations

    NASA Astrophysics Data System (ADS)

    Tlatov, A. G.; Pashchenko, M. P.; Ponyavin, D. I.; Svidskii, P. M.; Peshcherov, V. S.; Demidov, M. L.

    2016-12-01

    The paper discusses the results of the forecast of solar wind parameters at a distance of 1 AU made according to observations made by the STOP telescope magnetograph during 2014-2015. The Wang-Sheeley-Arge (WSA) empirical model is used to reconstruct the magnetic field topology in the solar corona and estimate the solar wind speed in the interplanetary medium. The proposed model is adapted to STOP magnetograph observations. The results of the calculation of solar wind parameters are compared with ACE satellite measurements. It is shown that the use of STOP observations provides a significant correlation of predicted solar wind speed values with the observed ones.

  13. Variations in the Solar Neutrino Flux

    DOE R&D Accomplishments Database

    Davis, R. Jr.; Cleveland, B. T.; Rowley, J. K.

    1987-08-02

    Observations are reported from the chlorine solar neutrino detector in the Homestake Gold Mine, South Dakota, USA. They extend from 1970 to 1985 and yield an average neutrino capture rate of 2.1 +- 0.3 SNU. The results from 1977 to 1985 show an anti-correlation with the solar activity cycle, and an apparent increased rate during large solar flares.

  14. Helioseismology Observations of Solar Cycles and Dynamo Modeling

    NASA Astrophysics Data System (ADS)

    Kosovichev, A. G.; Guerrero, G.; Pipin, V.

    2017-12-01

    Helioseismology observations from the SOHO and SDO, obtained in 1996-2017, provide unique insight into the dynamics of the Sun's deep interior for two solar cycles. The data allow us to investigate variations of the solar interior structure and dynamics, and compare these variations with dynamo models and simulations. We use results of the local and global helioseismology data processing pipelines at the SDO Joint Science Operations Center (Stanford University) to study solar-cycle variations of the differential rotation, meridional circulation, large-scale flows and global asphericity. By comparing the helioseismology results with the evolution of surface magnetic fields we identify characteristic changes associated the initiation and development of Solar Cycles 23 and 24. For the physical interpretation of observed variations, the results are compared with the current mean-field dynamo models and 3D MHD dynamo simulations. It is shown that the helioseismology inferences provide important constraints on the solar dynamo mechanism, may explain the fundamental difference between the two solar cycles, and also give information about the next solar cycle.

  15. Variations of Solar Radius Observed with RHESSI

    NASA Astrophysics Data System (ADS)

    Fivian, M. D.; Hudson, H. S.; Lin, R. P.

    2003-12-01

    The Solar Aspect System (SAS) of the rotating (at 15 rpm) RHESSI spacecraft has three subsystems. Each of these measures the position of the limb by sampling the full solar chord profile with a linear CCD using a narrow bandwidth filter at 670 nm. With a resolution of each CCD of 1.7 arcsec/pixel, the accuracy of each of the 6 limb positions is theoretically better than 50 mas using 4 pixels at each limb. Since the launch of RHESSI early 2002, solar limbs are sampled with at least 100 Hz. That provides a database of currently 4 x 109 single radius measurements. The main function of SAS is to determine the RHESSI pointing relative to Sun center. The observed precision of this determination has a typical instantaneous (16 Hz) value of about 200 mas (rms). We show and discuss first results of variations of solar radius observed with RHESSI.

  16. Atmospheric Mining in the Outer Solar System: Resource Capturing, Exploration, and Exploitation

    NASA Technical Reports Server (NTRS)

    Palaszewski, Bryan

    2015-01-01

    Atmospheric mining in the outer solar system (AMOSS) has been investigated as a means of fuel production for high-energy propulsion and power. Fusion fuels such as helium 3 (He-3) and hydrogen can be wrested from the atmospheres of Uranus and Neptune and either returned to Earth or used in-situ for energy production. 3He and hydrogen (deuterium, etc.) were the primary gases of interest, with hydrogen being the primary propellant for nuclear thermal solid core and gas core rocket-based atmospheric flight. A series of analyses were undertaken to investigate resource capturing aspects of AMOSS. These analyses included the gas capturing rate, storage options, and different methods of direct use of the captured gases. Additional supporting analyses were conducted to illuminate vehicle sizing and orbital transportation issues. While capturing 3He, large amounts of hydrogen and helium 4 (He-4) are produced. With these two additional gases, the potential exists for fueling small and large fleets of additional exploration and exploitation vehicles. Additional aerospacecraft or other aerial vehicles (UAVs, balloons, rockets, etc.) could fly through the outer-planet atmosphere to investigate cloud formation dynamics, global weather, localized storms or other disturbances, wind speeds, the poles, and so forth. Deep-diving aircraft (built with the strength to withstand many atmospheres of pressure) powered by the excess hydrogen or 4He may be designed to probe the higher density regions of the gas giants.

  17. Large-Scale periodic solar velocities: An observational study

    NASA Technical Reports Server (NTRS)

    Dittmer, P. H.

    1977-01-01

    Observations of large-scale solar velocities were made using the mean field telescope and Babcock magnetograph of the Stanford Solar Observatory. Observations were made in the magnetically insensitive ion line at 5124 A, with light from the center (limb) of the disk right (left) circularly polarized, so that the magnetograph measures the difference in wavelength between center and limb. Computer calculations are made of the wavelength difference produced by global pulsations for spherical harmonics up to second order and of the signal produced by displacing the solar image relative to polarizing optics or diffraction grating.

  18. New Views of the Solar Corona from STEREO and SDO

    NASA Astrophysics Data System (ADS)

    Vourlidas, A.

    2012-01-01

    In the last few years, we have been treated to an unusual visual feast of solar observations of the corona in EUV wavelengths. The observations from the two vantage points of STEREO/SECCHI are now capturing the entire solar atmosphere simultaneously in four wavelengths. The SDO/AIA images provide us with arcsecond resolution images of the full visible disk in ten wavelengths. All these data are captured with cadences of a few seconds to a few minutes. In this talk, I review some intriguing results from our first attempts to deal with these observations which touch upon the problems of coronal mass ejection initiation and solar wind generation. I will also discuss data processing techniques that may help us recover even more information from the images. The talk will contain a generous portion of beautiful EUV images and movies of the solar corona.

  19. High resolution solar observations from first principles to applications

    NASA Astrophysics Data System (ADS)

    Verdoni, Angelo P.

    2009-10-01

    The expression "high-resolution observations" in Solar Physics refers to the spatial, temporal and spectral domains in their entirety. High-resolution observations of solar fine structure are a necessity to answer many of the intriguing questions related to solar activity. However, a researcher building instruments for high-resolution observations has to cope with the fact that these three domains often have diametrically opposed boundary conditions. Many factors have to be considered in the design of a successful instrument. Modern post-focus instruments are more closely linked with the solar telescopes that they serve than in past. In principle, the quest for high-resolution observations already starts with the selection of the observatory site. The site survey of the Advanced Technology Solar Telescope (ATST) under the stewardship of the National Solar Observatory (NSO) has identified Big Bear Solar Observatory (BBSO) as one of the best sites for solar observations. In a first step, the seeing characteristics at BBSO based on the data collected for the ATST site survey are described. The analysis will aid in the scheduling of high-resolution observations at BBSO as well as provide useful information concerning the design and implementation of a thermal control system for the New Solar Telescope (NST). NST is an off-axis open-structure Gregorian-style telescope with a 1.6 m aperture. NST will be housed in a newly constructed 5/8-sphere ventilated dome. With optics exposed to the surrounding air, NST's open-structure design makes it particularly vulnerable to the effects of enclosure-related seeing. In an effort to mitigate these effects, the initial design of a thermal control system for the NST dome is presented. The goal is to remediate thermal related seeing effects present within the dome interior. The THermal Control System (THCS) is an essential component for the open-telescope design of NST to work. Following these tasks, a calibration routine for the

  20. Piecewise mass flows within a solar prominence observed by the New Vacuum Solar Telescope

    NASA Astrophysics Data System (ADS)

    Li, Hongbo; Liu, Yu; Tam, Kuan Vai; Zhao, Mingyu; Zhang, Xuefei

    2018-06-01

    The material of solar prominences is often observed in a state of flowing. These mass flows (MF) are important and useful for us to understand the internal structure and dynamics of prominences. In this paper, we present a high resolution Hα observation of MFs within a quiescent solar prominence. From the observation, we find that the plasma primarily has a circular motion and a downward motion separately in the middle section and legs of the prominence, which creates a piecewise mass flow along the observed prominence. Moreover, the observation also shows a clear displacement of MF's velocity peaks in the middle section of the prominence. All of these provide us with a detailed record of MFs within a solar prominence and show a new approach to detecting the physical properties of prominence.

  1. Recent Variability Observations of Solar System Giant Planets: Fresh Context for Understanding Exoplanet and Brown Dwarf Weather

    NASA Astrophysics Data System (ADS)

    Marley, Mark S.; Kepler Giant Planet Variability Team, Spitzer Ice Giant Variability Team

    2016-10-01

    Over the past several years a number of of high cadence photometric observations of solar system giant planets have been acquired by various platforms. Such observations are of interest as they provide points of comparison to the already expansive set of brown dwarf variability observations and the small, but growing, set of exoplanet variability observations. By measuring how rapidly the integrated light from solar system giant planets can evolve, variability observations of substellar objects that are unlikely to ever be resolved can be placed in a fuller context. Examples of brown dwarf variability observations include extensive work from the ground (e.g., Radigan et al. 2014), Spitzer (e.g., Metchev et al. 2015), Kepler (Gizis et al. 2015), and HST (Yang et al. 2015). Variability has been measured on the planetary mass companion to the brown dwarf 2MASS 1207b (Zhou et al. 2016) and further searches are planned in thermal emission for the known directly imaged planets with ground based telescopes (Apai et al. 2016) and in reflected light with future space based telescopes. Recent solar system variability observations include Kepler monitoring of Neptune (Simon et al. 2016) and Uranus, Spitzer observations of Neptune (Stauffer et al. 2016), and Cassini observations of Jupiter (West et al. in prep). The Cassini observations are of particular interest as they measured the variability of Jupiter at a phase angle of ˜60○, comparable to the viewing geometry expected for space based direct imaging of cool extrasolar Jupiters in reflected light. These solar system analog observations capture many of the characteristics seen in brown dwarf variability, including large amplitudes and rapid light curve evolution on timescales as short as a few rotation periods. Simon et al. (2016) attribute such variations at Neptune to a combination of large scale, stable cloud structures along with smaller, more rapidly varying, cloud patches. The observed brown dwarf and exoplanet

  2. Recent Variability Observations of Solar System Giant Planets: Fresh Context for Understanding Exoplanet and Brown Dwarf Weather

    NASA Technical Reports Server (NTRS)

    Marley, Mark Scott

    2016-01-01

    Over the past several years a number of high cadence photometric observations of solar system giant planets have been acquired by various platforms. Such observations are of interest as they provide points of comparison to the already expansive set of brown dwarf variability observations and the small, but growing, set of exoplanet variability observations. By measuring how rapidly the integrated light from solar system giant planets can evolve, variability observations of substellar objects that are unlikely to ever be resolved can be placed in a fuller context. Examples of brown dwarf variability observations include extensive work from the ground (e.g., Radigen et al. 2014), Spitzer (e.g., Metchev et al. 2015), Kepler (Gizis et al. 2015), and HST (Yang et al. 2015).Variability has been measured on the planetary mass companion to the brown dwarf 2MASS 1207b (Zhou et al. 2016) and further searches are planned in thermal emission for the known directly imaged planets with ground based telescopes (Apai et al. 2016) and in reflected light with future space based telescopes. Recent solar system variability observations include Kepler monitoring of Neptune (Simon et al. 2016) and Uranus, Spitzer observations of Neptune (Stauffer et al. 2016), and Cassini observations of Jupiter (West et al. in prep). The Cassini observations are of particular interest as they measured the variability of Jupiter at a phase angle of approximately 60 deg, comparable to the viewing geometry expected for space based direct imaging of cool extrasolar Jupiters in reflected light. These solar system analog observations capture many of the characteristics seen in brown dwarf variability, including large amplitudes and rapid light curve evolution on timescales as short as a few rotation periods. Simon et al. (2016) attribute such variations at Neptune to a combination of large scale, stable cloud structures along with smaller, more rapidly varying, cloud patches. The observed brown dwarf and

  3. Solar Flares Observed with the Ramaty High Energy Solar Spectroscopic Imager (RHESSI)

    NASA Technical Reports Server (NTRS)

    Holman, Gordon D.

    2004-01-01

    Solar flares are impressive examples of explosive energy release in unconfined, magnetized plasma. It is generally believed that the flare energy is derived from the coronal magnetic field. However, we have not been able to establish the specific energy release mechanism(s) or the relative partitioning of the released energy between heating, particle acceleration (electrons and ions), and mass motions. NASA's RHESSI Mission was designed to study the acceleration and evolution of electrons and ions in flares by observing the X-ray and gamma-ray emissions these energetic particles produce. This is accomplished through the combination of high-resolution spectroscopy and spectroscopic imaging, including the first images of flares in gamma rays. RHESSI has observed over 12,000 solar flares since its launch on February 5, 2002. I will demonstrate how we use the RHESSI spectra to deduce physical properties of accelerated electrons and hot plasma in flares. Using images to estimate volumes, w e typically find that the total energy in accelerated electrons is comparable to that in the thermal plasma. I will also present flare observations that provide strong support for the presence of magnetic reconnection in a large-scale, vertical current sheet in the solar corona. RHESSI observations such as these are allowing us to probe more deeply into the physics of solar flares.

  4. Mass motion in upper solar chromosphere detected from solar eclipse observation

    NASA Astrophysics Data System (ADS)

    Li, Zhi; Qu, Zhongquan; Yan, Xiaoli; Dun, Guangtao; Chang, Liang

    2016-05-01

    The eclipse-observed emission lines formed in the upper solar atmosphere can be used to diagnose the atmosphere dynamics which provides an insight to the energy balance of the outer atmosphere. In this paper, we analyze the spectra formed in the upper chromospheric region by a new instrument called Fiber Arrayed Solar Optic Telescope (FASOT) around the Gabon total solar eclipse on November 3, 2013. The double Gaussian fits of the observed profiles are adopted to show enhanced emission in line wings, while red-blue (RB) asymmetry analysis informs that the cool line (about 104 K) profiles can be decomposed into two components and the secondary component is revealed to have a relative velocity of about 16-45 km s^{-1}. The other profiles can be reproduced approximately with single Gaussian fits. From these fittings, it is found that the matter in the upper solar chromosphere is highly dynamic. The motion component along the line-of-sight has a pattern asymmetric about the local solar radius. Most materials undergo significant red shift motions while a little matter show blue shift. Despite the discrepancy of the motion in different lines, we find that the width and the Doppler shifts both are function of the wavelength. These results may help us to understand the complex mass cycle between chromosphere and corona.

  5. An Airborne Infrared Spectrometer for Solar Eclipse Observations

    NASA Astrophysics Data System (ADS)

    Samra, Jenna; DeLuca, Edward E.; Golub, Leon; Cheimets, Peter; Philip, Judge

    2016-05-01

    The airborne infrared spectrometer (AIR-Spec) is an innovative solar spectrometer that will observe the 2017 solar eclipse from the NSF/NCAR High-Performance Instrumented Airborne Platform for Environmental Research (HIAPER). AIR-Spec will image five infrared coronal emission lines to determine whether they may be useful probes of coronal magnetism.The solar magnetic field provides the free energy that controls coronal heating, structure, and dynamics. Energy stored in coronal magnetic fields is released in flares and coronal mass ejections and ultimately drives space weather. Therefore, direct coronal field measurements have significant potential to enhance understanding of coronal dynamics and improve solar forecasting models. Of particular interest are observations of field lines in the transitional region between closed and open flux systems, providing important information on the origin of the slow solar wind.While current instruments routinely observe only the photospheric and chromospheric magnetic fields, AIR-Spec will take a step toward the direct observation of coronal fields by measuring plasma emission in the infrared at high spatial and spectral resolution. During the total solar eclipse of 2017, AIR-Spec will observe five magnetically sensitive coronal emission lines between 1.4 and 4 µm from the HIAPER Gulfstream V at an altitude above 14.9 km. The instrument will measure emission line intensity, width, and Doppler shift, map the spatial distribution of infrared emitting plasma, and search for waves in the emission line velocities.AIR-Spec consists of an optical system (feed telescope, grating spectrometer, and infrared detector) and an image stabilization system, which uses a fast steering mirror to correct the line-of-sight for platform perturbations. To ensure that the instrument meets its research goals, both systems are undergoing extensive performance modeling and testing. These results are shown with reference to the science requirements.

  6. AAVSO Solar Observers Worldwide

    NASA Astrophysics Data System (ADS)

    Howe, R.

    2013-06-01

    (Abstract only) For visual solar observers there has been no biological change in the "detector" (human eye) - at century scales (eye + visual cortex) does not change much over time. Our capacity to "integrate" seeing distortions is not just simple averaging! The visual cortex plays an essential role, and until recently only the SDO-HMI (Solar Dynamics Observatory, Helioseismic and Magnetic Imager) has had the capacity to detect the smallest sunspots, called pores. Prior to this the eye was superior to photography and CCD. Imaged data are not directly comparable or substitutable to counts by eye, as the effects of sensor/optical resolution and seeing will have a different influence on the resulting sunspot counts for images when compared to the human eye. Also contributing to the complex task of counting sunspots is differentiating between a sunspot (which is usually defined as having a darker center (umbra) and lighter outer ring (penumbra)) and a pore, made even more complex by the conflicting definitions of the word "pore" in the solar context: "pore" can mean a small spot without penumbra or "pore" can mean a random intergranular blemish that is not a true sunspot. The overall agreement is that the smallest spot size is near 2,000 km or ~3 arc sec, (Loughhead, R. E. and Bray, R. J. 1961, Australian J. Phys., 14, 347). Sunspot size is dictated by granulation dynamics rather than spot size (cancellation of convective motion), and by the lifetime of the pore, which averages from 10 to 30 minutes. There is no specific aperture required for AAVSO observers contributing sunspot observations. However, the detection of the smallest spots is influenced by the resolution of the telescope. Two factors to consider are the theoretical optical resolution (unobstructed aperture), Rayleigh criterion: theta = 138 / D(mm), and Dawes criterion: theta = 116 / D(mm) (http://www.telescope-optics.net/telescope_resolution.htm). However, seeing is variable with time; daytime range will

  7. Enhanced performance of solar cells with optimized surface recombination and efficient photon capturing via anisotropic-etching of black silicon

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

    Chen, H. Y.; Peng, Y., E-mail: gdyuan@semi.ac.cn, E-mail: py@usst.edu.cn; Hong, M.

    2014-05-12

    We report an enhanced conversion efficiency of femtosecond-laser treated silicon solar cells by surface modification of anisotropic-etching. The etching improves minority carrier lifetime inside modified black silicon area substantially; moreover, after the etching, an inverted pyramids/upright pyramids mixed texture surface is obtained, which shows better photon capturing capability than that of conventional pyramid texture. Combing of these two merits, the reformed solar cells show higher conversion efficiency than that of conventional pyramid textured cells. This work presents a way for fabricating high performance silicon solar cells, which can be easily applied to mass-production.

  8. Physics of the Solar Active Regions from Radio Observations

    NASA Astrophysics Data System (ADS)

    Gelfreikh, G. B.

    1999-12-01

    Localized increase of the magnetic field observed by routine methods on the photosphere result in the growth of a number of active processes in the solar atmosphere and the heliosphere. These localized regions of increased magnetic field are called active regions (AR). The main processes of transfer, accumulation and release of energy in an AR is, however, out of scope of photospheric observations being essentially a 3D-process and happening either under photosphere or up in the corona. So, to investigate these plasma structures and processes we are bound to use either extrapolation of optical observational methods or observations in EUV, X-rays and radio. In this review, we stress and illustrate the input to the problem gained from radio astronomical methods and discuss possible future development of their applicatications. Historically speaking each new step in developing radio technique of observations resulted in detecting some new physics of ARs. The most significant progress in the last few years in radio diagnostics of the plasma structures of magnetospheres of the solar ARs is connected with the developing of the 2D full disk analysis on regular basis made at Nobeyama and detailed multichannel spectral-polarization (but one-dimensional and one per day) solar observations at the RATAN-600. In this report the bulk of attention is paid to the new approach to the study of solar activity gained with the Nobeyama radioheliograph and analyzing the ways for future progress. The most important new features of the multicomponent radio sources of the ARs studied using Nobeyama radioheliograph are as follow: 1. The analysis of magnetic field structures in solar corona above sunspot with 2000 G. Their temporal evolution and fluctuations with the periods around 3 and 5 minutes, due to MHD-waves in sunspot magnetic tubes and surrounding plasma. These investigations are certainly based on an analysis of thermal cyclotron emission of lower corona and CCTR above sunspot

  9. XMM-Newton Observations of Solar Wind Charge Exchange Emission

    NASA Technical Reports Server (NTRS)

    Snowden, S. L.; Collier, M. R.; Kuntz, K. D.

    2004-01-01

    We present an XMM-Newton spectrum of diffuse X-ray emission from within the solar system. The spectrum is dominated by O VII and O VIII lines at 0.57 keV and 0.65 keV, O VIII (and possibly Fe XVII) lines at approximately 0.8 keV, Ne IX lines at approximately 0.92 keV, and Mg XI lines at approximately 1.35 keV. This spectrum is consistent with what is expected from charge exchange emission between the highly ionized solar wind and either interstellar neutrals in the heliosphere or material from Earth's exosphere. The emission is clearly seen as a low-energy ( E less than 1.5 keV) spectral enhancement in one of a series of observations of the Hubble Deep Field North. The X-ray enhancement is concurrent with an enhancement in the solar wind measured by the ACE satellite. The solar wind enhancement reaches a flux level an order of magnitude more intense than typical fluxes at 1 AU, and has ion ratios with significantly enhanced higher ionization states. Whereas observations of the solar wind plasma made at a single point reflect only local conditions which may only be representative of solar wind properties with spatial scales ranging from less than half of an Earth radii (approximately 10 s) to 100 Earth radii, X-ray observations of solar wind charge exchange are remote sensing measurements which may provide observations which are significantly more global in character. Besides being of interest in its own right for studies of the solar system, this emission can have significant consequences for observations of more cosmological objects. It can provide emission lines at zero redshift which are of particular interest (e.g., O VII and O VIII) in studies of diffuse thermal emission, and which can therefore act as contamination in objects which cover the entire detector field of view. We propose the use of solar wind monitoring data, such as from the ACE and Wind spacecraft, as a diagnostic to screen for such possibilities.

  10. Concentrator photovoltaic module architectures with capabilities for capture and conversion of full global solar radiation

    PubMed Central

    Lee, Kyu-Tae; Yao, Yuan; He, Junwen; Fisher, Brent; Sheng, Xing; Lumb, Matthew; Xu, Lu; Anderson, Mikayla A.; Scheiman, David; Han, Seungyong; Kang, Yongseon; Gumus, Abdurrahman; Bahabry, Rabab R.; Lee, Jung Woo; Paik, Ungyu; Bronstein, Noah D.; Alivisatos, A. Paul; Meitl, Matthew; Burroughs, Scott; Hussain, Muhammad Mustafa; Lee, Jeong Chul; Nuzzo, Ralph G.; Rogers, John A.

    2016-01-01

    Emerging classes of concentrator photovoltaic (CPV) modules reach efficiencies that are far greater than those of even the highest performance flat-plate PV technologies, with architectures that have the potential to provide the lowest cost of energy in locations with high direct normal irradiance (DNI). A disadvantage is their inability to effectively use diffuse sunlight, thereby constraining widespread geographic deployment and limiting performance even under the most favorable DNI conditions. This study introduces a module design that integrates capabilities in flat-plate PV directly with the most sophisticated CPV technologies, for capture of both direct and diffuse sunlight, thereby achieving efficiency in PV conversion of the global solar radiation. Specific examples of this scheme exploit commodity silicon (Si) cells integrated with two different CPV module designs, where they capture light that is not efficiently directed by the concentrator optics onto large-scale arrays of miniature multijunction (MJ) solar cells that use advanced III–V semiconductor technologies. In this CPV+ scheme (“+” denotes the addition of diffuse collector), the Si and MJ cells operate independently on indirect and direct solar radiation, respectively. On-sun experimental studies of CPV+ modules at latitudes of 35.9886° N (Durham, NC), 40.1125° N (Bondville, IL), and 38.9072° N (Washington, DC) show improvements in absolute module efficiencies of between 1.02% and 8.45% over values obtained using otherwise similar CPV modules, depending on weather conditions. These concepts have the potential to expand the geographic reach and improve the cost-effectiveness of the highest efficiency forms of PV power generation. PMID:27930331

  11. Concentrator photovoltaic module architectures with capabilities for capture and conversion of full global solar radiation

    DOE PAGES

    Lee, Kyu-Tae; Yao, Yuan; He, Junwen; ...

    2016-12-05

    Emerging classes ofconcentrator photovoltaic (CPV) modules reach efficiencies that are far greater than those of even the highest performance flat-plate PV technologies, with architectures that have the potential to provide the lowest cost of energy in locations with high direct normal irradiance (DNI). A disadvantage is their inability to effectively use diffuse sunlight, thereby constraining widespread geographic deployment and limiting performance even under the most favorable DNI conditions. This study introduces a module design that integrates capabilities in flat-plate PV directly with the most sophisticated CPV technologies, for capture of both direct and diffuse sunlight, thereby achieving efficiency in PVmore » conversion of the global solar radiation. Specific examples of this scheme exploit commodity silicon (Si) cells integrated with two different CPV module designs, where they capture light that is not efficiently directed by the concentrator optics onto large-scale arrays of miniature multijunction (MJ) solar cells that use advanced III-V semiconductor technologies. In this CPV + scheme ("+" denotes the addition of diffuse collector), the Si and MJ cells operate independently on indirect and direct solar radiation, respectively. On-sun experimental studies of CPV + modules at latitudes of 35.9886° N (Durham, NC), 40.1125° N (Bondville, IL), and 38.9072° N (Washington, DC) show improvements in absolute module efficiencies of between 1.02% and 8.45% over values obtained using otherwise similar CPV modules, depending on weather conditions. These concepts have the potential to expand the geographic reach and improve the cost-effectiveness of the highest efficiency forms of PV power generation.« less

  12. Concentrator photovoltaic module architectures with capabilities for capture and conversion of full global solar radiation

    NASA Astrophysics Data System (ADS)

    Lee, Kyu-Tae; Yao, Yuan; He, Junwen; Fisher, Brent; Sheng, Xing; Lumb, Matthew; Xu, Lu; Anderson, Mikayla A.; Scheiman, David; Han, Seungyong; Kang, Yongseon; Gumus, Abdurrahman; Bahabry, Rabab R.; Lee, Jung Woo; Paik, Ungyu; Bronstein, Noah D.; Alivisatos, A. Paul; Meitl, Matthew; Burroughs, Scott; Mustafa Hussain, Muhammad; Lee, Jeong Chul; Nuzzo, Ralph G.; Rogers, John A.

    2016-12-01

    Emerging classes of concentrator photovoltaic (CPV) modules reach efficiencies that are far greater than those of even the highest performance flat-plate PV technologies, with architectures that have the potential to provide the lowest cost of energy in locations with high direct normal irradiance (DNI). A disadvantage is their inability to effectively use diffuse sunlight, thereby constraining widespread geographic deployment and limiting performance even under the most favorable DNI conditions. This study introduces a module design that integrates capabilities in flat-plate PV directly with the most sophisticated CPV technologies, for capture of both direct and diffuse sunlight, thereby achieving efficiency in PV conversion of the global solar radiation. Specific examples of this scheme exploit commodity silicon (Si) cells integrated with two different CPV module designs, where they capture light that is not efficiently directed by the concentrator optics onto large-scale arrays of miniature multijunction (MJ) solar cells that use advanced III-V semiconductor technologies. In this CPV+ scheme (“+” denotes the addition of diffuse collector), the Si and MJ cells operate independently on indirect and direct solar radiation, respectively. On-sun experimental studies of CPV+ modules at latitudes of 35.9886° N (Durham, NC), 40.1125° N (Bondville, IL), and 38.9072° N (Washington, DC) show improvements in absolute module efficiencies of between 1.02% and 8.45% over values obtained using otherwise similar CPV modules, depending on weather conditions. These concepts have the potential to expand the geographic reach and improve the cost-effectiveness of the highest efficiency forms of PV power generation.

  13. Concentrator photovoltaic module architectures with capabilities for capture and conversion of full global solar radiation.

    PubMed

    Lee, Kyu-Tae; Yao, Yuan; He, Junwen; Fisher, Brent; Sheng, Xing; Lumb, Matthew; Xu, Lu; Anderson, Mikayla A; Scheiman, David; Han, Seungyong; Kang, Yongseon; Gumus, Abdurrahman; Bahabry, Rabab R; Lee, Jung Woo; Paik, Ungyu; Bronstein, Noah D; Alivisatos, A Paul; Meitl, Matthew; Burroughs, Scott; Hussain, Muhammad Mustafa; Lee, Jeong Chul; Nuzzo, Ralph G; Rogers, John A

    2016-12-20

    Emerging classes of concentrator photovoltaic (CPV) modules reach efficiencies that are far greater than those of even the highest performance flat-plate PV technologies, with architectures that have the potential to provide the lowest cost of energy in locations with high direct normal irradiance (DNI). A disadvantage is their inability to effectively use diffuse sunlight, thereby constraining widespread geographic deployment and limiting performance even under the most favorable DNI conditions. This study introduces a module design that integrates capabilities in flat-plate PV directly with the most sophisticated CPV technologies, for capture of both direct and diffuse sunlight, thereby achieving efficiency in PV conversion of the global solar radiation. Specific examples of this scheme exploit commodity silicon (Si) cells integrated with two different CPV module designs, where they capture light that is not efficiently directed by the concentrator optics onto large-scale arrays of miniature multijunction (MJ) solar cells that use advanced III-V semiconductor technologies. In this CPV + scheme ("+" denotes the addition of diffuse collector), the Si and MJ cells operate independently on indirect and direct solar radiation, respectively. On-sun experimental studies of CPV + modules at latitudes of 35.9886° N (Durham, NC), 40.1125° N (Bondville, IL), and 38.9072° N (Washington, DC) show improvements in absolute module efficiencies of between 1.02% and 8.45% over values obtained using otherwise similar CPV modules, depending on weather conditions. These concepts have the potential to expand the geographic reach and improve the cost-effectiveness of the highest efficiency forms of PV power generation.

  14. Observational Signatures of Magnetic Reconnection

    NASA Technical Reports Server (NTRS)

    Savage, Sabrina

    2014-01-01

    Magnetic reconnection is often referred to as the primary source of energy release during solar flares. Directly observing reconnection occurring in the solar atmosphere, however, is not trivial considering that the scale size of the diffusion region is magnitudes smaller than the observational capabilities of current instrumentation, and coronal magnetic field measurements are not currently sufficient to capture the process. Therefore, predicting and studying observationally feasible signatures of the precursors and consequences of reconnection is necessary for guiding and verifying the simulations that dominate our understanding. I will present a set of such observations, particularly in connection with long-duration solar events, and compare them with recent simulations and theoretical predictions.

  15. The Solar Wind from Pseudostreamers and their Environs: Opportunities for Observations with Parker Solar Probe and Solar Orbiter

    NASA Astrophysics Data System (ADS)

    Panasenco, O.; Velli, M.; Panasenco, A.; Lionello, R.

    2017-12-01

    The solar dynamo and photospheric convection lead to three main types of structures extending from the solar surface into the corona - active regions, solar filaments (prominences when observed at the limb) and coronal holes. These structures exist over a wide range of scales, and are interlinked with each other in evolution and dynamics. Active regions can form clusters of magnetic activity and the strongest overlie sunspots. In the decay of active regions, the boundaries separating opposite magnetic polarities (neutral lines) develop specific structures called filament channels above which filaments form. In the presence of flux imbalance decaying active regions can also give birth to lower latitude coronal holes. The accumulation of magnetic flux at coronal hole boundaries also creates conditions for filament formation: polar crown filaments are permanently present at the boundaries of the polar coronal holes. Mid-latitude and equatorial coronal holes - the result of active region evolution - can create pseudostreamers if other coronal holes of the same polarity are present. While helmet streamers form between open fields of opposite polarities, the pseudostreamer, characterized by a smaller coronal imprint, typically shows a more prominent straight ray or stalk extending from the corona. The pseudostreamer base at photospheric heights is multipolar; often one observes tripolar magnetic configurations with two neutral lines - where filaments can form - separating the coronal holes. Here we discuss the specific role of filament channels on pseudostreamer topology and on solar wind properties. 1D numerical analysis of pseudostreamers shows that the properties of the solar wind from around PSs depend on the presence/absence of filament channels, number of channels and chirality at thepseudostreamer base low in the corona. We review and model possible coronal magnetic configurations and solar wind plasma properties at different distances from the solar surface that

  16. Solar Flare Impulsive Phase Observations from SDO and Other Observatories

    NASA Technical Reports Server (NTRS)

    Chamberlin, Phillip C.; Woods, Thomas N.; Schrijver, Karel; Warren, Harry; Milligan, Ryan; Christe, Steven; Brosius, Jeffrey W.

    2010-01-01

    With the start of normal operations of the Solar Dynamics Observatory in May 2010, the Extreme ultraviolet Variability Experiment (EVE) and the Atmospheric Imaging Assembly (AIA) have been returning the most accurate solar XUV and EUV measurements every 10 and 12 seconds, respectively, at almost 100% duty cycle. The focus of the presentation will be the solar flare impulsive phase observations provided by EVE and AIA and what these observations can tell us about the evolution of the initial phase of solar flares. Also emphasized throughout is how simultaneous observations with other instruments, such as RHESSI, SOHO-CDS, and HINODE-EIS, will help provide a more complete characterization of the solar flares and the evolution and energetics during the impulsive phase. These co-temporal observations from the other solar instruments can provide information such as extending the high temperature range spectra and images beyond that provided by the EUV and XUV wavelengths, provide electron density input into the lower atmosphere at the footpoints, and provide plasma flows of chromospheric evaporation, among other characteristics.

  17. Unique sudden onsets capture attention even when observers are in feature-search mode.

    PubMed

    Spalek, Thomas M; Yanko, Matthew R; Poiese, Paola; Lagroix, Hayley E P

    2012-01-01

    Two sources of attentional capture have been proposed: stimulus-driven (exogenous) and goal-oriented (endogenous). A resolution between these modes of capture has not been straightforward. Even such a clearly exogenous event as the sudden onset of a stimulus can be said to capture attention endogenously if observers operate in singleton-detection mode rather than feature-search mode. In four experiments we show that a unique sudden onset captures attention even when observers are in feature-search mode. The displays were rapid serial visual presentation (RSVP) streams of differently coloured letters with the target letter defined by a specific colour. Distractors were four #s, one of the target colour, surrounding one of the non-target letters. Capture was substantially reduced when the onset of the distractor array was not unique because it was preceded by other sets of four grey # arrays in the RSVP stream. This provides unambiguous evidence that attention can be captured both exogenously and endogenously within a single task.

  18. Solar spectral irradiance variability in cycle 24: observations and models

    NASA Astrophysics Data System (ADS)

    Marchenko, Sergey V.; DeLand, Matthew T.; Lean, Judith L.

    2016-12-01

    Utilizing the excellent stability of the Ozone Monitoring Instrument (OMI), we characterize both short-term (solar rotation) and long-term (solar cycle) changes of the solar spectral irradiance (SSI) between 265 and 500 nm during the ongoing cycle 24. We supplement the OMI data with concurrent observations from the Global Ozone Monitoring Experiment-2 (GOME-2) and Solar Radiation and Climate Experiment (SORCE) instruments and find fair-to-excellent, depending on wavelength, agreement among the observations, and predictions of the Naval Research Laboratory Solar Spectral Irradiance (NRLSSI2) and Spectral And Total Irradiance REconstruction for the Satellite era (SATIRE-S) models.

  19. Resource Letter OSE-1: Observing Solar Eclipses

    NASA Astrophysics Data System (ADS)

    Pasachoff, Jay M.; Fraknoi, Andrew

    2017-07-01

    This Resource Letter provides a guide to the available literature, listing selected books, articles, and online resources about scientific, cultural, and practical issues related to observing solar eclipses. It is timely, given that a total solar eclipse will cross the continental United States on August 21, 2017. The next total solar eclipse path crossing the U.S. and Canada will be on April 8, 2024. In 2023, the path of annularity of an annular eclipse will cross Mexico, the United States, and Canada, with partial phases visible throughout those countries.

  20. Observations of hysteresis in solar cycle variations among seven solar activity indicators

    NASA Technical Reports Server (NTRS)

    Bachmann, Kurt T.; White, Oran R.

    1994-01-01

    We show that smoothed time series of 7 indices of solar activity exhibit significant solar cycle dependent differences in their relative variations during the past 20 years. In some cases these observed hysteresis patterns start to repeat over more than one solar cycle, giving evidence that this is a normal feature of solar variability. Among the indices we study, we find that the hysteresis effects are approximately simple phase shifts, and we quantify these phase shifts in terms of lag times behind the leading index, the International Sunspot Number. Our measured lag times range from less than one month to greater than four months and can be much larger than lag times estimated from short-term variations of these same activity indices during the emergence and decay of major active regions. We argue that hysteresis represents a real delay in the onset and decline of solar activity and is an important clue in the search for physical processes responsible for changing solar emission at various wavelengths.

  1. Asymmetric capture of Dirac dark matter by the Sun

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

    Blennow, Mattias; Clementz, Stefan

    2015-08-18

    Current problems with the solar model may be alleviated if a significant amount of dark matter from the galactic halo is captured in the Sun. We discuss the capture process in the case where the dark matter is a Dirac fermion and the background halo consists of equal amounts of dark matter and anti-dark matter. By considering the case where dark matter and anti-dark matter have different cross sections on solar nuclei as well as the case where the capture process is considered to be a Poisson process, we find that a significant asymmetry between the captured dark particles andmore » anti-particles is possible even for an annihilation cross section in the range expected for thermal relic dark matter. Since the captured number of particles are competitive with asymmetric dark matter models in a large range of parameter space, one may expect solar physics to be altered by the capture of Dirac dark matter. It is thus possible that solutions to the solar composition problem may be searched for in these type of models.« less

  2. Wind Observations of Anomalous Cosmic Rays from Solar Minimum to Maximum

    NASA Technical Reports Server (NTRS)

    Reames, D. V.; McDonald, F. B.

    2003-01-01

    We report the first observation near Earth of the time behavior of anomalous cosmic-ray N, O, and Ne ions through the period surrounding the maximum of the solar cycle. These observations were made by the Wind spacecraft during the 1995-2002 period spanning times from solar minimum through solar maximum. Comparison of anomalous and galactic cosmic rays provides a powerful tool for the study of the physics of solar modulation throughout the solar cycle.

  3. Study of photon emission by electron capture during solar nuclei acceleration. 3: Photon production evaluations

    NASA Technical Reports Server (NTRS)

    Perez-Peraza, J.; Alvarez, M.; Gallegos, A.

    1985-01-01

    Lower limits of photon fluxes were evaluated from electron capture during acceleration in solar flares, because the arbitrary q sub c asterisk assumed in this work evolves very slow with velocity, probably much more slowly than the physical actual situation: in fact, more emission is expected toward the IR region. Nevertheless the authors claim to show that the factibility of sounding acceleration processes, charge evolution processes and physical parameters of the source itself, by the observational analysis of this kind of emissions. For instance, it would be interesting to search observationally, for the predicted flux and energy drift of F sub e ions interacting with the atomic 0 and F sub e of the source matter, or, even more feasible for the X-ray lines at 4.2 keV and 2.624 + 0.003 KeV from Fe and S ions in ionized Fe at T = 10 to the 7th power K respectively, the 418 + or - 2 eV and 20 + or - 4 eV lines of Fe and S in ionized Fe at 5 x 10 to the 6th power K, which are predicted from Fermi acceleration.

  4. LASCO Observations Of The K-Corona From Solar Minimum To Solar Maximum And Beyond

    NASA Astrophysics Data System (ADS)

    Andrews, Michael D.; Howard, Russell A.

    2003-09-01

    The LASCO C2 and C3 coronagraphs on SOHO have been recording a regular series of images of the corona since May 1996. This sequence of data covers the period of solar minimum, the increase to solar maximum, and the beginning of the decline toward the next solar minimum. The images have been analyzed to determine the brightness of the K-corona (solar photons Thomson scattered from free electrons). The total brightness of the K-corona is approximately constant from May 1996 through May 1997. The brightness is then seen to increase steadily until early in the year 2000. The structure of the K-corona changes dramatically with solar cycle. The shape as seen in C2 becomes almost circular at solar maximum while the C3 images continue to show equatorial streamers. The magnitude of the solar cycle variation decreases as the height increases. We present data animations (movies) to show the large-scale structure. We have inverted 28-day averages of the white light images to determine radial profiles of electron density. We present these electron profiles, show how they vary as a function of both latitude and time, and compare our observed profiles with other models and observations.

  5. MAVEN observations of the solar cycle 24 space weather conditions at Mars

    NASA Astrophysics Data System (ADS)

    Lee, C. O.; Hara, T.; Halekas, J. S.; Thiemann, E.; Chamberlin, P.; Eparvier, F.; Lillis, R. J.; Larson, D. E.; Dunn, P. A.; Espley, J. R.; Gruesbeck, J.; Curry, S. M.; Luhmann, J. G.; Jakosky, B. M.

    2017-03-01

    The Mars Atmosphere and Volatile EvolutioN (MAVEN) spacecraft has been continuously observing the variability of solar soft X-rays and EUV irradiance, monitoring the upstream solar wind and interplanetary magnetic field conditions and measuring the fluxes of solar energetic ions and electrons since its arrival to Mars. In this paper, we provide a comprehensive overview of the space weather events observed during the first ˜1.9 years of the science mission, which includes the description of the solar and heliospheric sources of the space weather activity. To illustrate the variety of upstream conditions observed, we characterize a subset of the event periods by describing the Sun-to-Mars details using observations from the MAVEN solar Extreme Ultraviolet Monitor, solar energetic particle (SEP) instrument, Solar Wind Ion Analyzer, and Magnetometer together with solar observations using near-Earth assets and numerical solar wind simulation results from the Wang-Sheeley-Arge-Enlil model for some global context of the event periods. The subset of events includes an extensive period of intense SEP electron particle fluxes triggered by a series of solar flares and coronal mass ejection (CME) activity in December 2014, the impact by a succession of interplanetary CMEs and their associated SEPs in March 2015, and the passage of a strong corotating interaction region (CIR) and arrival of the CIR shock-accelerated energetic particles in June 2015. However, in the context of the weaker heliospheric conditions observed throughout solar cycle 24, these events were moderate in comparison to the stronger storms observed previously at Mars.

  6. Amateur observations of solar eclipses and derivation of scientific data

    NASA Astrophysics Data System (ADS)

    Stoev, A. D.; Stoeva, P. V.

    2008-12-01

    This work presents the educational approach of using total solar eclipse occurrences as a scientific process learning aid. The work reviews the basic scientific aims and experiments included in the observational programs "Total solar eclipse 1999 and 2006" (Stoev, A., Kiskinova, N., Muglova, P. et al. Complex observational programme of the Yuri Gagarin Public Astronomical Observatory and STIL, BAS, Stara Zagora Department for the August 11, 1999 total solar eclipse, in: Total Solar Eclipse 1999 - Observational Programmes and Coordination, Proceedings, Recol, Haskovo, pp. 133-137, 1999a (in Bulgarian); Stoeva, P.V., Stoev, A.D., Kostadinov, I.N. et al. Solar Corona and Atmospheric Effects during the March 29, 2006 Total Solar Eclipse, in: 11th International Science Conference SOLAR-Terrestrial Influences, Sofia, November 24-25, pp. 69-72, 2005). Results from teaching and training the students in the procedures, methods and equipment necessary for the observation of a total solar eclipse (TSE) at the Yuri Gagarin Public Astronomical Observatory (PAO) in Stara Zagora, Bulgaria, as well as the selection process used in determining participation in the different observational teams are discussed. The final stages reveal the special methodology used to investigate the level of "pretensions", the levels of ambition displayed by the students in achieving each independent goal, and the setting of goals in context with their problem solving capabilities and information gathering abilities in the scientific observation process. Results obtained from the observational experiments are interpreted mainly in the following themes: Investigation of the structure of the white-light solar corona and evolution of separate coronal elements during the total phase of the eclipse; Photometry of the white-light solar corona and specific emission lines; Meteorological, actinometrical and optical atmospheric investigations; Astrometry of the Moon during the phase evolution of the eclipse and

  7. Observations and statistical simulations of a proposed solar cycle/QBO/weather relationship

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

    Baldwin, M.P.; Dunkerton, T.J.

    1989-08-01

    The 10.7 cm solar flux is observed to be highly correlated with north pole stratospheric temperatures when partitioned according to the phase of the equatorial stratospheric winds (the quasi-biennial oscillation, or QBO). The authors supplement observations with calculations showing that temperatures over most of the northern hemisphere are highly correlated or anticorrelated with north pole temperatures. The observed spatial pattern of solar cycle correlations at high latitudes is shown to be not unique to the solar cycle. The authors present results, similar to the observed solar cycle correlations, with simulated harmonics of various periods replacing the solar cycle. These calculationsmore » demonstrate the correlations at least as high as those for the solar cycle results may be obtained using simulated harmonics.« less

  8. Description and primary results of Total Solar Irradiance Monitor, a solar-pointing instrument on an Earth observing satellite

    NASA Astrophysics Data System (ADS)

    Wang, Hongrui; Fang, Wei; Li, Huiduan

    2015-04-01

    Solar driving mechanism for Earth climate has been a controversial problem for centuries. Long-time data of solar activity is required by the investigations of the solar driving mechanism, such as Total Solar Irradiance (TSI) record. Three Total Solar Irradiance Monitors (TSIM) have been developed by Changchun Institute of Optics, Fine Mechanics and Physics for China Meteorological Administration to maintain continuities of TSI data series which lasted for nearly 4 decades.The newest TSIM has recorded TSI daily with accurate solar pointing on the FY-3C meteorological satellite since Oct 2013. TSIM/FY-3C has a pointing system for automatic solar tracking, onboard the satellite designed mainly for Earth observing. Most payloads of FY-3C are developed for observation of land, ocean and atmosphere. Consequently, the FY-3C satellite is a nadir-pointing spacecraft with its z axis to be pointed at the center of the Earth. Previous TSIMs onboard the FY-3A and FY-3B satellites had no pointing system, solar observations were only performed when the sun swept through field-of-view of the instruments. And TSI measurements are influenced inevitably by the solar pointing errors. Corrections of the solar pointing errors were complex. The problem is now removed by TSIM/FY-3C.TSIM/FY-3C follows the sun accurately by itself using its pointing system based on scheme of visual servo control. The pointing system is consisted of a radiometer package, two motors for solar tracking, a sun sensor and etc. TSIM/FY-3C has made daily observations of TSI for more than one year, with nearly zero solar pointing errors. Short time-scale variations in TSI detected by TSIM/FY-3C are nearly the same with VIRGO/SOHO and TIM/SORCE.Instrument details, primary results of solar pointing control, solar observations and etc will be given in the presentation.

  9. Ionospheric model-observation comparisons: E layer at Arecibo Incorporation of SDO-EVE solar irradiances

    NASA Astrophysics Data System (ADS)

    Sojka, Jan J.; Jensen, Joseph B.; David, Michael; Schunk, Robert W.; Woods, Tom; Eparvier, Frank; Sulzer, Michael P.; Gonzalez, Sixto A.; Eccles, J. Vincent

    2014-05-01

    This study evaluates how the new irradiance observations from the NASA Solar Dynamics Observatory (SDO) Extreme Ultraviolet Variability Experiment (EVE) can, with its high spectral resolution and 10 s cadence, improve the modeling of the E region. To demonstrate this a campaign combining EVE observations with that of the NSF Arecibo incoherent scatter radar (ISR) was conducted. The ISR provides E region electron density observations with high-altitude resolution, 300 m, and absolute densities using the plasma line technique. Two independent ionospheric models were used, the Utah State University Time-Dependent Ionospheric Model (TDIM) and Space Environment Corporation's Data-Driven D Region (DDDR) model. Each used the same EVE irradiance spectrum binned at 1 nm resolution from 0.1 to 106 nm. At the E region peak the modeled TDIM density is 20% lower and that of the DDDR is 6% higher than observed. These differences could correspond to a 36% lower (TDIM) and 12% higher (DDDR) production rate if the differences were entirely attributed to the solar irradiance source. The detailed profile shapes that included the E region altitude and that of the valley region were only qualitatively similar to observations. Differences on the order of a neutral-scale height were present. Neither model captured a distinct dawn to dusk tilt in the E region peak altitude. A model sensitivity study demonstrated how future improved spectral resolution of the 0.1 to 7 nm irradiance could account for some of these model shortcomings although other relevant processes are also poorly modeled.

  10. Observational methods for solar origin diagnostics of energetic protons

    NASA Astrophysics Data System (ADS)

    Miteva, Rositsa

    2017-12-01

    The aim of the present report is to outline the observational methods used to determine the solar origin - in terms of flares and coronal mass ejections (CMEs) - of the in situ observed solar energetic protons. Several widely used guidelines are given and different sources of uncertainties are summarized and discussed. In the present study, a new quality factor is proposed as a certainty check on the so-identified flare-CME pairs. In addition, the correlations between the proton peak intensity and the properties of their solar origin are evaluated as a function of the quality factor.

  11. Solar flares observed simultaneously with SphinX, GOES and RHESSI

    NASA Astrophysics Data System (ADS)

    Mrozek, Tomasz; Gburek, Szymon; Siarkowski, Marek; Sylwester, Barbara; Sylwester, Janusz; Kępa, Anna; Gryciuk, Magdalena

    2013-07-01

    In February 2009, during recent deepest solar minimum, Polish Solar Photometer in X-rays (SphinX) begun observations of the Sun in the energy range of 1.2-15 keV. SphinX was almost 100 times more sensitive than GOES X-ray Sensors. The silicon PIN diode detectors used in the experiment were carefully calibrated on the ground using Synchrotron Radiation Source BESSY II. The SphinX energy range overlaps with the Ramaty High Energy Solar Spectroscopic Imager (RHESSI) energy range. The instrument provided us with observations of hundreds of very small flares and X-ray brightenings. We have chosen a group of solar flares observed simultaneously with GOES, SphinX and RHESSI and performed spectroscopic analysis of observations wherever possible. The analysis of thermal part of the spectra showed that SphinX is a very sensitive complementary observatory for RHESSI and GOES.

  12. Thermalization time scales for WIMP capture by the Sun in effective theories

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

    Widmark, A., E-mail: axel.widmark@fysik.su.se

    I study the process of dark matter capture by the Sun, under the assumption of a Weakly Interacting Massive Particle (WIMP), in the framework of non-relativistic effective field theory. Hypothetically, WIMPs from the galactic halo can scatter against atomic nuclei in the solar interior, settle to thermal equilibrium with the solar core and annihilate to produce an observable flux of neutrinos. In particular, I examine the thermalization process using Monte-Carlo integration of WIMP trajectories. I consider WIMPs in a mass range of 10–1000 GeV and WIMP-nucleon interaction operators with different dependence on spin and transferred momentum. I find that themore » density profiles of captured WIMPs are in accordance with a thermal profile described by the Sun's gravitational potential and core temperature. Depending on the operator that governs the interaction, the majority of the thermalization time is spent in either the solar interior or exterior. If normalizing the WIMP-nuclei interaction strength to a specific capture rate, I find that the thermalization time differs at most by 3 orders of magnitude between operators. In most cases of interest, the thermalization time is many orders of magnitude shorter than the age of the solar system.« less

  13. Solar energy microclimate as determined from satellite observations

    NASA Technical Reports Server (NTRS)

    Vonder Haar, T. H.; Ellis, J. S.

    1975-01-01

    A method is presented for determining solar insolation at the earth's surface using satellite broadband visible radiance and cloud imagery data, along with conventional in situ measurements. Conventional measurements are used to both tune satellite measurements and to develop empirical relationships between satellite observations and surface solar insolation. Cloudiness is the primary modulator of sunshine. The satellite measurements as applied in this method consider cloudiness both explicitly and implicitly in determining surface solar insolation at space scales smaller than the conventional pyranometer network.

  14. Solar System Observations with the James Webb Space Telescope

    NASA Technical Reports Server (NTRS)

    Norwood, James; Hammel, Heidi; Milam, Stefanie; Stansberry, John; Lunine, Jonathan; Chanover, Nancy; Hines, Dean; Sonneborn, George; Tiscareno, Matthew; Brown, Michael; hide

    2016-01-01

    The James Webb Space Telescope (JWST) will enable a wealth of new scientific investigations in the near- and mid-infrared, with sensitivity and spatial/spectral resolution greatly surpassing its predecessors. In this paper, we focus upon Solar System science facilitated by JWST, discussing the most current information available concerning JWST instrument properties and observing techniques relevant to planetary science. We also present numerous example observing scenarios for a wide variety of Solar System targets to illustrate the potential of JWST science to the Solar System community. This paper updates and supersedes the Solar System white paper published by the JWST Project in 2010. It is based both on that paper and on a workshop held at the annual meeting of the Division for Planetary Sciences in Reno, NV, in 2012.

  15. Common SphinX and RHESSI observations of solar flares

    NASA Astrophysics Data System (ADS)

    Mrozek, T.; Gburek, S.; Siarkowski, M.; Sylwester, B.; Sylwester, J.; Gryciuk, M.

    The Polish X-ray spectrofotometer SphinX has observed a great number of solar flares in the year 2009 - during the most quiet solar minimum almost over the last 100 years. Hundreds of flares have been recorded due to excellent sensitivity of SphinX's detectors. The Si-PIN diodes are about 100 times more sensitive to X-rays than GOES X-ray Monitors. SphinX detectors were absolutely calibrated on Earth with a use of the BESSY synchrotron. In space observations were made in the range 1.2-15~keV with 480~eV energy resolution. SphinX data overlap with the low-energy end of the Ramaty High Energy Solar Spectroscopic Imager (RHESSI) data. RHESSI detectors are quite old (7 years in 2009), but still sensitive enough to provide us with observations of extremely weak solar flares such as those which occurred in 2009. We have selected a group of flares simultaneously observed by RHESSI and SphinX and performed a spectroscopic analysis of the data. Moreover, we compared the physical parameters of these flares plasma. Preliminary results of the comparison show very good agreement between both instruments.

  16. Continued Analysis of EUVE Solar System Observations

    NASA Technical Reports Server (NTRS)

    Gladstone, G. Randall

    2001-01-01

    This is the final report for this project. We proposed to continue our work on extracting important results from the EUVE (Extreme UltraViolet Explorer) archive of lunar and jovian system observations. In particular, we planned to: (1) produce several monochromatic images of the Moon at the wavelengths of the brightest solar EUV emission lines; (2) search for evidence of soft X-ray emissions from the Moon and/or X-ray fluorescence at specific EUV wavelengths; (3) search for localized EUV and soft X-ray emissions associated with each of the Galilean satellites; (4) search for correlations between localized Io Plasma Torus (IPT) brightness and volcanic activity on Io; (5) search for soft X-ray emissions from Jupiter; and (6) determine the long term variability of He 58.4 nm emissions from Jupiter, and relate these to solar variability. However, the ADP review panel suggested that the work concentrate on the Jupiter/IPT observations, and provided half the requested funding. Thus we have performed no work on the first two tasks, and instead concentrated on the last three. In addition we used funds from this project to support reduction and analysis of EUVE observations of Venus. While this was not part of the original statement of work, it is entirely in keeping with extracting important results from EUVE solar system observations.

  17. Results of solar observations by the CORONAS-F payload

    NASA Astrophysics Data System (ADS)

    Kuznetsov, V. D.; Sobelman, I. I.; Zhitnik, I. A.; Kuzin, S. V.; Kotov, Yu. D.; Charikov, Yu. E.; Kuznetsov, S. N.; Mazets, E. P.; Nusinov, A. A.; Pankov, A. M.; Sylwester, J.

    2011-05-01

    The CORONAS-F mission experiments and results have been reviewed. The observations with the DIFOS multi-channel photometer in a broad spectral range from 350 to 1500 nm have revealed the dependence of the relative amplitudes of p-modes of the global solar oscillations on the wavelength that agrees perfectly well with the earlier data obtained in a narrower spectral ranges. The SPIRIT EUV observations have enabled the study of various manifestations of solar activity and high-temperature events on the Sun. The data from the X-ray spectrometer RESIK, gamma spectrometer HELICON, flare spectrometer IRIS, amplitude-temporal spectrometer AVS-F, and X-ray spectrometer RPS-1 have been used to analyze the X- and gamma-ray emission from solar flares and for diagnostics of the flaring plasma. The absolute and relative content of various elements (such as potassium, argon, and sulfur) of solar plasma in flares has been determined for the first time with the X-ray spectrometer RESIK. The Solar Cosmic Ray Complex monitored the solar flare effects in the Earth's environment. The UV emission variations recorded during solar flares in the vicinity of the 120-nm wavelength have been analyzed and the amplitude of relative variations has been determined.

  18. Elemental GCR Observations during the 2009-2010 Solar Minimum Period

    NASA Technical Reports Server (NTRS)

    Lave, K. A.; Israel, M. H.; Binns, W. R.; Christian, E. R.; Cummings, A. C.; Davis, A. J.; deNolfo, G. A.; Leske, R. A.; Mewaldt, R. A.; Stone, E. C.; hide

    2013-01-01

    Using observations from the Cosmic Ray Isotope Spectrometer (CRIS) onboard the Advanced Composition Explorer (ACE), we present new measurements of the galactic cosmic ray (GCR) elemental composition and energy spectra for the species B through Ni in the energy range approx. 50-550 MeV/nucleon during the record setting 2009-2010 solar minimum period. These data are compared with our observations from the 1997-1998 solar minimum period, when solar modulation in the heliosphere was somewhat higher. For these species, we find that the intensities during the 2009-2010 solar minimum were approx. 20% higher than those in the previous solar minimum, and in fact were the highest GCR intensities recorded during the space age. Relative abundances for these species during the two solar minimum periods differed by small but statistically significant amounts, which are attributed to the combination of spectral shape differences between primary and secondary GCRs in the interstellar medium and differences between the levels of solar modulation in the two solar minima. We also present the secondary-to-primary ratios B/C and (Sc+Ti+V)/Fe for both solar minimum periods, and demonstrate that these ratios are reasonably well fit by a simple "leaky-box" galactic transport model that is combined with a spherically symmetric solar modulation model.

  19. UV solar irradiance in observations and the NRLSSI and SATIRE-S models

    NASA Astrophysics Data System (ADS)

    Yeo, K. L.; Ball, W. T.; Krivova, N. A.; Solanki, S. K.; Unruh, Y. C.; Morrill, J.

    2015-08-01

    Total solar irradiance and UV spectral solar irradiance has been monitored since 1978 through a succession of space missions. This is accompanied by the development of models aimed at replicating solar irradiance by relating the variability to solar magnetic activity. The Naval Research Laboratory Solar Spectral Irradiance (NRLSSI) and Spectral And Total Irradiance REconstruction for the Satellite era (SATIRE-S) models provide the most comprehensive reconstructions of total and spectral solar irradiance over the period of satellite observation currently available. There is persistent controversy between the various measurements and models in terms of the wavelength dependence of the variation over the solar cycle, with repercussions on our understanding of the influence of UV solar irradiance variability on the stratosphere. We review the measurement and modeling of UV solar irradiance variability over the period of satellite observation. The SATIRE-S reconstruction is consistent with spectral solar irradiance observations where they are reliable. It is also supported by an independent, empirical reconstruction of UV spectral solar irradiance based on Upper Atmosphere Research Satellite/Solar Ultraviolet Spectral Irradiance Monitor measurements from an earlier study. The weaker solar cycle variability produced by NRLSSI between 300 and 400 nm is not evident in any available record. We show that although the method employed to construct NRLSSI is principally sound, reconstructed solar cycle variability is detrimentally affected by the uncertainty in the SSI observations it draws upon in the derivation. Based on our findings, we recommend, when choosing between the two models, the use of SATIRE-S for climate studies.

  20. Solar Control of Earth's Ionosphere: Observations from Solar Cycle 23

    NASA Astrophysics Data System (ADS)

    Doe, R. A.; Thayer, J. P.; Solomon, S. C.

    2005-05-01

    A nine year database of sunlit E-region electron density altitude profiles (Ne(z)) measured by the Sondrestrom ISR has been partitioned over a 30-bin parameter space of averaged 10.7 cm solar radio flux (F10.7) and solar zenith angle (χ) to investigate long-term solar and thermospheric variability, and to validate contemporary EUV photoionization models. A two stage filter, based on rejection of Ne(z) profiles with large Hall to Pedersen ratio, is used to minimize auroral contamination. Resultant filtered mean Ne(z) compares favorably with subauroral Ne measured for the same F10.7 and χ conditions at the Millstone Hill ISR. Mean Ne, as expected, increases with solar activity and decreases with large χ, and the variance around mean Ne is shown to be greatest at low F10.7 (solar minimum). ISR-derived mean Ne is compared with two EUV models: (1) a simple model without photoelectrons and based on the 5 -- 105 nm EUVAC model solar flux [Richards et al., 1994] and (2) the GLOW model [Solomon et al., 1988; Solomon and Abreu, 1989] suitably modified for inclusion of XUV spectral components and photoelectron flux. Across parameter space and for all altitudes, Model 2 provides a closer match to ISR mean Ne and suggests that the photoelectron and XUV enhancements are essential to replicate measured plasma densities below 150 km. Simulated Ne variance envelopes, given by perturbing the Model 2 neutral atmosphere input by the measured extremum in Ap, F10.7, and Te, are much narrower than ISR-derived geophysical variance envelopes. We thus conclude that long-term variability of the EUV spectra dominates over thermospheric variability and that EUV spectral variability is greatest at solar minimum. ISR -- model comparison also provides evidence for the emergence of an H (Lyman β) Ne feature at solar maximum. Richards, P. G., J. A. Fennelly, and D. G. Torr, EUVAC: A solar EUV flux model for aeronomic calculations, J. Geophys. Res., 99, 8981, 1994. Solomon, S. C., P. B. Hays

  1. Solar Observations as Educational Tools (P8)

    NASA Astrophysics Data System (ADS)

    Shylaja, B. S.

    2006-11-01

    taralaya89@yahoo.co.in Solar observations are very handy tools to expose the students to the joy of research. In this presentation I briefly discuss the various experiments already done here with a small 6" Coude refractor. These include simple experiments like eclipse observations, rotation measurements, variation in the angular size of the sun through the year as well as sun spot size variations, Doppler measurements, identification of elements from solar spectrum (from published high resolution spectrum), limb darkening measurements, deriving the curve of growth (from published data). I also describe the theoretical implications of the experiments and future plans to develop this as a platform for motivating students towards a career in basic science research.

  2. Solar observations carried out at the INAF - Catania Astrophysical Observatory

    NASA Astrophysics Data System (ADS)

    Zuccarello, F.; Contarino, L.; Romano, P.

    2011-10-01

    Solar observations at the INAF - Catania Astrophysical Observatory are carried out by means of an equatorial spar, which includes: a Cook refractor, used to make daily drawings of sunspot groups from visual observations; a 150-mm refractor with an Hα Lyot filter for chromospheric observations; a 150-mm refractor feeding an Hα Halle filter for limb observations of the chromosphere. The photospheric and chromospheric data are daily distributed to several international Solar Data Centers. Recently, a program of Flare Warning has been implemented, with the aim of determining the probability that an active region yields a flare on the basis of its characteristics deduced from optical observations. Some science results obtained by means of solar data acquired at the INAF - Catania Astrophysical Observatory, as well as by space-instruments data, are briefly described.

  3. Nucleosynthesis: Stellar and Solar Abundances and Atomic Data

    NASA Technical Reports Server (NTRS)

    Cowan, John J.; Lawler, James E.; Sneden, Christopher; DenHartog, E. A.; Collier, Jason; Dodge, Homer L.

    2006-01-01

    Abundance observations indicate the presence of often surprisingly large amounts of neutron capture (i.e., s- and r-process) elements in old Galactic halo and globular cluster stars. These observations provide insight into the nature of the earliest generations of stars in the Galaxy the progenitors of the halo stars responsible for neutron-capture synthesis. Comparisons of abundance trends can be used to understand the chemical evolution of the Galaxy and the nature of heavy element nucleosynthesis. In addition age determinations, based upon long-lived radioactive nuclei abundances, can now be obtained. These stellar abundance determinations depend critically upon atomic data. Improved laboratory transition probabilities have been recently obtained for a number of elements. These new gf values have been used to greatly refine the abundances of neutron-capture elemental abundances in the solar photosphere and in very metal-poor Galactic halo stars. The newly determined stellar abundances are surprisingly consistent with a (relative) Solar System r-process pattern, and are also consistent with abundance predictions expected from such neutron-capture nucleosynthesis.

  4. Solar and Galactic Cosmic Rays Observed by SOHO

    NASA Astrophysics Data System (ADS)

    Fleck, Bernhard; Curdt, Werner; Olive, Jean-Philippe; van Overbeek, Ton

    2015-04-01

    Both the Cosmic Ray Flux (CRF) and Solar Energetic Particles (SEPs) have left an imprint on SOHO technical systems. While the solar array efficiency degraded irreversibly down to 75% of its original level over 1 ½ solar cycles, Single Event Upsets (SEUs) in the solid state recorder (SSR) have been reversed by the memory protection mechanism. We compare the daily CRF observed by the Oulu station with the daily SOHO SEU rate and with the degradation curve of the solar arrays. The Oulu CRF and the SOHO SSR SEU rate are both modulated by the solar cycle and are highly correlated, except for sharp spikes in the SEU rate, caused by isolated SEP events, which also show up as discontinuities in the otherwise slowly decreasing solar ray efficiency. This allows to discriminate between effects with solar and non-solar origin and to compare the relative strength of both. We find that the total number of SSR SEUs with solar origin over the 17 ½ years from January 1996 through June 2013 is of the same order as those generated by cosmic ray hits. 49% of the total solar array degradation during that time can be attributed to proton events, i.e. the effect of a series of short-lived, violent events (SEPs) is comparable to the cycle-integrated damage by cosmic rays.

  5. Integrated Access to Solar Observations With EGSO

    NASA Astrophysics Data System (ADS)

    Csillaghy, A.

    2003-12-01

    {\\b Co-Authors}: J.Aboudarham (2), E.Antonucci (3), R.D.Bentely (4), L.Ciminiera (5), A.Finkelstein (4), J.B.Gurman(6), F.Hill (7), D.Pike (8), I.Scholl (9), V.Zharkova and the EGSO development team {\\b Institutions}: (2) Observatoire de Paris-Meudon (France); (3) INAF - Istituto Nazionale di Astrofisica (Italy); (4) University College London (U.K.); (5) Politecnico di Torino (Italy), (6) NASA Goddard Space Flight Center (USA); (7) National Solar Observatory (USA); (8) Rutherford Appleton Lab. (U.K.); (9) Institut d'Astrophysique Spatial, Universite de Paris-Sud (France) ; (10) University of Bradford (U.K) {\\b Abstract}: The European Grid of Solar Observations is the European contribution to the deployment of a virtual solar observatory. The project is funded under the Information Society Technologies (IST) thematic programme of the European Commission's Fifth Framework. EGSO started in March 2002 and will last until March 2005. The project is categorized as a computer science effort. Evidently, a fair amount of issues it addresses are general to grid projects. Nevertheless, EGSO is also of benefit to the application domains, including solar physics, space weather, climate physics and astrophysics. With EGSO, researchers as well as the general public can access and combine solar data from distributed archives in an integrated virtual solar resource. Users express queries based on various search parameters. The search possibilities of EGSO extend the search possibilities of traditional data access systems. For instance, users can formulate a query to search for simultaneous observations of a specific solar event in a given number of wavelengths. In other words, users can search for observations on the basis of events and phenomena, rather than just time and location. The software architecture consists of three collaborating components: a consumer, a broker and a provider. The first component, the consumer, organizes the end user interaction and controls requests

  6. Simultaneous multi-frequency imaging observations of solar microwave bursts

    NASA Technical Reports Server (NTRS)

    Kundu, M. R.; White, S. M.; Schmahl, E. J.

    1989-01-01

    The results of simultaneous two-frequency imaging observations of solar microwave bursts with the Very Large Array are reviewed. Simultaneous 2 and 6 cm observations have been made of bursts which are optically thin at both frequencies, or optically thick at the lower frequency. In the latter case, the source structure may differ at the two frequencies, but the two sources usually seem to be related. However, this is not always true of simultaneous 6 and 20 cm observations. The results have implications for the analysis of nonimaging radio data of solar and stellar flares.

  7. Open Surface Solar Irradiance Observations - A Challenge

    NASA Astrophysics Data System (ADS)

    Menard, Lionel; Nüst, Daniel; Jirka, Simon; Maso, Joan; Ranchin, Thierry; Wald, Lucien

    2015-04-01

    The newly started project ConnectinGEO funded by the European Commission aims at improving the understanding on which environmental observations are currently available in Europe and subsequently providing an informational basis to close gaps in diverse observation networks. The project complements supporting actions and networking activities with practical challenges to test and improve the procedures and methods for identifying observation data gaps, and to ensure viability in real world scenarios. We present a challenge on future concepts for building a data sharing portal for the solar energy industry as well as the state of the art in the domain. Decision makers and project developers of solar power plants have identified the Surface Solar Irradiance (SSI) and its components as an important factor for their business development. SSI observations are crucial in the process of selecting suitable locations for building new plants. Since in-situ pyranometric stations form a sparse network, the search for locations starts with global satellite data and is followed by the deployment of in-situ sensors in selected areas for at least one year. To form a convincing picture, answers must be sought in the conjunction of these EO systems, and although companies collecting SSI observations are willing to share this information, the means to exchange in-situ measurements across companies and between stakeholders in the market are still missing. We present a solution for interoperable exchange of SSI data comprising in-situ time-series observations as well as sensor descriptions based on practical experiences from other domains. More concretely, we will apply concepts and implementations of the Sensor Web Enablement (SWE) framework of the Open Geospatial Consortium (OGC). The work is based on an existing spatial data infrastructure (SDI), which currently comprises metadata, maps and coverage data, but no in-situ observations yet. This catalogue is already registered in the

  8. Our Sun IV: The Standard Model and Helioseismology: Consequences of Uncertainties in Input Physics and in Observed Solar Parameters

    NASA Technical Reports Server (NTRS)

    Boothroyd, Arnold I.; Sackmann, I.-Juliana

    2001-01-01

    extreme Z/X values yielded envelope helium abundance outside this range. We found that other current uncertainties, namely, in the solar age and luminosity, in nuclear rates other than the pp reaction, in the low-temperature molecular opacities, and in the low-density equation of state, have no significant effect on the quantities that can be inferred from helioseismic observations. The predicted pre-main-sequence lithium depletion is uncertain by a factor of 2. The predicted neutrino capture rate is uncertain by approximately 30% for the Cl-27 experiment and by approximately 3% for Ga-71 experiments, while the B-8 neutrino flux is uncertain by approximately 30%.

  9. Periodicities observed on solar flux index (F10.7) during geomagnetic disturbances

    NASA Astrophysics Data System (ADS)

    Adhikari, B.; Narayan, C.; Chhatkuli, D. N.

    2017-12-01

    Solar activities change within the period of 11 years. Sometimes the greatest event occurs in the period of solar maxima and the lowest activity occurs in the period of solar minimum. During the time period of solar activity sunspots number will vary. A 10.7 cm solar flux measurement is a determination of the strength of solar radio emission. The solar flux index is more often used for the prediction and monitoring of the solar activity. This study mainly focused on the variation on solar flux index and amount of electromagnetic wave in the atmosphere. Both seasonal and yearly variation on solar F10.7 index. We also analyzed the dataset obatained from riometer.Both instruments show seasonal and yearly variations. We also observed the solar cycle dependence on solar flux index and found a strong dependence on solar activity. Results also show that solar intensities higher during the rising phase of solar cycle. We also observed periodicities on solar flux index using wavelet analysis. Through this analysis, it was found that the power intensities of solar flux index show a high spectral variability.

  10. Forbush Decrease Prediction Based on Remote Solar Observations

    NASA Astrophysics Data System (ADS)

    Dumbovic, Mateja; Vrsnak, Bojan; Calogovic, Jasa

    2016-04-01

    We study the relation between remote observations of coronal mass ejections (CMEs), their associated solar flares and short-term depressions in the galactic cosmic-ray flux (so called Forbush decreases). Statistical relations between Forbush decrease magnitude and several CME/flare parameters are examined. In general we find that Forbush decrease magnitude is larger for faster CMEs with larger apparent width, which is associated with stronger flares that originate close to the center of the solar disk and are (possibly) involved in a CME-CME interaction. The statistical relations are quantified and employed to forecast expected Forbush decrease magnitude range based on the selected remote solar observations of the CME and associated solar flare. Several verification measures are used to evaluate the forecast method. We find that the forecast is most reliable in predicting whether or not a CME will produce a Forbush decrease with a magnitude >3 %. The main advantage of the method is that it provides an early prediction, 1-4 days in advance. Based on the presented research, an online forecast tool was developed (Forbush Decrease Forecast Tool, FDFT) available at Hvar Observatory web page: http://oh.geof.unizg.hr/FDFT/fdft.php. We acknowledge the support of Croatian Science Foundation under the project 6212 "Solar and Stellar Variability" and of European social fond under the project "PoKRet".

  11. Multi-wavelength and High-resolution Observations of Solar Eruptive Activities

    NASA Astrophysics Data System (ADS)

    Shen, Y. D.

    2014-09-01

    In recent years, various solar eruptive activities have been observed in the solar atmosphere, such as solar flares, filament eruptions, jets, coronal mass ejections (CMEs), and magnetohydrodynamics (MHD) waves. Previous observations have indicated that solar magnetic field plays a dominant role in the processes of all kinds of solar activities. Since many large-scale solar eruptive activities can cause significant effects on the space environment of the Earth as well as the human life, studying and forecasting the solar activities are urgent tasks for us. In addition, the Sun is the nearest star to the Earth, so that people can directly observe and study it in detail. Hence, studying the Sun can also provide a reference to study other stars in the universe. This thesis focuses on the multi-wavelength and high-resolution observations of three types of solar eruptive activities: filament eruptions, coronal jets, and coronal MHD waves. By analyzing various observations taken by ground-based and space-borne instruments, we try to understand the inherent physical mechanisms, and construct models to interpret different kinds of solar eruptive activities. The triggering mechanism and the cause of a failed filament eruption are studied in Chapter 3, which indicates that the energy released in the flare is a key factor to the fate of the filament. Two successive filament eruptions are studied in Chapter 4, which indicates that the magnetic implosion could be the physical linkage between them, and the structures of coronal magnetic fields are important for producing sympathetic eruptions. A magnetic unwinding jet and a blowout jet are studied in Chapters 5 and 6, respectively. The former exhibits obvious radial expansion, which undergoes three distinct phases: the slow expansion phase, the fast expansion phase, and the steady phase. In addition, calculation indicates that the non-potential magnetic field in the jet can supply sufficient energy for producing the unwinding

  12. High-energy solar flare observations at the Y2K maximum

    NASA Astrophysics Data System (ADS)

    Emslie, A. Gordon

    2000-04-01

    Solar flares afford an opportunity to observe processes associated with the acceleration and propagation of high-energy particles at a level of detail not accessible in any other astrophysical source. I will review some key results from previous high-energy solar flare observations, including those from the Compton Gamma-Ray Observatory, and the problems that they pose for our understanding of energy release and particle acceleration processes in the astrophysical environment. I will then discuss a program of high-energy observations to be carried out during the upcoming 2000-2001 solar maximum that is aimed at addressing and resolving these issues. A key element in this observational program is the High Energy Solar Spectroscopic Imager (HESSI) spacecraft, which will provide imaging spectroscopic observations with spatial, temporal, and energy resolutions commensurate with the physical processes believed to be operating, and will in addition provide the first true gamma-ray spectroscopy of an astrophysical source. .

  13. Observed ozone response to variations in solar ultraviolet radiation

    NASA Technical Reports Server (NTRS)

    Gille, J. C.; Smythe, C. M.; Heath, D. F.

    1984-01-01

    During the winter of 1979, the solar ultraviolet irradiance varied with a period of 13.5 days and an amplitude of 1 percent. The zonal mean ozone values in the tropics varied with the solar irradiance, with an amplitude of 0.25 to 0.60 percent. This observation agrees with earlier calculations, although the response may be overestimated. These results imply changes in ozone at an altitude of 48 kilometers of up to 12 percent over an 11-year solar cycle. Interpretation of ozone changes in the upper stratosphere will require measurements of solar ultraviolet radiation at wavelengths near 200 nanometers.

  14. Distribution and solar wind control of compressional solar wind-magnetic anomaly interactions observed at the Moon by ARTEMIS

    NASA Astrophysics Data System (ADS)

    Halekas, J. S.; Poppe, A. R.; Lue, C.; Farrell, W. M.; McFadden, J. P.

    2017-06-01

    A statistical investigation of 5 years of observations from the two-probe Acceleration, Reconnection, Turbulence, and Electrodynamics of Moon's Interaction with the Sun (ARTEMIS) mission reveals that strong compressional interactions occur infrequently at high altitudes near the ecliptic but can form in a wide range of solar wind conditions and can occur up to two lunar radii downstream from the lunar limb. The compressional events, some of which may represent small-scale collisionless shocks ("limb shocks"), occur in both steady and variable interplanetary magnetic field (IMF) conditions, with those forming in steady IMF well organized by the location of lunar remanent crustal magnetization. The events observed by ARTEMIS have similarities to ion foreshock phenomena, and those observed in variable IMF conditions may result from either local lunar interactions or distant terrestrial foreshock interactions. Observed velocity deflections associated with compressional events are always outward from the lunar wake, regardless of location and solar wind conditions. However, events for which the observed velocity deflection is parallel to the upstream motional electric field form in distinctly different solar wind conditions and locations than events with antiparallel deflections. Consideration of the momentum transfer between incoming and reflected solar wind populations helps explain the observed characteristics of the different groups of events.Plain Language SummaryWe survey the environment around the Moon to determine when and where strong amplifications in the charged particle density and magnetic field strength occur. These structures may be some of the smallest shock waves in the <span class="hlt">solar</span> system, and learning about their formation informs us about the interaction of charged particles with small-scale magnetic fields throughout the <span class="hlt">solar</span> system and beyond. We find that these compressions occur in an extended region</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20150008280','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20150008280"><span>Approaching <span class="hlt">Solar</span> Maximum 24 with Stereo-Multipoint <span class="hlt">Observations</span> of <span class="hlt">Solar</span> Energetic Particle Events</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Dresing, N.; Cohen, C. M. S.; Gomez-Herrero, R.; Heber, B.; Klassen, A.; Leske, R. A.; Mason, G. M.; Mewaldt, R. A.; von Rosenvinge, T. T.</p> <p>2014-01-01</p> <p>Since the beginning of the <span class="hlt">Solar</span> Terrestrial Relations Observatory (STEREO) mission at the end of 2006, the two spacecraft have now separated by more than 130? degrees from the Earth. A 360-degree view of the Sun has been possible since February 2011, providing multipoint in situ and remote sensing <span class="hlt">observations</span> of unprecedented quality. Combining STEREO <span class="hlt">observations</span> with near-Earth measurements allows the study of <span class="hlt">solar</span> energetic particle (SEP) events over a wide longitudinal range with minimal radial gradient effects. This contribution provides an overview of recent results obtained by the STEREO/IMPACT team in combination with <span class="hlt">observations</span> by the ACE and SOHO spacecraft. We focus especially on multi-spacecraft investigations of SEP events. The large longitudinal spread of electron and 3He-rich events as well as unusual anisotropies will be presented and discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2004A%26A...427..717A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2004A%26A...427..717A"><span>Comparison of CCD astrolabe multi-site <span class="hlt">solar</span> diameter <span class="hlt">observations</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Andrei, A. H.; Boscardin, S. C.; Chollet, F.; Delmas, C.; Golbasi, O.; Jilinski, E. G.; Kiliç, H.; Laclare, F.; Morand, F.; Penna, J. L.; Reis Neto, E.</p> <p>2004-11-01</p> <p>Results are presented of measured variations of the photospheric <span class="hlt">solar</span> diameter, as concurrently <span class="hlt">observed</span> at three sites of the R2S3 (Réseau de Suivi au Sol du Rayon Solaire) consortium in 2001. Important <span class="hlt">solar</span> flux variations appeared in that year, just after the maximum of <span class="hlt">solar</span> activity cycle 23, make that time stretch particularly promising for a comparison of the multi-site results. The sites are those in Turkey, France and Brasil. All <span class="hlt">observations</span> are made with similar CCD <span class="hlt">solar</span> astrolabes, and at nearby effective wavelengths. The data reductions share algorithms, that are alike, the outcomes of which are here treated after applying a normalization correction using the Fried parameter. Since the sites are geographically quite far, atmospheric conditions are dismissed as possible causes of the large common trend found. Owing to particularities of each site, the common continuous <span class="hlt">observational</span> period extends from April to September. The standard deviation for the daily averages is close to 0.47 arcsec for the three sites. Accordingly, the three series are smoothed by a low-pass-band Fourier filter of 150 <span class="hlt">observations</span> (typically one month). The main common features found are a declining linear trend, of the order of 0.7 mas/day, and a relative maximum, around MJD 2120, of the order of 100 mas. Standard statistical tests endorse the correlation of the three series.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012decs.confE..86M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012decs.confE..86M"><span><span class="hlt">Observational</span> Evidence of Magnetic Waves in the <span class="hlt">Solar</span> Atmosphere</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>McIntosh, Scott W.</p> <p>2012-03-01</p> <p>The <span class="hlt">observational</span> evidence in supporting the presence of magnetic waves in the outer <span class="hlt">solar</span> atmosphere is growing rapidly - we will discuss recent <span class="hlt">observations</span> and place them in context with salient <span class="hlt">observations</span> made in the past. While the clear delineation of these magnetic wave "modes" is unclear, much can be learned about the environment in which they originated and possibly how they are removed from the system from the <span class="hlt">observations</span>. Their diagnostic power is, as yet, untapped and their energy content (both as a mechanical source for the heating of coronal material and acceleration of the <span class="hlt">solar</span> wind) remains in question, but can be probed <span class="hlt">observationally</span> - raising challenges for modeling efforts. We look forward to the IRIS mission by proposing some sample <span class="hlt">observing</span> sequences to help resolve some of the zoological issues present in the literature.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20170008030','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20170008030"><span><span class="hlt">Solar</span> Spectral Irradiance Variability in Cycle 24: Model Predictions and OMI <span class="hlt">Observations</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Marchenko, S.; DeLand, M.; Lean, J.</p> <p>2016-01-01</p> <p>Utilizing the excellent stability of the Ozone Monitoring Instrument (OMI), we characterize both short-term (<span class="hlt">solar</span> rotation) and long-term (<span class="hlt">solar</span> cycle) changes of the <span class="hlt">solar</span> spectral irradiance (SSI) between 265-500 nanometers during the ongoing Cycle 24. We supplement the OMI data with concurrent <span class="hlt">observations</span> from the GOME-2 (Global Ozone Monitoring Experiment - 2) and SORCE (<span class="hlt">Solar</span> Radiation and Climate Experiment) instruments and find fair-to-excellent agreement between the <span class="hlt">observations</span> and predictions of the NRLSSI2 (Naval Research Laboratory <span class="hlt">Solar</span> Spectral Irradiance - post SORCE) and SATIRE-S (the Naval Research Laboratory's Spectral And Total Irradiance REconstruction for the Satellite era) models.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMSH14B..03M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMSH14B..03M"><span>Do In Situ <span class="hlt">Observations</span> Contain Signatures of Intermittent Fast <span class="hlt">Solar</span> Wind Acceleration?</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Matteini, L.; Horbury, T. S.; Stansby, D.</p> <p>2017-12-01</p> <p>Disentangling local plasma properties and <span class="hlt">Solar</span> origin structures in in situ data is a crucial aspect for the understanding of <span class="hlt">solar</span> wind acceleration and evolution. This is particularly challenging at 1 AU and beyond, where structures of various origin have had time to interact and merge, smoothing out their main characteristics. <span class="hlt">Observations</span> of more pristine plasma closer to the Sun are therefore needed. In preparation of the forthcoming <span class="hlt">Solar</span> Orbiter and Parker <span class="hlt">Solar</span> Probe missions, Helios <span class="hlt">observations</span> as close as to 0.3 AU - although old, not yet fully exploited - can be used to test our expectations and make new predictions. Recent <span class="hlt">observations</span> (Matteini et al. 2014, 2015) have outlined the presence of intense (up to 1000km/s) and short-living velocity peaks that ubiquitously characterize the typical profile of the fast <span class="hlt">solar</span> wind at 0.3 AU, suggesting that these features could be remnants of processes occurring in the <span class="hlt">Solar</span> atmosphere and a signature of intermittent <span class="hlt">solar</span> wind acceleration from coronal holes. We discuss results about statistics of these events, characterizing their physical properties and trying to link them with typical <span class="hlt">Solar</span> temporal and spatial scales. Finally we also discuss how these velocity peaks will likely affect the future in situ exploration of the inner heliosphere by <span class="hlt">Solar</span> Orbiter and the Parker <span class="hlt">Solar</span> Probe.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19850025584','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19850025584"><span>Simultaneous <span class="hlt">Solar</span> Maximum Mission and Very Large Array (VLA) <span class="hlt">observations</span> of <span class="hlt">solar</span> active regions</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Lang, K. R.</p> <p>1985-01-01</p> <p>Simultaneous <span class="hlt">observations</span> of <span class="hlt">solar</span> active regions with the <span class="hlt">Solar</span> Maximum Mission (SMM) Satellite and the Very Large Array (VLA) have been obtained and analyzed. Combined results enhance the scientific return for beyond that expeted from using either SMM or VLA alone. A total of two weeks of simultaneous SMM/VLA data were obtained. The multiple wavelength VLA <span class="hlt">observations</span> were used to determine the temperature and magnetic structure at different heights within coronal loops. These data are compared with simultaneous SMM <span class="hlt">observations</span>. Several papers on the subject are in progress. They include VLA <span class="hlt">observations</span> of compact, transient sources in the transition region; simultaneous SMM/VLA <span class="hlt">observations</span> of the coronal loops in one active region and the evolution of another one; and sampling of the coronal plasma using thermal cyclotron lines (magnetic field - VLA) and soft X ray spectral lines (electron density and electron temperaure-SMM).</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_4");'>4</a></li> <li><a href="#" onclick='return showDiv("page_5");'>5</a></li> <li class="active"><span>6</span></li> <li><a href="#" onclick='return showDiv("page_7");'>7</a></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_6 --> <div id="page_7" 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_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> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="121"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19870003089','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19870003089"><span>Simultaneous <span class="hlt">Solar</span> Maximum Mission (SMM) and very large array <span class="hlt">observations</span> of <span class="hlt">solar</span> active regions</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Lang, K. R.</p> <p>1986-01-01</p> <p>The research deals mainly with Very Large Array and <span class="hlt">Solar</span> Maximum Mission <span class="hlt">observations</span> of the ubiquitous coronal loops that dominate the structure of the low corona. As illustrated, the <span class="hlt">observations</span> of thermal cyclotron lines at microwave wavelengths provide a powerful new method of accurately specifying the coronal magnetic field strength. Processes are delineated that trigger <span class="hlt">solar</span> eruptions from coronal loops, including preburst heating and the magnetic interaction of coronal loops. Evidence for coherent burst mechanisms is provided for both the Sun and nearby stars, while other <span class="hlt">observations</span> suggest the presence of currents that may amplify the coronal magnetic field to unexpectedly high levels. The existence is reported of a new class of compact, variable moving sources in regions of apparently weak photospheric field.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20020069138&hterms=firenze&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dfirenze','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20020069138&hterms=firenze&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dfirenze"><span><span class="hlt">Solar</span> Wind Characteristics from SOHO-Sun-Ulysses Quadrature <span class="hlt">Observations</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Poletto, Giannina; Suess, Steve T.; Six, N. Frank (Technical Monitor)</p> <p>2002-01-01</p> <p>Over the past few years, we have been running SOHO (<span class="hlt">Solar</span> and Heliospheric Observatory)-Sun-Ulysses quadrature campaigns, aimed at comparing the plasma properties at coronal altitudes with plasma properties at interplanetary distances. Coronal plasma has been <span class="hlt">observed</span> by SOHO experiments: mainly, we used LASCO (Large Angle and Spectrometric Coronagraph Experiment) data to understand the overall coronal configuration at the time of quadratures and analyzed SUMER (<span class="hlt">Solar</span> Ultraviolet Measurements of Emitted Radiation), CDS (Coronal Diagnostic Spectrometer) and UVCS (Ultraviolet Coronagraph Spectrometer) data to derive its physical characteristics. At interplanetary distances, SWICS (<span class="hlt">Solar</span> Wind Ion Composition Spectrometer) and SWOOPS (<span class="hlt">Solar</span> Wind <span class="hlt">Observation</span> over the Poles of the Sun) aboard Ulysses provided us with interplanetary plasma data. Here we report on results from some of the campaigns. We notice that, depending on the geometry of the quadrature, i.e. on whether the radial to Ulysses traverses the corona at high or low latitudes, we are able to study different kinds of <span class="hlt">solar</span> wind. In particular, a comparison between low-latitude and high-latitude wind, allowed us to provide evidence for differences in the acceleration of polar, fast plasma and equatorial, slow plasma: the latter occurring at higher levels and through a more extended region than fast wind. These properties are shared by both the proton and heavy ions outflows. Quadrature <span class="hlt">observations</span> may provide useful information also on coronal vs. in situ elemental composition. To this end, we analyzed spectra taken in the corona, at altitudes ranging between approx. 1.02 and 2.2 <span class="hlt">solar</span> radii, and derived the abundances of a number of ions, including oxygen and iron. Values of the O/Fe ratio, at coronal levels, have been compared with measurements of this ratio made by SWICS at interplanetary distances. Our results are compared with previous findings and predictions from modeling efforts.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015CEAB...39..109C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015CEAB...39..109C"><span><span class="hlt">Solar</span> and Galactic Cosmic Rays <span class="hlt">Observed</span> by SOHO</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Curdt, W.; Fleck, B.</p> <p></p> <p>Both the Cosmic Ray Flux (CRF) and <span class="hlt">Solar</span> Energetic Particles (SEPs) have left an imprint on SOHO technical systems. While the <span class="hlt">solar</span> array efficiency degraded irreversibly down to ≈77% of its original level over roughly 1 1/2 <span class="hlt">solar</span> cycles, Single Event Upsets (SEUs) in the solid state recorder (SSR) have been reversed by the memory protection mechanism. We compare the daily CRF <span class="hlt">observed</span> by the Oulu station with the daily SOHO SEU rate and with the degradation curve of the <span class="hlt">solar</span> arrays. The Oulu CRF and the SOHO SSR SEU rate are both modulated by the <span class="hlt">solar</span> cycle and are highly correlated, except for sharp spikes in the SEU rate, caused by isolated SEP events, which also show up as discontinuities in the otherwise slowly decreasing <span class="hlt">solar</span> ray efficiency. This allows to discriminate between effects with <span class="hlt">solar</span> and non-<span class="hlt">solar</span> origin and to compare the relative strength of both. We find that during <span class="hlt">solar</span> cycle 23 (1996 Apr 1 -- 2008 Aug 31) only 6% of the total number of SSR SEUs were caused by SEPs; the remaining 94% were due to galactic cosmic rays. During the maximum period of cycle 23 (2000 Jan 1 -- 2003 Dec 31), the SEP contribution increased to 22%, and during 2001, the year with the highest SEP rate, to 30%. About 40% of the total <span class="hlt">solar</span> array degradation during the 17 years from Jan 1996 through Feb 2013 can be attributed to proton events, i.e. the effect of a series of short-lived, violent SEP events is comparable to the cycle-integrated damage by cosmic rays.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012ASPC..463..439S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012ASPC..463..439S"><span>Instrument Design of the Large Aperture <span class="hlt">Solar</span> UV Visible and IR <span class="hlt">Observing</span> Telescope (SUVIT) for the <span class="hlt">SOLAR</span>-C Mission</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Suematsu, Y.; Katsukawa, Y.; Shimizu, T.; Ichimoto, K.; Takeyama, N.</p> <p>2012-12-01</p> <p>We present an instrumental design of one major <span class="hlt">solar</span> <span class="hlt">observation</span> payload planned for the <span class="hlt">SOLAR</span>-C mission: the <span class="hlt">Solar</span> Ultra-violet Visible and near IR <span class="hlt">observing</span> Telescope (SUVIT). The SUVIT is designed to provide high-angular-resolution investigation of the lower <span class="hlt">solar</span> atmosphere, from the photosphere to the uppermost chromosphere, with enhanced spectroscopic and spectro-polarimetric capability in wide wavelength regions from 280 nm (Mg II h&k lines) to 1100 nm (He I 1083 nm line) with 1.5 m class aperture and filtergraphic and spectrographic instruments.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2002AstHe..95..179T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2002AstHe..95..179T"><span><span class="hlt">Observation</span> of the total <span class="hlt">solar</span> eclipse on 21 June 2001 in Zambia</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Takahashi, Noritsugu; Yumoto, Kiyohumi; Ichimoto, Kiyoshi</p> <p>2002-04-01</p> <p>On 21 June 2001, path of totality in Angola, Zambia, Zimbabwe, Mozambique, and Madagascar in Africa. The Japan Scientific <span class="hlt">Observation</span> Team, consisting primarily of the members of the <span class="hlt">Solar</span> Eclipse Subcommittee of the Committee for International Collaboration in Astronomy of the Science Council of JAPAN, visited Lusaka in Zambia to <span class="hlt">observe</span> the total <span class="hlt">solar</span> eclipse. Blessed with fine weather, the <span class="hlt">observation</span> was successful. The outline of the influence of <span class="hlt">solar</span> eclipse on the terrestrial magnetism, polarization of the flash spectrum, and other <span class="hlt">observation</span> data, as well as the way educational activities were carried out, are reported.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017SoPh..292...49T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017SoPh..292...49T"><span>Imaging Spectropolarimeter for the Multi-Application <span class="hlt">Solar</span> Telescope at Udaipur <span class="hlt">Solar</span> Observatory: Characterization of Polarimeter and Preliminary <span class="hlt">Observations</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tiwary, Alok Ranjan; Mathew, Shibu K.; Bayanna, A. Raja; Venkatakrishnan, P.; Yadav, Rahul</p> <p>2017-04-01</p> <p>The Multi-Application <span class="hlt">Solar</span> Telescope (MAST) is a 50 cm off-axis Gregorian telescope that has recently become operational at the Udaipur <span class="hlt">Solar</span> Observatory (USO). An imaging spectropolarimeter is being developed as one of the back-end instruments of MAST to gain a better understanding of the evolution and dynamics of <span class="hlt">solar</span> magnetic and velocity fields. This system consists of a narrow-band filter and a polarimeter. The polarimeter includes a linear polarizer and two sets of liquid crystal variable retarders (LCVRs). The instrument is intended for simultaneous <span class="hlt">observations</span> in the spectral lines 6173 Å and 8542 Å, which are formed in the photosphere and chromosphere, respectively. In this article, we present results from the characterization of the LCVRs for the spectral lines of interest and the response matrix of the polarimeter. We also present preliminary <span class="hlt">observations</span> of an active region obtained using the spectropolarimeter. For verification purposes, we compare the Stokes <span class="hlt">observations</span> of the active region obtained from the Helioseismic Magnetic Imager (HMI) onboard the <span class="hlt">Solar</span> Dynamics Observatory (SDO) with that of MAST <span class="hlt">observations</span> in the spectral line 6173 Å. We find good agreement between the two <span class="hlt">observations</span>, considering the fact that MAST <span class="hlt">observations</span> are limited by seeing.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19890006492','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19890006492"><span>Millimeter wavelength <span class="hlt">observations</span> of <span class="hlt">solar</span> flares for Max 1991</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kundu, M. R.; Gopalswamy, N.; Nitta, N.; Schmahl, E. J.; White, S. M.; Welch, W. J.</p> <p>1988-01-01</p> <p>The Hat Creek millimeter-wave interferometer (to be known as the Berkeley-Illinois-Maryland Array, BIMA) is being upgraded. The improved array will become available during the coming <span class="hlt">solar</span> maximum, and will have guaranteed time for <span class="hlt">solar</span> <span class="hlt">observing</span>. The Hat Creek millimeter-wave interferometer is described along with the improvements. The scientific objectives are briefly discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMSH31B2730P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMSH31B2730P"><span><span class="hlt">Solar</span> Energetic Particle Composition over Two <span class="hlt">Solar</span> Cycles as <span class="hlt">Observed</span> by the Ulysses/HISCALE and ACE/EPAM Pulse Height Analyzers.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Patterson, J. D.; Madanian, H.; Manweiler, J. W.; Lanzerotti, L. J.</p> <p>2017-12-01</p> <p>We present the compositional variation in the <span class="hlt">Solar</span> Energetic Particle (SEP) population in the inner heliosphere over two <span class="hlt">solar</span> cycles using data from the Ulysses Heliospheric Instrument for Spectra, Composition, and Anisotropy at Low Energies (HISCALE) and Advanced Composition Explorer (ACE) Electron Proton Alpha Monitor (EPAM). The Ulysses mission was active from late 1990 to mid-2009 in a heliopolar orbit inclined by 80° with a perihelion of 1.3 AU and an aphelion of 5.4 AU. The ACE mission has been active since its launch in late 1997 and is in a halo orbit about L1. These two missions provide a total of 27 years of continuous <span class="hlt">observation</span> in the inner heliosphere with twelve years of simultaneous <span class="hlt">observation</span>. HISCALE and EPAM data provide species-resolved differential flux and density of SEP between 0.5-5 MeV/nuc. Several ion species (He, C, O, Ne, Si, Fe) are identified using the Pulse Height Analyzer (PHA) system of the Composition Aperture for both instruments. The He density shows a noticeable increase at high <span class="hlt">solar</span> activity followed by a moderate drop at the quiet time of the <span class="hlt">solar</span> minimum between cycles 23 and 24. The density of heavier ions (i.e. O and Fe) change minimally with respect to the F10.7 index variations however, certain energy-specific count rates decrease during <span class="hlt">solar</span> minimum. With Ulysses and ACE <span class="hlt">observing</span> in different regions of the inner heliosphere, there are significant latitudinal differences in how the O/He ratios vary with the <span class="hlt">solar</span> cycle. At <span class="hlt">solar</span> minimum, there is reasonable agreement between the <span class="hlt">observations</span> from both instruments. At <span class="hlt">solar</span> max 23, the differences in composition over the course of the <span class="hlt">solar</span> cycle, and as <span class="hlt">observed</span> at different heliospheric locations can provide insight to the origins of and acceleration processes differentially affecting <span class="hlt">solar</span> energetic ions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMSH13B2477B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMSH13B2477B"><span>Polarization <span class="hlt">Observations</span> of the Total <span class="hlt">Solar</span> Eclipse of August 21, 2017</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Burkepile, J.; Boll, A.; Casini, R.; de Toma, G.; Elmore, D. F.; Gibson, K. L.; Judge, P. G.; Mitchell, A. M.; Penn, M.; Sewell, S. D.; Tomczyk, S.; Yanamandra-Fisher, P. A.</p> <p>2017-12-01</p> <p>A total <span class="hlt">solar</span> eclipse offers ideal sky conditions for viewing the <span class="hlt">solar</span> corona. Light from the corona is composed of three components: the E-corona, made up of spectral emission lines produced by ionized elements in the corona; the K-corona, produced by photospheric light that is Thomson scattered by coronal electrons; and the F-corona, produced by sunlight scattered from dust particles in the near Sun environment and in interplanetary space. Polarized white light <span class="hlt">observations</span> of the corona provide a way of isolating the K-corona to determine its structure, brightness, and density. This work focuses on broadband white light polarization <span class="hlt">observations</span> of the corona during the upcoming <span class="hlt">solar</span> eclipse from three different instruments. We compare coronal polarization brightness <span class="hlt">observations</span> of the August 21, 2017 total <span class="hlt">solar</span> eclipse from the NCAR/High Altitude Observatory (HAO) Rosetta Stone experiment using the 4-D Technology PolarCam camera with the two Citizen PACA_CATE17Pol telescopes that will acquire linear polarization <span class="hlt">observations</span> of the eclipse and the NCAR/HAO K-Cor white light coronagraph <span class="hlt">observations</span> from the Mauna Loa <span class="hlt">Solar</span> Observatory in Hawaii. This comparison includes a discussion of the cross-calibration of the different instruments and reports the results of the coronal polarization brightness and electron density of the corona. These <span class="hlt">observations</span> will be compared with results from previous coronal measurements taken at different phases of the <span class="hlt">solar</span> cycle. In addition, we report on the performance of the three different polarimeters. The 4-D PolarCam uses a linear polarizer array, PACA_CATE17Pol uses a nematic liquid crystal retarder in a single beam configuration and K-Cor uses a pair of ferroelectric liquid crystal retarders in a dual-beam configuration. The use of the 4-D PolarCam camera in the Rosetta Stone experiment is to demonstrate the technology for acquiring high cadence polarization measurements. The Rosetta Stone experiment is funded through</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19860022990&hterms=SMM&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3DSMM','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19860022990&hterms=SMM&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3DSMM"><span><span class="hlt">Observations</span> of Halley's Comet by the <span class="hlt">Solar</span> Maximum Mission (SMM)</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Niedner, M. B.</p> <p>1986-01-01</p> <p><span class="hlt">Solar</span> Maximum Mission coronagraph/polarimeter <span class="hlt">observations</span> of large scale phenomena in Halley's Comet are discussed. <span class="hlt">Observations</span> of the hydrogen coma with the UV spectrometer are considered. It is concluded that coronograph/polarimeter <span class="hlt">observations</span> of the disconnection event, in which the entire plasma tail uproots itself from the head of the comet, is convected away in the <span class="hlt">solar</span> wind at speeds in the 50 to 100 km/sec range (relative to the head), and is replaced by a plasma tail constructed from folding ion-tail rays, are the most interesting.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011A%26A...530A..71B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011A%26A...530A..71B"><span><span class="hlt">Solar</span> irradiance variability: a six-year comparison between SORCE <span class="hlt">observations</span> and the SATIRE model</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ball, W. T.; Unruh, Y. C.; Krivova, N. A.; Solanki, S.; Harder, J. W.</p> <p>2011-06-01</p> <p>Aims: We investigate how well modeled <span class="hlt">solar</span> irradiances agree with measurements from the SORCE satellite, both for total <span class="hlt">solar</span> irradiance and broken down into spectral regions on timescales of several years. Methods: We use the SATIRE model and compare modeled total <span class="hlt">solar</span> irradiance (TSI) with TSI measurements over the period 25 February 2003 to 1 November 2009. Spectral <span class="hlt">solar</span> irradiance over 200-1630 nm is compared with the SIM instrument on SORCE over the period 21 April 2004 to 1 November 2009. We discuss the overall change in flux and the rotational and long-term trends during this period of decline from moderate activity to the recent <span class="hlt">solar</span> minimum in ~10 nm bands and for three spectral regions of significant interest: the UV integrated over 200-300 nm, the visible over 400-691 nm and the IR between 972-1630 nm. Results: The model <span class="hlt">captures</span> 97% of the <span class="hlt">observed</span> TSI variation. This is on the order at which TSI detectors agree with each other during the period considered. In the spectral comparison, rotational variability is well reproduced, especially between 400 and 1200 nm. The magnitude of change in the long-term trends is many times larger in SIM at almost all wavelengths while trends in SIM oppose SATIRE in the visible between 500 and 700 nm and again between 1000 and 1200 nm. We discuss the remaining issues with both SIM data and the identified limits of the model, particularly with the way facular contributions are dealt with, the limit of flux identification in MDI magnetograms during <span class="hlt">solar</span> minimum and the model atmospheres in the IR employed by SATIRE. However, it is unlikely that improvements in these areas will significantly enhance the agreement in the long-term trends. This disagreement implies that some mechanism other than surface magnetism is causing SSI variations, in particular between 2004 and 2006, if the SIM data are correct. Since SATIRE was able to reproduce UV irradiance between 1991 and 2002 from UARS, either the <span class="hlt">solar</span> mechanism for SSI</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUFMSH51D..02L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUFMSH51D..02L"><span><span class="hlt">Solar</span> Polar Imager: <span class="hlt">Observing</span> Coronal Transients from a New Perspective (Invited)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Liewer, P. C.</p> <p>2013-12-01</p> <p>The heliophysics community has long recognized the need for a mission to <span class="hlt">observe</span> the Sun and corona from a polar perspective. One mission concept, the <span class="hlt">Solar</span> Polar Imager (SPI), has been studied extensively (Liewer et al in NASA Space Science Vision Missions, 2008). In this concept, a <span class="hlt">solar</span> sail is used to place a spacecraft in a circular 0.48-AU heliocentric orbit with an inclination of ~75 degrees. This orbit enables crucial <span class="hlt">observations</span> not possible from lower latitude perspectives. Magnetograph and Doppler <span class="hlt">observations</span> from a polar vantage point would revolutionize our understanding of the mechanism of <span class="hlt">solar</span> activity cycles, polar magnetic field reversals, the internal structure and dynamics of the Sun and its atmosphere. The rapid 4-month polar orbit combined with both in situ and remote sensing instrumentation further enables unprecedented studies of the physical connection between the Sun, the <span class="hlt">solar</span> wind, and <span class="hlt">solar</span> energetic particles. From the polar perspective, white light imagers could be used to track CMEs and predict their arrival at Earth (as demonstrated by STEREO). SPI is also well suited to study the relative roles of CME-driven shock versus flare-associated processes in <span class="hlt">solar</span> energetic particle acceleration. With the circular 0.48 AU orbit, <span class="hlt">solar</span> energetic particles could be more easily traced to their sources and their variation with latitude can be studied at a constant radius. This talk will discuss the science objectives, instrumentation and mission design for the SPI mission.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012IAUSS...6E.401U','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012IAUSS...6E.401U"><span><span class="hlt">Observing</span> strategies for future <span class="hlt">solar</span> facilities: the ATST test case</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Uitenbroek, H.; Tritschler, A.</p> <p>2012-12-01</p> <p>Traditionally <span class="hlt">solar</span> <span class="hlt">observations</span> have been scheduled and performed very differently from night time efforts, in particular because we have been <span class="hlt">observing</span> the Sun for a long time, requiring new combinations of <span class="hlt">observables</span> to make progress, and because <span class="hlt">solar</span> physics <span class="hlt">observations</span> are often event driven on time scales of hours to days. With the proposal pressure that is expected for new large-aperture facilities, we can no longer afford the time spent on custom setups, and will have to rethink our scheduling and operations. We will discuss our efforts at Sac Peak in preparing for this new era, and outline the planned scheduling and operations planning for the ATST in particular.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2005AAS...206.5001C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2005AAS...206.5001C"><span>Stellar Abundance <span class="hlt">Observations</span> and Heavy Element Formation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Cowan, J. J.</p> <p>2005-05-01</p> <p>Abundance <span class="hlt">observations</span> indicate the presence of rapid-neutron <span class="hlt">capture</span> (i.e., r-process) elements in old Galactic halo and globular cluster stars. These <span class="hlt">observations</span> provide insight into the nature of the earliest generations of stars in the Galaxy -- the progenitors of the halo stars -- responsible for neutron-<span class="hlt">capture</span> synthesis of the heavy elements. Abundance comparisons among the r-process-rich halo stars show that the heaviest neutron-<span class="hlt">capture</span> elements (i.e., Ba and above) are consistent with a scaled <span class="hlt">solar</span> system r-process abundance distribution, while the lighter neutron-<span class="hlt">capture</span> elements do not conform to the <span class="hlt">solar</span> pattern. These comparisons suggest the possibility of two r-process sites in stars. The large star-to-star scatter <span class="hlt">observed</span> in the abundances of neutron-<span class="hlt">capture</span> element/iron ratios at low metallicities -- which disappears with increasing metallicity or [Fe/H] -- suggests the formation of these heavy elements (presumably from certain types of supernovae) was rare in the early Galaxy. The stellar abundances also indicate a change from the r-process to the slow neutron <span class="hlt">capture</span> (i.e., s-) process at higher metallicities in the Galaxy and provide insight into Galactic chemical evolution. Finally, the detection of thorium and uranium in halo and globular cluster stars offers an independent age-dating technique that can put lower limits on the age of the Galaxy, and hence the Universe. This work has been supported in part by NSF grant AST 03-07279 (J.J.C.) and by STScI grants GO-8111, GO-8342 and GO-9359.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1986ormo.conf..471S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1986ormo.conf..471S"><span>Origin of the moon by <span class="hlt">capture</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Singer, S. Fred</p> <p></p> <p>A coherent account is presented here based on the hypothesis that the moon formed separately in a heliocentric orbit similar to the earth's and was later <span class="hlt">captured</span> by the earth. The adoption of this hypothesis, together with the <span class="hlt">observed</span> depletion of iron in the moon, sets some important constraints on the condensation and agglomeration phenomena in the primeval <span class="hlt">solar</span> nebula that led to the formation of planetesimals, and ultimately to planets. <span class="hlt">Capture</span> of the moon also defines a severe heating event whereby the earth's kinetic energy of rotation is largely dissipated internally by the mechanism of tidal friction. From this melting event dates the geologic, atmospheric, and oceanic history of the earth. An attempt is made to account for the unique development of the earth, especially in relation to Mars and Venus, its neighboring planets. A <span class="hlt">capture</span> origin of the moon that employs a 'push-pull' tidal theory does not strain the laws of physics, involves a minimum of ad hoc assumptions, and has a probability that is commensurate with the evidence of the existence of a unique moon.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19890062593&hterms=Qbo&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3DQbo','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19890062593&hterms=Qbo&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3DQbo"><span><span class="hlt">Observations</span> and statistical simulations of a proposed <span class="hlt">solar</span> cycle/QBO/weather relationship</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Baldwin, Mark P.; Dunkerton, Timothy J.</p> <p>1989-01-01</p> <p>The 10.7-cm <span class="hlt">solar</span> flux is <span class="hlt">observed</span> to be highly correlated with North Pole stratospheric temperatures when partitioned according to the phase of the equatorial stratospheric winds (the quasi-biennial oscillation, or QBO). Calculations show that temperatures over most of the Northern Hemisphere are highly correlated or anticorrelated with North Pole temperatures. The <span class="hlt">observed</span> spatial pattern of <span class="hlt">solar</span>-cycle correlations at high latitudes is shown to be not unique to the <span class="hlt">solar</span> cycle.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20150002558','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20150002558"><span>Cross-Scale <span class="hlt">Observational</span> Signatures of Magnetic Reconnection</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Savage, Sabrina; Malaspina, David</p> <p>2014-01-01</p> <p>Magnetic reconnection is a significant mechanism for energy release across many astrophysical applications. In the <span class="hlt">solar</span> atmosphere, reconnection is considered a primary contributor of flare evolution and coronal heating. Directly <span class="hlt">observing</span> reconnection occurring in the <span class="hlt">solar</span> atmosphere, however, is not trivial considering that the scale size of the diffusion region is magnitudes smaller than the <span class="hlt">observational</span> capabilities of current instrumentation, and coronal magnetic field measurements are not currently sufficient to <span class="hlt">capture</span> the process. Meanwhile, reconnection occurring in the Earth's magnetosphere transfers energy from the <span class="hlt">solar</span> wind through a comparable process, although on vastly different scales. Magnetospheric measurements are made in situ rather than remotely; ergo, comparison of <span class="hlt">observations</span> between the two regimes allows for potentially significant insight into reconnection as a stochastic and possibly turbulent process. We will present a set of <span class="hlt">observations</span> from long-duration <span class="hlt">solar</span> events and compare them to in situ measurements from the magnetosphere.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFMSH22A..08S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFMSH22A..08S"><span>Cross-scale <span class="hlt">Observational</span> Signatures of Magnetic Reconnection</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Savage, S. L.; Malaspina, D.</p> <p>2014-12-01</p> <p>Magnetic reconnection is a significant mechanism for energy release across many astrophysical applications. In the <span class="hlt">solar</span> atmosphere, reconnection is considered a primary contributor of flare evolution and coronal heating. Directly <span class="hlt">observing</span> reconnection occurring in the <span class="hlt">solar</span> atmosphere, however, is not trivial considering that the scale size of the diffusion region is magnitudes smaller than the <span class="hlt">observational</span> capabilities of current instrumentation, and coronal magnetic field measurements are not currently sufficient to <span class="hlt">capture</span> the process. Meanwhile, reconnection occurring in the Earth's magnetosphere transfers energy from the <span class="hlt">solar</span> wind through a comparable process, although on vastly different scales. Magnetospheric measurements are made in situ rather than remotely; ergo, comparison of <span class="hlt">observations</span> between the two regimes allows for potentially significant insight into reconnection as a stochastic and possibly turbulent process. We will present a set of <span class="hlt">observations</span> from long-duration <span class="hlt">solar</span> events and compare them to in situ measurements from the magnetosphere.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2001RaSc...36..773C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2001RaSc...36..773C"><span>Total <span class="hlt">solar</span> eclipse effects on VLF signals: <span class="hlt">Observations</span> and modeling</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Clilverd, Mark A.; Rodger, Craig J.; Thomson, Neil R.; Lichtenberger, János; Steinbach, Péter; Cannon, Paul; Angling, Matthew J.</p> <p></p> <p>During the total <span class="hlt">solar</span> eclipse <span class="hlt">observed</span> in Europe on August 11, 1999, measurements were made of the amplitude and phase of four VLF transmitters in the frequency range 16-24 kHz. Five receiver sites were set up, and significant variations in phase and amplitude are reported for 17 paths, more than any previously during an eclipse. Distances from transmitter to receiver ranged from 90 to 14,510 km, although the majority were <2000 km. Typically, positive amplitude changes were <span class="hlt">observed</span> throughout the whole eclipse period on path lengths <2000 km, while negative amplitude changes were <span class="hlt">observed</span> on paths >10,000 km. Negative phase changes were <span class="hlt">observed</span> on most paths, independent of path length. Although there was significant variation from path to path, the typical changes <span class="hlt">observed</span> were ~3 dB and ~50°. The changes <span class="hlt">observed</span> were modeled using the Long Wave Propagation Capability waveguide code. Maximum eclipse effects occurred when the Wait inverse scale height parameter β was 0.5 km-1 and the effective ionospheric height parameter H' was 79 km, compared with β=0.43km-1 and H'=71km for normal daytime conditions. The resulting changes in modeled amplitude and phase show good agreement with the majority of the <span class="hlt">observations</span>. The modeling undertaken provides an interpretation of why previous estimates of height change during eclipses have shown such a range of values. A D region gas-chemistry model was compared with electron concentration estimates inferred from the <span class="hlt">observations</span> made during the <span class="hlt">solar</span> eclipse. Quiet-day H' and β parameters were used to define the initial ionospheric profile. The gas-chemistry model was then driven only by eclipse-related <span class="hlt">solar</span> radiation levels. The calculated electron concentration values at 77 km altitude throughout the period of the <span class="hlt">solar</span> eclipse show good agreement with the values determined from <span class="hlt">observations</span> at all times, which suggests that a linear variation in electron production rate with <span class="hlt">solar</span> ionizing radiation is reasonable</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018AAS...23124202J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018AAS...23124202J"><span><span class="hlt">Observations</span> of Fe XIV Line Intensity Variations in the <span class="hlt">Solar</span> Corona During the 21 August 2017 <span class="hlt">Solar</span> Eclipse</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Johnson, Payton; Ladd, Edwin</p> <p>2018-01-01</p> <p>We present time- and spatially-resolved <span class="hlt">observations</span> of the inner <span class="hlt">solar</span> corona in the 5303 Å line of Fe XIV, taken during the 21 August 2017 <span class="hlt">solar</span> eclipse from a field <span class="hlt">observing</span> site in Crossville, TN. These <span class="hlt">observations</span> are used to characterize the intensity variations in this coronal emission line, and to compare with oscillation predictions from models for heating the corona by magnetic wave dissipation.The <span class="hlt">observations</span> were taken with two Explore Scientific ED 102CF 102 mm aperture triplet apochromatic refractors. One system used a DayStar custom-built 5 Å FWHM filter centered on the Fe XIV coronal spectral line and an Atik Titan camera for image collection. The setup produced images with a pixel size of 2.15 arcseconds (~1.5 Mm at the distance to the Sun), and a field of view of 1420 x 1060 arcseconds, covering approximately 20% of the entire <span class="hlt">solar</span> limb centered near the emerging sunspot complex AR 2672. We obtained images with an exposure time of 0.22 seconds and a frame rate of 2.36 Hz, for a total of 361 images during totality.An identical, co-aligned telescope/camera system <span class="hlt">observed</span> the same portion of the <span class="hlt">solar</span> corona, but with a 100 Å FWHM Baader Planetarium <span class="hlt">solar</span> continuum filter centered on a wavelength of 5400 Å. Images with an exposure time of 0.01 seconds were obtained with a frame rate of 4.05 Hz. These simultaneous <span class="hlt">observations</span> are used as a control to monitor brightness variations not related to coronal line oscillations.</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/2006SunGe...1a..68S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006SunGe...1a..68S"><span>Derivation of Heliophysical Scientific Data from Amateur <span class="hlt">Observations</span> of <span class="hlt">Solar</span> Eclipses</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Stoev, A. D.; Stoeva, P. V.</p> <p>2006-03-01</p> <p>The basic scientific aims and <span class="hlt">observational</span> experiments included in the complex <span class="hlt">observational</span> program - Total <span class="hlt">Solar</span> Eclipse '99 - are described in the work. Results from teaching and training students of total <span class="hlt">solar</span> eclipse (TSE) <span class="hlt">observation</span> in the Public Astronomical Observatory (PAO) in Stara Zagora and their selection for participation in different <span class="hlt">observational</span> teams are also discussed. During the final stage, a special system of methods for investigation of the level of pretensions (the level of ambition as to what he/she feels capable of achieving in the context of problem solving/<span class="hlt">observation</span>) of the students is applied. Results obtained from the <span class="hlt">observational</span> experiments are interpreted mainly in the following themes: Investigation of the structure of the white-light <span class="hlt">solar</span> corona and evolution of separate coronal elements during the total phase of the eclipse; Photometry of the white-light <span class="hlt">solar</span> corona and specific emission lines; Meteorological, actinometrical and optical atmospheric investigations; Astrometry of the Moon during the phase evolution of the eclipse; Biological and behavioral reactions of highly organized colonies (ants and bats) during the eclipse. It is also shown that data processing, <span class="hlt">observational</span> results and their interpretation, presentation and publishing in specialized and amateur editions is a peak in the independent creative activity of students and amateur astronomers. This enables students from the Astronomy schools at Public Astronomical Observatories and Planetariums (PAOP) to develop creative skills, emotional - volitional personal qualities, orientation towards scientific work, <span class="hlt">observations</span> and experiments, and build an effective scientific style of thinking.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19900063357&hterms=background+wind&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dbackground%2Bwind','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19900063357&hterms=background+wind&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dbackground%2Bwind"><span><span class="hlt">Solar</span> minimum Lyman alpha sky background <span class="hlt">observations</span> from Pioneer Venus orbiter ultraviolet spectrometer - <span class="hlt">Solar</span> wind latitude variation</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Ajello, J. M.</p> <p>1990-01-01</p> <p>Measurements of interplanetary H I Lyman alpha over a large portion of the celestial sphere were made at the recent <span class="hlt">solar</span> minimum by the Pioneer Venus orbiter ultraviolet spectrometer. These measurements were performed during a series of spacecraft maneuvers conducted to <span class="hlt">observe</span> Halley's comet in early 1986. Analysis of these data using a model of the passage of interstellar wind hydrogen through the <span class="hlt">solar</span> system shows that the rate of charge exchange with <span class="hlt">solar</span> wind protons is 30 percent less over the <span class="hlt">solar</span> poles than in the ecliptic. This result is in agreement with a similar experiment performed with Mariner 10 at the previous <span class="hlt">solar</span> minimum.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUFMSH42A..06D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUFMSH42A..06D"><span><span class="hlt">Observational</span> evidence for Alfven waves in the <span class="hlt">solar</span> atmosphere (Invited)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>De Pontieu, B.</p> <p>2013-12-01</p> <p>Alfven waves have long been suspected of playing an important role in both heating the corona and accelerating the <span class="hlt">solar</span> wind. Recently, more and more <span class="hlt">observational</span> evidence for the presence of such waves has been reported in both the corona and the lower <span class="hlt">solar</span> atmosphere. I will review <span class="hlt">observations</span> of the properties and presence of Alfven waves from CoMP, Hinode, AIA and ground-based telescopes in both coronal lines and the lower <span class="hlt">solar</span> atmosphere. I will discuss our current understanding of the importance of these waves for the energy balance of the corona. I will also present initial results of the Interface Region Imaging Spectrograph (IRIS) which was launched in June 2013 and obtains images and spectra in both the far and near ultraviolet.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018ApJ...852...79Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018ApJ...852...79Y"><span>Two <span class="hlt">Solar</span> Tornadoes <span class="hlt">Observed</span> with the Interface Region Imaging Spectrograph</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yang, Zihao; Tian, Hui; Peter, Hardi; Su, Yang; Samanta, Tanmoy; Zhang, Jingwen; Chen, Yajie</p> <p>2018-01-01</p> <p>The barbs or legs of some prominences show an apparent motion of rotation, which are often termed <span class="hlt">solar</span> tornadoes. It is under debate whether the apparent motion is a real rotating motion, or caused by oscillations or counter-streaming flows. We present analysis results from spectroscopic <span class="hlt">observations</span> of two tornadoes by the Interface Region Imaging Spectrograph. Each tornado was <span class="hlt">observed</span> for more than 2.5 hr. Doppler velocities are derived through a single Gaussian fit to the Mg II k 2796 Å and Si IV 1393 Å line profiles. We find coherent and stable redshifts and blueshifts adjacent to each other across the tornado axes, which appears to favor the interpretation of these tornadoes as rotating cool plasmas with temperatures of 104 K–105 K. This interpretation is further supported by simultaneous <span class="hlt">observations</span> of the Atmospheric Imaging Assembly on board the <span class="hlt">Solar</span> Dynamics Observatory, which reveal periodic motions of dark structures in the tornadoes. Our results demonstrate that spectroscopic <span class="hlt">observations</span> can provide key information to disentangle different physical processes in <span class="hlt">solar</span> prominences.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23383910','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23383910"><span>Ion kinetic scale in the <span class="hlt">solar</span> wind <span class="hlt">observed</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Śafránková, Jana; Němeček, Zdeněk; Přech, Lubomír; Zastenker, Georgy N</p> <p>2013-01-11</p> <p>This Letter shows the first results from the <span class="hlt">solar</span> wind monitor onboard the Spektr-R spacecraft which measures plasma moments with a time resolution of 31 ms. This high-time resolution allows us to make direct <span class="hlt">observations</span> of <span class="hlt">solar</span> wind turbulence below ion kinetic length scales. We present examples of the frequency spectra of the density, velocity, and thermal velocity. Our study reveals that although these parameters exhibit the same behavior at the magnetohydrodynamic scale, their spectra are remarkably different at the kinetic scale.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19740018557','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19740018557"><span><span class="hlt">Solar</span> radio <span class="hlt">observations</span> in support of Skylab A</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Gotwols, B. L.</p> <p>1974-01-01</p> <p>The <span class="hlt">solar</span> radio spectra were recorded in real time, both on film and magnetic tape, during the period from November 1972 to February 1974. A catalogue of the <span class="hlt">observations</span> is given for the frequency range 565-1000 MHz and includes descriptions of the bursts, intensity scales, and pertinent remarks. Some theoretical considerations resulting from the research are given. Equipment modified for the experiment is described and the text of the final report which summarizes the research on type IV <span class="hlt">solar</span> radio bursts is included.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016JPhCS.771a2038M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016JPhCS.771a2038M"><span>Stellar background <span class="hlt">observation</span> during Total <span class="hlt">Solar</span> Eclipse March 9th 2016</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mumtahana, Farahhati; Timur Jaelani, Anton; Muhamad, Johan; Sutastio, Heri</p> <p>2016-11-01</p> <p>We report <span class="hlt">observation</span> and an early analysis of stellar background from total <span class="hlt">solar</span> eclipse in Ternate, Indonesia. The eclipse phenomena which occurred on March, 9th 2016 was <span class="hlt">observed</span> with certain portable instruments in order to obtain the stars behind the Sun in particular field of view and resolution. From our <span class="hlt">observation</span> site in Ternate city, <span class="hlt">solar</span> eclipse occurred in the late morning when the weather was unfortunately cloudy. However, during the darkness of totality, we obtained several point source objects between the gaps of the moving clouds and we suspected them as very faint stars due to their appearance in several frames. Those so called stars have been identified and measured with respect to their positions toward the center of the Sun. The main purpose of this research is to revisit strong lensing calculation of the Sun during total <span class="hlt">solar</span> eclipse by measuring the deflection angle of the background stars as it had been calculated by Einstein and proved by Eddington at a total <span class="hlt">solar</span> eclipse in 1919. To accomplish this aim, we need to conduct another <span class="hlt">observation</span> to measure position of the same stars in the next period when those stars appear in the night sky.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016DPS....4811705P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016DPS....4811705P"><span>The 2016 Transit of Mercury <span class="hlt">Observed</span> from Major <span class="hlt">Solar</span> Telescopes and Satellites</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pasachoff, Jay M.; Schneider, Glenn; Gary, Dale; Chen, Bin; Sterling, Alphonse C.; Reardon, Kevin P.; Dantowitz, Ronald; Kopp, Greg A.</p> <p>2016-10-01</p> <p>We report <span class="hlt">observations</span> from the ground and space of the 9 May 2016 transit of Mercury. We build on our explanation of the black-drop effect in transits of Venus based on spacecraft <span class="hlt">observations</span> of the 1999 transit of Mercury (Schneider, Pasachoff, and Golub, Icarus 168, 249, 2004). In 2016, we used the 1.6-m New <span class="hlt">Solar</span> Telescope at the Big Bear <span class="hlt">Solar</span> Observatory with active optics to <span class="hlt">observe</span> Mercury's transit at high spatial resolution. We again saw a small black-drop effect as 3rd contact neared, confirming the data that led to our earlier explanation as a confluence of the point-spread function and the extreme <span class="hlt">solar</span> limb darkening (Pasachoff, Schneider, and Golub, in IAU Colloq. 196, 2004). We again used IBIS on the Dunn <span class="hlt">Solar</span> Telescope of the Sacramento Peak Observatory, as A. Potter continued his <span class="hlt">observations</span>, previously made at the 2006 transit of Mercury, at both telescopes of the sodium exosphere of Mercury (Potter, Killen, Reardon, and Bida, Icarus 226, 172, 2013). We imaged the transit with IBIS as well as with two RED Epic IMAX-quality cameras alongside it, one with a narrow passband. We show animations of our high-resolution ground-based <span class="hlt">observations</span> along with <span class="hlt">observations</span> from XRT on JAXA's Hinode and from NASA's <span class="hlt">Solar</span> Dynamics Observatory. Further, we report on the limit of the transit change in the Total <span class="hlt">Solar</span> Irradiance, continuing our interest from the transit of Venus TSI (Schneider, Pasachoff, and Willson, ApJ 641, 565, 2006; Pasachoff, Schneider, and Willson, AAS 2005), using NASA's SORCE/TIM and the Air Force's TCTE/TIM. See http://transitofvenus.info and http://nicmosis.as.arizona.edu.Acknowledgments: We were glad for the collaboration at Big Bear of Claude Plymate and his colleagues of the staff of the Big Bear <span class="hlt">Solar</span> Observatory. We also appreciate the collaboration on the transit studies of Robert Lucas (Sydney, Australia) and Evan Zucker (San Diego, California). JMP appreciates the sabbatical hospitality of the Division of Geosciences and</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011SPD....42.1501S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011SPD....42.1501S"><span><span class="hlt">Solar</span> Hard X-ray <span class="hlt">Observations</span> with NuSTAR</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Smith, David M.; Krucker, S.; Hudson, H. S.; Hurford, G. J.; White, S. M.; Mewaldt, R. A.; Stern, D.; Grefenstette, B. W.; Harrison, F. A.</p> <p>2011-05-01</p> <p>High-sensitivity imaging of coronal hard X-rays allows detection of freshly accelerated nonthermal electrons at the acceleration site. A few such <span class="hlt">observations</span> have been made with Yohkoh and RHESSI, but a leap in sensitivity could help pin down the time, place, and manner of reconnection. In 2012, the Nuclear Spectroscopic Telescope Array (NuSTAR), a NASA Small Explorer for high energy astrophysics that uses grazing-incidence optics to focus X-rays up to 80 keV, will be launched. NuSTAR is capable of <span class="hlt">solar</span> pointing, and three weeks will be dedicated to <span class="hlt">solar</span> <span class="hlt">observing</span> during the baseline two-year mission. NuSTAR will be 200 times more sensitive than RHESSI in the hard X-ray band. This will allow the following new <span class="hlt">observations</span>, among others: 1) Extrapolation of the micro/nanoflare distribution by two orders of magnitude down in flux 2) Search for hard X-rays from network nanoflares (soft X-ray bright points) and evaluation of their role in coronal heating 3) Discovery of hard X-ray bremsstrahlung from the electron beams driving type III radio bursts, and measurement of their electron spectrum 4) Hard X-ray studies of polar soft X-ray jets and impulsive <span class="hlt">solar</span> energetic particle events at the edge of coronal holes, and comparison of these events with <span class="hlt">observations</span> of 3He and other particles in interplanetary space 5) Study of coronal bremsstrahlung from particles accelerated by coronal mass ejections as they are first launched 6) Study of particles at the coronal reconnection site when flare footpoints are occulted; and 7) Search for hypothetical axion particles created in the <span class="hlt">solar</span> core via the hard X-ray signal from their conversion to X-rays in the coronal magnetic field. NuSTAR will also serve as a pathfinder for a future dedicated space mission with enhanced capabilities, such as a satellite version of the FOXSI sounding rocket.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EGUGA..1813412E','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EGUGA..1813412E"><span><span class="hlt">Solar</span> system plasma Turbulence: <span class="hlt">Observations</span>, inteRmittency and Multifractals</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Echim, Marius M.</p> <p>2016-04-01</p> <p>The FP7 project STORM is funded by the European Commission to "add value to existing data bases through a more comprehensive interpretation". STORM targets plasma and magnetic field databases collected in the <span class="hlt">solar</span> wind (Ulysses and also some planetary missions), planetary magnetospheres (Venus Express, Cluster, a few orbits from Cassini), cometary magnetosheaths (e.g. Haley from Giotto <span class="hlt">observations</span>). The project applies the same package of analysis methods on geomagnetic field <span class="hlt">observations</span> from ground and on derived indices (e.g. AE, AL, AU, SYM-H). The analysis strategy adopted in STORM is built on the principle of increasing complexity, from lower (like, e.g., the Power Spectral Density - PSD) to higher order analyses (the Probability Distribution Functions - PDFs, Structure Functions - SFs, Fractals and Multifractals - MFs). Therefore STORM targets not only the spectral behavior of turbulent fluctuations but also their topology and scale behavior inferred from advanced mathematical algorithms and geometrical-like analogs. STORM started in January 2013 and ended in December 2015. We will report on a selection of scientific and technical achievements and will highlight: (1) the radial evolution of <span class="hlt">solar</span> wind turbulence and intermittency based on Ulysses data with some contributions from Venus Express and Cluster; (2) comparative study of fast and slow wind turbulence and intermittency at <span class="hlt">solar</span> minimum; (3) comparative study of the planetary response (Venus and Earth magnetosheaths) to turbulent <span class="hlt">solar</span> wind; (4) the critical behavior of geomagnetic fluctuations and indices; (5) an integrated library for non-linear analysis of time series that includes all the approaches adopted in STORM to investigate <span class="hlt">solar</span> system plasma turbulence. STORM delivers an unprecedented volume of analysed data for turbulence. The project made indeed a systematic survey, orbit by orbit, of data available from ESA repositories and Principal Investigators and provides results ordered as a</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012hell.conf....5M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012hell.conf....5M"><span><span class="hlt">Solar</span> <span class="hlt">observations</span> with a low frequency radio telescope</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Myserlis, I.; Seiradakis, J.; Dogramatzidis, M.</p> <p>2012-01-01</p> <p>We have set up a low frequency radio monitoring station for <span class="hlt">solar</span> bursts at the Observatory of the Aristotle University in Thessaloniki. The station consists of a dual dipole phased array, a radio receiver and a dedicated computer with the necessary software installed. The constructed radio receiver is based on NASA's Radio Jove project. It operates continuously, since July 2010, at 20.1 MHz (close to the long-wavelength ionospheric cut-off of the radio window) with a narrow bandwidth (~5 kHz). The system is properly calibrated, so that the recorded data are expressed in antenna temperature. Despite the high interference level of an urban region like Thessaloniki (strong broadcasting shortwave radio stations, periodic experimental signals, CBs, etc), we have detected several low frequency <span class="hlt">solar</span> radio bursts and correlated them with <span class="hlt">solar</span> flares, X-ray events and other low frequency <span class="hlt">solar</span> <span class="hlt">observations</span>. The received signal is monitored in ordinary ASCII format and as audio signal, in order to investigate and exclude man-made radio interference. In order to exclude narrow band interference and calculate the spectral indices of the <span class="hlt">observed</span> events, a second monitoring station, working at 36 MHz, is under construction at the village of Nikiforos near the town of Drama, about 130 km away of Thessaloniki. Finally, we plan to construct a third monitoring station at 58 MHz, in Thessaloniki. This frequency was revealed to be relatively free of interference, after a thorough investigation of the region.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013CoSka..43...81M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013CoSka..43...81M"><span><span class="hlt">Solar</span> radio <span class="hlt">observations</span> and radio interference monitoring in Roztoky</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Monstein, C.; Baluďanský, D.</p> <p>2013-10-01</p> <p>This paper is part of a planned measurement campaign in which spectrum measurements were carried out at different locations worldwide within potential locations of the e-Callisto network. The results of measurements at the Callisto <span class="hlt">observing</span> station in Roztoky, which took place at the beginning of May 2013, are presented. Measurements were made out with a special low cost broadband logarithmic periodic antenna connected to a Callisto spectrometer designed and built at ETH Zurich (Benz, 2004). This study provides the technical basis to decide whether it is possible to make <span class="hlt">solar</span> spectroscopic measurements below 1 GHz (λ>30 cm) at the <span class="hlt">observing</span> station. In terms of electromagnetic interference, Roztoky is not perfect for broadband spectroscopic <span class="hlt">solar</span> radio astronomy <span class="hlt">observations</span> due to non negligible radio interference level from the nearby FM-transmitters. Nevertheless, low frequency <span class="hlt">observations</span> below 80 MHz, as well as <span class="hlt">observations</span> in some small bands above 116 MHz can be done.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19730008067','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19730008067"><span>Space <span class="hlt">observations</span> of the variability of <span class="hlt">solar</span> irradiance in the near and far ultraviolet</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Heath, D. F.</p> <p>1972-01-01</p> <p>Satellite <span class="hlt">observations</span> of the ultraviolet <span class="hlt">solar</span> irradiance in selected wavelength bands between 1200 and 3000 a were made continuously by photometers consisting of broad-band sensors operated on Numbus 3 and 4 which were launched in April 1969 and 1970. In addition, spectrophotometer measurements of the <span class="hlt">solar</span> irradiance were made with a dispersive instrument at 12 selected wavelengths from 2550 to 3400 a with a 10 a bandpass on Nimbus 4. Variations of the <span class="hlt">solar</span> irradiance associated with the <span class="hlt">solar</span> rotational period were <span class="hlt">observed</span> since the launch of Nimbus 3. These variations are apparently associated with two source regions separated by about 180 deg in <span class="hlt">solar</span> longitude. The change in irradiance with <span class="hlt">solar</span> rotation was found to increase with decreasing wavelengths. Different types of the <span class="hlt">observed</span> variations in uv <span class="hlt">solar</span> irradiance can be classified in accordance with characteristics times, e.g. in the order of increasing periods as follows: (1)flare associated enhancements (2) 27-day variations due to <span class="hlt">solar</span> rotation; (3) a possible biennial effect; and (4) long term variations associated with the 11-year <span class="hlt">solar</span> cycle.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19920038086&hterms=text+historical&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Dtext%2Bhistorical','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19920038086&hterms=text+historical&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Dtext%2Bhistorical"><span>Sir William Herschel's notebooks - Abstracts of <span class="hlt">solar</span> <span class="hlt">observations</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Hoyt, Douglas V.; Schatten, Kenneth H.</p> <p>1992-01-01</p> <p>An introduction to the background of Sir William Herschel's notebooks and the historical context within which his <span class="hlt">observations</span> were made are provided. The <span class="hlt">observations</span> have relevance in reconstructing <span class="hlt">solar</span> behavior, as discussed in a separate analysis paper by Hoyt and Schatten (1992), and in understanding active features on the sun such as faculae. The text of Herschel's notebooks with modern terms used throughout forms the body of this paper. The complete text has not previously been published and is not easily accessible to scholars. Herschel used different words for <span class="hlt">solar</span> features than are used today, and thus, for clarity, his terminology is changed on two occasions. A glossary explains the terminology changed. In the text of the notebooks, several contemporaries are mentioned; a brief description of Herschel's colleagues is provided.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20000000500&hterms=solar+intensity+measurement&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Dsolar%2Bintensity%2Bmeasurement','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20000000500&hterms=solar+intensity+measurement&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Dsolar%2Bintensity%2Bmeasurement"><span>The Hadean, Through a Glass Telescopically: <span class="hlt">Observations</span> of Young <span class="hlt">Solar</span> Analogs</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Gaidos, E. J.</p> <p>1998-01-01</p> <p>Investigations into the Earth's surface environment during the Hadean eon (prior to 3.8 Ga) are hampered by the paucity of the geological and geochemical record and the relative inaccessibility of better-preserved surfaces with possibly similar early histories (i.e., Mars). One approach is to <span class="hlt">observe</span> nearby, young <span class="hlt">solar</span>-mass stars as analogs to the Hadean Sun and its environment. A catalog of 38 G and early K stars within 25 pc was constructed based on main-sequence status, bolometric luminosity, lack of known stellar companions within 800 AU, and coronal X-ray luminosities commensurate with the higher activity of <span class="hlt">solar</span>-mass stars <0.8 b.y. old. Spectroscopic data support the assignment of ages of 0.2 - 0.8 Ga for most of these stars. <span class="hlt">Observations</span> of these objects will provide insight into external forces that influenced Hadean atmosphere, ocean, and surface evolution (and potential ecosystems), including <span class="hlt">solar</span> luminosity evolution, the flux and spectrum of <span class="hlt">solar</span> ultraviolet radiation, the intensity of the <span class="hlt">solar</span> wind, and the intensity and duration of a late period of heavy bombardment. The standard model of <span class="hlt">solar</span> evolution predicts a luminosity of 0.75 <span class="hlt">solar</span> luminosity at the end of the Hadean, implying a terrestrial surface temperature inconsistent with the presence of liquid water and motivating atmospheric greenhouse models. An alternative model fo <span class="hlt">solar</span> evolution that invokes mass loss, constructed to explain <span class="hlt">solar</span> Li depletion, attenuates or reverses this luminosity evolution of the atmospheres of Earth and the other terrestrial planets. This model can be tested by Li abundance measurements. The continuum emission from stellar wind plasma during significant mass loss may be detectable at millimeter and radio wavelengths. The Earth (and Moon) experienced a period of intense bombardment prior to 3.8 Ga, long after accretion was completed in the inner <span class="hlt">solar</span> system and possibly associated with the clearing of residual planetesimals in the outer <span class="hlt">solar</span> system. Such</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20170005301','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20170005301"><span>The MSFC <span class="hlt">Solar</span> Activity Future Estimation (MSAFE) Model</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Suggs, Ron</p> <p>2017-01-01</p> <p>The MSAFE model provides forecasts for the <span class="hlt">solar</span> indices SSN, F10.7, and Ap. These <span class="hlt">solar</span> indices are used as inputs to space environment models used in orbital spacecraft operations and space mission analysis. Forecasts from the MSAFE model are provided on the MSFC Natural Environments Branch's <span class="hlt">solar</span> web page and are updated as new monthly <span class="hlt">observations</span> become available. The MSAFE prediction routine employs a statistical technique that calculates deviations of past <span class="hlt">solar</span> cycles from the mean cycle and performs a regression analysis to calculate the deviation from the mean cycle of the <span class="hlt">solar</span> index at the next future time interval. The forecasts are initiated for a given cycle after about 8 to 9 monthly <span class="hlt">observations</span> from the start of the cycle are collected. A forecast made at the beginning of cycle 24 using the MSAFE program <span class="hlt">captured</span> the cycle fairly well with some difficulty in discerning the double peak that occurred at <span class="hlt">solar</span> cycle maximum.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22126712-hemispheric-asymmetries-polar-solar-wind-observed-ulysses-near-minima-solar-cycles','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22126712-hemispheric-asymmetries-polar-solar-wind-observed-ulysses-near-minima-solar-cycles"><span>HEMISPHERIC ASYMMETRIES IN THE POLAR <span class="hlt">SOLAR</span> WIND <span class="hlt">OBSERVED</span> BY ULYSSES NEAR THE MINIMA OF <span class="hlt">SOLAR</span> CYCLES 22 AND 23</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>Ebert, R. W.; Dayeh, M. A.; Desai, M. I.</p> <p>2013-05-10</p> <p>We examined <span class="hlt">solar</span> wind plasma and interplanetary magnetic field (IMF) <span class="hlt">observations</span> from Ulysses' first and third orbits to study hemispheric differences in the properties of the <span class="hlt">solar</span> wind and IMF originating from the Sun's large polar coronal holes (PCHs) during the declining and minimum phase of <span class="hlt">solar</span> cycles 22 and 23. We identified hemispheric asymmetries in several parameters, most notably {approx}15%-30% south-to-north differences in averages for the <span class="hlt">solar</span> wind density, mass flux, dynamic pressure, and energy flux and the radial and total IMF magnitudes. These differences were driven by relatively larger, more variable <span class="hlt">solar</span> wind density and radial IMF betweenmore » {approx}36 Degree-Sign S-60 Degree-Sign S during the declining phase of <span class="hlt">solar</span> cycles 22 and 23. These <span class="hlt">observations</span> indicate either a hemispheric asymmetry in the PCH output during the declining and minimum phase of <span class="hlt">solar</span> cycles 22 and 23 with the southern hemisphere being more active than its northern counterpart, or a <span class="hlt">solar</span> cycle effect where the PCH output in both hemispheres is enhanced during periods of higher <span class="hlt">solar</span> activity. We also report a strong linear correlation between these <span class="hlt">solar</span> wind and IMF parameters, including the periods of enhanced PCH output, that highlight the connection between the <span class="hlt">solar</span> wind mass and energy output and the Sun's magnetic field. That these enhancements were not matched by similar sized variations in <span class="hlt">solar</span> wind speed points to the mass and energy responsible for these increases being added to the <span class="hlt">solar</span> wind while its flow was subsonic.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/15791734','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/15791734"><span><span class="hlt">Solar</span> particle events <span class="hlt">observed</span> at Mars: dosimetry measurements and model calculations.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Cleghorn, Timothy F; Saganti, Premkumar B; Zeitlin, Cary J; Cucinotta, Francis A</p> <p>2004-01-01</p> <p>During the period from March 13, 2002 to mid-September, 2002, six <span class="hlt">solar</span> particle events (SPE) were <span class="hlt">observed</span> by the MARIE instrument onboard the Odyssey Spacecraft in Martian Orbit. These events were <span class="hlt">observed</span> also by the GOES 8 satellite in Earth orbit, and thus represent the first time that the same SPE have been <span class="hlt">observed</span> at these separate locations. The characteristics of these SPE are examined, given that the active regions of the <span class="hlt">solar</span> disc from which the event originated can usually be identified. The dose rates at Martian orbit are calculated, both for the galactic and <span class="hlt">solar</span> components of the ionizing particle radiation environment. The dose rates due to galactic cosmic rays (GCR) agree well with the HZETRN model calculations. Published by Elsevier Ltd on behalf of COSPAR.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20050164094&hterms=caries&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dcaries','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20050164094&hterms=caries&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dcaries"><span><span class="hlt">Solar</span> particle events <span class="hlt">observed</span> at Mars: dosimetry measurements and model calculations</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Cleghorn, Timothy F.; Saganti, Premkumar B.; Zeitlin, Cary J.; Cucinotta, Francis A.</p> <p>2004-01-01</p> <p>During the period from March 13, 2002 to mid-September, 2002, six <span class="hlt">solar</span> particle events (SPE) were <span class="hlt">observed</span> by the MARIE instrument onboard the Odyssey Spacecraft in Martian Orbit. These events were <span class="hlt">observed</span> also by the GOES 8 satellite in Earth orbit, and thus represent the first time that the same SPE have been <span class="hlt">observed</span> at these separate locations. The characteristics of these SPE are examined, given that the active regions of the <span class="hlt">solar</span> disc from which the event originated can usually be identified. The dose rates at Martian orbit are calculated, both for the galactic and <span class="hlt">solar</span> components of the ionizing particle radiation environment. The dose rates due to galactic cosmic rays (GCR) agree well with the HZETRN model calculations. Published by Elsevier Ltd on behalf of COSPAR.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015ASPC..500...43P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015ASPC..500...43P"><span>Preparing for and <span class="hlt">Observing</span> the 2017 Total <span class="hlt">Solar</span> Eclipse</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pasachoff, J.</p> <p>2015-11-01</p> <p>I discuss ongoing plans and discussions for EPO and scientific <span class="hlt">observing</span> of the 21 August 2017 total <span class="hlt">solar</span> eclipse. I discuss aspects of EPO based on my experiences at the 60 <span class="hlt">solar</span> eclipses I have seen. I share cloud statistics along the eclipse path compiled by Jay Anderson, the foremost eclipse meteorologist. I show some sample <span class="hlt">observations</span> of composite imagery, of spectra, and of terrestrial temperature changes based on <span class="hlt">observations</span> of recent eclipses, including 2012 from Australia and 2013 from Gabon. Links to various mapping sites of totality, partial phases, and other eclipse-related information, including that provided by Michael Zeiler, Fred Espenak (retired from NASA) and Xavier Jubier can be found on the website I run for the International Astronomical Union's Working Group on Eclipses at http://www.eclipses.info.</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('https://ntrs.nasa.gov/search.jsp?R=19990111727&hterms=hack&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dhack','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19990111727&hterms=hack&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dhack"><span>Absorption of <span class="hlt">Solar</span> Radiation by Clouds: <span class="hlt">Observations</span> Versus Models</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Cess, R. D.; Zhang, M. H.; Minnis, P.; Corsetti, L.; Dutton, E. G.; Forgan, B. W.; Garber, D. P.; Gates, W. L.; Hack, J. J.; Harrison, E. F.; <a style="text-decoration: none; " href="javascript:void(0); " onClick="displayelement('author_19990111727'); toggleEditAbsImage('author_19990111727_show'); toggleEditAbsImage('author_19990111727_hide'); "> <img style="display:inline; width:12px; height:12px; " src="images/arrow-up.gif" width="12" height="12" border="0" alt="hide" id="author_19990111727_show"> <img style="width:12px; height:12px; display:none; " src="images/arrow-down.gif" width="12" height="12" border="0" alt="hide" id="author_19990111727_hide"></p> <p>1995-01-01</p> <p>There has been a long history of unexplained anomalous absorption of <span class="hlt">solar</span> radiation by clouds. Collocated satellite and surface measurements of <span class="hlt">solar</span> radiation at five geographically diverse locations showed significant <span class="hlt">solar</span> absorption by clouds, resulting in about 25 watts per square meter more global-mean absorption by the cloudy atmosphere than predicted by theoretical models. It has often been suggested that tropospheric aerosols could increase cloud absorption. But these aerosols are temporally and spatially heterogeneous, whereas the <span class="hlt">observed</span> cloud absorption is remarkably invariant with respect to season and location. Although its physical cause is unknown, enhanced cloud absorption substantially alters our understanding of the atmosphere's energy budget.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20100015397','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20100015397"><span>JWST Planetary <span class="hlt">Observations</span> Within the <span class="hlt">Solar</span> System</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Lunine, Jonathan; Hammel, Heidi; Schaller, Emily; Sonneborn, George; Orton, Glenn; Rieke, George; Rieke, Marcia</p> <p>2010-01-01</p> <p>JWST provides capabilities unmatched by other telescopic facilities in the near to mid infrared part of the electromagnetic spectrum. Its combination of broad wavelength range, high sensitivity and near diffraction-limited imaging around two microns wavelength make it a high value facility for a variety of <span class="hlt">Solar</span> System targets. Beyond Neptune, a class of cold, large bodies that include Pluto, Triton and Eris exhibits surface deposits of nitrogen, methane, and other molecules that are poorly <span class="hlt">observed</span> from the ground, but for which JWST might provide spectral mapping at high sensitivity and spatial resolution difficult to match with the current generation of ground-based observatories. The observatory will also provide unique sensitivity in a variety of near and mid infrared windows for <span class="hlt">observing</span> relatively deep into the atmospheres of Uranus and Neptune, searching there for minor species. It will examine the Jovian aurora in a wavelength regime where the background atmosphere is dark. Special provision of a subarray <span class="hlt">observing</span> strategy may allow <span class="hlt">observation</span> of Jupiter and Saturn over a larger wavelength range despite their large surface brightnesses, allowing for detailed <span class="hlt">observation</span> of transient phenomena including large scale storms and impact-generation disturbances. JWST's <span class="hlt">observations</span> of Saturn's moon Titan will overlap with and go beyond the 2017 end-of-mission for Cassini, providing an important extension to the time-series of meteorological studies for much of northern hemisphere summer. It will overlap with a number of other planetary missions to targets for which JWST can make unique types of <span class="hlt">observations</span>. JWST provides a platform for linking <span class="hlt">solar</span> system and extrasolar planet studies through its unique <span class="hlt">observational</span> capabilities in both arenas.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011AGUFMSH33A2035S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011AGUFMSH33A2035S"><span>Radio Imaging <span class="hlt">Observations</span> of <span class="hlt">Solar</span> Activity Cycle and Its Anomaly</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Shibasaki, K.</p> <p>2011-12-01</p> <p>The 24th <span class="hlt">solar</span> activity cycle has started and relative sunspot numbers are increasing. However, their rate of increase is rather slow compared to previous cycles. Active region sizes are small, lifetime is short, and big (X-class) flares are rare so far. We study this anomalous situation using data from Nobeyama Radioheliograph (NoRH). Radio imaging <span class="hlt">observations</span> have been done by NoRH since 1992. Nearly 20 years of daily radio images of the Sun at 17 GHz are used to synthesize a radio butterfly diagram. Due to stable operation of the instrument and a robust calibration method, uniform datasets are available covering the whole period of <span class="hlt">observation</span>. The radio butterfly diagram shows bright features corresponding to active region belts and their migration toward low latitude as the <span class="hlt">solar</span> cycle progresses. In the present <span class="hlt">solar</span> activity cycle (24), increase of radio brightness is delayed and slow. There are also bright features around both poles (polar brightening). Their brightness show <span class="hlt">solar</span> cycle dependence but peaks around <span class="hlt">solar</span> minimum. Comparison between the last minimum and the previous one shows decrease of its brightness. This corresponds to weakening of polar magnetic field activity between them. In the northern pole, polar brightening is already weakened in 2011, which means it is close to <span class="hlt">solar</span> maximum in the northern hemisphere. Southern pole does not show such feature yet. Slow rise of activity in active region belt, weakening of polar activity during the minimum, and large north-south asymmetry in polar activity imply that global <span class="hlt">solar</span> activity and its synchronization are weakening.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22519953-new-horizons-solar-wind-around-pluto-swap-observations-solar-wind-from-au','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22519953-new-horizons-solar-wind-around-pluto-swap-observations-solar-wind-from-au"><span>THE NEW HORIZONS <span class="hlt">SOLAR</span> WIND AROUND PLUTO (SWAP) <span class="hlt">OBSERVATIONS</span> OF THE <span class="hlt">SOLAR</span> WIND FROM 11–33 au</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>Elliott, H. A.; McComas, D. J.; Valek, P.</p> <p></p> <p>The <span class="hlt">Solar</span> Wind Around Pluto (SWAP) instrument on National Aeronautics and Space Administration's New Horizons Pluto mission has collected <span class="hlt">solar</span> wind <span class="hlt">observations</span> en route from Earth to Pluto, and these <span class="hlt">observations</span> continue beyond Pluto. Few missions have explored the <span class="hlt">solar</span> wind in the outer heliosphere making this dataset a critical addition to the field. We created a forward model of SWAP count rates, which includes a comprehensive instrument response function based on laboratory and flight calibrations. By fitting the count rates with this model, the proton density (n), speed (V), and temperature (T) parameters are determined. Comparisons between SWAP parametersmore » and both propagated 1 au <span class="hlt">observations</span> and prior Voyager 2 <span class="hlt">observations</span> indicate consistency in both the range and mean wind values. These comparisons as well as our additional findings confirm that small and midsized <span class="hlt">solar</span> wind structures are worn down with increasing distance due to dynamic interaction of parcels of wind with different speed. For instance, the T–V relationship steepens, as the range in V is limited more than the range in T with distance. At times the T–V correlation clearly breaks down beyond 20 au, which may indicate wind currently expanding and cooling may have an elevated T reflecting prior heating and compression in the inner heliosphere. The power of wind parameters at shorter periodicities decreases with distance as the longer periodicities strengthen. The <span class="hlt">solar</span> rotation periodicity is present in temperature beyond 20 au indicating the <span class="hlt">observed</span> parcel temperature may reflect not only current heating or cooling, but also heating occurring closer to the Sun.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012SPIE.8448E..0AK','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012SPIE.8448E..0AK"><span>Optimisation of <span class="hlt">solar</span> synoptic <span class="hlt">observations</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Klvaña, Miroslav; Sobotka, Michal; Švanda, Michal</p> <p>2012-09-01</p> <p>The development of instrumental and computer technologies is connected with steadily increasing needs for archiving of large data volumes. The current trend to meet this requirement includes the data compression and growth of storage capacities. This approach, however, has technical and practical limits. A further reduction of the archived data volume can be achieved by means of an optimisation of the archiving that consists in data selection without losing the useful information. We describe a method of optimised archiving of <span class="hlt">solar</span> images, based on the selection of images that contain a new information. The new information content is evaluated by means of the analysis of changes detected in the images. We present characteristics of different kinds of image changes and divide them into fictitious changes with a disturbing effect and real changes that provide a new information. In block diagrams describing the selection and archiving, we demonstrate the influence of clouds, the recording of images during an active event on the Sun, including a period before the event onset, and the archiving of long-term history of <span class="hlt">solar</span> activity. The described optimisation technique is not suitable for helioseismology, because it does not conserve the uniform time step in the archived sequence and removes the information about <span class="hlt">solar</span> oscillations. In case of long-term synoptic <span class="hlt">observations</span>, the optimised archiving can save a large amount of storage capacities. The actual capacity saving will depend on the setting of the change-detection sensitivity and on the capability to exclude the fictitious changes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19840005044','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19840005044"><span>Iron charge states <span class="hlt">observed</span> in the <span class="hlt">solar</span> wind</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Ipavich, F. M.; Galvin, A. B.; Gloeckler, G.; Hovestadt, D.; Klecker, B.; Scholer, M.</p> <p>1983-01-01</p> <p><span class="hlt">Solar</span> wind measurements from the ULECA sensor of the Max-Planck-Institut/University of Maryland experiment on ISEE-3 are reported. The low energy section of approx the ULECA sensor selects particles by their energy per charge (over the range 3.6 keV/Q to 30 keV/Q) and simultaneously measures their total energy with two low-noise solid state detectors. <span class="hlt">Solar</span> wind Fe charge state measurements from three time periods of high speed <span class="hlt">solar</span> wind occurring during a post-shock flow and a coronal hole-associated high speed stream are presented. Analysis of the post-shock flow <span class="hlt">solar</span> wind indicates the charge state distributions for Fe were peaked at approx +16, indicative of an unusually high coronal temperature (3,000,000 K). In contrast, the Fe charge state distribution <span class="hlt">observed</span> in a coronal hole-associated high speed stream peaks at approx -9, indicating a much lower coronal temperature (1,400,000 K). This constitutes the first reported measurements of iron charge states in a coronal hole-associated high speed stream.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015MNRAS.453.3157J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015MNRAS.453.3157J"><span>How Sedna and family were <span class="hlt">captured</span> in a close encounter with a <span class="hlt">solar</span> sibling</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jílková, Lucie; Portegies Zwart, Simon; Pijloo, Tjibaria; Hammer, Michael</p> <p>2015-11-01</p> <p>The discovery of 2012 VP113 initiated the debate on the origin of the Sedna family of planetesimals in orbit around the Sun. Sednitos roam the outer regions of the <span class="hlt">Solar</span> system between the Egeworth-Kuiper belt and the Oort Cloud, in extraordinary wide (a > 150 au) orbits with a large perihelion distance of q > 30 au compared to the Earth's (a ≡ 1 au and eccentricity e ≡ (1 - q/a) ≃ 0.0167 or q ≃ 1 au). This population is composed of a dozen objects, which we consider a family because they have similar perihelion distance and inclination with respect to the ecliptic i = 10°-30°. They also have similar argument of perihelion ω = 340° ± 55°. There is no ready explanation for their origin. Here we show that these orbital parameters are typical for a <span class="hlt">captured</span> population from the planetesimal disc of another star. Assuming that the orbital elements of Sednitos have not changed since they acquired their orbits, we reconstruct the encounter that led to their <span class="hlt">capture</span>. We conclude that they might have been <span class="hlt">captured</span> in a near miss with a 1.8 M⊙ star that impacted the Sun at ≃ 340 au at an inclination with respect to the ecliptic of 17°-34° with a relative velocity at infinity of ˜4.3 km s-1. We predict that the Sednitos region is populated by 930 planetesimals and the inner Oort Cloud acquired ˜440 planetesimals through the same encounter.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19750044107&hterms=effect+global+warming&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Deffect%2Bglobal%2Bwarming','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19750044107&hterms=effect+global+warming&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Deffect%2Bglobal%2Bwarming"><span>Recent advances in satellite <span class="hlt">observations</span> of <span class="hlt">solar</span> variability and global atmospheric ozone</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Heath, D. F.</p> <p>1974-01-01</p> <p>A description is given of the temporal behavior of the sun as an ultraviolet variable star in relation to daily zonal means of atmospheric ozone from the total amount to that above the 10-mb and 4-mb pressure levels. A significant correlation has been <span class="hlt">observed</span> between enhancements in the ultraviolet <span class="hlt">solar</span> irradiances and terrestrial passages of the <span class="hlt">solar</span> magnetic field sector boundary structure. However, it has not yet been possible to separate <span class="hlt">solar</span> from the dynamical effects on the variability in the zonal means of ozone. Attention is given to global changes in ozone which have been derived from the satellite <span class="hlt">observations</span> in terms of season, <span class="hlt">solar</span> variability, and major stratospheric disturbances such as stratospheric warmings.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.P54C..05K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.P54C..05K"><span>Correlating <span class="hlt">Solar</span> Wind Modulation with Ionospheric Variability at Mars from MEX and MAVEN <span class="hlt">Observations</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kopf, A. J.; Morgan, D. D.; Halekas, J. S.; Ruhunusiri, S.; Gurnett, D. A.; Connerney, J. E. P.</p> <p>2017-12-01</p> <p>The synthesis of <span class="hlt">observations</span> by the Mars Express and Mars Atmosphere and Volatiles Evolution (MAVEN) spacecraft allows for a unique opportunity to study variability in the Martian ionosphere from multiple perspectives. One major source for this variability is the <span class="hlt">solar</span> wind. Due to its elliptical orbit which precesses over time, MAVEN periodically spends part of its orbit outside the Martian bow shock, allowing for direct measurements of the <span class="hlt">solar</span> wind impacting the Martian plasma environment. When the Mars Advanced Radar for Subsurface and Ionosphere Sounding (MARSIS) instrument aboard Mars Express is simultaneously sounding the ionosphere, the influence from changes in the <span class="hlt">solar</span> wind can be <span class="hlt">observed</span>. Previous studies have suggested a positive correlation, connecting ionospheric density to the <span class="hlt">solar</span> wind proton flux, but depended on Earth-based measurements for <span class="hlt">solar</span> wind conditions. More recently, research has indicated that <span class="hlt">observations</span> of ionospheric variability from these two spacecraft can be connected in special cases, such as shock wave impacts or specific <span class="hlt">solar</span> wind magnetic field orientations. Here we extend this to more general <span class="hlt">solar</span> wind conditions and examine how changes in the <span class="hlt">solar</span> wind properties measured by MAVEN instruments correlate with ionospheric structure and dynamics <span class="hlt">observed</span> simultaneously in MARSIS remote and local measurements.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22521848-observing-cascades-solar-bullets-high-resolution-ii','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22521848-observing-cascades-solar-bullets-high-resolution-ii"><span><span class="hlt">OBSERVING</span> CASCADES OF <span class="hlt">SOLAR</span> BULLETS AT HIGH RESOLUTION. II</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>Scullion, E.; Engvold, O.; Lin, Y.</p> <p></p> <p>High resolution <span class="hlt">observations</span> from the Swedish 1-m <span class="hlt">Solar</span> Telescope revealed bright, discrete, blob-like structures (which we refer to as <span class="hlt">solar</span> bullets) in the Hα 656.28 nm line core that appear to propagate laterally across the <span class="hlt">solar</span> atmosphere as clusters in active regions (ARs). These small-scale structures appear to be field aligned and many bullets become triggered simultaneously and traverse collectively as a cluster. Here, we conduct a follow-up study on these rapidly evolving structures with coincident <span class="hlt">observations</span> from the <span class="hlt">Solar</span> Dynamics Observatory/Atmospheric Imaging Assembly. With the co-aligned data sets, we reveal (a) an evolving multithermal structure in the bullet clustermore » ranging from chromospheric to at least transition region temperatures, (b) evidence for cascade-like behavior and corresponding bidirectional motions in bullets within the cluster, which indicate that there is a common source of the initial instability leading to bullet formation, and (c) a direct relationship between co-incident bullet velocities <span class="hlt">observed</span> in Hα and He ii 30.4 nm and an inverse relationship with respect to bullet intensity in these channels. We find evidence supporting that bullets are typically composed of a cooler, higher density core detectable in Hα with a less dense, hotter, and fainter co-moving outer sheath. Bullets unequivocally demonstrate the finely structured nature of the AR corona. We have no clear evidence for bullets being associated with locally heated (or cooled), fast flowing plasma. Fast MHD pulses (such as solitons) could best describe the dynamic properties of bullets whereas the presence of a multithermal structure is new.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70175395','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70175395"><span>Evaluating the effectiveness of wildlife detection and <span class="hlt">observation</span> technologies at a <span class="hlt">solar</span> power tower facility</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Diehl, Robert H.; Valdez, Ernest W.; Preston, Todd M.; Wellik, Mike J.; Cryan, Paul</p> <p>2016-01-01</p> <p><span class="hlt">Solar</span> power towers produce electrical energy from sunlight at an industrial scale. Little is known about the effects of this technology on flying animals and few methods exist for automatically detecting or <span class="hlt">observing</span> wildlife at <span class="hlt">solar</span> towers and other tall anthropogenic structures. Smoking objects are sometimes <span class="hlt">observed</span> co-occurring with reflected, concentrated light (“<span class="hlt">solar</span> flux”) in the airspace around <span class="hlt">solar</span> towers, but the identity and origins of such objects can be difficult to determine. In this <span class="hlt">observational</span> pilot study at the world’s largest <span class="hlt">solar</span> tower facility, we assessed the efficacy of using radar, surveillance video, and insect trapping to detect and <span class="hlt">observe</span> animals flying near the towers. During site visits in May and September 2014, we monitored the airspace surrounding towers and <span class="hlt">observed</span> insects, birds, and bats under a variety of environmental and operational conditions. We detected and broadly differentiated animals or objects moving through the airspace generally using radar and near <span class="hlt">solar</span> towers using several video imaging methods. Video revealed what appeared to be mostly small insects burning in the <span class="hlt">solar</span> flux. Also, we occasionally detected birds flying in the <span class="hlt">solar</span> flux but could not accurately identify birds to species or the types of insects and small objects composing the vast majority of smoking targets. Insect trapping on the ground was somewhat effective at sampling smaller insects around the tower, and presence and abundance of insects in the traps generally trended with radar and video <span class="hlt">observations</span>. Traps did not tend to sample the larger insects we sometimes <span class="hlt">observed</span> flying in the <span class="hlt">solar</span> flux or found dead on the ground beneath the towers. Some of the methods we tested (e.g., video surveillance) could be further assessed and potentially used to automatically detect and <span class="hlt">observe</span> flying animals in the vicinity of <span class="hlt">solar</span> towers to advance understanding about their effects on wildlife.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27462989','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27462989"><span>Evaluating the Effectiveness of Wildlife Detection and <span class="hlt">Observation</span> Technologies at a <span class="hlt">Solar</span> Power Tower Facility.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Diehl, Robert H; Valdez, Ernest W; Preston, Todd M; Wellik, Michael J; Cryan, Paul M</p> <p>2016-01-01</p> <p><span class="hlt">Solar</span> power towers produce electrical energy from sunlight at an industrial scale. Little is known about the effects of this technology on flying animals and few methods exist for automatically detecting or <span class="hlt">observing</span> wildlife at <span class="hlt">solar</span> towers and other tall anthropogenic structures. Smoking objects are sometimes <span class="hlt">observed</span> co-occurring with reflected, concentrated light ("<span class="hlt">solar</span> flux") in the airspace around <span class="hlt">solar</span> towers, but the identity and origins of such objects can be difficult to determine. In this <span class="hlt">observational</span> pilot study at the world's largest <span class="hlt">solar</span> tower facility, we assessed the efficacy of using radar, surveillance video, and insect trapping to detect and <span class="hlt">observe</span> animals flying near the towers. During site visits in May and September 2014, we monitored the airspace surrounding towers and <span class="hlt">observed</span> insects, birds, and bats under a variety of environmental and operational conditions. We detected and broadly differentiated animals or objects moving through the airspace generally using radar and near <span class="hlt">solar</span> towers using several video imaging methods. Video revealed what appeared to be mostly small insects burning in the <span class="hlt">solar</span> flux. Also, we occasionally detected birds flying in the <span class="hlt">solar</span> flux but could not accurately identify birds to species or the types of insects and small objects composing the vast majority of smoking targets. Insect trapping on the ground was somewhat effective at sampling smaller insects around the tower, and presence and abundance of insects in the traps generally trended with radar and video <span class="hlt">observations</span>. Traps did not tend to sample the larger insects we sometimes <span class="hlt">observed</span> flying in the <span class="hlt">solar</span> flux or found dead on the ground beneath the towers. Some of the methods we tested (e.g., video surveillance) could be further assessed and potentially used to automatically detect and <span class="hlt">observe</span> flying animals in the vicinity of <span class="hlt">solar</span> towers to advance understanding about their effects on wildlife.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4963080','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4963080"><span>Evaluating the Effectiveness of Wildlife Detection and <span class="hlt">Observation</span> Technologies at a <span class="hlt">Solar</span> Power Tower Facility</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Diehl, Robert H.; Valdez, Ernest W.; Preston, Todd M.; Wellik, Michael J.; Cryan, Paul M.</p> <p>2016-01-01</p> <p><span class="hlt">Solar</span> power towers produce electrical energy from sunlight at an industrial scale. Little is known about the effects of this technology on flying animals and few methods exist for automatically detecting or <span class="hlt">observing</span> wildlife at <span class="hlt">solar</span> towers and other tall anthropogenic structures. Smoking objects are sometimes <span class="hlt">observed</span> co-occurring with reflected, concentrated light (“<span class="hlt">solar</span> flux”) in the airspace around <span class="hlt">solar</span> towers, but the identity and origins of such objects can be difficult to determine. In this <span class="hlt">observational</span> pilot study at the world’s largest <span class="hlt">solar</span> tower facility, we assessed the efficacy of using radar, surveillance video, and insect trapping to detect and <span class="hlt">observe</span> animals flying near the towers. During site visits in May and September 2014, we monitored the airspace surrounding towers and <span class="hlt">observed</span> insects, birds, and bats under a variety of environmental and operational conditions. We detected and broadly differentiated animals or objects moving through the airspace generally using radar and near <span class="hlt">solar</span> towers using several video imaging methods. Video revealed what appeared to be mostly small insects burning in the <span class="hlt">solar</span> flux. Also, we occasionally detected birds flying in the <span class="hlt">solar</span> flux but could not accurately identify birds to species or the types of insects and small objects composing the vast majority of smoking targets. Insect trapping on the ground was somewhat effective at sampling smaller insects around the tower, and presence and abundance of insects in the traps generally trended with radar and video <span class="hlt">observations</span>. Traps did not tend to sample the larger insects we sometimes <span class="hlt">observed</span> flying in the <span class="hlt">solar</span> flux or found dead on the ground beneath the towers. Some of the methods we tested (e.g., video surveillance) could be further assessed and potentially used to automatically detect and <span class="hlt">observe</span> flying animals in the vicinity of <span class="hlt">solar</span> towers to advance understanding about their effects on wildlife. PMID:27462989</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20170005305','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20170005305"><span>The MSFC <span class="hlt">Solar</span> Activity Future Estimation (MSAFE) Model</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Suggs, Ronnie J.</p> <p>2017-01-01</p> <p>The MSAFE model provides forecasts for the <span class="hlt">solar</span> indices SSN, F10.7, and Ap. These <span class="hlt">solar</span> indices are used as inputs to many space environment models used in orbital spacecraft operations and space mission analysis. Forecasts from the MSAFE model are provided on the MSFC Natural Environments Branch's <span class="hlt">solar</span> webpage and are updated as new monthly <span class="hlt">observations</span> come available. The MSAFE prediction routine employs a statistical technique that calculates deviations of past <span class="hlt">solar</span> cycles from the mean cycle and performs a regression analysis to predict the deviation from the mean cycle of the <span class="hlt">solar</span> index at the next future time interval. The prediction algorithm is applied recursively to produce monthly smoothed <span class="hlt">solar</span> index values for the remaining of the cycle. The forecasts are initiated for a given cycle after about 8 to 12 months of <span class="hlt">observations</span> are collected. A forecast made at the beginning of cycle 24 using the MSAFE program <span class="hlt">captured</span> the cycle fairly well with some difficulty in discerning the double peak that occurred at <span class="hlt">solar</span> cycle maximum.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JGRA..122.9815K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JGRA..122.9815K"><span>Applying Nyquist's method for stability determination to <span class="hlt">solar</span> wind <span class="hlt">observations</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Klein, Kristopher G.; Kasper, Justin C.; Korreck, K. E.; Stevens, Michael L.</p> <p>2017-10-01</p> <p>The role instabilities play in governing the evolution of <span class="hlt">solar</span> and astrophysical plasmas is a matter of considerable scientific interest. The large number of sources of free energy accessible to such nearly collisionless plasmas makes general modeling of unstable behavior, accounting for the temperatures, densities, anisotropies, and relative drifts of a large number of populations, analytically difficult. We therefore seek a general method of stability determination that may be automated for future analysis of <span class="hlt">solar</span> wind <span class="hlt">observations</span>. This work describes an efficient application of the Nyquist instability method to the Vlasov dispersion relation appropriate for hot, collisionless, magnetized plasmas, including the <span class="hlt">solar</span> wind. The algorithm recovers the familiar proton temperature anisotropy instabilities, as well as instabilities that had been previously identified using fits extracted from in situ <span class="hlt">observations</span> in Gary et al. (2016). Future proposed applications of this method are discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19960021396&hterms=dropout&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Ddropout','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19960021396&hterms=dropout&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Ddropout"><span>Suprathermal electron loss cone distributions in the <span class="hlt">solar</span> wind: Ulysses <span class="hlt">observations</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Phillips, J. L.; Feldman, W. C.; Gosling, J. T.; Hammond, C. M.; Forsyth, R. J.</p> <p>1995-01-01</p> <p><span class="hlt">Solar</span> wind suprathermal electron distributions in the <span class="hlt">solar</span> wind generally carry a field-aligned antisunward heat flux. Within coronal mass ejections and upstream of strong shocks driven by corotating interaction regions (CIRs), counterstreaming electron beams are <span class="hlt">observed</span>. We present <span class="hlt">observations</span> by the Ulysses <span class="hlt">solar</span> wind plasma experiment of a new class of suprathermal electron signatures. At low <span class="hlt">solar</span> latitudes and heliocentric distances beyond 3.5 AU Ulysses encountered several intervals, ranging in duration from 1 hour to 22 hours, in which the suprathermal distributions included an antisunward field-aligned beam and a return population with a flux dropout typically spanning +/- 60 deg from the sunward field-aligned direction. All events occurred within CIRs, downstream of the forward and reverse shocks or waves bounding the interaction regions. We evaluate the hypothesis that the sunward-moving electrons result from reflection of the antisunward beams at magnetic field compressions downstream from the <span class="hlt">observations</span>, with wide loss cones caused by the relatively weak compression ratio. This hypothesis requires that field magnitude within the CIRs actually increase with increasing field-aligned distance from the Sun. Details of the electron distributions and ramifications for CIR and shock geometry will be presented.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018AdSpR..61...74P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018AdSpR..61...74P"><span>Improving magnetosphere in situ <span class="hlt">observations</span> using <span class="hlt">solar</span> sails</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Parsay, Khashayar; Schaub, Hanspeter; Schiff, Conrad; Williams, Trevor</p> <p>2018-01-01</p> <p>Past and current magnetosphere missions employ conventional spacecraft formations for in situ <span class="hlt">observations</span> of the geomagnetic tail. Conventional spacecraft flying in inertially fixed Keplerian orbits are only aligned with the geomagnetic tail once per year, since the geomagnetic tail is always aligned with the Earth-Sun line, and therefore, rotates annually. <span class="hlt">Solar</span> sails are able to artificially create sun-synchronous orbits such that the orbit apse line remains aligned with the geomagnetic tail line throughout the entire year. This continuous presence in the geomagnetic tail can significantly increase the science phase for magnetosphere missions. In this paper, the problem of <span class="hlt">solar</span> sail formation design is explored using nonlinear programming to design optimal two-craft, triangle, and tetrahedron <span class="hlt">solar</span> sail formations, in terms of formation quality and formation stability. The designed formations are directly compared to the formations used in NASA's Magnetospheric Multi-Scale mission.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018SoPh..293...90K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018SoPh..293...90K"><span>Combined Radio and Space-Based <span class="hlt">Solar</span> <span class="hlt">Observations</span>: From Techniques to New Results - Preface</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kontar, Eduard P.; Nindos, Alexander</p> <p>2018-06-01</p> <p>The phenomena <span class="hlt">observed</span> at the Sun have a variety of unique radio signatures that can be used to diagnose the processes in the <span class="hlt">solar</span> atmosphere. The insights provided by radio <span class="hlt">observations</span> are further enhanced when they are combined with <span class="hlt">observations</span> from space-based telescopes. This Topical collection demonstrates the power of combination methodology at work and provides new results on i) type I <span class="hlt">solar</span> radio bursts and thermal emission to study active regions; ii) type II and IV bursts to better understand the structure of coronal mass ejections; and iii) non-thermal gyro-synchrotron and/or type III bursts to improve the characterisation of particle acceleration in <span class="hlt">solar</span> flares. The ongoing improvements in time, frequency, and spatial resolutions of ground-based telescopes reveal new levels in the complexity of <span class="hlt">solar</span> phenomena and pose new questions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22520118-observations-hierarchical-solar-type-multiple-star-systems','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22520118-observations-hierarchical-solar-type-multiple-star-systems"><span><span class="hlt">OBSERVATIONS</span> OF HIERARCHICAL <span class="hlt">SOLAR</span>-TYPE MULTIPLE STAR 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>Roberts, Lewis C. Jr.; Tokovinin, Andrei; Mason, Brian D.</p> <p>2015-10-15</p> <p>Twenty multiple stellar systems with <span class="hlt">solar</span>-type primaries were <span class="hlt">observed</span> at high angular resolution using the PALM-3000 adaptive optics system at the 5 m Hale telescope. The goal was to complement the knowledge of hierarchical multiplicity in the <span class="hlt">solar</span> neighborhood by confirming recent discoveries by the visible Robo-AO system with new near-infrared <span class="hlt">observations</span> with PALM-3000. The physical status of most, but not all, of the new pairs is confirmed by photometry in the Ks band and new positional measurements. In addition, we resolved for the first time five close sub-systems: the known astrometric binary in HIP 17129AB, companions to the primariesmore » of HIP 33555, and HIP 118213, and the companions to the secondaries in HIP 25300 and HIP 101430. We place the components on a color–magnitude diagram and discuss each multiple system individually.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20110007245&hterms=Butterfly&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3DButterfly','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20110007245&hterms=Butterfly&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3DButterfly"><span><span class="hlt">Solar</span> Sources and Geospace Consequences of Interplanetary Magnetic Clouds <span class="hlt">Observed</span> During <span class="hlt">Solar</span> Cycle 23</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Gopalswamy, N.; Akiyama, S.; Yashiro, S.; Michalek, G.; Lepping, R. P.</p> <p>2007-01-01</p> <p>We present results of a statistical investigation of 99 magnetic clouds (MCs) <span class="hlt">observed</span> during 1995-2005. The MC-associated coronal mass ejections (CMEs) are faster and wider on the average and originate within +/-30deg from the <span class="hlt">solar</span> disk center. The <span class="hlt">solar</span> sources of MCs also followed the butterfly diagram. The correlation between the magnetic field strength and speed of MCs was found to be valid over a much wider range of speeds. The number of south-north (SN) MCs was dominant and decreased with <span class="hlt">solar</span> cycle, while the number of north-south (NS) MCs increased confirming the odd-cycle behavior. Two-thirds of MCs were geoeffective; the Dst index was highly correlated with speed and magnetic field in MCs as well as their product. Many (55%) fully northward (FN) MCs were geoeffective solely due to their sheaths. The non-geoeffective MCs were slower (average speed approx. 382 km/s), had a weaker southward magnetic field (average approx. -5.2nT), and occurred mostly during the rise phase of the <span class="hlt">solar</span> activity cycle.</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('http://adsabs.harvard.edu/abs/2009cwse.conf...63T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009cwse.conf...63T"><span>Hinode ``a new <span class="hlt">solar</span> observatory in space''</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tsuneta, S.; Harra, L. K.; Masuda, S.</p> <p>2009-05-01</p> <p>Since its launch in September 2006, the Japan-US-UK <span class="hlt">solar</span> physics satellite, Hinode, has continued its <span class="hlt">observation</span> of the sun, sending back <span class="hlt">solar</span> images of unprecedented clarity every day. Hinode is equipped with three telescopes, a visible light telescope, an X-ray telescope, and an extreme ultraviolet imaging spectrometer. The Hinode optical telescope has a large primary mirror measuring 50 centimeters in diameter and is the world's largest space telescope for <span class="hlt">observing</span> the sun and its vector magnetic fields. The impact of Hinode as an optical telescope on <span class="hlt">solar</span> physics is comparable to that of the Hubble Space Telescope on optical astronomy. While the optical telescope <span class="hlt">observes</span> the sun's surface, the Hinode X-ray telescope <span class="hlt">captures</span> images of the corona and the high-temperature flares that range between several million and several tens of millions of degrees. The telescope has <span class="hlt">captured</span> coronal structures that are clearer than ever. The Hinode EUV imaging spectrometer possesses approximately ten times the sensitivity and four times the resolution of a similar instrument on the SOHO satellite. The source of energy for the sun is in the nuclear fusion reaction that takes place at its core. Here temperature drops closer to the surface, where the temperature measures about 6,000 degrees. Mysteriously, the temperature starts rising again above the surface, and the temperature of the corona is exceptionally high, several millions of degrees. It is as if water were boiling fiercely in a kettle placed on a stove with no fire, inconceivable as it may sound. The phenomenon is referred to as the coronal heating problem, and it is one of the major astronomical mysteries. The Hinode observatory was designed to solve this mystery. It is expected that Hinode would also provide clues to unraveling why strong magnetic fields are formed and how <span class="hlt">solar</span> flares are triggered. An overview on the initial results from Hinode is presented. Dynamic video pictures <span class="hlt">captured</span> by Hinode can be</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMSH53A2546J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMSH53A2546J"><span>Lessons Learned from 10 Years of STEREO <span class="hlt">Solar</span> Wind <span class="hlt">Observations</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jian, L. K.; Russell, C. T.; Luhmann, J. G.; Galvin, A. B.</p> <p>2017-12-01</p> <p>We have conducted long-term <span class="hlt">observations</span> of large-scale <span class="hlt">solar</span> wind structures since the launch of STEREO spacecraft, specifically interplanetary CMEs (ICMEs), slow-to-fast stream interaction regions (SIRs), and interplanetary shocks. In combination with our previous <span class="hlt">observations</span> of the same <span class="hlt">solar</span> wind structures in 1995-2009 using Wind/ACE data and the same identification criteria, we have first studied the <span class="hlt">solar</span> cycle variations of these structures, especially for the same phases of <span class="hlt">solar</span> cycles 23 and 24. Attributing the shocks to the interplanetary drivers, we have statistically compared the shocks driven by ICMEs and SIRs, and explained the shocks without a clear local driver. In addition, using the longitudinal and latitudinal separations between the twin spacecraft, we have investigated the recurrence and variability of ICMEs and SIRs, and gained the critical implications for the proposed L5 mission. At last, we have associated the heliospheric current sheet (HCS) crossings with the ICMEs and SIRs, and compared the properties of SIRs with and without HCS crossings, which correspond to the helmet streamers and pseudostreamers, respectively. The findings are important constraints on the theories of slow wind origin.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/22587539','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/22587539"><span>Clinical information transfer and data <span class="hlt">capture</span> in the acute myocardial infarction pathway: an <span class="hlt">observational</span> study.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Kesavan, Sujatha; Kelay, Tanika; Collins, Ruth E; Cox, Benita; Bello, Fernando; Kneebone, Roger L; Sevdalis, Nick</p> <p>2013-10-01</p> <p>Acute myocardial infarctions (MIs) or heart attacks are the result of a complete or an incomplete occlusion of the lumen of the coronary artery with a thrombus. Prompt diagnosis and early coronary intervention results in maximum myocardial salvage, hence time to treat is of the essence. Adequate, accurate and complete information is vital during the early stages of admission of an MI patient and can impact significantly on the quality and safety of patient care. This study aimed to record how clinical information between different clinical teams during the journey of a patient in the MI care pathway is <span class="hlt">captured</span> and to review the flow of information within this care pathway. A prospective, descriptive, structured <span class="hlt">observational</span> study to assess (i) current clinical information systems (CIS) utilization and (ii) real-time information availability within an acute cardiac care setting was carried out. Completeness and availability of patient information <span class="hlt">capture</span> across four key stages of the MI care pathway were assessed prospectively. Thirteen separate information systems were utilized during the four phases of the MI pathway. <span class="hlt">Observations</span> revealed fragmented CIS utilization, with users accessing an average of six systems to gain a complete set of patient information. Data <span class="hlt">capture</span> was found to vary between each pathway stage and in both patient cohort risk groupings. The highest level of information completeness (100%) was <span class="hlt">observed</span> only in the discharge stage of the MI care pathway. The lowest level of information completeness (58%) was <span class="hlt">observed</span> in the admission stage. The study highlights fragmentation, CIS duplication, and discrepancies in the current clinical information <span class="hlt">capture</span> and data transfer across the MI care pathway in an acute cardiac care setting. The development of an integrated and user-friendly electronic data <span class="hlt">capture</span> and transfer system would reduce duplication and would facilitate efficient and complete information provision at the point of care. © 2012</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19820047282&hterms=lazarus&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAuthor-Name%26N%3D0%26No%3D80%26Ntt%3Dlazarus','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19820047282&hterms=lazarus&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAuthor-Name%26N%3D0%26No%3D80%26Ntt%3Dlazarus"><span>Voyager <span class="hlt">observations</span> of <span class="hlt">solar</span> wind proton temperature - 1-10 AU</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Gazis, P. R.; Lazarus, A. J.</p> <p>1982-01-01</p> <p>Simultaneous measurements are made of the <span class="hlt">solar</span> wind proton temperatures by the Voyager 1 and 2 spacecraft, far from earth, and the IMP 8 spacecraft in earth orbit. This technique permits a separation of radial and temporal variations of <span class="hlt">solar</span> wind parameters. The average value of the proton temperature between 1 and 9 AU is <span class="hlt">observed</span> to decrease as r (the heliocentric radius) to the -(0.7 + or - 0.2). This is slower than would be expected for adiabatic expansion. A detailed examination of the <span class="hlt">solar</span> wind stream structure shows that considerable heating occurs at the interface between high and low speed streams.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19910009603','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19910009603"><span>Simultaneous <span class="hlt">Solar</span> Maximum Mission (SMM) and Very Large Array (VLA) <span class="hlt">observations</span> of <span class="hlt">solar</span> active regions</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Willson, Robert F.</p> <p>1991-01-01</p> <p>Very Large Array <span class="hlt">observations</span> at 20 cm wavelength can detect the hot coronal plasma previously <span class="hlt">observed</span> at soft x ray wavelengths. Thermal cyclotron line emission was detected at the apex of coronal loops where the magnetic field strength is relatively constant. Detailed comparison of simultaneous <span class="hlt">Solar</span> Maximum Mission (SMM) Satellite and VLA data indicate that physical parameters such as electron temperature, electron density, and magnetic field strength can be obtained, but that some coronal loops remain invisible in either spectral domain. The unprecedent spatial resolution of the VLA at 20 cm wavelength showed that the precursor, impulsive, and post-flare components of <span class="hlt">solar</span> bursts originate in nearby, but separate loops or systems of loops.. In some cases preburst heating and magnetic changes are <span class="hlt">observed</span> from loops tens of minutes prior to the impulsive phase. Comparisons with soft x ray images and spectra and with hard x ray data specify the magnetic field strength and emission mechanism of flaring coronal loops. At the longer 91 cm wavelength, the VLA detected extensive emission interpreted as a hot 10(exp 5) K interface between cool, dense H alpha filaments and the surrounding hotter, rarefield corona. <span class="hlt">Observations</span> at 91 cm also provide evidence for time-correlated bursts in active regions on opposite sides of the <span class="hlt">solar</span> equator; they are attributed to flare triggering by relativistic particles that move along large-scale, otherwise-invisible, magnetic conduits that link active regions in opposite hemispheres of the Sun.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018ApJ...856L..10M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018ApJ...856L..10M"><span>Heliosphere Responds to a Large <span class="hlt">Solar</span> Wind Intensification: Decisive <span class="hlt">Observations</span> from IBEX</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>McComas, D. J.; Dayeh, M. A.; Funsten, H. O.; Heerikhuisen, J.; Janzen, P. H.; Reisenfeld, D. B.; Schwadron, N. A.; Szalay, J. R.; Zirnstein, E. J.</p> <p>2018-03-01</p> <p>Our heliosphere—the bubble in the local interstellar medium produced by the Sun’s outflowing <span class="hlt">solar</span> wind—has finally responded to a large increase in <span class="hlt">solar</span> wind output and pressure in the second half of 2014. NASA’s Interstellar Boundary Explorer (IBEX) mission remotely monitors the outer heliosphere by <span class="hlt">observing</span> energetic neutral atoms (ENAs) returning from the heliosheath, the region between the termination shock and heliopause. IBEX <span class="hlt">observed</span> a significant enhancement in higher energy ENAs starting in late 2016. While IBEX <span class="hlt">observations</span> over the previous decade reflected a general reduction of ENA intensities, indicative of a deflating heliosphere, new <span class="hlt">observations</span> show that the large (∼50%), persistent increase in the <span class="hlt">solar</span> wind dynamic pressure has modified the heliosheath, producing enhanced ENA emissions. The combination of these new <span class="hlt">observations</span> with simulation results indicate that this pressure is re-expanding our heliosphere, with the termination shock and heliopause already driven outward in the locations closest to the Sun. The timing between the IBEX <span class="hlt">observations</span>, a large transient pressure enhancement seen by Voyager 2, and the simulations indicates that the pressure increase propagated through the heliosheath, reflected off the heliopause, and the enhanced density of the <span class="hlt">solar</span> wind filled the heliosheath behind it before generating significantly enhanced ENA emissions. The coming years should see significant changes in anomalous cosmic rays, galactic cosmic radiation, and the filtration of interstellar neutral atoms into the inner heliosphere.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2002cosp...34E2215C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2002cosp...34E2215C"><span><span class="hlt">Solar</span> particle events <span class="hlt">observed</span> at Mars: dosimetry measurements and model calculations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Cleghorn, T.; Saganti, P.; Zeitlin, C.; Cucinotta, F.</p> <p></p> <p>The first <span class="hlt">solar</span> particle events from a Martian orbit are <span class="hlt">observed</span> with the MARIE (Martian Radiation Environment Experiment) on the 2001 Mars Odyssey space -craft that is currently in orbit and collecting the mapping data of the red planet. These <span class="hlt">solar</span> particle events <span class="hlt">observed</span> at Mars during March and April 2002, are correlated with the GOES-8 and ACE satellite data from the same time period at Earth orbits. Dosimetry measurements for the Mars orbit from the period of March 13t h through April 29t h . Particle count rate and the corresponding dose rate enhancements were <span class="hlt">observed</span> on March 16t h through 20t h and on April 22n d corresponding to <span class="hlt">solar</span> particle events that were <span class="hlt">observed</span> at Earth orbit on March 16t h through 21s t and beginning on April 21s t respectively. The model calculations with the HZETRN (High Z=atomic number and high Energy Transport) code estimated the background GCR (Galactic Cosmic Rays) dose rates. The dose rates <span class="hlt">observed</span> by the MARIE instrument are within 10% of the model calculations. Dosimetry measurements and model calculation will be presented.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017SPIE10565E..0RS','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017SPIE10565E..0RS"><span>Optical and thermal design of 1.5-m aperture <span class="hlt">solar</span> UV visible and IR <span class="hlt">observing</span> telescope for <span class="hlt">Solar</span>-C mission</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Suematsu, Y.; Katsukawa, Y.; Shimizu, T.; Ichimoto, K.; Horiuchi, T.; Matsumoto, Y.; Takeyama, N.</p> <p>2017-11-01</p> <p>The next Japanese <span class="hlt">solar</span> mission, <span class="hlt">SOLAR</span>-C, which has been envisaged after successful science operation of Hinode (<span class="hlt">SOLAR</span>-B) mission, is perusing two plans: plan-A and plan-B, and under extensive study from science objectives as well as engineering point of view. The plan-A aims at performing out-of-ecliptic <span class="hlt">observations</span> for investigating, with helioseismic approach, internal structure and dynamo mechanisms of the Sun. It also explores polar regions where fast <span class="hlt">solar</span> wind is believed to originate. A baseline orbit for plan-A is a circular orbit of 1 AU distance from the Sun with its inclination at around or greater than 40 degrees. The plan-B aims to study small-scale plasma processes and structures in the <span class="hlt">solar</span> atmosphere which attract researchers' growing interest, followed by many Hinode discoveries [1], for understanding fully dynamism and magnetic nature of the atmosphere. With plan-B, high-angular-resolution investigation of the entire <span class="hlt">solar</span> atmosphere (from the photosphere to the corona, including their interface layers, i.e., chromosphere and transition region) is to be performed with enhanced spectroscopic and spectro-polarimetric capability as compared with Hinode, together with enhanced sensitivity towards ultra-violet wavelengths. The orbit of plan-B is either a <span class="hlt">solar</span> synchronous polar orbit of altitude around 600 km or a geosynchronous orbit to ensure continuous <span class="hlt">solar</span> <span class="hlt">observations</span>. After the decision of any one of the two plans, the <span class="hlt">SOLAR</span>-C will be proposed for launch in mid-2010s. In this paper, we will present a basic design of one of major planned instrumental payload for the plan-B: the <span class="hlt">Solar</span> Ultra-violet Visible and near IR <span class="hlt">observing</span> Telescope (hereafter referred to as SUVIT). The basic concept in designing the SUVIT is to utilize as much as possible a heritage of successful telescope of the <span class="hlt">Solar</span> Optical Telescope (SOT) aboard Hinode [2]. Major differences of SUVIT from SOT are the three times larger aperture of 1.5 m, which enables to collect one</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1993nhud.rept.....V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1993nhud.rept.....V"><span>A search for energetic ion directivity in large <span class="hlt">solar</span> flares</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Vestrand, W. Thomas</p> <p></p> <p>One of the key <span class="hlt">observational</span> questions for <span class="hlt">solar</span> flare physics is: What is the number, the energy spectrum, and the angular distribution of flare accelerated ions? The standard method for deriving ion spectral shape employs the ratio of influences <span class="hlt">observed</span> on the 4-7 MeV band to the narrow neutron <span class="hlt">capture</span> line at 2.223 MeV. The 4-7 MeV band is dominated by the principal nuclear de-excitation lines from C-12 and O-16 which are generated in the low chromosphere by the direct excitation or spallation of nuclei by energetic ions. In contrast, the narrow 2.223 MeV line is produced by the <span class="hlt">capture</span> of thermal neutrons on protons in the photosphere. These <span class="hlt">capture</span> neutrons are generated by energetic ion interactions and thermalized by scattering in the <span class="hlt">solar</span> atmosphere. In a series of papers, Ramaty, Lingenfelter, and their collaborators have calculated the expected ratio of fluence in the 4-7 MeV band to the 2.223 MeV line for a wide range of energetic ion spectral shapes (see, e.g. Hua and Lingenfelter 1987). Another technique for deriving ion spectral shapes and angular distributions uses the relative strength of the Compton tail associated with the 2.223 MeV neutron <span class="hlt">capture</span> line (Vestrand 1988, 1990). This technique can independently constrain both the angular and the energy distribution of the energetic parent ions. The combination of this tail/line strength diagnostic with the line/(4-7) MeV fluence ratio can allow one to constrain both properties of the energetic ion distributions. The primary objective of our <span class="hlt">Solar</span> Maximum Mission (SMM) guest investigator program was to study measurements of neutron <span class="hlt">capture</span> line emission and prompt nuclear de-excitation for large flares detected by the <span class="hlt">Solar</span> Maximum Mission/ Gamma-Ray Spectrometer (SMM/GRS) and to use these established line diagnostics to study the properties of flare accelerated ions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22356468-solar-wind-neon-abundance-observed-ace-swics-ulysses-swics','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22356468-solar-wind-neon-abundance-observed-ace-swics-ulysses-swics"><span>The <span class="hlt">solar</span> wind neon abundance <span class="hlt">observed</span> with ACE/SWICS and ULYSSES/SWICS</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>Shearer, Paul; Raines, Jim M.; Lepri, Susan T.</p> <p></p> <p>Using in situ ion spectrometry data from ACE/SWICS, we determine the <span class="hlt">solar</span> wind Ne/O elemental abundance ratio and examine its dependence on wind speed and evolution with the <span class="hlt">solar</span> cycle. We find that Ne/O is inversely correlated with wind speed, is nearly constant in the fast wind, and correlates strongly with <span class="hlt">solar</span> activity in the slow wind. In fast wind streams with speeds above 600 km s{sup –1}, we find Ne/O = 0.10 ± 0.02, in good agreement with the extensive polar <span class="hlt">observations</span> by Ulysses/SWICS. In slow wind streams with speeds below 400 km s{sup –1}, Ne/O ranges from amore » low of 0.12 ± 0.02 at <span class="hlt">solar</span> maximum to a high of 0.17 ± 0.03 at <span class="hlt">solar</span> minimum. These measurements place new and significant empirical constraints on the fractionation mechanisms governing <span class="hlt">solar</span> wind composition and have implications for the coronal and photospheric abundances of neon and oxygen. The results are made possible by a new data analysis method that robustly identifies rare elements in the measured ion spectra. The method is also applied to Ulysses/SWICS data, which confirms the ACE <span class="hlt">observations</span> and extends our view of <span class="hlt">solar</span> wind neon into the three-dimensional heliosphere.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMSH41A2749N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMSH41A2749N"><span>Statistical and <span class="hlt">observational</span> research of <span class="hlt">solar</span> flare for total spectra and geometrical features</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Nishimoto, S.; Watanabe, K.; Imada, S.; Kawate, T.; Lee, K. S.</p> <p>2017-12-01</p> <p>Impulsive energy release phenomena such as <span class="hlt">solar</span> flares, sometimes affect to the <span class="hlt">solar</span>-terrestrial environment. Usually, we use soft X-ray flux (GOES class) as the index of flare scale. However, the magnitude of effect to the <span class="hlt">solar</span>-terrestrial environment is not proportional to that scale. To identify the relationship between <span class="hlt">solar</span> flare phenomena and influence to the <span class="hlt">solar</span>-terrestrial environment, we need to understand the full spectrum of <span class="hlt">solar</span> flares. There is the <span class="hlt">solar</span> flare irradiance model named the Flare Irradiance Spectral Model (FISM) (Chamberlin et al., 2006, 2007, 2008). The FISM can estimate <span class="hlt">solar</span> flare spectra with high wavelength resolution. However, this model can not express the time evolution of emitted plasma during the <span class="hlt">solar</span> flare, and has low accuracy on short wavelength that strongly effects and/or controls the total flare spectra. For the purpose of obtaining the time evolution of total <span class="hlt">solar</span> flare spectra, we are performing statistical analysis of the electromagnetic data of <span class="hlt">solar</span> flares. In this study, we select <span class="hlt">solar</span> flare events larger than M-class from the Hinode flare catalogue (Watanabe et al., 2012). First, we focus on the EUV emission <span class="hlt">observed</span> by the SDO/EVE. We examined the intensities and time evolutions of five EUV lines of 55 flare events. As a result, we found positive correlation between the "soft X-ray flux" and the "EUV peak flux" for all EVU lines. Moreover, we found that hot lines peaked earlier than cool lines of the EUV light curves. We also examined the hard X-ray data obtained by RHESSI. When we analyzed 163 events, we found good correlation between the "hard X-ray intensity" and the "soft X-ray flux". Because it seems that the geometrical features of <span class="hlt">solar</span> flares effect to those time evolutions, we also looked into flare ribbons <span class="hlt">observed</span> by SDO/AIA. We examined 21 flare events, and found positive correlation between the "GOES duration" and the "ribbon length". We also found positive correlation between the "ribbon</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19740054880&hterms=Exciter&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3DExciter','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19740054880&hterms=Exciter&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3DExciter"><span>Satellite <span class="hlt">observations</span> of type III <span class="hlt">solar</span> radio bursts at low frequencies</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Fainberg, J.; Stone, R. G.</p> <p>1974-01-01</p> <p>Type III <span class="hlt">solar</span> radio bursts have been <span class="hlt">observed</span> from 10 MHz to 10 kHz by satellite experiments above the terrestrial plasmasphere. <span class="hlt">Solar</span> radio emission in this frequency range results from excitation of the interplanetary plasma by energetic particles propagating outward along open field lines over distances from 5 earth radii to at least 1 AU from the sun. This review summarizes the morphology, characteristics, and analysis of individual as well as storms of bursts. Substantial evidence is available to show that the radio emission is <span class="hlt">observed</span> at the second harmonic instead of the fundamental of the plasma frequency. This brings the density scale derived by radio <span class="hlt">observations</span> into better agreement with direct <span class="hlt">solar</span> wind density measurements at 1 AU and relaxes the requirement for type III propagation along large density-enhanced regions. This density scale with the measured direction of arrival of the radio burst allows the trajectory of the exciter path to be determined from 10 earth radii to 1 AU.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1999AAS...194.8003A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1999AAS...194.8003A"><span>YOHKOH <span class="hlt">Observations</span> at the Y2K <span class="hlt">Solar</span> Maximum</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Aschwanden, M. J.</p> <p>1999-05-01</p> <p>Yohkoh will provide simultaneous co-aligned soft X-ray and hard X-ray <span class="hlt">observations</span> of <span class="hlt">solar</span> flares at the coming <span class="hlt">solar</span> maximum. The Yohkoh Soft X-ray Telescope (SXT) covers the approximate temperature range of 2-20 MK with a pixel size of 2.46\\arcsec, and thus complements ideally the EUV imagers sensitive in the 1-2 MK plasma, such as SoHO/EIT and TRACE. The Yohkoh Hard X-ray Telescope (HXT) offers hard X-ray imaging at 20-100 keV at a time resolution of down to 0.5 sec for major events. In this paper we review the major SXT and HXT results from Yohkoh <span class="hlt">solar</span> flare <span class="hlt">observations</span>, and anticipate some of the key questions that can be addressed through joint <span class="hlt">observations</span> with other ground and space-based observatories. This encompasses the dynamics of flare triggers (e.g. emerging flux, photospheric shear, interaction of flare loops in quadrupolar geometries, large-scale magnetic reconfigurations, eruption of twisted sigmoid structures, coronal mass ejections), the physics of particle dynamics during flares (acceleration processes, particle propagation, trapping, and precipitation), and flare plasma heating processes (chromospheric evaporation, coronal energy loss by nonthermal particles). In particular we will emphasize on how Yohkoh data analysis is progressing from a qualitative to a more quantitative science, employing 3-dimensional modeling and numerical simulations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010EGUGA..12.6000S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010EGUGA..12.6000S"><span>Interaction between <span class="hlt">Solar</span> Wind and Lunar Magnetic Anomalies <span class="hlt">observed</span> by Kaguya MAP-PACE</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Saito, Yoshifumi; Yokota, Shoichiro; Tanaka, Takaaki; Asamura, Kazushi; Nishino, Masaki; Yamamoto, Tadateru; Uemura, Kota; Tsunakawa, Hideo</p> <p>2010-05-01</p> <p>It is known that Moon has neither global intrinsic magnetic field nor thick atmosphere. Different from the Earth's case where the intrinsic global magnetic field prevents the <span class="hlt">solar</span> wind from penetrating into the magnetosphere, <span class="hlt">solar</span> wind directly impacts the lunar surface. Since the discovery of the lunar crustal magnetic field in 1960s, several papers have been published concerning the interaction between the <span class="hlt">solar</span> wind and the lunar magnetic anomalies. MAG/ER on Lunar Prospector found heating of the <span class="hlt">solar</span> wind electrons presumably due to the interaction between the <span class="hlt">solar</span> wind and the lunar magnetic anomalies and the existence of the mini-magnetosphere was suggested. However, the detailed mechanism of the interaction has been unclear mainly due to the lack of the in-situ <span class="hlt">observed</span> data of low energy ions. MAgnetic field and Plasma experiment - Plasma energy Angle and Composition Experiment (MAP-PACE) on Kaguya (SELENE) completed its ˜1.5-year <span class="hlt">observation</span> of the low energy charged particles around the Moon on 10 June, 2009. Kaguya was launched on 14 September 2007 by H2A launch vehicle from Tanegashima Space Center in Japan. Kaguya was inserted into a circular lunar polar orbit of 100km altitude and continued <span class="hlt">observation</span> for nearly 1.5 years till it impacted the Moon on 10 June 2009. During the last 5 months, the orbit was lowered to ˜50km-altitude between January 2009 and April 2009, and some orbits had further lower perilune altitude of ˜10km after April 2009. MAP-PACE consisted of 4 sensors: ESA (Electron Spectrum Analyzer)-S1, ESA-S2, IMA (Ion Mass Analyzer), and IEA (Ion Energy Analyzer). All the sensors performed quite well as expected from the laboratory experiment carried out before launch. Since each sensor had hemispherical field of view, two electron sensors and two ion sensors that were installed on the spacecraft panels opposite to each other could cover full 3-dimensional phase space of low energy electrons and ions. One of the ion sensors IMA was</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19880002239','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19880002239"><span>Large-scale horizontal flows from SOUP <span class="hlt">observations</span> of <span class="hlt">solar</span> granulation</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>November, L. J.; Simon, G. W.; Tarbell, T. D.; Title, A. M.; Ferguson, S. H.</p> <p>1987-01-01</p> <p>Using high resolution time sequence photographs of <span class="hlt">solar</span> granulation from the SOUP experiment on Spacelab 2, large scale horizontal flows were <span class="hlt">observed</span> in the <span class="hlt">solar</span> surface. The measurement method is based upon a local spatial cross correlation analysis. The horizontal motions have amplitudes in the range 300 to 1000 m/s. Radial outflow of granulation from a sunspot penumbra into surrounding photosphere is a striking new discovery. Both the supergranulation pattern and cellular structures having the scale of mesogranulation are seen. The vertical flows that are inferred by continuity of mass from these <span class="hlt">observed</span> horizontal flows have larger upflow amplitudes in cell centers than downflow amplitudes at cell boundaries.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1987NASCP2483..121N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1987NASCP2483..121N"><span>Large-scale horizontal flows from SOUP <span class="hlt">observations</span> of <span class="hlt">solar</span> granulation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>November, L. J.; Simon, G. W.; Tarbell, T. D.; Title, A. M.; Ferguson, S. H.</p> <p>1987-09-01</p> <p>Using high-resolution time-sequence photographs of <span class="hlt">solar</span> granulation from the SOUP experiment on Spacelab 2 the authors <span class="hlt">observed</span> large-scale horizontal flows in the <span class="hlt">solar</span> surface. The measurement method is based upon a local spatial cross correlation analysis. The horizontal motions have amplitudes in the range 300 to 1000 m/s. Radial outflow of granulation from a sunspot penumbra into the surrounding photosphere is a striking new discovery. Both the supergranulation pattern and cellular structures having the scale of mesogranulation are seen. The vertical flows that are inferred by continuity of mass from these <span class="hlt">observed</span> horizontal flows have larger upflow amplitudes in cell centers than downflow amplitudes at cell boundaries.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19930004279','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19930004279"><span><span class="hlt">Observations</span> of <span class="hlt">solar</span> wind ion charge exchange in the comet Halley coma</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Fuselier, S. A.; Shelley, E. G.; Goldstein, B. E.; Goldstein, R.; Neugebauer, M.; Ip, W.-H.; Balsiger, H.; Reme, H.</p> <p>1991-01-01</p> <p>Giotto Ion Mass Spectrometer/High Energy Range Spectrometer (IMS/HERS) <span class="hlt">observations</span> of <span class="hlt">solar</span> wind ions show charge exchange effects and <span class="hlt">solar</span> wind compositional changes in the coma of comet Halley. As the comet was approached, the He(++) to proton density ratio increased until about 1 hour before closest approach after which time it decreased. Abrupt increases in this ratio were also <span class="hlt">observed</span> in the beginning and near the end of the so-called Mystery Region (8.6 - 5.5(10)(exp 5) km from the comet along the spacecraft trajectory). These abrupt increases in the density ratio were well correlated with enhanced fluxes of keV electrons as measured by the Giotto plasma electron spectrometer. The general increase and then decrease of the He(++) to proton density ratio is quantitatively consistent with a combination of the addition of protons of cometary origin to the plasma and loss of plasma through charge exchange of protons and He(++). In general agreement with the <span class="hlt">solar</span> wind proton and He(++) <span class="hlt">observations</span>, <span class="hlt">solar</span> wind oxygen and carbon ions were <span class="hlt">observed</span> to charge exchange from higher to lower charge states with decreasing distance to the comet. The more abrupt increases in the He(++) to proton and the He(++) to O(6+) density ratios in the mystery region require a change in the <span class="hlt">solar</span> wind ion composition in this region while the correlation with energetic electrons indicates processes associated with the comet.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018AdSpR..61.2531K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018AdSpR..61.2531K"><span><span class="hlt">Observation</span> of a 27-day <span class="hlt">solar</span> signature in noctilucent cloud altitude</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Köhnke, Merlin C.; von Savigny, Christian; Robert, Charles E.</p> <p>2018-05-01</p> <p>Previous studies have identified <span class="hlt">solar</span> 27-day signatures in several parameters in the Mesosphere/Lower thermosphere region, including temperature and Noctilucent cloud (NLC) occurrence frequency. In this study we report on a <span class="hlt">solar</span> 27-day signature in NLC altitude with peak-to-peak variations of about 400 m. We use SCIAMACHY limb-scatter <span class="hlt">observations</span> from 2002 to 2012 to detect NLCs. The superposed epoch analysis method is applied to extract <span class="hlt">solar</span> 27-day signatures. A 27-day signature in NLC altitude can be identified in both hemispheres in the SCIAMACHY dataset, but the signature is more pronounced in the northern hemisphere. The <span class="hlt">solar</span> signature in NLC altitude is found to be in phase with <span class="hlt">solar</span> activity and temperature for latitudes ≳ 70 ° N. We provide a qualitative explanation for the positive correlation between <span class="hlt">solar</span> activity and NLC altitude based on published model simulations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2002EGSGA..27.1460L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2002EGSGA..27.1460L"><span><span class="hlt">Observed</span> Reduction In Surface <span class="hlt">Solar</span> Radiation - Aerosol Forcing Versus Cloud Feedback?</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Liepert, B.</p> <p></p> <p>The <span class="hlt">solar</span> radiation reaching the ground is a key parameter for the climate system. It drives the hydrological cycle and numerous biological processes. Surface <span class="hlt">solar</span> radi- ation revealed an estimated 7W/m2 or 4% decline at sites worldwide from 1961 to 1990. The strongest decline occurred at the United States sites with 19W/m2 or 10%. Increasing air pollution and hence direct and indirect aerosol effect, as we know today can only explain part of the reduction in <span class="hlt">solar</span> radiation. Increasing cloud optical thick- ness - possibly due to global warming - is a more likely explanation for the <span class="hlt">observed</span> reduction in <span class="hlt">solar</span> radiation in the United States. The analysis of surface <span class="hlt">solar</span> radiation data will be shown and compared with GCM results of the direct and indirect aerosol effect. It will be argued that the residual declines in surface <span class="hlt">solar</span> radiation is likely due to cloud feedback.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018ApJ...859..121K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018ApJ...859..121K"><span>Motions in Prominence Barbs <span class="hlt">Observed</span> on the <span class="hlt">Solar</span> Limb</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kucera, T. A.; Ofman, L.; Tarbell, T. D.</p> <p>2018-06-01</p> <p>We analyze and discuss an example of prominence barbs <span class="hlt">observed</span> on the limb on 2016 January 7 by the Hinode/<span class="hlt">Solar</span> Optical Telescope in Ca II and Hα, the Interface Region Imaging Spectrograph, with slit jaw images and Mg II spectral data, and the <span class="hlt">Solar</span> Dynamics Observatory’s Atmospheric Imaging Assembly. In the recent literature there has been a debate concerning whether these features, sometimes referred to as “tornadoes,” are rotating. Our data analysis provides no evidence for systematic rotation in the barbs. We do find line-of-sight motions in the barbs that vary with location and time. We also discuss <span class="hlt">observations</span> of features moving along the barbs. These moving features are elongated parallel to the <span class="hlt">solar</span> limb and tend to come in clusters of features moving along the same or similar paths in the plane of the sky during a period of 10 minutes to an hour, moving toward or away from the limb. The motion may have a component along the line of sight as well. The spectral data indicate that the features are Doppler shifted. We discuss possible explanations for these features.</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://hdl.handle.net/2060/20100040500','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20100040500"><span><span class="hlt">Solar</span> Spicules Near and at the Limb, <span class="hlt">Observed</span> from Hinode</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Sterling, A. C.; Moore, R. L.</p> <p>2010-01-01</p> <p><span class="hlt">Solar</span> spicules appear as narrow jets emanating from the chromosphere and extending into the corona. They have been <span class="hlt">observed</span> for over a hundred years, mainly in chromospheric spectral lines such as H-alpha. Because they are at the limit of visibility of ground-based instruments, their nature has long been a puzzle. In recent years however, vast progress has been made in understanding them both theoretically and <span class="hlt">observationally</span>, as spicule studies have undergone a revolution because of the superior resolution and time cadence of ground-based and space-based instruments. Even more rapid progress is currently underway, due to the <span class="hlt">Solar</span> Optical Telescope (SOT) instrument on the Hinode spacecraft. Here we present <span class="hlt">observations</span> of spicules from Hinode SOT, as seen near the limb with the Ca II filtergraph.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUFMSH33A2036C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUFMSH33A2036C"><span>New <span class="hlt">Observations</span> of Soft X-ray (0.5-5 keV) <span class="hlt">Solar</span> Spectra</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Caspi, A.; Woods, T. N.; Mason, J. P.; Jones, A. R.; Warren, H. P.</p> <p>2013-12-01</p> <p>The <span class="hlt">solar</span> corona is the brightest source of X-rays in the <span class="hlt">solar</span> system, and the X-ray emission is highly variable on many time scales. However, the actual <span class="hlt">solar</span> soft X-ray (SXR) (0.5-5 keV) spectrum is not well known, particularly during <span class="hlt">solar</span> quiet periods, as, with few exceptions, this energy range has not been systematically studied in many years. Previous <span class="hlt">observations</span> include high-resolution but very narrow-band spectra from crystal spectrometers (e.g., Yohkoh/BCS), or integrated broadband irradiances from photometers (e.g., GOES/XRS, TIMED/XPS, etc.) that lack detailed spectral information. In recent years, broadband measurements with moderate energy resolution (~0.5-0.7 keV FWHM) were made by SphinX on CORONAS-Photon and SAX on MESSENGER, although they did not extend to energies below ~1 keV. We present <span class="hlt">observations</span> of <span class="hlt">solar</span> SXR emission obtained using new instrumentation flown on recent SDO/EVE calibration rocket underflights. The photon-counting spectrometer, a commercial Amptek X123 with a silicon drift detector and an 8 μm Be window, measures the <span class="hlt">solar</span> disk-integrated SXR emission from ~0.5 to >10 keV with ~0.15 keV FWHM resolution and 1 s cadence. A novel imager, a pinhole X-ray camera using a cooled frame-transfer CCD (15 μm pixel pitch), Ti/Al/C filter, and 5000 line/mm Au transmission grating, images the full Sun in multiple spectral orders from ~0.1 to ~5 nm with ~10 arcsec/pixel and ~0.01 nm/pixel spatial and spectral detector scales, respectively, and 10 s cadence. These instruments are prototypes for future CubeSat missions currently being developed. We present new results of <span class="hlt">solar</span> <span class="hlt">observations</span> on 04 October 2013 (NASA sounding rocket 36.290). We compare with previous results from 23 June 2012 (NASA sounding rocket 36.286), during which <span class="hlt">solar</span> activity was low and no signal was <span class="hlt">observed</span> above ~4 keV. We compare our spectral and imaging measurements with spectra and broadband irradiances from other instruments, including SDO/EVE, GOES/XRS, TIMED</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1998IAUS..185..453N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1998IAUS..185..453N"><span>MHD oscillations <span class="hlt">observed</span> in the <span class="hlt">solar</span> photosphere with the Michelson Doppler Imager</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Norton, A.; Ulrich, R. K.; Bogart, R. S.; Bush, R. I.; Hoeksema, J. T.</p> <p></p> <p>Magnetohydrodynamic oscillations are <span class="hlt">observed</span> in the <span class="hlt">solar</span> photosphere with the Michelson Doppler Imager (MDI). Images of <span class="hlt">solar</span> surface velocity and magnetic field strength with 4'' spatial resolution and a 60 second temporal resolution are analyzed. A two dimensional gaussian aperture with a FWHM of 10'' is applied to the data in regions of sunspot, plage and quiet sun and the resulting averaged signal is returned each minute. Significant power is <span class="hlt">observed</span> in the magnetic field oscillations with periods of five minutes. The effect of misregistration between MDI's left circularly polarized (LCP) and right circularly polarized (RCP) images has been investigated and is found not to be the cause of the <span class="hlt">observed</span> magnetic oscillations. It is assumed that the large amplitude acoustic waves with 5 minute periods are the driving mechanism behind the magnetic oscillations. The nature of the magnetohydrodynamic oscillations are characterized by their phase relations with simultaneously <span class="hlt">observed</span> <span class="hlt">solar</span> surface velocity oscillations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22679862-clasp-sj-observations-rapid-time-variations-ly-emission-solar-active-region','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22679862-clasp-sj-observations-rapid-time-variations-ly-emission-solar-active-region"><span>CLASP/SJ <span class="hlt">Observations</span> of Rapid Time Variations in the Ly α Emission in a <span class="hlt">Solar</span> Active Region</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>Ishikawa, Shin-nosuke; Kubo, Masahito; Katsukawa, Yukio</p> <p></p> <p>The Chromospheric Ly α SpectroPolarimeter (CLASP) is a sounding rocket experiment launched on 2015 September 3 to investigate the <span class="hlt">solar</span> chromosphere and transition region. The slit-jaw (SJ) optical system <span class="hlt">captured</span> Ly α images with a high time cadence of 0.6 s. From the CLASP/SJ <span class="hlt">observations</span>, many variations in the <span class="hlt">solar</span> chromosphere and transition region emission with a timescale of <1 minute were discovered. In this paper, we focus on the active region within the SJ field of view and investigate the relationship between short (<30 s) temporal variations in the Ly α emission and the coronal structures <span class="hlt">observed</span> by Solarmore » Dynamics Observatory/Atmospheric Imaging Assembly (AIA). We compare the Ly α temporal variations at the coronal loop footpoints <span class="hlt">observed</span> in the AIA 211 Å (≈2 MK) and AIA 171 Å (≈0.6 MK) channels with those in the regions with bright Ly α features without a clear association with the coronal loop footpoints. We find more short (<30 s) temporal variations in the Ly α intensity in the footpoint regions. Those variations did not depend on the temperature of the coronal loops. Therefore, the temporal variations in the Ly α intensity at this timescale range could be related to the heating of the coronal structures up to temperatures around the sensitivity peak of 171 Å. No signature was found to support the scenario that these Ly α intensity variations were related to the nanoflares. Waves or jets from the lower layers (lower chromosphere or photosphere) are possible causes for this phenomenon.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017SPIE10235E..0BV','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017SPIE10235E..0BV"><span>Joint <span class="hlt">observations</span> of <span class="hlt">solar</span> corona in space projects ARKA and KORTES</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Vishnyakov, Eugene A.; Bogachev, Sergey A.; Kirichenko, Alexey S.; Reva, Anton A.; Loboda, Ivan P.; Malyshev, Ilya V.; Ulyanov, Artem S.; Dyatkov, Sergey Yu.; Erkhova, Nataliya F.; Pertsov, Andrei A.; Kuzin, Sergey V.</p> <p>2017-05-01</p> <p>ARKA and KORTES are two upcoming <span class="hlt">solar</span> space missions in extreme ultraviolet and X-ray wavebands. KORTES is a sun-oriented mission designed for the Russian segment of International Space Station. KORTES consists of several imaging and spectroscopic instruments that will <span class="hlt">observe</span> the <span class="hlt">solar</span> corona in a number of wavebands, covering EUV and X-ray ranges. The surveillance strategy of KORTES is to cover a wide range of <span class="hlt">observations</span> including simultaneous imaging, spectroscopic and polarization measurements. ARKA is a small satellite <span class="hlt">solar</span> mission intended to take highresolution images of the Sun at the extreme ultraviolet wavelengths. ARKA will be equipped with two high-resolution EUV telescopes designed to collect images of the Sun with approximately 150 km spatial resolution in the field of view of about 10'×10'. The scientific results of the mission may have a significant impact on the theory of coronal heating and may help to clarify the physics of small-scale <span class="hlt">solar</span> structures and phenomena including oscillations of fine coronal structures and the physics of micro- and nanoflares.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.P11D..08D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.P11D..08D"><span>Effects of <span class="hlt">Solar</span> Irradiance on Ion Fluxes at Mars. MARS EXPRESS and MAVEN <span class="hlt">Observations</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Dubinin, E.; Fraenz, M.; McFadden, J. P.; Eparvier, F. G.; Brain, D. A.; Jakosky, B. M.; Andrews, D. J.; Barbash, S.</p> <p>2016-12-01</p> <p>Recent <span class="hlt">observations</span> by Mars Express and MAVEN spacecraft have shown that the Martian atmosphere/ionosphere is exposed to the impact of <span class="hlt">solar</span> wind which results in losses of volatiles from Mars. This erosion is an important factor for the evolution of the Martian atmosphere and its water inventory. To estimate the escape forced by the <span class="hlt">solar</span> wind during the early <span class="hlt">Solar</span> system conditions we need to know how the ionosphere of Mars and escape fluxes depend on variations in the strength of the external drivers, in particularly, of <span class="hlt">solar</span> wind and <span class="hlt">solar</span> EUV flux. We present multi-instrument <span class="hlt">observations</span> of the influence of the <span class="hlt">solar</span> irradiance on the Martian ionosphere and escape fluxes. We use data obtained by the ASPERA-3 and MARSIS experiments on Mars Express and by the STATIC instrument and EUV monitor on MAVEN. <span class="hlt">Observations</span> by Mars Express supplemented by the EUV monitoring at Earth orbit and translated to Mars orbit provide us information about this dependence over more than 10 years whereas the measurements made by MAVEN provide us for the first time the opportunity to study these processes with simultaneous monitoring of the ionospheric variations, planetary ion fluxes and <span class="hlt">solar</span> irradiance. We can show that fluxes of planetary ions through different escape channels (trans-terminator fluxes, ion plume, plasma sheet) respond differently on the EUV variations. The most significant effect on the ion scavenging with increase of the <span class="hlt">solar</span> irradiance is <span class="hlt">observed</span> for low energy ions extracted from the ionosphere while the ion fluxes in the plume are almost insensitive to the EUV variations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19900049938&hterms=SMM&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3DSMM','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19900049938&hterms=SMM&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3DSMM"><span><span class="hlt">Solar</span> wind and coronal structure near sunspot minimum - Pioneer and SMM <span class="hlt">observations</span> from 1985-1987</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Mihalov, J. D.; Barnes, A.; Hundhausen, A. J.; Smith, E. J.</p> <p>1990-01-01</p> <p>Changes in <span class="hlt">solar</span> wind speed and magnetic polarity <span class="hlt">observed</span> at the Pioneer spacecraft are discussed here in terms of the changing magnetic geometry implied by SMM coronagraph <span class="hlt">observations</span> over the period 1985-1987. The pattern of recurrent <span class="hlt">solar</span> wind streams, the long-term average speed, and the sector polarity of the interplanetary magnetic field all changed in a manner suggesting both a temporal variation, and a changing dependence on heliographic latitude. Coronal <span class="hlt">observations</span> during this epoch show a systematic variation in coronal structure and the magnetic structure imposed on the expanding <span class="hlt">solar</span> wind. These <span class="hlt">observations</span> suggest interpretation of the <span class="hlt">solar</span> wind speed variations in terms of the familiar model where the speed increases with distance from a nearly flat interplanetary current sheet, and where this current sheet becomes aligned with the <span class="hlt">solar</span> equatorial plane as sunspot minimum approaches, but deviates rapidly from that orientation after minimum.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMSM11B2312S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMSM11B2312S"><span>Vortex, ULF wave and Aurora <span class="hlt">Observation</span> after <span class="hlt">Solar</span> Wind Dynamic Pressure Change</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Shi, Q.</p> <p>2017-12-01</p> <p>Here we will summarize our recent study and show some new results on the Magnetosphere and Ionosphere Response to Dynamic Pressure Change/disturbances in the <span class="hlt">Solar</span> Wind and foreshock regions. We study the step function type <span class="hlt">solar</span> wind dynamic pressure change (increase/decrease) interaction with the magnetosphere using THEMIS satellites at both dayside and nightside in different geocentric distances. Vortices generated by the dynamic pressure change passing along the magnetopause are found and compared with model predictions. ULF waves and vortices are excited in the dayside and nightside plasma sheet when dynamic pressure change hit the magnetotail. The related ionospheric responses, such as aurora and TCVs, are also investigated. We compare Global MHD simulations with the <span class="hlt">observations</span>. We will also show some new results that dayside magnetospheric FLRs might be caused by foreshock structures.Shi, Q. Q. et al. (2013), THEMIS <span class="hlt">observations</span> of ULF wave excitation in the nightside plasma sheet during sudden impulse events, J. Geophys. Res. Space Physics, 118, doi:10.1029/2012JA017984. Shi, Q. Q. et al. (2014), <span class="hlt">Solar</span> wind pressure pulse-driven magnetospheric vortices and their global consequences, J. Geophys. Res. Space Physics, 119, doi:10.1002/2013JA019551. Tian, A.M. et al.(2016), Dayside magnetospheric and ionospheric responses to <span class="hlt">solar</span> wind pressure increase: Multispacecraft and ground <span class="hlt">observations</span>, J. Geophys. Res., 121, doi:10.1002/2016JA022459. Shen, X.C. et al.(2015), Magnetospheric ULF waves with increasing amplitude related to <span class="hlt">solar</span> wind dynamic pressure changes: THEMIS <span class="hlt">observations</span>, J. Geophys. Res., 120, doi:10.1002/2014JA020913Zhao, H. Y. et al. (2016), Magnetospheric vortices and their global effect after a <span class="hlt">solar</span> wind dynamic pressure decrease, J. Geophys. Res. Space Physics, 121, doi:10.1002/2015JA021646. Shen, X. C., et al. (2017), Dayside magnetospheric ULF wave frequency modulated by a <span class="hlt">solar</span> wind dynamic pressure negative impulse, J. Geophys. Res</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014cosp...40E1451K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014cosp...40E1451K"><span>Common <span class="hlt">observations</span> of <span class="hlt">solar</span> X-rays from SPHINX/CORONAS-PHOTON and XRS/MESSENGER</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kepa, Anna; Sylwester, Janusz; Sylwester, Barbara; Siarkowski, Marek; Mrozek, Tomasz; Gryciuk, Magdalena; Phillips, Kenneth</p> <p></p> <p>SphinX was a soft X-ray spectrophotometer constructed in the Space Research Centre of Polish Academy of Sciences. The instrument was launched on 30 January 2009 aboard CORONAS-PHOTON satellite as a part of TESIS instrument package. SphinX measured total <span class="hlt">solar</span> X-ray flux in the energy range from 1 to 15 keV during the period of very low <span class="hlt">solar</span> activity from 20 February to 29 November 2009. For these times the <span class="hlt">solar</span> detector (X-ray Spectrometer - XRS) onboard MESSENGER also <span class="hlt">observed</span> the <span class="hlt">solar</span> X-rays from a different vantage point. XRS measured the radiation in similar energy range. We present results of the comparison of <span class="hlt">observations</span> from both instruments and show the preliminary results of physical analysis of spectra for selected flares.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19790041801&hterms=wind+monitor&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Dwind%2Bmonitor','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19790041801&hterms=wind+monitor&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Dwind%2Bmonitor"><span>Signatures of <span class="hlt">solar</span> wind latitudinal structure in interplanetary Lyman-alpha emissions - Mariner 10 <span class="hlt">observations</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kumar, S.; Broadfoot, A. L.</p> <p>1979-01-01</p> <p>A detailed analysis is conducted which shows that signatures in the interplanetary Lyman-alpha emissions <span class="hlt">observed</span> in three different data sets from Mariner 10 (corresponding to different locations of the spacecraft) provide firm evidence that the intensity departures are correlated with a decrease in <span class="hlt">solar</span> wind flux with increasing latitude. It is suggested that <span class="hlt">observations</span> of the interplanetary emission can be used to monitor average <span class="hlt">solar</span> wind activity at high latitudes. The asymmetry in the <span class="hlt">solar</span> radiation field as a source of <span class="hlt">observed</span> departures in L-alpha data is considered and attention is given to the interstellar hydrogen and helium density.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22086330-ace-swics-observations-heavy-ion-dropouts-within-solar-wind','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22086330-ace-swics-observations-heavy-ion-dropouts-within-solar-wind"><span>ACE/SWICS <span class="hlt">OBSERVATIONS</span> OF HEAVY ION DROPOUTS WITHIN THE <span class="hlt">SOLAR</span> WIND</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>Weberg, Micah J.; Zurbuchen, Thomas H.; Lepri, Susan T., E-mail: mjweberg@umich.edu, E-mail: thomasz@umich.edu, E-mail: slepri@umich.edu</p> <p>2012-11-20</p> <p>We present the first in situ <span class="hlt">observations</span> of heavy ion dropouts within the slow <span class="hlt">solar</span> wind, <span class="hlt">observed</span> for select elements ranging from helium to iron. For iron, these dropouts manifest themselves as depletions of the Fe/H ratio by factors up to {approx}25. The events often exhibit mass-dependent fractionation and are contained in slow, unsteady wind found within a few days from known stream interfaces. We propose that such dropouts are evidence of gravitational settling within large coronal loops, which later undergo interchange reconnection and become source regions of slow, unsteady wind. Previously, spectroscopic studies by Raymond et al. in 1997more » (and later Feldman et al. in 1999) have yielded strong evidence for gravitational settling within these loops. However, their expected in situ signature plasma with heavy elements fractionated by mass was not <span class="hlt">observed</span> prior to this study. Using data from the SWICS instrument on board the Advanced Composition Explorer (ACE), we investigate the composition of the <span class="hlt">solar</span> wind within these dropouts and explore long term trends over most of a <span class="hlt">solar</span> cycle.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19760038407&hterms=Extinction+threshold&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3DExtinction%2Bthreshold','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19760038407&hterms=Extinction+threshold&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3DExtinction%2Bthreshold"><span>The <span class="hlt">solar</span>-flare infrared continuum - <span class="hlt">Observational</span> techniques and upper limits</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Hudson, H. S.</p> <p>1975-01-01</p> <p>Exploratory <span class="hlt">observations</span> at 20 microns and 350 microns have determined detection thresholds for <span class="hlt">solar</span> flares in these wavelengths. In the 20-micron range, <span class="hlt">solar</span> atmospheric fluctuations (the 'temperature field') set the basic limits on flare detectability at about 5 K; at 350 microns, extinction in the earth's atmosphere provides the basic limitation of about 30 K. These thresholds are low enough for the successful detection of several infrared-emitting components of large flares. The upper limits obtained for subflares indicate that the thickness of the H-alpha flare region does not exceed approximately 10 km. This result confirms the conclusion of Suemoto and Hiei (1959) regarding the small effective thickness of the H-alpha-emitting regions in <span class="hlt">solar</span> flares.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22654390-observations-reconnection-flows-flare-solar-disk','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22654390-observations-reconnection-flows-flare-solar-disk"><span><span class="hlt">Observations</span> of Reconnection Flows in a Flare on the <span class="hlt">Solar</span> Disk</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, Juntao; Simões, P. J. A.; Jeffrey, N. L. S.</p> <p></p> <p>Magnetic reconnection is a well-accepted part of the theory of <span class="hlt">solar</span> eruptive events, though the evidence is still circumstantial. Intrinsic to the reconnection picture of a <span class="hlt">solar</span> eruptive event, particularly in the standard model for two-ribbon flares (CSHKP model), are an advective flow of magnetized plasma into the reconnection region, expansion of field above the reconnection region as a flux rope erupts, retraction of heated post-reconnection loops, and downflows of cooling plasma along those loops. We report on a unique set of <span class="hlt">Solar</span> Dynamics Observatory /Atmospheric Imaging Assembly imaging and Hinode /EUV Imaging Spectrometer spectroscopic <span class="hlt">observations</span> of the disk flaremore » SOL2016-03-23T03:54 in which all four flows are present simultaneously. This includes spectroscopic evidence for a plasma upflow in association with large-scale expanding closed inflow field. The reconnection inflows are symmetric, and consistent with fast reconnection, and the post-reconnection loops show a clear cooling and deceleration as they retract. <span class="hlt">Observations</span> of coronal reconnection flows are still rare, and most events are <span class="hlt">observed</span> at the <span class="hlt">solar</span> limb, obscured by complex foregrounds, making their relationship to the flare ribbons, cusp field, and arcades formed in the lower atmosphere difficult to interpret. The disk location and favorable perspective of this event have removed these ambiguities giving a clear picture of the reconnection dynamics.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015Ap%26SS.358...25G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015Ap%26SS.358...25G"><span>Improved SOT (Hinode mission) high resolution <span class="hlt">solar</span> imaging <span class="hlt">observations</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Goodarzi, H.; Koutchmy, S.; Adjabshirizadeh, A.</p> <p>2015-08-01</p> <p>We consider the best today available <span class="hlt">observations</span> of the Sun free of turbulent Earth atmospheric effects, taken with the <span class="hlt">Solar</span> Optical Telescope (SOT) onboard the Hinode spacecraft. Both the instrumental smearing and the <span class="hlt">observed</span> stray light are analyzed in order to improve the resolution. The Point Spread Function (PSF) corresponding to the blue continuum Broadband Filter Imager (BFI) near 450 nm is deduced by analyzing (i) the limb of the Sun and (ii) images taken during the transit of the planet Venus in 2012. A combination of Gaussian and Lorentzian functions is selected to construct a PSF in order to remove both smearing due to the instrumental diffraction effects (PSF core) and the large-angle stray light due to the spiders and central obscuration (wings of the PSF) that are responsible for the parasitic stray light. A Max-likelihood deconvolution procedure based on an optimum number of iterations is discussed. It is applied to several <span class="hlt">solar</span> field images, including the granulation near the limb. The normal non-magnetic granulation is compared to the abnormal granulation which we call magnetic. A new feature appearing for the first time at the extreme- limb of the disk (the last 100 km) is discussed in the context of the definition of the <span class="hlt">solar</span> edge and of the <span class="hlt">solar</span> diameter. A single sunspot is considered in order to illustrate how effectively the restoration works on the sunspot core. A set of 125 consecutive deconvolved images is assembled in a 45 min long movie illustrating the complexity of the dynamical behavior inside and around the sunspot.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.P51C2600L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.P51C2600L"><span>Analysis of <span class="hlt">Solar</span> Wind Precipitation on Mars Using MAVEN/SWIA <span class="hlt">Observations</span> of Spacecraft-Scattered Ions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lue, C.; Halekas, J. S.</p> <p>2017-12-01</p> <p>Particle sensors on the MAVEN spacecraft (SWIA, SWEA, STATIC) <span class="hlt">observe</span> precipitating <span class="hlt">solar</span> wind ions during MAVEN's periapsis passes in the Martian atmosphere (at 120-250 km altitude). The signature is <span class="hlt">observed</span> as positive and negative particles at the <span class="hlt">solar</span> wind energy, traveling away from the Sun. The <span class="hlt">observations</span> can be explained by the <span class="hlt">solar</span> wind penetrating the Martian magnetic barrier in the form of energetic neutral atoms (ENAs) due to charge-exchange with the Martian hydrogen corona, and then being reionized in positive or negative form upon impact with the atmosphere (1). These findings have elucidated <span class="hlt">solar</span> wind precipitation dynamics at Mars, and can also be used to monitor the <span class="hlt">solar</span> wind even when MAVEN is at periapsis (2). In the present study, we focus on a SWIA instrument background signal that has been interpreted as spacecraft/instrument-scattered ions (2). We aim to model and subtract the scattered ion signal from the <span class="hlt">observations</span> including those of reionized <span class="hlt">solar</span> wind. We also aim to use the scattered ion signal to track hydrogen ENAs impacting the spacecraft above the reionization altitude. We characterize the energy spectrum and directional scattering function for <span class="hlt">solar</span> wind scattering off the SWIA aperture structure, the radome and the spacecraft body. We find a broad scattered-ion energy spectrum up to the <span class="hlt">solar</span> wind energy, displaying increased energy loss and reduced flux with increasing scattering angle, allowing correlations with the <span class="hlt">solar</span> wind direction, energy, and flux. We develop models that can be used to predict the scattered signal based on the direct <span class="hlt">solar</span> wind <span class="hlt">observations</span> or to infer the <span class="hlt">solar</span> wind properties based on the <span class="hlt">observed</span> scattered signal. We then investigate deviations to the models when the spacecraft is in the Martian atmosphere and evaluate the plausibility of that these are caused by ENAs. We also perform SIMION modeling of the scattering process and the resulting signal detection by SWIA, to study the results from</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017eaa..book..771O','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017eaa..book..771O"><span>British <span class="hlt">Observations</span> of the 18 August 1868 Total <span class="hlt">Solar</span> Eclipse from Guntoor, India</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Orchiston, Wayne; Lee, Eun-Hee; Ahn, Young-Sook</p> <p></p> <p>The total <span class="hlt">solar</span> eclipse of 18 August 1868 was <span class="hlt">observed</span> in Aden, India, Siam (present-day Thailand) and the Dutch East Indies (present-day Indonesia). One Indian expedition was sponsored by the Royal Astronomical Society, and led by Major J.F. Tennant. In this chapter we describe the <span class="hlt">observing</span> team and instruments, discuss their <span class="hlt">observations</span>, and conclude with some remarks on the place of the 1868 eclipse in <span class="hlt">solar</span> studies and later nineteenth century European astronomical expeditions to India.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012AAS...22052112M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012AAS...22052112M"><span><span class="hlt">Solar</span> Hard X-ray <span class="hlt">Observations</span> with NuSTAR</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Marsh, Andrew; Smith, D. M.; Krucker, S.; Hudson, H. S.; Hurford, G. J.; White, S. M.; Mewaldt, R. A.; Harrison, F. A.; Grefenstette, B. W.; Stern, D.</p> <p>2012-05-01</p> <p>High-sensitivity imaging of coronal hard X-rays allows detection of freshly accelerated nonthermal electrons at the acceleration site. A few such <span class="hlt">observations</span> have been made with Yohkoh and RHESSI, but a leap in sensitivity could help pin down the time, place, and manner of reconnection. Around the time of this meeting, the Nuclear Spectroscopic Telescope ARray (NuSTAR), a NASA Small Explorer for high energy astrophysics that uses grazing-incidence optics to focus X-rays up to 80 keV, will be launched. Three weeks will be dedicated to <span class="hlt">solar</span> <span class="hlt">observing</span> during the baseline two-year mission. NuSTAR will be 200 times more sensitive than RHESSI in the hard X-ray band. This will allow the following new <span class="hlt">observations</span>, among others: 1) Extrapolation of the micro/nanoflare distribution by two orders of magnitude down in flux; 2) Search for hard X-rays from network nanoflares (soft X-ray bright points) and evaluation of their role in coronal heating; 3) Discovery of hard X-ray bremsstrahlung from the electron beams driving type III radio bursts, and measurement of their electron spectrum; 4) Hard X-ray studies of polar soft X-ray jets and impulsive <span class="hlt">solar</span> energetic particle events at the edge of coronal holes; 5) Study of coronal bremsstrahlung from particles accelerated by coronal mass ejections as they are first launched; 6) Study of particles at the coronal reconnection site when flare footpoints and loops are occulted; 7) Search for weak high-temperature coronal plasmas in active regions that are not flaring; and 8) Search for hypothetical axion particles created in the <span class="hlt">solar</span> core via the hard X-ray signal from their conversion to X-rays in the coronal magnetic field. NuSTAR will also serve as a pathfinder for a future dedicated space mission with enhanced capabilities, such as a satellite version of the FOXSI sounding rocket.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19840013920','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19840013920"><span><span class="hlt">Observations</span> of <span class="hlt">solar</span>-cell metallization corrosion</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Mon, G. R.</p> <p>1983-01-01</p> <p>The Engineering Sciences Area of the Jet Propulsion Laboratory (JPL) Flat-Plate <span class="hlt">Solar</span> Array Project is performing long term environmental tests on photovoltaic modules at Wyle Laboratories in Huntsville, Alabama. Some modules have been exposed to 85 C/85% RH and 40 C/93% RH for up to 280 days. Other modules undergoing temperature-only exposures ( 3% RH) at 85 C and 100 C have been tested for more than 180 days. At least two modules of each design type are exposed to each environment - one with, and the other without a 100-mA forward bias. Degradation is both visually <span class="hlt">observed</span> and electrically monitored. Visual <span class="hlt">observations</span> of changes in appearance are recorded at each inspection time. Significant visual <span class="hlt">observations</span> relating to metallization corrosion (and/or metallization-induced corrosion) include discoloration (yellowing and browning) of grid lines, migration of grid line material into the encapsulation (blossoming), the appearance of rainbow-like diffraction patterns on the grid lines, and brown spots on collectors and grid lines. All of these <span class="hlt">observations</span> were recorded for electrically biased modules in the 280-day tests with humidity.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20060029839&hterms=corona&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3Dcorona','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20060029839&hterms=corona&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3Dcorona"><span>Ka-band and X-band <span class="hlt">observations</span> of the <span class="hlt">solar</span> corona acquired during the Cassini 2001 superior conjunction</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Morabito, D. D.</p> <p>2002-01-01</p> <p>Simultaneous dual-frequency Ka-band (32 GHz) and X-band (8.4 GHz) carrier signal data have been acquired during the superior conjunction of the Cassini spacecraft June 2001, using the NASA Deep Space Network's facilities located in Goldstone, California. The <span class="hlt">solar</span> elongation angle of the <span class="hlt">observations</span> varied from -4.1 degrees (-16 <span class="hlt">solar</span> radii) to -0.6 degrees (-2.3 <span class="hlt">solar</span> radii). The <span class="hlt">observed</span> coronal and <span class="hlt">solar</span> effects on the signals include spectral broadening, amplitude scintillation, phase scintillation, and increased noise. The measurements were generally consistent with existing <span class="hlt">solar</span> models, except during <span class="hlt">solar</span> transient events when the signatures of the measurements were <span class="hlt">observed</span> to increase significantly above the quiet background levels. This is the second <span class="hlt">solar</span> conjunction of Cassini for which simultaneous X/Ka data were acquired. Both <span class="hlt">solar</span> conjunctions, conducted in May 2000 and June 2001, occurred near the peak of the current 11 year <span class="hlt">solar</span> cycle.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018A%26A...611A..36V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018A%26A...611A..36V"><span><span class="hlt">Solar</span>-wind predictions for the Parker <span class="hlt">Solar</span> Probe orbit. Near-Sun extrapolations derived from an empirical <span class="hlt">solar</span>-wind model based on Helios and OMNI <span class="hlt">observations</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Venzmer, M. S.; Bothmer, V.</p> <p>2018-03-01</p> <p>Context. The Parker <span class="hlt">Solar</span> Probe (PSP; formerly <span class="hlt">Solar</span> Probe Plus) mission will be humanitys first in situ exploration of the <span class="hlt">solar</span> corona with closest perihelia at 9.86 <span class="hlt">solar</span> radii (R⊙) distance to the Sun. It will help answer hitherto unresolved questions on the heating of the <span class="hlt">solar</span> corona and the source and acceleration of the <span class="hlt">solar</span> wind and <span class="hlt">solar</span> energetic particles. The scope of this study is to model the <span class="hlt">solar</span>-wind environment for PSPs unprecedented distances in its prime mission phase during the years 2018 to 2025. The study is performed within the Coronagraphic German And US <span class="hlt">Solar</span>ProbePlus Survey (CGAUSS) which is the German contribution to the PSP mission as part of the Wide-field Imager for <span class="hlt">Solar</span> PRobe. Aim. We present an empirical <span class="hlt">solar</span>-wind model for the inner heliosphere which is derived from OMNI and Helios data. The German-US space probes Helios 1 and Helios 2 flew in the 1970s and <span class="hlt">observed</span> <span class="hlt">solar</span> wind in the ecliptic within heliocentric distances of 0.29 au to 0.98 au. The OMNI database consists of multi-spacecraft intercalibrated in situ data obtained near 1 au over more than five <span class="hlt">solar</span> cycles. The international sunspot number (SSN) and its predictions are used to derive dependencies of the major <span class="hlt">solar</span>-wind parameters on <span class="hlt">solar</span> activity and to forecast their properties for the PSP mission. Methods: The frequency distributions for the <span class="hlt">solar</span>-wind key parameters, magnetic field strength, proton velocity, density, and temperature, are represented by lognormal functions. In addition, we consider the velocity distributions bi-componental shape, consisting of a slower and a faster part. Functional relations to <span class="hlt">solar</span> activity are compiled with use of the OMNI data by correlating and fitting the frequency distributions with the SSN. Further, based on the combined data set from both Helios probes, the parameters frequency distributions are fitted with respect to <span class="hlt">solar</span> distance to obtain power law dependencies. Thus an empirical <span class="hlt">solar</span>-wind model for the inner</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('http://adsabs.harvard.edu/abs/2003fuse.prop.D089D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2003fuse.prop.D089D"><span>FUSE <span class="hlt">Observations</span> of Neutron-<span class="hlt">Capture</span> Elements in Wolf-Rayet Planetary Nebulae</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Dinerstein, H.</p> <p></p> <p>We propose to obtain FUSE <span class="hlt">observations</span> of planetary nebula central stars of the WC Wolf-Rayet ([WC]) class, in order to search for the products of neutron-<span class="hlt">capture</span> processes in these stars and provide constraints on their evolutionary status. Although the origin of the [WC]'s is controversial, their H-deficient, C-rich surface compositions indicate that they have experienced a high degree of mixing and/or mass loss. Thus one might expect the nebulae they produce to show enhanced concentrations of He-burning and other nuclear products, such as nuclei produced by slow neutron <span class="hlt">capture</span> during the AGB phase. We have already detected an absorption line from one such element, Germanium (Sterling, Dinerstein, & Bowers 2002), while conducting a search for H2 absorption from nebular molecular material FUSE GI programs A085 and B069). Since the strongest Ge enhancements were found in PNe with [WC] central stars, we propose to enlarge the sample of such objects <span class="hlt">observed</span> by FUSE. THIS TEMPORARY AND PARTIAL SCRIPT COVERS ONE TARGET, HE 2-99, AND REQUESTS AN EXPOSURE TIME OF 15 KSEC. PHASE 2 INFORMATION FOR THE REMAINDER OF THE PROGRAM'S TOTAL TIME ALLOCATION OF 60 KSEC WILL BE SUBMITTED AT A LATER TIME.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015IAUGA..2236038H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015IAUGA..2236038H"><span>42 Years of Continuous <span class="hlt">Observations</span> of the <span class="hlt">Solar</span> Diameter - 1974 to 2015</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Humberto Andrei, Alexandre; Calderari Boscardin, Sergio; Lousada Penna, Jucira; Vani Leister, Nelson</p> <p>2015-08-01</p> <p>We present an analysis of 42 years of continuous measurements of the photospheric <span class="hlt">solar</span> diameter, taken at major national observatories, using the same fundamental method, and similar apparatus. Such a series overlap <span class="hlt">observations</span> from the Calern Observatory/France (<span class="hlt">Solar</span> Astrolabe in 1975-2003 to 253 obs/year lead by F. Laclare and C. Delmas; Doraysol in 2000-2005 to 3,070 obs/year lead by C. Delmas and V. Sinceac), from the IAG/USP/Brazil (<span class="hlt">Solar</span> Astrolabe in 1974-1994 to 95 obs/year lead by N. VaniLeister, P. Benevides and M. Emilio), from the Antalya Observatory/Turkey (CCD Astrolabe in 2000-2007 to 400 obs/year lead by F. Chollet and OI. Golbasi), from the San Fernando Observatory/Spain (<span class="hlt">Solar</span> Astrolabe in 1972-1975 to 133 obs/year lead by J. Muiños), from Observatório Nacional/Brasil (CCD Astrolabe in 1998-2009 to 1,820 obs/year lead by J. Penna, E. Reis Neto and A.H. Andrei; Heliometer 2010-2015 to 8,509 obs/year lead by S.C. Boscardin, J.L. Penna and A.H. Andrei). The Heliometer is fully automatized in its <span class="hlt">observations</span> and continues in regular operation with no plan of stopping; it shares with the former instruments the physical/mathematical definition of the limb, and the instruments aperture and focal length. We perform a reconciliation of all these series, using the common stretches. A modulation with the 11 years cycle of <span class="hlt">solar</span> activity is evident. However when such modulation is removed, both from the <span class="hlt">solar</span> diameter compound series and from the <span class="hlt">solar</span> activity series (given by the sunspots count), a very strong anti-correlation surfaces. This suggests a smaller diameter for the forthcoming cycles, in a behavior similar to that on the Minima of Dalton and Maunder. This study stresses the importance of keeping and make available such long, continuous, and uniform series of <span class="hlt">solar</span> diameter measurements. Maybe even the more by the controversy about its magnitude and origin. This presentation is dedicated to all the teams that developed and sustained the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20070014939&hterms=puzzle&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dpuzzle','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20070014939&hterms=puzzle&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dpuzzle"><span>Implications of RHESSI <span class="hlt">Observations</span> for <span class="hlt">Solar</span> Flare Models and Energetics</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Holman, Gordon D.</p> <p>2006-01-01</p> <p><span class="hlt">Observations</span> of <span class="hlt">solar</span> flares in X-rays and gamma-rays provide the most direct information about the hottest plasma and energetic electrons and ions accelerated in flares. The Ramaty High Energy <span class="hlt">Solar</span> Spectroscopic Imager (RHESSI) has <span class="hlt">observed</span> over 18000 <span class="hlt">solar</span> flares in X-rays and gamma-rays since its launch in February of 2002. RHESSI <span class="hlt">observes</span> the full Sun at photon energies from as low as 3 keV to as high as 17 MeV with a spectral resolution on the order of 1 keV. It also provides images in arbitrary bands within this energy range with spatial resolution as good as 3 seconds of arc. Full images are typically produced every 4 seconds, although higher time resolution is possible. This unprecedented combination of spatial, spectral, and temporal resolution, spectral range and flexibility has led to fundamental advances in our understanding of flares. I will show RHESSI and coordinated <span class="hlt">observations</span> that confirm coronal magnetic reconnection models for eruptive flares and coronal mass ejections, but also present new puzzles for these models. I will demonstrate how the analysis of RHESSI spectra has led to a better determination of the energy flux and total energy in accelerated electrons, and of the energy in the hot, thermal flare plasma. I will discuss how these energies compare with each other and with the energy contained in other flare-related phenomena such as interplanetary particles and coronal mass ejections.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3627923','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3627923"><span>Three-dimensional exploration of the <span class="hlt">solar</span> wind using <span class="hlt">observations</span> of interplanetary scintillation</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>TOKUMARU, Munetoshi</p> <p>2013-01-01</p> <p>The <span class="hlt">solar</span> wind, a supersonic plasma flow continuously emanating from the Sun, governs the space environment in a vast region extending to the boundary of the heliosphere (∼100 AU). Precise understanding of the <span class="hlt">solar</span> wind is of importance not only because it will satisfy scientific interest in an enigmatic astrophysical phenomenon, but because it has broad impacts on relevant fields. Interplanetary scintillation (IPS) of compact radio sources at meter to centimeter wavelengths serves as a useful ground-based method for investigating the <span class="hlt">solar</span> wind. IPS measurements of the <span class="hlt">solar</span> wind at a frequency of 327 MHz have been carried out regularly since the 1980s using the multi-station system of the <span class="hlt">Solar</span>-Terrestrial Environment Laboratory (STEL) of Nagoya University. This paper reviews new aspects of the <span class="hlt">solar</span> wind revealed from our IPS <span class="hlt">observations</span>. PMID:23391604</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20060050341&hterms=white+cane&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dwhite%2Bcane','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20060050341&hterms=white+cane&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dwhite%2Bcane"><span>On the Rates of Coronal Mass Ejections: Remote <span class="hlt">Solar</span> and In Situ <span class="hlt">Observations</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Riley, Pete; Schatzman, C.; Cane, H. V.; Richardson, I. G.; Gopalswamy, N.</p> <p>2006-01-01</p> <p>We compare the rates of coronal mass ejections (CMEs) as inferred from remote <span class="hlt">solar</span> <span class="hlt">observations</span> and interplanetary CMEs (ICMEs) as inferred from in situ <span class="hlt">observations</span> at both 1 AU and Ulyssses from 1996 through 2004. We also distinguish between those ICMEs that contain a magnetic cloud (MC) and those that do not. While the rates of CMEs and ICMEs track each other well at <span class="hlt">solar</span> minimum, they diverge significantly in early 1998, during the ascending phase of the <span class="hlt">solar</span> cycle, with the remote <span class="hlt">solar</span> <span class="hlt">observations</span> yielding approximately 20 times more events than are seen at 1 AU. This divergence persists through 2004. A similar divergence occurs between MCs and non-MC ICMEs. We argue that these divergences are due to the birth of midlatitude active regions, which are the sites of a distinct population of CMEs, only partially intercepted by Earth, and we present a simple geometric argument showing that the CME and ICME rates are consistent with one another. We also acknowledge contributions from (1) an increased rate of high-latitude CMEs and (2) focusing effects from the global <span class="hlt">solar</span> field. While our analysis, coupled with numerical modeling results, generally supports the interpretation that whether one <span class="hlt">observes</span> a MC within an ICME is sensitive to the trajectory of the spacecraft through the ICME (i.e., an <span class="hlt">observational</span> selection effect), one result directly contradicts it. Specifically, we find no systematic offset between the latitudinal origin of ICMEs that contain MCs at 1 AU in the ecliptic plane and that of those that do not.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19960021428&hterms=micro+wind&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dmicro%2Bwind','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19960021428&hterms=micro+wind&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dmicro%2Bwind"><span><span class="hlt">Observations</span> of micro-turbulence in the <span class="hlt">solar</span> wind near the sun with interplanetary scintillation</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Yamauchi, Y.; Misawa, H.; Kojima, M.; Mori, H.; Tanaka, T.; Takaba, H.; Kondo, T.; Tokumaru, M.; Manoharan, P. K.</p> <p>1995-01-01</p> <p>Velocity and density turbulence of <span class="hlt">solar</span> wind were inferred from interplanetary scintillation (IPS) <span class="hlt">observations</span> at 2.3 GHz and 8.5 GHz using a single-antenna. The <span class="hlt">observations</span> were made during September and October in 1992 - 1994. They covered the distance range between 5 and 76 <span class="hlt">solar</span> radii (Rs). We applied the spectrum fitting method to obtain a velocity, an axial ratio, an inner scale and a power-law spectrum index. We examined the difference of the turbulence properties near the Sun between low-speed <span class="hlt">solar</span> wind and high-speed <span class="hlt">solar</span> wind. Both of <span class="hlt">solar</span> winds showed acceleration at the distance range of 10 - 30 Rs. The radial dependence of anisotropy and spectrum index did not have significant difference between low-speed and high-speed <span class="hlt">solar</span> winds. Near the sun, the radial dependence of the inner scale showed the separation from the linear relation as reported by previous works. We found that the inner scale of high-speed <span class="hlt">solar</span> wind is larger than that of low-speed wind.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/21313770-solar-cycle-lost-early-sunspot-observations-resolve-old-mystery','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/21313770-solar-cycle-lost-early-sunspot-observations-resolve-old-mystery"><span>A <span class="hlt">SOLAR</span> CYCLE LOST IN 1793-1800: EARLY SUNSPOT <span class="hlt">OBSERVATIONS</span> RESOLVE THE OLD MYSTERY</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>Usoskin, Ilya G.; Mursula, Kalevi; Arlt, Rainer</p> <p>2009-08-01</p> <p>Because of the lack of reliable sunspot <span class="hlt">observations</span>, the quality of the sunspot number series is poor in the late 18th century, leading to the abnormally long <span class="hlt">solar</span> cycle (1784-1799) before the Dalton minimum. Using the newly recovered <span class="hlt">solar</span> drawings by the 18-19th century <span class="hlt">observers</span> Staudacher and Hamilton, we construct the <span class="hlt">solar</span> butterfly diagram, i.e., the latitudinal distribution of sunspots in the 1790s. The sudden, systematic occurrence of sunspots at high <span class="hlt">solar</span> latitudes in 1793-1796 unambiguously shows that a new cycle started in 1793, which was lost in the traditional Wolf sunspot series. This finally confirms the existence of themore » lost cycle that has been proposed earlier, thus resolving an old mystery. This Letter brings the attention of the scientific community to the need of revising the sunspot series in the 18th century. The presence of a new short, asymmetric cycle implies changes and constraints to sunspot cycle statistics, <span class="hlt">solar</span> activity predictions, and <span class="hlt">solar</span> dynamo theories, as well as for <span class="hlt">solar</span>-terrestrial relations.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19960021265&hterms=faraday&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dfaraday','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19960021265&hterms=faraday&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dfaraday"><span>Faraday rotation fluctutation spectra <span class="hlt">observed</span> during <span class="hlt">solar</span> occultation of the Helios spacecraft</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Andreev, V.; Efimov, A. I.; Samoznaev, L.; Bird, M. K.</p> <p>1995-01-01</p> <p>Faraday rotation (FR) measurements using linearly polarized radio signals from the two Helios spacecraft were carried out during the period from 1975 to 1984. This paper presents the results of a spectral analysis of the Helios S-band FR fluctuations <span class="hlt">observed</span> at heliocentric distances from 2.6 to 15 <span class="hlt">solar</span> radii during the superior conjunctions 1975-1983. The mean intensity of the FR fluctuations does not exceed the noise level for <span class="hlt">solar</span> offsets greater than ca. 15 <span class="hlt">solar</span> radii. The rms FR fluctuation amplitude increases rapidly as the radio ray path approaches the Sun, varying according to a power law (exponent: 2.85 +/- 0.15) at <span class="hlt">solar</span> distances 4-12 <span class="hlt">solar</span> radii. At distances inside 4 <span class="hlt">solar</span> radii the increase is even steeper (exponent: 5.6 +/- 0.2). The equivalent two-dimensional FR fluctuation spectrum is well modeled by a single power-law over the frequency range from 5 to 50 mHz. For heliocentric distances larger than 4 <span class="hlt">solar</span> radii the spectral index varies between 1.1 and 1.6 with a mean value of 1.4 +/- 0.2, corresponding to a 3-D spectral index p = 2.4. FR fluctuations thus display a somwhat lower spectral index compared with phase and amplitude fluctuations. Surprisingly high values of the spectral index were found for measurements inside 4 <span class="hlt">solar</span> radii (p = 2.9 +/- 0.2). This may arise from the increasingly dominant effect of the magnetic field on radio wave propagation at small <span class="hlt">solar</span> offsets. Finally, a quasiperiodic component, believed to be associated with Alfven waves, was discovered in some (but not all!) fluctuation spectra <span class="hlt">observed</span> simultaneously at two ground stations. Characteristic periods and bulk velocities of this component were 240 +/- 30 sec and 300 +/- 60 km/s, respectively.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20100002102&hterms=puzzle&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dpuzzle','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20100002102&hterms=puzzle&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dpuzzle"><span><span class="hlt">Solar</span> Spicules Near and at the Limb, <span class="hlt">Observed</span> from Hinode</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Sterling, Alphonse C.; Moore, Ronald</p> <p>2009-01-01</p> <p><span class="hlt">Solar</span> spicules appear as narrow jets emanating from the chromosphere and extending into the corona. They have been <span class="hlt">observed</span> for over a hundred years, mainly in chromospheric spectral lines such as H-alpha. Because they are at the limit of visibility of ground-based instruments, their nature has long been a puzzle (Beckers 1968, 1972; Sterling 2000). In recent years however, vast progress has been made in understanding them both theoretically and <span class="hlt">observationally</span>, as spicule studies have undergone a revolution because of the superior resolution and time cadence of ground-based and space-based instruments (e.g., DePontieu et al. 2004). Even more rapid progress is currently underway, due to the <span class="hlt">Solar</span> Optical Telescope (SOT) instrument on the Hinode spacecraft (e.g., De Pontieu et al. 2007a, 2007b). Here we present <span class="hlt">observations</span> of spicules from Hinode SOT, as seen near the limb with the Ca II filtergraph.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20130013609','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20130013609"><span>What Do Millimeter Continuum and Spectral Line <span class="hlt">Observations</span> Tell Us about <span class="hlt">Solar</span> System Bodies?</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Milam, Stefanie N.</p> <p>2013-01-01</p> <p><span class="hlt">Solar</span> system objects are generally cold and radiate at low frequencies and tend to have strong molecular rotational transitions. Millimeter continuum and spectral line <span class="hlt">observations</span> provide detailed information for nearly all <span class="hlt">solar</span> system bodies. At these wavelengths, details of the bulk physical composition of icy surfaces, the size and albedo of small objects, the composition of planetary atmospheres can be measured as well as monitoring of time variable phenomena for extended periods (not restricted to nighttime <span class="hlt">observations</span>), etc. Major issues in <span class="hlt">solar</span> system science can be addressed by <span class="hlt">observations</span> in the millimeter/sub-millimeter regime such as the origin of the <span class="hlt">solar</span> system (isotope ratios, composition) and the evolution of <span class="hlt">solar</span> system objects (dynamics, atmospheric constituents, etc). ALMA s exceptional sensitivity, large spectral bandwidth, high spectral resolution, and angular resolution (down to 10 milliarcsec) will enable researchers for the first time to better resolve the smallest bodies in the <span class="hlt">solar</span> system and provide detailed maps of the larger objects. Additionally, measurements with nearly 8 GHz of instantaneous bandwidth to fully characterize <span class="hlt">solar</span> system object s spectrum and detect trace species. The spatial information and line profiles can be obtained over 800 GHz of bandwidth in 8 receiver bands to not only assist in the identification of spectral lines and emission components for a given species but also to help elucidate the chemistry of the extraterrestrial bodies closest to us.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AN....337.1064T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AN....337.1064T"><span>Daniel K. Inouye <span class="hlt">Solar</span> Telescope: High-resolution <span class="hlt">observing</span> of the dynamic Sun</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tritschler, A.; Rimmele, T. R.; Berukoff, S.; Casini, R.; Kuhn, J. R.; Lin, H.; Rast, M. P.; McMullin, J. P.; Schmidt, W.; Wöger, F.; DKIST Team</p> <p>2016-11-01</p> <p>The 4-m aperture Daniel K. Inouye <span class="hlt">Solar</span> Telescope (DKIST) formerly known as the Advanced Technology <span class="hlt">Solar</span> Telescope (ATST) is currently under construction on Haleakalā (Maui, Hawai'i) projected to start operations in 2019. At the time of completion, DKIST will be the largest ground-based <span class="hlt">solar</span> telescope providing unprecedented resolution and photon collecting power. The DKIST will be equipped with a set of first-light facility-class instruments offering unique imaging, spectroscopic and spectropolarimetric <span class="hlt">observing</span> opportunities covering the visible to infrared wavelength range. This first-light instrumentation suite will include: a Visible Broadband Imager (VBI) for high-spatial and -temporal resolution imaging of the <span class="hlt">solar</span> atmosphere; a Visible Spectro-Polarimeter (ViSP) for sensitive and accurate multi-line spectropolarimetry; a Fabry-Pérot based Visible Tunable Filter (VTF) for high-spatial resolution spectropolarimetry; a fiber-fed Diffraction-Limited Near Infra-Red Spectro-Polarimeter (DL-NIRSP) for two-dimensional high-spatial resolution spectropolarimetry (simultaneous spatial and spectral information); and a Cryogenic Near Infra-Red Spectro-Polarimeter (Cryo-NIRSP) for coronal magnetic field measurements and on-disk <span class="hlt">observations</span> of, e.g., the CO lines at 4.7 μm. We will provide an overview of the DKIST's unique capabilities with strong focus on the first-light instrumentation suite, highlight some of the additional properties supporting <span class="hlt">observations</span> of transient and dynamic <span class="hlt">solar</span> phenomena, and touch on some operational strategies and the DKIST critical science plan.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018IAUS..330...63H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018IAUS..330...63H"><span>Local tests of gravitation with Gaia <span class="hlt">observations</span> of <span class="hlt">Solar</span> System Objects</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hees, Aurélien; Le Poncin-Lafitte, Christophe; Hestroffer, Daniel; David, Pedro</p> <p>2018-04-01</p> <p>In this proceeding, we show how <span class="hlt">observations</span> of <span class="hlt">Solar</span> System Objects with Gaia can be used to test General Relativity and to constrain modified gravitational theories. The high number of <span class="hlt">Solar</span> System objects <span class="hlt">observed</span> and the variety of their orbital parameters associated with the impressive astrometric accuracy will allow us to perform local tests of General Relativity. In this communication, we present a preliminary sensitivity study of the Gaia <span class="hlt">observations</span> on dynamical parameters such as the Sun quadrupolar moment and on various extensions to general relativity such as the parametrized post-Newtonian parameters, the fifth force formalism and a violation of Lorentz symmetry parametrized by the Standard-Model extension framework. We take into account the time sequences and the geometry of the <span class="hlt">observations</span> that are particular to Gaia for its nominal mission (5 years) and for an extended mission (10 years).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016A%26A...596A..42B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016A%26A...596A..42B"><span>Mass-loading of the <span class="hlt">solar</span> wind at 67P/Churyumov-Gerasimenko. <span class="hlt">Observations</span> and modelling</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Behar, E.; Lindkvist, J.; Nilsson, H.; Holmström, M.; Stenberg-Wieser, G.; Ramstad, R.; Götz, C.</p> <p>2016-11-01</p> <p>Context. The first long-term in-situ <span class="hlt">observation</span> of the plasma environment in the vicinity of a comet, as provided by the European Rosetta spacecraft. Aims: Here we offer characterisation of the <span class="hlt">solar</span> wind flow near 67P/Churyumov-Gerasimenko (67P) and its long term evolution during low nucleus activity. We also aim to quantify and interpret the deflection and deceleration of the flow expected from ionization of neutral cometary particles within the undisturbed <span class="hlt">solar</span> wind. Methods: We have analysed in situ ion and magnetic field data and combined this with hybrid modeling of the interaction between the <span class="hlt">solar</span> wind and the comet atmosphere. Results: The <span class="hlt">solar</span> wind deflection is increasing with decreasing heliocentric distances, and exhibits very little deceleration. This is seen both in <span class="hlt">observations</span> and in modeled <span class="hlt">solar</span> wind protons. According to our model, energy and momentum are transferred from the <span class="hlt">solar</span> wind to the coma in a single region, centered on the nucleus, with a size in the order of 1000 km. This interaction affects, over larger scales, the downstream modeled <span class="hlt">solar</span> wind flow. The energy gained by the cometary ions is a small fraction of the energy available in the <span class="hlt">solar</span> wind. Conclusions: The deflection of the <span class="hlt">solar</span> wind is the strongest and clearest signature of the mass-loading for a small, low-activity comet, whereas there is little deceleration of the <span class="hlt">solar</span> wind.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20040088897&hterms=Paradox+value&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3DParadox%2Bvalue','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20040088897&hterms=Paradox+value&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3DParadox%2Bvalue"><span>The faint young Sun paradox: an <span class="hlt">observational</span> test of an alternative <span class="hlt">solar</span> model</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Gaidos, E. J.; Gudel, M.; Blake, G. A.</p> <p>2000-01-01</p> <p>We report the results of deep <span class="hlt">observations</span> at radio (3.6 cm) wavelengths of the nearby <span class="hlt">solar</span>-type star pi 01 Ursa Majoris with the Very Large Array (VLA) intended to test an alternative theory of <span class="hlt">solar</span> luminosity evolution. The standard model predicts a <span class="hlt">solar</span> luminosity only 75% of the present value and surface temperatures below freezing on Earth and Mars at 4 Ga, seemingly in conflict with geologic evidence for liquid water on these planets. An alternative model invokes a compensatory mass loss through a declining <span class="hlt">solar</span> wind that results in a more consistent early luminosity. The free-free emission from an enhanced wind around nearby young Sun-like stars should be detectable at microwave frequencies. Our <span class="hlt">observations</span> of pi 01 UMa, a 300 million year-old <span class="hlt">solar</span>-mass star, place an upper limit on the mass loss rate of 4-5 x 10(-11) M(<span class="hlt">solar</span>) yr-1. Total mass loss from such a star over 4 Gyr would be less than 6%. If this star is indeed an analog of the early Sun, it casts doubt on the alternative model as a solution to the faint young Sun paradox, particularly for Mars.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20040015316','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20040015316"><span>Limitation of Ground-based Estimates of <span class="hlt">Solar</span> Irradiance Due to Atmospheric Variations</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Wen, Guoyong; Cahalan, Robert F.; Holben, Brent N.</p> <p>2003-01-01</p> <p>The uncertainty in ground-based estimates of <span class="hlt">solar</span> irradiance is quantitatively related to the temporal variability of the atmosphere's optical thickness. The upper and lower bounds of the accuracy of estimates using the Langley Plot technique are proportional to the standard deviation of aerosol optical thickness (approx. +/- 13 sigma(delta tau)). The estimates of spectral <span class="hlt">solar</span> irradiance (SSI) in two Cimel sun photometer channels from the Mauna Loa site of AERONET are compared with satellite <span class="hlt">observations</span> from SOLSTICE (<span class="hlt">Solar</span> Stellar Irradiance Comparison Experiment) on UARS (Upper Atmospheric Research Satellite) for almost two years of data. The true <span class="hlt">solar</span> variations related to the 27-day <span class="hlt">solar</span> rotation cycle <span class="hlt">observed</span> from SOLSTICE are about 0.15% at the two sun photometer channels. The variability in ground-based estimates is statistically one order of magnitude larger. Even though about 30% of these estimates from all Level 2.0 Cimel data fall within the 0.4 to approx. 0.5% variation level, ground-based estimates are not able to <span class="hlt">capture</span> the 27-day <span class="hlt">solar</span> variation <span class="hlt">observed</span> from SOLSTICE.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018nova.pres.3196H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018nova.pres.3196H"><span>Probing the Structure of Our <span class="hlt">Solar</span> System's Edge</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hensley, Kerry</p> <p>2018-02-01</p> <p>The boundary between the <span class="hlt">solar</span> wind and the interstellar medium (ISM) at the distant edge of our <span class="hlt">solar</span> system has been probed remotely and directly by spacecraft, but questions about its properties persist. What can models tell us about the structure of this region?The Heliopause: A Dynamic BoundarySchematic illustrating different boundaries of our <span class="hlt">solar</span> system and the locations of the Voyager spacecraft. [Walt Feimer/NASA GSFCs Conceptual Image Lab]As our <span class="hlt">solar</span> system travels through interstellar space, the magnetized <span class="hlt">solar</span> wind flows outward and pushes back on the oncoming ISM, forming a bubble called the heliosphere. The clash of plasmas generates a boundary region called the heliopause, the shape of which depends strongly on the properties of the <span class="hlt">solar</span> wind and the local ISM.Much of our understanding of the outer heliosphere and the local ISM comes from <span class="hlt">observations</span> made by the International Boundary Explorer (IBEX) and the Voyager 1 and Voyager 2 spacecraft. IBEX makes global maps of the flux of neutral atoms, while Voyagers 1 and 2 record the plasma density and magnetic field parameters along their trajectories as they exit the <span class="hlt">solar</span> system. In order to interpret the IBEX and Voyager <span class="hlt">observations</span>, astronomers rely on complex models that must <span class="hlt">capture</span> both global and local effects.Simulations of the plasma density in the meridional plane of the heliosphere due to the interaction of the <span class="hlt">solar</span> wind with the ISM for the case of a relatively dense ISM with a weak magnetic field. [Adapted from Pogorelov et al. 2017]Modeling the Edge of the <span class="hlt">Solar</span> SystemIn this study, Nikolai Pogorelov (University of Alabama in Huntsville) and collaborators use a hybrid magneto-hydrodynamical (MHD) and kinetic simulation to <span class="hlt">capture</span> fully the physical processes happening in the outer heliosphere.MHD models have been used to understand many aspects of plasma flow in the heliosphere. However, they struggle to <span class="hlt">capture</span> processes that are better described kinetically, like charge exchange</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19810030756&hterms=Dunham&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAuthor-Name%26N%3D0%26No%3D90%26Ntt%3DDunham','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19810030756&hterms=Dunham&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAuthor-Name%26N%3D0%26No%3D90%26Ntt%3DDunham"><span><span class="hlt">Observations</span> of a probable change in the <span class="hlt">solar</span> radius between 1715 and 1979</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Dunham, D. W.; Sofia, S.; Fiala, A. D.; Muller, P. M.; Herald, D.</p> <p>1980-01-01</p> <p>A decrease in the <span class="hlt">solar</span> radius is determined using the technique of Dunham and Dunham (1973), in which timed <span class="hlt">observations</span> are made just inside the path edges. When the method is applied to the <span class="hlt">solar</span> eclipses of 1715, 1976, and 1979, the <span class="hlt">solar</span> radius for 1715 is 0.34 + or - 0.2 arc second larger than the recent values, with no significant change between 1976 and 1979. The duration of totality is examined as a function of distance from the edges of the path. Corrections to the radius of the sun derived from <span class="hlt">observations</span> of the 1976 and 1979 eclipses by the International Occultation Timing Association are also presented.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018AAS...23131505K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018AAS...23131505K"><span>Helioseismic <span class="hlt">Observations</span> of Two <span class="hlt">Solar</span> Cycles and Constraints on Dynamo Theory</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kosovichev, Alexander</p> <p>2018-01-01</p> <p>Helioseismology data from the SOHO and SDO, obtained in 1996-2017 for almost two <span class="hlt">solar</span> cycles, provide a unique opportunity to investigate variations of the <span class="hlt">solar</span> interior structure and dynamics, and link these variations to the current dynamo models and simulations. The <span class="hlt">solar</span> oscillation frequencies and frequency splitting of medium-degree p- and f-modes, as well as helioseismic inversions have been used to analyze variations of the differential rotation (“torsional oscillations”) and the global asphericity. By comparing the helioseismology results with the synoptic surface magnetic fields we identify characteristic changes associated the initiation and evolution of the <span class="hlt">solar</span> cycles, 23 and 24. The <span class="hlt">observational</span> results are compared with the current mean-field dynamo models and 3D MHD dynamo simulations. It is shown that the helioseismology inferences provide important constraints on the dynamics of the tachocline and near-surface shear layer, and also may explain the fundamental difference between the two <span class="hlt">solar</span> cycles and detect the onset of the next cycle.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/21452700-detection-vortex-tubes-solar-granulation-from-observations-sunrise','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/21452700-detection-vortex-tubes-solar-granulation-from-observations-sunrise"><span>DETECTION OF VORTEX TUBES IN <span class="hlt">SOLAR</span> GRANULATION FROM <span class="hlt">OBSERVATIONS</span> WITH SUNRISE</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>Steiner, O.; Franz, M.; Bello Gonzalez, N.</p> <p>2010-11-10</p> <p>We have investigated a time series of continuum intensity maps and corresponding Dopplergrams of granulation in a very quiet <span class="hlt">solar</span> region at the disk center, recorded with the Imaging Magnetograph eXperiment (IMaX) on board the balloon-borne <span class="hlt">solar</span> observatory SUNRISE. We find that granules frequently show substructure in the form of lanes composed of a leading bright rim and a trailing dark edge, which move together from the boundary of a granule into the granule itself. We find strikingly similar events in synthesized intensity maps from an ab initio numerical simulation of <span class="hlt">solar</span> surface convection. From cross sections through the computationalmore » domain of the simulation, we conclude that these granular lanes are the visible signature of (horizontally oriented) vortex tubes. The characteristic optical appearance of vortex tubes at the <span class="hlt">solar</span> surface is explained. We propose that the <span class="hlt">observed</span> vortex tubes may represent only the large-scale end of a hierarchy of vortex tubes existing near the <span class="hlt">solar</span> surface.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20120016043','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20120016043"><span>ROSAT <span class="hlt">Observations</span> of <span class="hlt">Solar</span> Wind Charge Exchange with the Lunar Exosphere</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Collier, Michael R.; Snowden, S. L.; Benna, M.; Carter, J. A.; Cravens, T. E.; Hills, H. Kent; Hodges, R. R.; Kuntz, K. D.; Porter, F. Scott; Read, A.; <a style="text-decoration: none; " href="javascript:void(0); " onClick="displayelement('author_20120016043'); toggleEditAbsImage('author_20120016043_show'); toggleEditAbsImage('author_20120016043_hide'); "> <img style="display:inline; width:12px; height:12px; " src="images/arrow-up.gif" width="12" height="12" border="0" alt="hide" id="author_20120016043_show"> <img style="width:12px; height:12px; display:none; " src="images/arrow-down.gif" width="12" height="12" border="0" alt="hide" id="author_20120016043_hide"></p> <p>2012-01-01</p> <p>We analyze the ROSAT PSPC soft X-ray image of the Moon taken on 29 June 1990 by examining the radial profile of the count rate in three wedges, two wedges (one north and one south) 13-32 degrees off (19 degrees wide) the terminator towards the dark side and one wedge 38 degrees wide centered on the anti-<span class="hlt">solar</span> direction. The radial profiles of both the north and the south wedges show substantial limb brightening that is absent in the 38 degree wide antisolar wedge. An analysis of the count rate increase associated with the limb brightening shows that its magnitude is consistent with that expected due to <span class="hlt">solar</span> wind charge exchange (SWCX) with the tenuous lunar atmosphere. Along with Mars, Venus, and Earth, the Moon represents another <span class="hlt">solar</span> system body at which <span class="hlt">solar</span> wind charge exchange has been <span class="hlt">observed</span>. This technique can be used to explore the <span class="hlt">solar</span> wind-lunar interaction.</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://hdl.handle.net/2060/20090025890','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20090025890"><span>STEREO <span class="hlt">Observations</span> of Energetic Neutral Hydrogen Atoms during the 5 December 2006 <span class="hlt">Solar</span> Flare</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Mewaldt, R. A.; Leske, R. A.; Stone, E. C.; Barghouty, A. F.; Labrador, A. W.; Cohen, C. M. S.; Cummings, A. C.; Davis, A. J.; vonRosenvinge, T. T.; Wiedenbeck, M. E.</p> <p>2009-01-01</p> <p>We report the discovery of energetic neutral hydrogen atoms emitted during the X9 <span class="hlt">solar</span> event of December 5, 2006. Beginning 1 hour following the onset of this E79 flare, the Low Energy Telescopes (LETs) on both the STEREO A and B spacecraft <span class="hlt">observed</span> a sudden burst of 1.6 to 15 MeV protons beginning hours before the onset of the main <span class="hlt">solar</span> energetic particle (SEP) event at Earth. More than 70% of these particles arrived from a longitude within 10 of the Sun, consistent with the measurement resolution. The derived emission profile at the Sun had onset and peak times remarkably similar to the GOES soft X-ray profile and continued for more than an hour. The <span class="hlt">observed</span> arrival directions and energy spectrum argue strongly that the particle events less than 5 MeV were due to energetic neutral hydrogen atoms (ENAs). To our knowledge, this is the first reported <span class="hlt">observation</span> of ENA emission from a <span class="hlt">solar</span> flare/coronal mass ejection. Possible origins for the production of ENAs in a large <span class="hlt">solar</span> event are considered. We conclude that the <span class="hlt">observed</span> ENAs were most likely produced in the high corona and that charge-transfer reactions between accelerated protons and partially-stripped coronal ions are an important source of ENAs in <span class="hlt">solar</span> events.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19850039166&hterms=population+characteristic&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dpopulation%2Bcharacteristic*','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19850039166&hterms=population+characteristic&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dpopulation%2Bcharacteristic*"><span>Characteristics of <span class="hlt">solar</span> and heliospheric ion populations <span class="hlt">observed</span> near earth</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Gloeckler, G.</p> <p>1984-01-01</p> <p>The composition and spectra of ions in <span class="hlt">solar</span>-energetic-particle and energetic-storm-particle events, of diffuse ions upstream of the earth bow shock, and of ions in deep-geomagnetic-tail plasmoids are characterized in a summary of in situ <span class="hlt">observations</span>. Data are presented in graphs and tables, and remarkable similarities are noted in the distribution functions of the heliospheric ion populations. The <span class="hlt">solar</span> wind, acting through acceleration mechanisms associated with shocks and turbulence, is identified as the major plasma source of suprathermal and energetic particles.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20170003114&hterms=Wind&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3DWind','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20170003114&hterms=Wind&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3DWind"><span>Slow <span class="hlt">Solar</span> Wind: <span class="hlt">Observations</span> and Modeling</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Abbo, L.; Ofman, L.; Antiochos, S. K.; Hansteen, V. H.; Harra, L.; Ko, Y.-K.; Lapenta, G.; Li, B.; Riley, P.; Strachan, L.; <a style="text-decoration: none; " href="javascript:void(0); " onClick="displayelement('author_20170003114'); toggleEditAbsImage('author_20170003114_show'); toggleEditAbsImage('author_20170003114_hide'); "> <img style="display:inline; width:12px; height:12px; " src="images/arrow-up.gif" width="12" height="12" border="0" alt="hide" id="author_20170003114_show"> <img style="width:12px; height:12px; display:none; " src="images/arrow-down.gif" width="12" height="12" border="0" alt="hide" id="author_20170003114_hide"></p> <p>2016-01-01</p> <p>While it is certain that the fast <span class="hlt">solar</span> wind originates from coronal holes, where and how the slow <span class="hlt">solar</span> wind (SSW) is formed remains an outstanding question in <span class="hlt">solar</span> physics even in the post-SOHO era. The quest for the SSW origin forms a major objective for the planned future missions such as the <span class="hlt">Solar</span> Orbiter and <span class="hlt">Solar</span> Probe Plus. Nonetheless, results from spacecraft data, combined with theoretical modeling, have helped to investigate many aspects of the SSW. Fundamental physical properties of the coronal plasma have been derived from spectroscopic and imaging remote-sensing data and in situ data, and these results have provided crucial insights for a deeper understanding of the origin and acceleration of the SSW. Advanced models of the SSW in coronal streamers and other structures have been developed using 3D MHD and multi-fluid equations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010EGUGA..1211532P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010EGUGA..1211532P"><span>10Be in ice at high resolution: <span class="hlt">Solar</span> activity and climate signals <span class="hlt">observed</span> and GCM-modeled in Law Dome ice cores</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pedro, Joel; Heikkilä, Ulla; van Ommen, T. D.; Smith, A. M.</p> <p>2010-05-01</p> <p>Changes in <span class="hlt">solar</span> activity modulate the galactic cosmic ray flux, and in turn, the production rate of 10Be in the earth's atmosphere. The best archives of past changes in 10Be production rate are the polar ice cores. Key challenges in interpreting these archives as proxies for past <span class="hlt">solar</span> activity lie in separating the useful <span class="hlt">solar</span> activity (or production) signal from the interfering meteorological (or climate) signal, and furthermore, in determining the atmospheric source regions of 10Be deposited to the ice core site. In this study we use a new monthly resolution composite 10Be record, which spans the past decade, and a general circulation model (ECHAM5-HAM), to constrain both the production and climate signals in 10Be concentrations at the Law Dome ice core site, East Antarctica. This study differs from most previous work on 10Be in Antarctica due to the very high sample resolution achieved. This high resolution, through a time period where accurate instrumental measurements of <span class="hlt">solar</span> activity and climate are available, allows us to examine the response of 10Be concentrations in ice to short-term (monthly to annual) variations in <span class="hlt">solar</span> activity, and to short-term variations in climate, including seasonality. We find a significant correlation (r2 = 0.56, P < 0.005, n = 92) between <span class="hlt">observed</span> 10Be concentrations and <span class="hlt">solar</span> activity (represented by the neutron counting rate). The most pervasive climate influence is a seasonal cycle, which shows maximum concentrations in mid-to-late-summer and minimum concentrations in winter. Model results show reasonable agreement with <span class="hlt">observations</span>; both a <span class="hlt">solar</span> activity signal and seasonal cycle in 10Be are <span class="hlt">captured</span>. However, the modeled snow accumulation rate is too high by approximately 60%. According to the model, the main atmospheric source region of 10Be deposited to Law Dome is the 30-90°S stratosphere (~50%), followed by the 30-90°S troposphere (~30%). An enhancement in the fraction of 10Be arriving to Law Dome from the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20020021644&hterms=1064&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3D%2526%25231064','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20020021644&hterms=1064&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3D%2526%25231064"><span>The <span class="hlt">Capture</span> of Interstellar Dust: The Pure Poynting-Robertson Case</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Jackson, A. A.</p> <p>2001-01-01</p> <p>Ulysses and Galileo spacecraft have discovered interstellar dust particles entering the <span class="hlt">solar</span> system. In general, particles trajectories not altered by Lorentz forces or radiation pressure should encounter the sun on open orbits. Under Newtonian forces alone these particles return to the interstellar medium. Dissipative forces, such as Poynting Robertson (PR) and corpuscular drag and non-dissipative Lorentz forces can modify open orbits to become closed. In particular, it is possible for the orbits of particles that pass close to the Sun to become closed due to PR drag. Further, <span class="hlt">solar</span> irradiation will cause modification of the size of the dust particle by evaporation. The combination of these processes gives rise a class of <span class="hlt">capture</span> orbits and bound orbits with evaporation. Considering only the case of pure PR drag a minimum impact parameter is derived for initial <span class="hlt">capture</span> by Poynting-Robertson drag. Orbits in the <span class="hlt">solar</span> radiation field are computed numerically accounting for evaporation with optical and material properties for ideal interstellar particles modeled. The properties of this kind of particle <span class="hlt">capture</span> are discussed for the Sun but is applicable to other stars.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19750045079&hterms=orbiting+wind&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dorbiting%2Bwind','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19750045079&hterms=orbiting+wind&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dorbiting%2Bwind"><span>Direct <span class="hlt">observations</span> of a flare related coronal and <span class="hlt">solar</span> wind disturbance</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Gosling, J. T.; Hildner, E.; Macqueen, R. M.; Munro, R. H.; Poland, A. I.; Ross, C. L.</p> <p>1975-01-01</p> <p>Numerous mass ejections from the sun have been detected with orbiting coronagraphs. Here for the first time we document and discuss the direct association of a coronagraph <span class="hlt">observed</span> mass ejection, which followed a 2B flare, with a large interplanetary shock wave disturbance <span class="hlt">observed</span> at 1 AU. Estimates of the mass and energy content of the coronal disturbance are in reasonably good agreement with estimates of the mass and energy content of the <span class="hlt">solar</span> wind disturbance at 1 AU. The energy estimates as well as the transit time of the disturbance are also in good agreement with numerical models of shock wave propagation in the <span class="hlt">solar</span> wind.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27150619','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27150619"><span>Do different attention <span class="hlt">capture</span> paradigms measure different types of <span class="hlt">capture</span>?</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Roque, Nelson A; Wright, Timothy J; Boot, Walter R</p> <p>2016-10-01</p> <p>When something <span class="hlt">captures</span> our attention, why does it do so? This topic has been hotly debated, with some arguing that attention is <span class="hlt">captured</span> only by salient stimuli (bottom-up view) and others arguing <span class="hlt">capture</span> is always due to a match between a stimulus and our goals (top-down view). Many different paradigms have provided evidence for 1 view or the other. If either of these strong views are correct, then <span class="hlt">capture</span> represents a unitary phenomenon, and there should be a high correlation between <span class="hlt">capture</span> in these paradigms. But if there are different types of <span class="hlt">capture</span> (top-down, bottom-up), then some attention <span class="hlt">capture</span> effects should be correlated and some should not. In 2 studies, we collected data from several paradigms used in support of claims of top-down and bottom-up <span class="hlt">capture</span> in relatively large samples of participants. Contrary to either prediction, measures of <span class="hlt">capture</span> were not strongly correlated. Results suggest that <span class="hlt">capture</span> may in fact be strongly determined by idiosyncratic task demands and strategies. Relevant to this lack of relations among tasks, we <span class="hlt">observed</span> that classic measures of attention <span class="hlt">capture</span> demonstrated low reliability, especially among measures used to support bottom-up <span class="hlt">capture</span>. Implications for the low reliability of <span class="hlt">capture</span> measures are discussed. We also <span class="hlt">observed</span> that the proportion of participants demonstrating a pattern of responses consistent with <span class="hlt">capture</span> varied widely among classic measures of <span class="hlt">capture</span>. Overall, results demonstrate that, even for relatively simple laboratory measures of attention, there are still important gaps in knowledge regarding what these paradigms measure and how they are related.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19930066714&hterms=nu&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dnu%253Fl','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19930066714&hterms=nu&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dnu%253Fl"><span><span class="hlt">Observations</span> of intermediate degree <span class="hlt">solar</span> oscillations - 1989 April-June</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Bachmann, Kurt T.; Schou, Jesper; Brown, Timothy M.</p> <p>1993-01-01</p> <p>Frequencies, splittings, and line widths from 85 d of full disk Doppler <span class="hlt">observations</span> of <span class="hlt">solar</span> p-modes taken between April 4 and June 30, 1989 are presented. Comparison of the present mode parameters with published Big Bear <span class="hlt">Solar</span> Observatory (BBSO) results yields good agreement in general and is thus a confirmation of their work using an independent instrument and set of analysis routines. Average differences in p-mode frequencies measured by the two experiments in spring-summer 1989 are explained as a result of differences in the exact periods of data collection during a time of rapidly changing <span class="hlt">solar</span> activity. It is shown that the present a(1) splitting coefficients for p-modes with nu/L less than 45 micro-Hz suffer from a significant systematic error. Evidence is presented to the effect that a detector distortion or alignment problem, not a problem with the power spectra analysis, is the most likely explanation of this a(1) anomaly.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018EPJWC.16501053V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018EPJWC.16501053V"><span>The <span class="hlt">solar</span> Lithium problem: is the explanation due solely to mixing or also to the e-<span class="hlt">capture</span> decay rate of 7Be?</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Vescovi, Diego; Busso, Maurizio; Palmerini, Sara; Trippella, Oscar</p> <p>2018-01-01</p> <p>The nucleosynthesis of 7Li is one of the most crucial problems in nuclear as- trophysics, as its <span class="hlt">observations</span> in several sites are hard to be explained. Concerning the Sun, the most common interpretations of the low Li abundance invoke either burning in early stages or non-convective mixing below the envelope. Here we apply a diffusive mechanism of mixing, together with a recent estimate of the rate for e-<span class="hlt">captures</span> on 7Be, to establish whether the <span class="hlt">solar</span> Li destruction should be attributed to purely pre-Main Se- quence (MS) nuclear processes or if the coupling of mixing and nucleosynthesis on the MS can account for it. Our preliminary results indicate that, whether Li survives the pre- MS phase, the changes of the 7Be e--<span class="hlt">capture</span> rate do not affect its production/destruction. The low Li abundance should then depend only on diffusion processes from the bottom of the convective envelope to the lowerlying tachocline zone. We suggest that, if diffusive processes occurred over the age of the Sun, they required diffusive mass transfers of a few 10-13 M⊙/yr to explain the Li drop. This is a high estimate: future works will tell us if it is realistic or not. In this second case, pre-MS burning would remain the only alternative.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19760059724&hterms=rickets&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Drickets','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19760059724&hterms=rickets&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Drickets"><span>High-latitude <span class="hlt">observations</span> of <span class="hlt">solar</span> wind streams and coronal holes</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Ricket, B. J.; Sime, D. G.; Crockett, W. R.; Tousey, R.; Sheeley, N. R., Jr.</p> <p>1976-01-01</p> <p>Interplanetary scintillation <span class="hlt">observations</span> of the <span class="hlt">solar</span> wind velocity during 1973 and the first part of 1974 reveal several corotating high-speed streams. These streams, of heliographic latitudes from +40 deg to -60 deg, have been mapped back to the vicinity of the sun and have been compared with coronal holes identified in wide band XUV <span class="hlt">solar</span> images taken during the manned portions of the Skylab mission. There is some evidence that the high-speed streams are preferentially associated with coronal holes and that they can spread out from the hole boundaries up to about 20 deg in latitude. However, this association is not one to one; streams are <span class="hlt">observed</span> which do not map back to coronal holes, and holes are <span class="hlt">observed</span> which do not lie at the base of streams. To the extent that a statistical interpretation is possible the association is not highly significant, but individual consideration of streams and holes suggests that the statistical result is biased somewhat against a strong correlation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20060047740&hterms=Solar+still&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3DSolar%2Bstill','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20060047740&hterms=Solar+still&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3DSolar%2Bstill"><span>Initiation of <span class="hlt">Solar</span> Eruptions: Recent <span class="hlt">Observations</span> and Implications for Theories</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Sterling, A. C.</p> <p>2006-01-01</p> <p><span class="hlt">Solar</span> eruptions involve the violent disruption of a system of magnetic field. Just how the field is destabilized and explodes to produce flares and coronal mass ejections (CMEs) is still being debated in the <span class="hlt">solar</span> community. Here I discuss recent <span class="hlt">observational</span> work into these questions by ourselves (me and my colleagues) and others. Our work has concentrated mainly on eruptions that include filaments. We use the filament motion early in the event as a tracer of the motion of the general erupting coronal field in and around the filament, since that field itself is hard to distinguish otherwise. Our main data sources are EUV images from SOHO/EIT and TRACE, soft Xray images from Yohkoh, and magnetograms from SOHO/MDI, supplemented with coronagraph images from SOHO/LASCO, hard X-ray data, and ground-based <span class="hlt">observations</span>. We consider the <span class="hlt">observational</span> findings in terms of three proposed eruption-initiation mechanisms: (i) runaway internal tether-cutting reconnection, (ii) slow external tether-cutting reconnection ("breakout"), and (iii) ideal MHD instability.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20150023027','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20150023027"><span>Atmospheric Mining in the Outer <span class="hlt">Solar</span> System: Aerial Vehicle Mission and Design Issues</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Palaszewski, Bryan</p> <p>2015-01-01</p> <p>Atmospheric mining in the outer <span class="hlt">solar</span> system has been investigated as a means of fuel production for high energy propulsion and power. Fusion fuels such as Helium 3 (3He) and deuterium can be wrested from the atmospheres of Uranus and Neptune and either returned to Earth or used in-situ for energy production. Helium 3 and deuterium were the primary gases of interest with hydrogen being the primary propellant for nuclear thermal solid core and gas core rocket-based atmospheric flight. A series of analyses were undertaken to investigate resource <span class="hlt">capturing</span> aspects of atmospheric mining in the outer <span class="hlt">solar</span> system. This included the gas <span class="hlt">capturing</span> rate, storage options, and different methods of direct use of the <span class="hlt">captured</span> gases. While <span class="hlt">capturing</span> 3He, large amounts of hydrogen and 4He are produced. With these two additional gases, the potential for fueling small and large fleets of additional exploration and exploitation vehicles exists. The mining aerospacecraft (ASC) could fly through the outer planet atmospheres, for global weather <span class="hlt">observations</span>, localized storm or other disturbance investigations, wind speed measurements, polar <span class="hlt">observations</span>, etc. Analyses of orbital transfer vehicles (OTVs), landers, and in-situ resource utilization (ISRU) mining factories are included. Preliminary <span class="hlt">observations</span> are presented on near-optimal selections of moon base orbital locations, OTV power levels, and OTV and lander rendezvous points.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19850026423','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19850026423"><span>Study of photon emission by electron <span class="hlt">capture</span> during <span class="hlt">solar</span> nuclei acceleration. 2: Delimitation of conditions for charge transfert establishment</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Perez-Peraza, J.; Alvarez, M.; Gallegos, A.</p> <p>1985-01-01</p> <p>The conditions for establishment of charge transfer during acceleration of nuclei up to Fe, for typical conditions of <span class="hlt">solar</span> flare regions T = 5 x 10 to the 3rd power to 2.5 x 10 to the 8th power degrees K were explored. Results show that such conditions are widely assorted, depending on the acceleration mechanism, the kind of projections and their velocity, the target elements, the source temperature and consequently on the degree of ionization of matter and the local charge state of the accelerated ions. Nevertheless, in spite of that assorted behavior, there are some general tendencies that can be summarized as follows. In atomic H electron <span class="hlt">capture</span> is systematically established from thermal energies up to high energies, whatever the element and for both acceleration process. For a given element and fixed temperature (T), the probability and energy domain of electron <span class="hlt">capture</span> and loss with Fermi are higher than with Betatron acceleration. For a given acceleration process the heavier the ion the higher the probability and the wider the energy range for electron <span class="hlt">capture</span> and loss. For given acceleration mechanism and fixed element the importance and energy domain of <span class="hlt">capture</span> and loss increase with T: for those reasons, the energy range of charge equilibrium (illustrated with solid lines on the next figs.) is wider with Fermi and increases with temperature and atomic number of projectiles. For the same reasons, electron loss is smaller while the lighter the element, the lower the temperature and the Betatron process, such that there are conditions for which electron loss is not allowed at low energies, but only electron <span class="hlt">capture</span> is established.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017ApJ...851L..41D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017ApJ...851L..41D"><span>Tethered Prominence-CME Systems <span class="hlt">Captured</span> during the 2012 November 13 and 2013 November 3 Total <span class="hlt">Solar</span> Eclipses</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Druckmüller, Miloslav; Habbal, Shadia R.; Alzate, Nathalia; Emmanouilidis, Constantinos</p> <p>2017-12-01</p> <p>We report on white light <span class="hlt">observations</span> of high latitude tethered prominences acquired during the total <span class="hlt">solar</span> eclipses of 2012 November 13 and 2013 November 3, at <span class="hlt">solar</span> maximum, with a field of view spanning several <span class="hlt">solar</span> radii. Distinguished by their pinkish hue, characteristic of emission from neutral hydrogen and helium, the four tethered prominences were akin to twisted flux ropes, stretching out to the limit of the field of view, while remaining anchored at the Sun. Cotemporal <span class="hlt">observations</span> in the extreme ultraviolet from the <span class="hlt">Solar</span> Dynamics Observatory (SDO/AIA) clearly showed that the pinkish emission from the cool (≈ {10}4-{10}5 K) filamentary prominences was cospatial with the 30.4 nm He II emission, and was directly linked to filamentary structures emitting at coronal temperatures ≥slant {10}6 K in 17.1 and 19.3 nm. The tethered prominences evolved from typical tornado types. Each one formed the core of different types of coronal mass ejections (CMEs), as inferred from coordinated LASCO C2, C3, and STEREO A and B coronagraph <span class="hlt">observations</span>. Two of them evolved into a series of faint, unstructured puffs. One was a normal CME. The most striking one was a “light-bulb” type CME, whose three-dimensional structure was confirmed from all four coronagraphs. These first uninterrupted detections of prominence-CME systems anchored at the Sun, and stretching out to at least the edge of the field of view of LASCO C3, provide the first <span class="hlt">observational</span> confirmation for the source of counter-streaming electron fluxes measured in interplanetary CMEs, or ICMEs.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016DPS....4820607N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016DPS....4820607N"><span>Small is different: RPC <span class="hlt">observations</span> of a small scale comet interacting with the <span class="hlt">solar</span> wind</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Nilsson, Hans; Burch, James L.; Carr, Christopher M.; Eriksson, Anders I.; Glassmeier, Karl-Heinz; Henri, Pierre; Rosetta Plasma Consortium Team</p> <p>2016-10-01</p> <p>Rosetta followed comet 67P from low activity at more than 3 AU heliocentric distance to peak activity at perihelion and then out again. We study the evolution of the dynamic plasma environment using data from the Rosetta Plasma Consortium (RPC). <span class="hlt">Observations</span> of cometary plasma began in August 2014, at a distance of 100 km from the comet nucleus and at 3.6 AU from the Sun. As the comet approached the Sun, outgassing from the comet increased, as did the density of the cometary plasma. Measurements showed a highly heterogeneous cold ion environment, permeated by the <span class="hlt">solar</span> wind. The <span class="hlt">solar</span> wind was deflected due to the mass loading from newly added cometary plasma, with no discernible slowing down. The magnetic field magnitude increased significantly above the background level, and strong low frequency waves were <span class="hlt">observed</span> in the magnetic field, a.k.a. the "singing comet". Electron temperatures were high, leading to a frequently strongly negative spacecraft potential. In mid to late April 2015 the <span class="hlt">solar</span> wind started to disappear from the <span class="hlt">observation</span> region. This was associated with a <span class="hlt">solar</span> wind deflection reaching nearly 180°, indicating that mass loading became efficient enough to form a <span class="hlt">solar</span> wind-free region. Accelerated water ions, moving mainly in the anti-sunward direction, kept being <span class="hlt">observed</span> also after the <span class="hlt">solar</span> wind disappearance. Plasma boundaries began to form and a collisionopause was tentatively identified in the ion and electron data. At the time around perihelion, a diamagnetic cavity was also <span class="hlt">observed</span>, at a surprisingly large distance from the comet. In late 2016 the <span class="hlt">solar</span> wind re-appeared at the location of Rosetta, allowing for studies of asymmetry of the comet ion environment with respect to perihelion. A nightside excursion allowed us to get a glimpse of the electrodynamics of the innermost part of the plasma tail. Most of these phenomena are dependent on the small-scale physics of comet 67P, since for most of the Rosetta mission the <span class="hlt">solar</span> wind</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016SPIE.9914E..21C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016SPIE.9914E..21C"><span>Strategies on <span class="hlt">solar</span> <span class="hlt">observation</span> of Atacama Large Millimeter/submillimeter Array (ALMA) band-1 receiver</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chiong, Chau-Ching; Chiang, Po-Han; Hwang, Yuh-Jing; Huang, Yau-De</p> <p>2016-07-01</p> <p>ALMA covering 35-950 GHz is the largest existing telescope array in the world. Among the 10 receiver bands, Band-1, which covers 35-50 GHz, is the lowest. Due to its small dimension and its time-variant frequency-dependent gain characteristics, current <span class="hlt">solar</span> filter located above the cryostat cannot be applied to Band-1 for <span class="hlt">solar</span> <span class="hlt">observation</span>. Here we thus adopt new strategies to fulfill the goals. Thanks to the flexible dc biasing scheme of the HEMT-based amplifier in Band-1 front-end, bias adjustment of the cryogenic low noise amplifier is investigated to accomplish <span class="hlt">solar</span> <span class="hlt">observation</span> without using <span class="hlt">solar</span> filter. Large power handling range can be achieved by the de-tuning bias technique with little degradation in system performance.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20090028642&hterms=puzzle&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dpuzzle','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20090028642&hterms=puzzle&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dpuzzle"><span><span class="hlt">Solar</span> Spicules near and at The Limb, <span class="hlt">Observed</span> from Hinode</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Sterling, Alphonse C.</p> <p>2009-01-01</p> <p><span class="hlt">Solar</span> spicules appear as narrow jets emanating from the chromosphere and extending into the corona. They have been <span class="hlt">observed</span> for over a hundred years,mainly in chromospheric spectral lines such as H-alpha. Because they are at the limit of visibility of ground-based instruments, their nature has long been a puzzle. In recent years however, vast progress has been made in understanding them both theoretically and <span class="hlt">observationally</span>. Most recently, spicule studies have undergone revolution because of the superior resolution, time cadence, and atmosphere-free <span class="hlt">observations</span> from the <span class="hlt">Solar</span> Optical Telescope (SOT) instrument on the Hinode spacecraft. Here we present <span class="hlt">observations</span> of spicules from {\\sl Hinode} SOT, and consider how the <span class="hlt">observations</span> from Hinode compare with historical <span class="hlt">observations</span>. We include data taken in the blue and red wings of Halpha, where the spicules have widths of a few approx.100 kms, and the longest ones reach about 10(exp 4) km in extent,similar to sizes long reported from ground-based instruments. Their dynamics are not easy to generalize, with many showing the upward movement followed by falling or fading, as traditionally reported, but with others showing more dynamic or even ejective aspects. There is a strong transverse component to their motion, as extensively reported previously from the Hinode data as evidence for Alfven waves.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20080003790','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20080003790"><span><span class="hlt">Observations</span> of a Newly "<span class="hlt">Captured</span>" Magnetosheath Field Line: Evidence for "Double Reconnection"</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Chandler, Michael O.; Avanov, Levon A.; Craven, Paul D.; Mozer, Forrest S.; Moore, Thomas E.</p> <p>2007-01-01</p> <p>We have begun an investigation of the nature of the low-latitude boundary layer in the mid-altitude cusp region using data from the Polar spacecraft. This region has been routinely sampled for about three months each year for the periods 1999-2001 and 2004-2006. The low-to-mid-energy ion instruments frequently <span class="hlt">observed</span> dense, magnetosheath-like plasma deep (in terms of distance from the magnetopause and in invariant latitude) in the magnetosphere. One such case, taken during a period of northward interplanetary magnetic field (IMF), shows magnetosheath ions within the magnetosphere with velocity distributions resulting from two separate merging sites along the same field lines. Cold ionospheric ions were also <span class="hlt">observed</span> counterstreaming along the field lines, evidence that these field lines were closed. These results are consistent with the hypothesis that double merging can produce closed field .lines populated by <span class="hlt">solar</span> wind plasma. Through the use of individual cases such as this and statistical studies of a broader database we seek to understand the morphology of the LLBL as it projects from the sub-<span class="hlt">solar</span> region into the cusp. We will present preliminary results of our ongoing study.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19790034614&hterms=measures+LTE&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dmeasures%2BLTE','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19790034614&hterms=measures+LTE&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dmeasures%2BLTE"><span>Lyman continuum <span class="hlt">observations</span> of <span class="hlt">solar</span> flares</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Machado, M. E.; Noyes, R. W.</p> <p>1978-01-01</p> <p>A study is made of Lyman continuum <span class="hlt">observations</span> of <span class="hlt">solar</span> flares, using data obtained by the EUV spectroheliometer on the Apollo Telescope Mount. It is found that there are two main types of flare regions: an overall 'mean' flare coincident with the H-alpha flare region, and transient Lyman continuum kernels which can be identified with the H-alpha and X-ray kernels <span class="hlt">observed</span> by other authors. It is found that the ground level hydrogen population in flares is closer to LTE than in the quiet sun and active regions, and that the level of Lyman continuum formation is lowered in the atmosphere from a mass column density .000005 g/sq cm in the quiet sun to .0003 g/sq cm in the mean flare, and to .001 g/sq cm in kernels. From these results the amount of chromospheric material 'evaporated' into the high temperature region is derived, which is found to be approximately 10 to the 15th g, in agreement with <span class="hlt">observations</span> of X-ray emission measures.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/6289088-solar-cycle-evolution-solar-wind-speed-structure-between-observed-interplanetary-scintillation-method','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/6289088-solar-cycle-evolution-solar-wind-speed-structure-between-observed-interplanetary-scintillation-method"><span><span class="hlt">Solar</span> cycle evolution of <span class="hlt">solar</span> wind speed structure between 1973 and 1985 <span class="hlt">observed</span> with the interplanetary scintillation method</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>Kojima, M.; Kakinuma, T.</p> <p>1987-07-01</p> <p>The <span class="hlt">solar</span> cycle evolution of <span class="hlt">solar</span> wind speed structure was studied for the years from 1973 to 1985 on a basis of interplanetary scintillation <span class="hlt">observations</span> using a new method for mapping <span class="hlt">solar</span> wind speed to the source surface. The major minimum-speed regions are distributed along a neutral line through the whole period of a <span class="hlt">solar</span> cycle: when <span class="hlt">solar</span> activity is low, they are distributed on the wavy neutral line along the <span class="hlt">solar</span> equator; in the active phase they also tend to be distributed along the neutral line, which has a large latitudinal amplitude. The minimum-speed regions tend to be distributedmore » not only along the neutral line but also at low magnetic intensity regions and/or coronal bright regions which do not correspond to the neutral line. As the polar high-speed regions extend equatorward around the minimum phase, the latitudinal gradient of speed increases at the boundaries of the low-speed region, and the width of the low-speed region decreases. One or two years before the minimum of <span class="hlt">solar</span> activity, two localized minimum-speed regions appear on the neutral line, and their locations are longitudinally separated by 180. copyright American Geophysical Union 1987« 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_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/2010cosp...38..419S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010cosp...38..419S"><span>Interaction between <span class="hlt">solar</span> wind and lunar magnetic anomalies <span class="hlt">observed</span> by MAP-PACE on Kaguya</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Saito, Yoshifumi; Yokota, Shoichiro; Tanaka, Takaaki; Asamura, Kazushi; Nishino, Masaki N.; Yamamoto, Tadateru I.; Tsunakawa, Hideo</p> <p></p> <p>It is well known that the Moon has neither global intrinsic magnetic field nor thick atmosphere. Different from the Earth's case where the intrinsic global magnetic field prevents the <span class="hlt">solar</span> wind from penetrating into the magnetosphere, <span class="hlt">solar</span> wind directly impacts the lunar surface. MAgnetic field and Plasma experiment -Plasma energy Angle and Composition Experiment (MAP-PACE) on Kaguya (SELENE) completed its 1.5-year <span class="hlt">observation</span> of the low energy charged particles around the Moon on 10 June 2009. Kaguya was launched on 14 September 2007 by H2A launch vehicle from Tanegashima Space Center in Japan. Kaguya was inserted into a circular lunar polar orbit of 100km altitude and continued <span class="hlt">observation</span> for nearly 1.5 years till it impacted the Moon on 10 June 2009. During the last 5 months, the orbit was lowered to 50km-altitude between January 2009 and April 2009, and some orbits had further lower perilune altitude of 10km after April 2009. MAP-PACE consisted of 4 sensors: ESA (Electron Spectrum Analyzer)-S1, ESA-S2, IMA (Ion Mass Analyzer), and IEA (Ion Energy Analyzer). Since each sensor had hemispherical field of view, two electron sensors and two ion sensors that were installed on the spacecraft panels opposite to each other could cover full 3-dimensional phase space of low energy electrons and ions. One of the ion sensors IMA was an energy mass spectrometer. IMA measured mass identified ion energy spectra that had never been obtained at 100km altitude polar orbit around the Moon. When Kaguya flew over South Pole Aitken region, where strong magnetic anomalies exist, <span class="hlt">solar</span> wind ions reflected by magnetic anomalies were <span class="hlt">observed</span>. These ions had much higher flux than the <span class="hlt">solar</span> wind protons scattered at the lunar surface. The magnetically reflected ions had nearly the same energy as the incident <span class="hlt">solar</span> wind ions while the <span class="hlt">solar</span> wind protons scattered at the lunar surface had slightly lower energy than the incident <span class="hlt">solar</span> wind ions. At 100km altitude, when the reflected ions</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20090033104','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20090033104"><span><span class="hlt">Observation</span> and Interpretation of Energetic Neutral Hydrogen Atoms from the December 5, 2006 <span class="hlt">Solar</span> Flare</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Barghouty, A. F.; Mewaldt, R. A.; Leske, R. A.; Shih, A. Y.; Stone, E. C.; Cohen, C. M. S.; Cummings, A. C.; Labrador, A. W.; vonRosenvinge, T. T.; Wiedenbeck, M. E.</p> <p>2009-01-01</p> <p>We discuss <span class="hlt">observations</span> of energetic neutral hydrogen atoms (ENAs) from a <span class="hlt">solar</span> flare/coronal mass ejection event reported by Mewaldt et al. (2009). The <span class="hlt">observations</span> were made during the 5 December 2006 X9 <span class="hlt">solar</span> flare, located at E79, by the Low Energy Telescopes (LETs) on STEREO A and B. Prior to the arrival of the main <span class="hlt">solar</span> energetic particle (SEP) event at Earth, both LETs <span class="hlt">observed</span> a sudden burst of 1.6 to 15 MeV particles arriving from the Sun. The derived <span class="hlt">solar</span> emission profile, arrival directions, and energy spectrum all show that the <5 MeV particles were due to energetic neutral hydrogen atoms produced by either flare or shock-accelerated protons. RHESSI measurements of the 2.2-MeV gamma-ray line provide an estimate of the number of interacting flare-accelerated protons in this event, which leads to an improved estimate of ENA production by flare-accelerated protons. CME-driven shock acceleration is also considered. Taking into account ENA losses, we conclude that the <span class="hlt">observed</span> ENAs must have been produced in the high corona at heliocentric distances .2 <span class="hlt">solar</span> radii.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015IAUGA..2258483W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015IAUGA..2258483W"><span>Plans to <span class="hlt">Observe</span> the 2017 Total <span class="hlt">Solar</span> Eclipse from near the Path Edges</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Waring Dunham, David; Nugent, Richard; Guhl, Konrad; Bode, Hans-Joachim</p> <p>2015-08-01</p> <p>The August 21st, 2017 <span class="hlt">solar</span> eclipse provides a good opportunity, to time the totality contacts, other Baily’s bead phenomena, and <span class="hlt">observe</span> other dynamic edge phenomena, from locations near the edges of the path of totality. A good network of roads and generally favorable weather prospects means that more <span class="hlt">observers</span> will likely be able to deploy more equipment than during most previous eclipses. The value of contact and Baily’s bead timings of total <span class="hlt">solar</span> eclipses, for determining <span class="hlt">solar</span> diameter and intensity variations, was described in an earlier presentation in Focus Meeting 13. This presentation will concentrate on how <span class="hlt">observations</span> of different types that have been used during past eclipses can be made by different <span class="hlt">observers</span>, to obtain better information about the accuracy of the different types of <span class="hlt">observations</span> for determining the mean <span class="hlt">solar</span> diameter, and the systematic differences between them. A problem has been that the few <span class="hlt">observers</span> who have attempted recording Baily’s beads from path edge locations have wanted to use the latest technology, to try to record the <span class="hlt">observations</span> better, rather than try to make the <span class="hlt">observations</span> in the same ways that were used for many past eclipses. Several <span class="hlt">observers</span> trying different techniques at the same location, and doing that at several locations at different places along the path, is needed. Past techniques that we would like to compare include direct visual <span class="hlt">observation</span> (but keeping eye safety in mind); visual <span class="hlt">observation</span> of telescopically projected images; direct filtered video telescopic <span class="hlt">observations</span>; and recording the flash spectrum. There are several towns that straddle the path edges. The International Occultation Timing Association would like to mobilize people in those towns to <span class="hlt">observe</span> the eclipse from many places, to say whether or not the eclipse happened, and if it did, time it. A suitable cell phone app could be designed to report <span class="hlt">observations</span>, including the observer’s location, as was attempted for an</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=jupiter&pg=4&id=EJ449124','ERIC'); return false;" href="https://eric.ed.gov/?q=jupiter&pg=4&id=EJ449124"><span>Catch as Catch Can: The History of the Theory of Gravitational <span class="hlt">Capture</span>.</span></a></p> <p><a target="_blank" href="http://www.eric.ed.gov/ERICWebPortal/search/extended.jsp?_pageLabel=advanced">ERIC Educational Resources Information Center</a></p> <p>Osipov, Y.</p> <p>1992-01-01</p> <p>Traces cosmogonic history of <span class="hlt">solar</span> system from Laplace's hypothesis of revolving gas nebulae, to Newton's two-body problem with its mathematical impossibility of gravitational <span class="hlt">capture</span>, to the isosceles three-body problem of Schmidt and Sitnikov with its notion of partial <span class="hlt">capture</span>, and finally to the total <span class="hlt">capture</span> model of Alexeyev verified by the…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMSA21B2520D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMSA21B2520D"><span>Modeling of the Ionospheric Scintillation and Total Electron Content <span class="hlt">Observations</span> during the 21 August 2017 Total <span class="hlt">Solar</span> Eclipse</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Datta-Barua, S.; Gachancipa, J. N.; Deshpande, K.; Herrera, J. A.; Lehmacher, G. A.; Su, Y.; Gyuk, G.; Bust, G. S.; Hampton, D. L.</p> <p>2017-12-01</p> <p>High concentration of free electrons in the ionosphere can cause fluctuations in incoming electromagnetic waves, such as those from the different Global Navigation Satellite Systems (GNSS). The behavior of the ionosphere depends on time and location, and it is highly influenced by <span class="hlt">solar</span> activity. The purpose of this study is to determine the impact of a total <span class="hlt">solar</span> eclipse on the local ionosphere in terms of ionospheric scintillations, and on the global ionosphere in terms of TEC (Total Electron Content). The studied eclipse occurred on 21 August 2017 across the continental United States. During the eclipse, we expected to see a decrease in the scintillation strength, as well as in the TEC values. As a broader impact part of our recently funded NSF proposal, we temporarily deployed two GNSS receivers on the eclipse's totality path. One GNSS receiver was placed in Clemson, SC. This is a multi-frequency GNSS receiver (NovAtel GPStation-6) capable of measuring high and low rate scintillation data as well as TEC values from four different GNSS systems. We had the receiver operating before, during, and after the <span class="hlt">solar</span> eclipse to enable the comparison between eclipse and non-eclipse periods. A twin receiver collected data at Daytona Beach, FL during the same time, where an 85% partial <span class="hlt">solar</span> eclipse was <span class="hlt">observed</span>. Additionally, we set up a ground receiver onsite in the path of totality in Perryville, Missouri, from which the Adler Planetarium of Chicago launched a high-altitude balloon to <span class="hlt">capture</span> a 360-degree video of the eclipse from the stratosphere. By analyzing the collected data, this study looks at the effects of partial and total <span class="hlt">solar</span> eclipse periods on high rate GNSS scintillation data at mid-latitudes, which had not been explored in detail. This study also explores the impact of <span class="hlt">solar</span> eclipses on signals from different satellite constellations (GPS, GLONASS, and Galileo). Throughout the eclipse, the scintillation values did not appear to have dramatic changes</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19920012700','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19920012700"><span>Millimeter and hard x ray/gamma ray <span class="hlt">observations</span> of <span class="hlt">solar</span> flares during the June 1991 GRO campaign</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kundu, M. R.; White, S. M.; Gopalswamy, N.; Lim, J.</p> <p>1992-01-01</p> <p>We have carried out high-spatial-resolution millimeter <span class="hlt">observations</span> of <span class="hlt">solar</span> flares using the Berkeley-Illinois-Maryland Array (BIMA). At the present time, BIMA consists of only three elements, which is not adequate for mapping highly variable <span class="hlt">solar</span> phenomena, but is excellent for studies of the temporal structure of flares at millimeter wavelengths at several different spatial scales. We present BIMA <span class="hlt">observations</span> made during the Gamma Ray Observatories (GRO)/<span class="hlt">Solar</span> Max 1991 campaign in Jun. 1991 when <span class="hlt">solar</span> activity was unusually high. Our <span class="hlt">observations</span> covered the period 8-9 Jun. 1991; this period overlapped the period 4-15 Jun. when the Compton Telescope made the Sun a target of opportunity because of the high level of <span class="hlt">solar</span> activity.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20170003785&hterms=lack+exercise&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dlack%2Bexercise','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20170003785&hterms=lack+exercise&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dlack%2Bexercise"><span>Anomalous Temporal Behaviour of Broadband Ly Alpha <span class="hlt">Observations</span> During <span class="hlt">Solar</span> Flares from SDO/EVE</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Milligan, Ryan O.; Chamberlin, Phillip C.</p> <p>2016-01-01</p> <p>Although it is the most prominent emission line in the <span class="hlt">solar</span> spectrum, there has been a notable lack of studies devoted to variations in Lyman-alpha (Ly-alpha) emission during <span class="hlt">solar</span> flares in recent years. However, the few examples that do exist have shown Ly-alpha emission to be a substantial radiator of the total energy budget of <span class="hlt">solar</span> flares (of the order of 10 percent). It is also a known driver of fluctuations in the Earth's ionosphere. The EUV (Extreme Ultra-Violet) Variability Experiment (EVE) on board the <span class="hlt">Solar</span> Dynamics Observatory (SDO) now provides broadband, photometric Ly-alpha data at 10-second cadence with its Multiple EUV Grating Spectrograph-Photometer (MEGS-P) component, and has <span class="hlt">observed</span> scores of <span class="hlt">solar</span> flares in the 5 years since it was launched. However, the MEGS-P time profiles appear to display a rise time of tens of minutes around the time of the flare onset. This is in stark contrast to the rapid, impulsive increase <span class="hlt">observed</span> in other intrinsically chromospheric features (H-alpha, Ly-beta, LyC, C III, etc.). Furthermore, the emission detected by MEGS-P peaks around the time of the peak of thermal soft X-ray emission and not during the impulsive phase when energy deposition in the chromosphere (often assumed to be in the form of non-thermal electrons) is greatest. The time derivative of Ly-alpha lightcurves also appears to resemble that of the time derivative of soft X-rays, reminiscent of the Neupert effect. Given that spectrally-resolved Ly-alpha <span class="hlt">observations</span> during flares from SORCE / SOLSTICE (<span class="hlt">Solar</span> Radiation and Climate Experiment / <span class="hlt">Solar</span> Stellar Irradiance Comparison Experiment) peak during the impulsive phase as expected, this suggests that the atypical behaviour of MEGS-P data is a manifestation of the broadband nature of the <span class="hlt">observations</span>. This could imply that other lines andor continuum emission that becomes enhanced during flares could be contributing to the passband. Users are hereby urged to exercise caution when interpreting</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20030111605&hterms=poster+elements&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dposter%2Belements','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20030111605&hterms=poster+elements&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dposter%2Belements"><span><span class="hlt">Solar</span> System <span class="hlt">Observing</span> with the Space Infrared Telescope Facility (SIRTF)</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Cleve, J. Van; Meadows, V. S.; Stansberry, J.</p> <p>2003-01-01</p> <p>SIRTF is NASA's Space Infrared Telescope Facility. Currently planned for launch on 15 Apr 2003, it is the final element in NASA's Great Observatories Program. SIRTF has an 85 cm diameter f/12 lightweight beryllium telescope, cooled to lekss than 5.5K. It is diffraction-limited at 6.5 microns, and has wavelengthcoverage from 3-180 microns. Its estimated lifetime (limited by cryogen) is 2.5 years at minimum, with a goal of 5+ years. SIRTF has three instruments, IRAC, IRS, and MIPS. IRAC (InfraRed Array Camera) provides simultaneous images at wavelengths of 3.6, 4.5, 5.8, and 8.0 microns. IRS (InfraRed Spectrograph) has 4 modules providing low-resolution (R=60-120) spectra from 5.3 to 40 microns, high-resolution (R=600) spectra from 10 to 37 microns, and an autonomous target acquisition system (PeakUp) which includes small-field imaging at 15 microns. MIPS (Multiband Imaging Photometer for SIRTF)} does imaging photometry at 24, 70, and 160 m and low-resolution (R=15-25) spectroscopy (SED) between 55 and 96 microns. The SIRTF Guaranteed Time <span class="hlt">Observers</span> (GTOs) are planning to <span class="hlt">observe</span> Outer <span class="hlt">Solar</span> System satellites and planets, extinct comets and low-albedo asteroids, Centaurs and Kuiper Belt Objects, cometary dust trails, and a few active short-period comets. The GTO programs are listed in detail in the SIRTF Reserved <span class="hlt">Observations</span> Catalog (ROC). We would like to emphasize that there remain many interesting subjects for the General <span class="hlt">Observers</span> (GO). Proposal success for the planetary <span class="hlt">observer</span> community in the first SIRTF GO proposal cycle (GO-1) determines expectations for future GO calls and <span class="hlt">Solar</span> System use of SIRTF, so we would like promote a strong set of planetary GO-1 proposals. Towards that end, we present this poster, and we will convene a <span class="hlt">Solar</span> System GO workshop 3.5 months after launch.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19890045672&hterms=lazarus&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAuthor-Name%26N%3D0%26No%3D90%26Ntt%3Dlazarus','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19890045672&hterms=lazarus&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAuthor-Name%26N%3D0%26No%3D90%26Ntt%3Dlazarus"><span>Pioneer and Voyager <span class="hlt">observations</span> of the <span class="hlt">solar</span> wind at large heliocentric distances and latitudes</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Gazis, P. R.; Mihalov, J. D.; Barnes, A.; Lazarus, A. J.; Smith, E. J.</p> <p>1989-01-01</p> <p>Data obtained from the electrostatic analyzers aboard the Pioneer 10 and 11 spacecraft and from the Faraday cup aboard Voyager 2 were used to study spatial gradients in the distant <span class="hlt">solar</span> wind. Prior to mid-1985, both spacecraft <span class="hlt">observed</span> nearly identical <span class="hlt">solar</span> wind structures. After day 150 of 1985, the velocity structure at Voyager 2 became flatter, and the Voyager 2 velocities were smaller than those <span class="hlt">observed</span> by Pioneer 11. It is suggested that these changes in the <span class="hlt">solar</span> wind at low latitudes may be related to a change which occurred in the coronal hole structure in early 1985.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20110011240','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20110011240"><span>Thermodynamics of the <span class="hlt">Solar</span> Corona and Evolution of the <span class="hlt">Solar</span> Magnetic Field as Inferred from the Total <span class="hlt">Solar</span> Eclipse <span class="hlt">Observations</span> of 11 July 2010</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Habbal, Shadia Rifai; Druckmueller, Miloslav; Morgan, Huw; Ding, Adalbert; Johnson, Judd; Druckmuellerova, Hana; Daw, Adrian; Arndt, Martina B.; Dietzel, Martin; Saken, Jon</p> <p>2011-01-01</p> <p>We report on multi-wavelength <span class="hlt">observations</span> of the corona taken simultaneously in broadband white light, and in seven spectral lines, H-alpha 656.3 nm, Fe IX 435.9 nm, Fe X 637.4 nm, Fe XI 789.2 nm, Fe XIII 1074.7 nm, Fe XIV 530.3 nm and Ni XV 670.2 nm. The <span class="hlt">observations</span> were made during the total <span class="hlt">solar</span> eclipse of 11 July 2010 from the atoll of Tatakoto in French Polynesia. Simultaneous imaging with narrow bandpass filters in each of these spectral lines and in their corresponding underlying continua maximized the <span class="hlt">observing</span> time during less than ideal <span class="hlt">observing</span> conditions and yielded outstanding quality data. The application of two complementary image processing techniques revealed the finest details of coronal structures at 1" resolution in white light, and 6.5" in each of the spectral lines. This comprehensive wavelength coverage confirmed earlier eclipse findings that the <span class="hlt">solar</span> corona has a clear two-temperature structure: The open field lines, expanding outwards from the <span class="hlt">solar</span> surface, are characterized by electron temperatures near 1 X 10(exp 6) K, while the hottest plasma around 2X 10(exp 6) K resides in loop-like structures forming the bulges of streamers. The first images of the corona in the forbidden lines of Fe IX and Ni XV, showed that there was very little coronal plasma at temperatures below 5 X 10(exp 5) K and above 2.5X 10(exp 6) K. The data also enabled temperature differentiations as low as 0:2 X 10(exp 6) K in different density structures. These <span class="hlt">observations</span> showed how the passage of CMEs through the corona, prior to totality, produced large scale ripples and very sharp streaks, which could be identified with distinct temperatures for the first time. The ripples were most prominent in emission from spectral lines associated with temperatures around 10(exp 6) K. The most prominent streak was associated with a conical-shaped void in the emission from the coolest line of Fe IX and from the hottest line of Ni XV. A prominence, which erupted prior to</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMSM41D2461N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMSM41D2461N"><span>Diamagnetic effect in the foremoon <span class="hlt">solar</span> wind <span class="hlt">observed</span> by Kaguya</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Nishino, M. N.; Saito, Y.; Tsunakawa, H.; Miyake, Y.; Harada, Y.; Yokota, S.; Takahashi, F.; Matsushima, M.; Shibuya, H.; Shimizu, H.</p> <p>2016-12-01</p> <p>Interaction between the lunar surface and incident <span class="hlt">solar</span> wind is one of the crucial phenomena of the lunar plasma sciences. Recent <span class="hlt">observations</span> by lunar orbiters revealed that strength of the interplanetary magnetic field (IMF) at spacecraft altitude increases over crustal magnetic fields on the dayside. In addition, variations of the IMF on the lunar night side have been reported in the viewpoint of diamagnetic effect around the lunar wake. However, few studies have been performed for the IMF over non-magnetized regions on the dayside. Here we show an event where strength of the IMF decreases at 100 km altitude on the lunar dayside (i.e. in the foremoon <span class="hlt">solar</span> wind) when the IMF is almost parallel to the incident <span class="hlt">solar</span> wind flow, comparing the upstream <span class="hlt">solar</span> wind data from ACE and WIND with Kaguya magnetometer data. The lunar surface below the Kaguya orbit is not magnetized (or very weakly magnetized), and the sunward-travelling protons show signatures of those back-scattered at the lunar surface. We find that the decrease in the magnetic pressure is compensated by the thermal pressure of the back-scattered protons. In other words, the IMF strength in the foremoon <span class="hlt">solar</span> wind decreases by diamagnetic effect of sunward-travelling protons back-scattered at the lunar dayside surface. Such diamagnetic effect would be prominent in the high-beta <span class="hlt">solar</span> wind environment, and may be ubiquitous in the environment where planetary surface directly interacts with surrounding space plasma.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..19.5995N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..19.5995N"><span>Diamagnetic effect in the foremoon <span class="hlt">solar</span> wind <span class="hlt">observed</span> by Kaguya</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Nishino, Masaki N.; Saito, Yoshifumi; Tsunakawa, Hideo; Miyake, Yohei; Harada, Yuki; Yokota, Shoichiro; Takahashi, Futoshi; Matsushima, Masaki; Shibuya, Hidetoshi; Shimizu, Hisayoshi</p> <p>2017-04-01</p> <p>Direct interaction between the lunar surface and incident <span class="hlt">solar</span> wind is one of the crucial phenomena of the planetary plasma sciences. Recent <span class="hlt">observations</span> by lunar orbiters revealed that strength of the interplanetary magnetic field (IMF) at spacecraft altitude often increases over crustal magnetic fields on the dayside. In addition, variations of the IMF on the lunar night side have been reported in the viewpoint of diamagnetic effect around the lunar wake. However, few studies have been performed for the IMF over non-magnetized regions on the dayside. Here we show an event where strength of the IMF decreases at 100 km altitude on the lunar dayside (i.e. in the foremoon <span class="hlt">solar</span> wind) when the IMF is almost parallel to the incident <span class="hlt">solar</span> wind flow, comparing the upstream <span class="hlt">solar</span> wind data from ACE with Kaguya magnetometer data. The lunar surface below the Kaguya orbit is not magnetized (or very weakly magnetized), and the sunward-travelling protons show signatures of those back-scattered at the lunar surface. We find that the decrease in the magnetic pressure is compensated by the thermal pressure of the back-scattered protons. In other words, the IMF strength in the foremoon <span class="hlt">solar</span> wind decreases by diamagnetic effect of sunward-travelling protons back-scattered at the lunar dayside surface. Such an effect would be prominent in the high-beta <span class="hlt">solar</span> wind, and may be ubiquitous in the environment where planetary surface directly interacts with surrounding space plasma.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009AGUFM.P21A1202S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009AGUFM.P21A1202S"><span>Modeling the <span class="hlt">Solar</span> Probe Plus Dust Environment: Comparison with MESSENGER <span class="hlt">Observations</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Strong, S. B.; Strikwerda, T.</p> <p>2009-12-01</p> <p>NASA’s <span class="hlt">Solar</span> Probe Plus mission will be the first to approach the Sun as close as 9 <span class="hlt">solar</span> radii from the surface. This mission will provide the only in-situ <span class="hlt">observations</span> of the Sun’s corona. In the absence of <span class="hlt">observational</span> data (e.g. Helios, Pioneer), specifically at distances less than 0.4 AU, the precise ambient dust distributions at these distances remain unknown and limited to extrapolative models for distances < 1 AU (e.g. Mann et al. 2004). For the <span class="hlt">Solar</span> Probe Plus mission, it has become critical to characterize the inner <span class="hlt">solar</span> system dust environment in order to examine potential impacts on spacecraft health and attitude. We have implemented the Mann et al. (2004) and Grün et al. (1985) dust distribution theory along with Mie scattering effects to determine the magnitude of <span class="hlt">solar</span> irradiance scattered towards an optical sensor such as a star tracker as a function of ecliptic latitude and longitude for distances 0.05 to 1 AU. Background irradiance data from NASA’s MESSENGER mission (down to 0.3 AU) reveal trends consistent with our model predictions, potentially validating Mann et al. (2004) and Grün et al. (1985) theory, but perhaps suggesting an enhancement of dust density short ward of 0.3 AU. This paper will present the scattering model and analysis of MESSENGER data gathered to date, during the phasing orbits, and includes star tracker background irradiance, irradiance distribution over the sky, and effects on star magnitude sensitivity and position accuracy.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2001JASTP..63.1729T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2001JASTP..63.1729T"><span><span class="hlt">Solar</span> flare induced ionospheric D-region enhancements from VLF amplitude <span class="hlt">observations</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Thomson, N. R.; Clilverd, M. A.</p> <p>2001-11-01</p> <p>Enhancements of D-region electron densities caused by <span class="hlt">solar</span> flares are determined from <span class="hlt">observations</span> of VLF subionospheric amplitude changes and these enhancements are then related to the magnitudes of the X-ray fluxes measured by the GOES satellites. The electron densities are characterised by the two traditional parameters, /H' and /β (being measures of the ionospheric height and the rate of increase of electron density with height, respectively), which are found by VLF radio modelling of the <span class="hlt">observed</span> amplitudes using the NOSC Earth-ionosphere waveguide programs (LWPC and Modefinder) mainly on two paths, one short and one long. The short path measurements were made near Cambridge, UK, on the 18.3kHz signals from the French transmitter 617km to the south while the long path measurements were made near Dunedin, NZ, on the 24.8kHz signals from NLK in Seattle, USA, 12.3Mm across the Pacific Ocean. The <span class="hlt">observations</span> include flares up to a magnitude of about M5 (5×10-5Wm-2 at 0.1-0.8nm) which gave VLF amplitude enhancements up to about 8dB; these corresponded, under near <span class="hlt">solar</span> maximum conditions (1992), to a reduction in /H' from about 71km down to about 63km and an increase in /β from 0.43km-1 up to about 0.49km-1. The increased values of /β during a flare are caused by the <span class="hlt">solar</span> X-rays dominating all sources of ionisation during the flare in contrast with the normal unperturbed daytime values of /β which are significantly lower than for a single <span class="hlt">solar</span> UV or X-ray source due to the extra electrons from the normal galactic cosmic ray ionisation in the lowest parts of the D-region. This steady, normal (unperturbed) cosmic ray influence on /β, and hence unperturbed VLF attenuation, is more marked at times of reduced <span class="hlt">solar</span> Lyman-/α flux in the D-region such as at <span class="hlt">solar</span> minimum, high latitudes or early or late in the day, thus explaining the normal (unperturbed) higher VLF attenuation rates previously reported in these conditions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20170003267&hterms=theory+everything&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dtheory%2Beverything','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20170003267&hterms=theory+everything&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dtheory%2Beverything"><span><span class="hlt">Solar</span> Coronal Jets: <span class="hlt">Observations</span>, Theory, and Modeling</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Raouafi, N. E.; Patsourakos, S.; Pariat, E.; Young, P. R.; Sterling, A. C.; Savcheva, A.; Shimojo, M.; Moreno-Insertis, F.; DeVore, C. R.; Archontis, V.; <a style="text-decoration: none; " href="javascript:void(0); " onClick="displayelement('author_20170003267'); toggleEditAbsImage('author_20170003267_show'); toggleEditAbsImage('author_20170003267_hide'); "> <img style="display:inline; width:12px; height:12px; " src="images/arrow-up.gif" width="12" height="12" border="0" alt="hide" id="author_20170003267_show"> <img style="width:12px; height:12px; display:none; " src="images/arrow-down.gif" width="12" height="12" border="0" alt="hide" id="author_20170003267_hide"></p> <p>2016-01-01</p> <p>Coronal jets represent important manifestations of ubiquitous <span class="hlt">solar</span> transients, which may be the source of significant mass and energy input to the upper <span class="hlt">solar</span> atmosphere and the <span class="hlt">solar</span> wind. While the energy involved in a jet-like event is smaller than that of "nominal" <span class="hlt">solar</span> flares and coronal mass ejections (CMEs), jets share many common properties with these phenomena, in particular, the explosive magnetically driven dynamics. Studies of jets could, therefore, provide critical insight for understanding the larger, more complex drivers of the <span class="hlt">solar</span> activity. On the other side of the size-spectrum, the study of jets could also supply important clues on the physics of transients close or at the limit of the current spatial resolution such as spicules. Furthermore, jet phenomena may hint to basic process for heating the corona and accelerating the <span class="hlt">solar</span> wind; consequently their study gives us the opportunity to attack a broad range of <span class="hlt">solar</span>-heliospheric problems.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20170003317','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20170003317"><span><span class="hlt">Solar</span> Coronal Jets: <span class="hlt">Observations</span>, Theory, and Modeling</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Raouafi, N. E.; Patsourakos, S.; Pariat, E.; Young, P. R.; Sterling, A.; Savcheva, A.; Shimojo, M.; Moreno-Insertis, F.; Devore, C. R.; Archontis, V.; <a style="text-decoration: none; " href="javascript:void(0); " onClick="displayelement('author_20170003317'); toggleEditAbsImage('author_20170003317_show'); toggleEditAbsImage('author_20170003317_hide'); "> <img style="display:inline; width:12px; height:12px; " src="images/arrow-up.gif" width="12" height="12" border="0" alt="hide" id="author_20170003317_show"> <img style="width:12px; height:12px; display:none; " src="images/arrow-down.gif" width="12" height="12" border="0" alt="hide" id="author_20170003317_hide"></p> <p>2016-01-01</p> <p>Chromospheric and coronal jets represent important manifestations of ubiquitous <span class="hlt">solar</span> transients, which may be the source of signicant mass and energy input to the upper <span class="hlt">solar</span> atmosphere and the <span class="hlt">solar</span> wind. While the energy involved in a jet-like event is smaller than that of nominal <span class="hlt">solar</span> ares and Coronal Mass Ejections (CMEs), jets share many common properties with these major phenomena, in particular, the explosive magnetically driven dynamics. Studies of jets could, therefore, provide critical insight for understanding the larger, more complex drivers of the <span class="hlt">solar</span> activity. On the other side of the size-spectrum, the study of jets could also supply important clues on the physics of transients closeor at the limit of the current spatial resolution such as spicules. Furthermore, jet phenomena may hint to basic process for heating the corona and accelerating the <span class="hlt">solar</span> wind; consequently their study gives us the opportunity to attack a broadrange of <span class="hlt">solar</span>-heliospheric problems.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22270641-swap-observations-long-term-large-scale-evolution-extreme-ultraviolet-solar-corona','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22270641-swap-observations-long-term-large-scale-evolution-extreme-ultraviolet-solar-corona"><span>SWAP <span class="hlt">OBSERVATIONS</span> OF THE LONG-TERM, LARGE-SCALE EVOLUTION OF THE EXTREME-ULTRAVIOLET <span class="hlt">SOLAR</span> CORONA</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>Seaton, Daniel B.; De Groof, Anik; Berghmans, David</p> <p></p> <p>The Sun Watcher with Active Pixels and Image Processing (SWAP) EUV <span class="hlt">solar</span> telescope on board the Project for On-Board Autonomy 2 spacecraft has been regularly <span class="hlt">observing</span> the <span class="hlt">solar</span> corona in a bandpass near 17.4 nm since 2010 February. With a field of view of 54 × 54 arcmin, SWAP provides the widest-field images of the EUV corona available from the perspective of the Earth. By carefully processing and combining multiple SWAP images, it is possible to produce low-noise composites that reveal the structure of the EUV corona to relatively large heights. A particularly important step in this processing was tomore » remove instrumental stray light from the images by determining and deconvolving SWAP's point-spread function from the <span class="hlt">observations</span>. In this paper, we use the resulting images to conduct the first-ever study of the evolution of the large-scale structure of the corona <span class="hlt">observed</span> in the EUV over a three year period that includes the complete rise phase of <span class="hlt">solar</span> cycle 24. Of particular note is the persistence over many <span class="hlt">solar</span> rotations of bright, diffuse features composed of open magnetic fields that overlie polar crown filaments and extend to large heights above the <span class="hlt">solar</span> surface. These features appear to be related to coronal fans, which have previously been <span class="hlt">observed</span> in white-light coronagraph images and, at low heights, in the EUV. We also discuss the evolution of the corona at different heights above the <span class="hlt">solar</span> surface and the evolution of the corona over the course of the <span class="hlt">solar</span> cycle by hemisphere.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUFMSM52C..07C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUFMSM52C..07C"><span>Calculating Coronal Mass Ejection Magnetic Field at 1 AU Using <span class="hlt">Solar</span> <span class="hlt">Observables</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chen, J.; Kunkel, V.</p> <p>2013-12-01</p> <p>It is well-established that most major nonrecurrent geomagnetic storms are caused by <span class="hlt">solar</span> wind structures with long durations of strong southward (Bz < 0) interplanetary magnetic field (IMF). Such geoeffective IMF structures are associated with CME events at the Sun. Unfortunately, neither the duration nor the internal magnetic field vector of the ejecta--the key determinants of geoeffectiveness--is measurable until the <span class="hlt">observer</span> (e.g., Earth) passes through the ejecta. In this paper, we discuss the quantitative relationships between the ejecta magnetic field at 1 AU and remotely <span class="hlt">observable</span> <span class="hlt">solar</span> quantities associated with the eruption of a given CME. In particular, we show that <span class="hlt">observed</span> CME trajectories (position-time data) within, say, 1/3 AU of the Sun, contain sufficient information to allow the calculation of the ejecta magnetic field (magnitude and components) at 1 AU using the Erupting Flux Rope (EFR) model of CMEs. Furthermore, in order to accurately determine the size and arrival time of the ejecta as seen by a fixed <span class="hlt">observer</span> at 1 AU (e.g., ACE), it is essential to accurately calculate the three-dimensional geometry of the underlying magnetic structure. Accordingly, we have extended the physics-based EFR model to include a self-consistent calculation of the transverse expansion taking into account the non-symmetric drag coupling between an expanding CME flux rope and the ambient <span class="hlt">solar</span> wind. The dependence of the minor radius of the flux rope at 1 AU that determines the perceived size of the ejecta on <span class="hlt">solar</span> quantities is discussed. Work supported by the NRL Base Program.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19900003143','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19900003143"><span>Max '91 Workshop 2: Developments in <span class="hlt">Observations</span> and Theory for <span class="hlt">Solar</span> Cycle 22</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Winglee, Robert M. (Editor); Dennis, Brian R. (Editor)</p> <p>1989-01-01</p> <p>Papers and observatory reports presented at the second workshop of the Max '91 program are compiled along with discussion group summaries and invited reviews. The four discussion groups addressed the following subjects: high-energy flare physics; coordinated magnetograph <span class="hlt">observations</span>; flare theory and modeling; and Max '91 communications and coordination. A special session also took place on <span class="hlt">observations</span> of Active Region 5395 and the associated flares of March 1989. Other topics covered during the workshop include the scientific objectives of <span class="hlt">solar</span> gamma ray <span class="hlt">observations</span>, the <span class="hlt">solar</span> capabilities of each of the four instruments on the Gamma Ray Observatory, and access to Max '91 information.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/17832984','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/17832984"><span>Initial <span class="hlt">observations</span> of the pioneer venus orbiter <span class="hlt">solar</span> wind plasma experiment.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Wolfe, J; Intriligator, D S; Mihalov, J; Collard, H; McKibbin, D; Whitten, R; Barnes, A</p> <p>1979-02-23</p> <p>Initial results of <span class="hlt">observations</span> of the <span class="hlt">solar</span> wind interaction with Venus indicate that Venus has a well-defined, strong, standing bow shock wave. Downstream from the shock, an ionosheath is <span class="hlt">observed</span> in which the compressed and heated postshock plasma evidently interacts directly with the Venus ionosphere. Plasma ion velocity deflections <span class="hlt">observed</span> within the ionosheath are consistent with flow around the blunt shape of the ionopause. The ionopause boundary is <span class="hlt">observed</span> and defined by this experiment as the location where the ionosheath ion flow is first excluded. The positions of the bow shock and ionopause are variable and appear to respond to changes in the external <span class="hlt">solar</span> wind pressure. Near the terminator the bow shock was <span class="hlt">observed</span> at altitudes of approximately 4600 to approximately 12,000 kilometers. The ionopause altitutde ranged fromn as low as approximately 450 to approximately 1950 kilometers. Within the Venus ionosphere low-energy ions (energy per untit charge < 30 volts) were detected and have been tentatively idtentified as nonflowing ionospheric ions incident from a direction along the spacecraft velocity vector.</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/2013AGUFMSH42A..05T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUFMSH42A..05T"><span><span class="hlt">Observation</span> of Alfven Waves in the <span class="hlt">Solar</span> Corona (Invited)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tomczyk, S.</p> <p>2013-12-01</p> <p>I will review the extensive progress made in recent years on the <span class="hlt">observation</span> of Alfven waves in the <span class="hlt">solar</span> corona, with an emphasis on the measurements made with the Coronal Multi-channel Polarimeter. Application of the wave measurements to coronal seismology will be presented. Future prospects in the field will be discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22521635-observation-simulation-solar-coronal-twin-jets','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22521635-observation-simulation-solar-coronal-twin-jets"><span>ON THE <span class="hlt">OBSERVATION</span> AND SIMULATION OF <span class="hlt">SOLAR</span> CORONAL TWIN JETS</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>Liu, Jiajia; Wang, Yuming; Zhang, Quanhao</p> <p></p> <p>We present the first <span class="hlt">observation</span>, analysis, and modeling of <span class="hlt">solar</span> coronal twin jets, which occurred after a preceding jet. Detailed analysis on the kinetics of the preceding jet reveals its blowout-jet nature, which resembles the one studied in Liu et al. However, the erupting process and kinetics of the twin jets appear to be different from the preceding one. Lacking detailed information on the magnetic fields in the twin jet region, we instead use a numerical simulation using a three-dimensional (3D) MHD model as described in Fang et al., and find that in the simulation a pair of twin jetsmore » form due to reconnection between the ambient open fields and a highly twisted sigmoidal magnetic flux, which is the outcome of the further evolution of the magnetic fields following the preceding blowout jet. Based on the similarity between the synthesized and <span class="hlt">observed</span> emission, we propose this mechanism as a possible explanation for the <span class="hlt">observed</span> twin jets. Combining our <span class="hlt">observation</span> and simulation, we suggest that with continuous energy transport from the subsurface convection zone into the corona, <span class="hlt">solar</span> coronal twin jets could be generated in the same fashion addressed above.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012A%26A...542A..70M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012A%26A...542A..70M"><span><span class="hlt">Observations</span> of quasi-periodic phenomena associated with a large blowout <span class="hlt">solar</span> jet</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Morton, R. J.; Srivastava, A. K.; Erdélyi, R.</p> <p>2012-06-01</p> <p>Aims: A variety of periodic phenomena have been <span class="hlt">observed</span> in conjunction with large <span class="hlt">solar</span> jets. We aim to find further evidence for (quasi-)periodic behaviour in <span class="hlt">solar</span> jets and determine what the periodic behaviour can tell us about the excitation mechanism and formation process of the large <span class="hlt">solar</span> jet. Methods: Using the 304 Å (He-II), 171 Å (Fe IX), 193 Å (Fe XII/XXIV) and 131 Å (Fe VIII/XXI) filters onboard the <span class="hlt">Solar</span> Dynamic Observatory (SDO) Atmospheric Imaging Assembly (AIA), we investigate the intensity oscillations associated with a <span class="hlt">solar</span> jet. Results: Evidence is provided for multiple magnetic reconnection events occurring between a pre-twisted, closed field and open field lines. Components of the jet are seen in multiple SDO/AIA filters covering a wide range of temperatures, suggesting the jet can be classified as a blowout jet. Two bright, elongated features are <span class="hlt">observed</span> to be co-spatial with the large jet, appearing at the jet's footpoints. Investigation of these features reveal they are defined by multiple plasma ejections. The ejecta display (quasi-)periodic behaviour on timescales of 50 s and have rise velocities of 40-150 km s-1 along the open field lines. Due to the suggestion that the large jet is reconnection-driven and the <span class="hlt">observed</span> properties of the ejecta, we further propose that these ejecta events are similar to type-II spicules. The bright features also display (quasi)-periodic intensity perturbations on the timescale of 300 s. Possible explanations for the existence of the (quasi-)periodic perturbations in terms of jet dynamics and the response of the transition region are discussed. Movies are available in electronic form at http://www.aanda.org</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://images.nasa.gov/#/details-GSFC_20171208_Archive_e001163.html','SCIGOVIMAGE-NASA'); return false;" href="https://images.nasa.gov/#/details-GSFC_20171208_Archive_e001163.html"><span>X-class <span class="hlt">Solar</span> Flare on March 29, 2014</span></a></p> <p><a target="_blank" href="https://images.nasa.gov/">NASA Image and Video Library</a></p> <p></p> <p>2014-03-31</p> <p>Extreme ultraviolet light streams out of an X-class <span class="hlt">solar</span> flare as seen in this image <span class="hlt">captured</span> on March 29, 2014, by NASA's <span class="hlt">Solar</span> Dynamics Observatory. This image blends two wavelengths of light: 304 and 171 Angstroms, which help scientists <span class="hlt">observe</span> the lower levels of the sun's atmosphere. More info: The sun emitted a significant <span class="hlt">solar</span> flare, peaking at 1:48 p.m. EDT March 29, 2014, and NASA's <span class="hlt">Solar</span> Dynamics Observatory <span class="hlt">captured</span> images of the event. <span class="hlt">Solar</span> flares are powerful bursts of radiation. Harmful radiation from a flare cannot pass through Earth's atmosphere to physically affect humans on the ground, however -- when intense enough -- they can disturb the atmosphere in the layer where GPS and communications signals travel. To see how this event impacted Earth, please visit NOAA's Space Weather Prediction Center at spaceweather.gov, the U.S. government's official source for space weather forecasts, alerts, watches and warnings. This flare is classified as an X.1-class flare. X-class denotes the most intense flares, while the number provides more information about its strength. An X2 is twice as intense as an X1, an X3 is three times as intense, etc. Credit: NASA/SDO NASA image use policy. NASA Goddard Space Flight Center enables NASA’s mission through four scientific endeavors: Earth Science, Heliophysics, <span class="hlt">Solar</span> System Exploration, and Astrophysics. Goddard plays a leading role in NASA’s accomplishments by contributing compelling scientific knowledge to advance the Agency’s mission. Follow us on Twitter Like us on Facebook Find us on Instagram</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2004cosp...35.2259P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2004cosp...35.2259P"><span>3D <span class="hlt">Observations</span> techniques for the <span class="hlt">solar</span> corona</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Portier-Fozzani, F.; Papadopoulo, T.; Fermin, I.; Bijaoui, A.; Stereo/Secchi 3D Team; et al.</p> <p></p> <p>In this talk, we will present a review of the different 3D techniques concerning <span class="hlt">observations</span> of the <span class="hlt">solar</span> corona made by EUV imageur (such as SOHO/EIT and STEREO/SECCHI) and by coronagraphs (SOHO/LASCO and STEREO/SECCHI). Tomographic reconstructions need magnetic extrapolation to constraint the model (classical triangle mash reconstruction, or more evoluated pixon method). For 3D reconstruction the other approach is stereovision. Stereoscopic techniques are built in a specific way to take into account the optical thin medium of the <span class="hlt">solar</span> corona, which makes most of the classical stereo method not directly applicable. To improve such method we need to take into account how to describe an image by computer vision : an image is not only a set of intensities but its descriptions/representations in term of sub-objects is needed for the structures extractions and matching. We will describe optical flow methods to follow the structures, and decomposition in sub-areas depending of the <span class="hlt">solar</span> cycle. After recalling results obtained with geometric loops reconstructions and their consequences for twist measurement and helicity evaluation, we will describe how we can mix pixel and conceptual recontruction for stereovision. We could then include epipolar geometry and Multiscale Vision Model (MVM) to enhance the reconstruction. These concepts are under development for STEREO/SECCHI.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20140013144','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20140013144"><span><span class="hlt">Solar</span> Ion Processing of Itokawa Grains: Reconciling Model Predictions with Sample <span class="hlt">Observations</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Christoffersen, Roy; Keller, L. P.</p> <p>2014-01-01</p> <p>Analytical TEM <span class="hlt">observations</span> of Itokawa grains reported to date show complex <span class="hlt">solar</span> wind ion processing effects in the outer 30-100 nm of pyroxene and olivine grains. The effects include loss of long-range structural order, formation of isolated interval cavities or "bubbles", and other nanoscale compositional/microstructural variations. None of the effects so far described have, however, included complete ion-induced amorphization. To link the array of <span class="hlt">observed</span> relationships to grain surface exposure times, we have adapted our previous numerical model for progressive <span class="hlt">solar</span> ion processing effects in lunar regolith grains to the Itokawa samples. The model uses SRIM ion collision damage and implantation calculations within a framework of a constant-deposited-energy model for amorphization. Inputs include experimentally-measured amorphization fluences, a Pi steradian variable ion incidence geometry required for a rotating asteroid, and a numerical flux-versus-velocity <span class="hlt">solar</span> wind spectrum.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018LPICo2047.6110J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018LPICo2047.6110J"><span>Sodium Pick-Up Ion <span class="hlt">Observations</span> in the <span class="hlt">Solar</span> Wind Upstream of Mercury</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jasinski, J. M.; Raines, J. M.; Slavin, J. A.; Regoli, L. R.; Murphy, N.</p> <p>2018-05-01</p> <p>We present the first <span class="hlt">observations</span> of sodium pick-up ions upstream of Mercury’s magnetosphere. From these <span class="hlt">observations</span> we infer properties of Mercury’s sodium exosphere and implications for the <span class="hlt">solar</span> wind interaction with Mercury’s magnetosphere.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018AAS...23115807M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018AAS...23115807M"><span>Multi-wavelength <span class="hlt">Observations</span> of <span class="hlt">Solar</span> Acoustic Waves Near Active Regions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Monsue, Teresa; Pesnell, Dean; Hill, Frank</p> <p>2018-01-01</p> <p>Active region areas on the Sun are abundant with a variety of waves that are both acoustically helioseismic and magnetohydrodynamic in nature. The occurrence of a <span class="hlt">solar</span> flare can disrupt these waves, through MHD mode-mixing or scattering by the excitation of these waves. We take a multi-wavelength <span class="hlt">observational</span> approach to understand the source of theses waves by studying active regions where flaring activity occurs. Our approach is to search for signals within a time series of images using a Fast Fourier Transform (FFT) algorithm, by producing multi-frequency power map movies. We study active regions both spatially and temporally and correlate this method over multiple wavelengths using data from NASA’s <span class="hlt">Solar</span> Dynamics Observatory. By surveying the active regions on multiple wavelengths we are able to <span class="hlt">observe</span> the behavior of these waves within the <span class="hlt">Solar</span> atmosphere, from the photosphere up through the corona. We are able to detect enhancements of power around active regions, which could be acoustic power halos and of an MHD-wave propagating outward by the flaring event. We are in the initial stages of this study understanding the behaviors of these waves and could one day contribute to understanding the mechanism responsible for their formation; that has not yet been explained.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2006cosp...36.2514S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006cosp...36.2514S"><span><span class="hlt">Solar</span> <span class="hlt">observations</span> with the prototype of the Brazilian Decimetric Array</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sawant, H. S.; Ramesh, R.; Faria, C.; Cecatto, J. R.; Fernandes, F. C. R.; Madsen, F. H. R.; Subramanian, K. R.; Sundararajan, M. S.</p> <p></p> <p>The prototype of the Brazilian Decimetric Array BDA consists of 5 element alt-az mounted parabolic mesh type dishes of 4-meter diameter having base lines up to 220 meters in the E--W direction The array was put into regular operation at Cachoeira Paulista Brazil longitude 45 r 00 20 W and latitude 22 r 41 19 S This array operates in the frequency range of 1 2 -- 1 7 GHz <span class="hlt">Solar</span> <span class="hlt">observations</span> are carried at sim 1 4 GHz in transit and tracking modes Spatial fine structures superimposed on the one dimensional brightness map of the sun associated with active regions and or with <span class="hlt">solar</span> activity and their time evolution will be presented In the second phase of the project the frequency range will be increased to 1 2 - 1 7 2 8 and 5 6 GHz Central part of the array will consist of 26 antennas with 4-meter diameter laid out randomically in the square of 256 by 256 meter with minimum and maximum base lines of 8 and 256 meters respectively Details of this array with imaging capabilities in snap shot mode for <span class="hlt">solar</span> <span class="hlt">observations</span> and procedure of the phase and amplitude calibrations will be presented The development of instrument will be completed by the beginning of 2008</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/4238994-observations-low-energy-solar-cosmic-rays-from-flare-august','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/4238994-observations-low-energy-solar-cosmic-rays-from-flare-august"><span><span class="hlt">OBSERVATIONS</span> OF LOW ENERGY <span class="hlt">SOLAR</span> COSMIC RAYS FROM THE FLARE OF AUGUST 22, 1958</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>Anderson, K.A.; Arnoldy, R.; Hoffman, R.</p> <p>1959-10-31</p> <p><span class="hlt">Observations</span> were made of protons at balloon altitudes in the energy range 100 to 300 Mev following a <span class="hlt">solar</span> sequence of optical flare, r-f noise bursts, and long enduring noise storm. Other particles are shown to have low upper limits to their abundance. The flare particles continue to be <span class="hlt">observed</span> for at least 2 days and arguments are given to show that their storage and emission takes place in the <span class="hlt">solar</span> atmosphere. The differential energy spectrum is derived from ionization versus atmospheric depth data and is found to be E/sup -5/ dE. <span class="hlt">Observations</span> by riometer and VHF scatter propagation pathsmore » over the polar regions indicate that <span class="hlt">solar</span> acceleration of protons up to roughly 100 Mev energy is rather frequent. (auth)« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4316871','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4316871"><span><span class="hlt">Capturing</span> the complexity of first opinion small animal consultations using direct <span class="hlt">observation</span></span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Robinson, N. J.; Brennan, M. L.; Cobb, M.; Dean, R. S.</p> <p>2015-01-01</p> <p>Various different methods are currently being used to <span class="hlt">capture</span> data from small animal consultations. The aim of this study was to develop a tool to record detailed data from consultations by direct <span class="hlt">observation</span>. A second aim was to investigate the complexity of the consultation by examining the number of problems discussed per patient. A data collection tool was developed and used during direct <span class="hlt">observation</span> of small animal consultations in eight practices. Data were recorded on consultation type, patient signalment and number of problems discussed. During 16 weeks of data collection, 1901 patients were presented. Up to eight problems were discussed for some patients; more problems were discussed during preventive medicine consultations than during first consultations (P<0.001) or revisits (P<0.001). Fewer problems were discussed for rabbits than cats (P<0.001) or dogs (P<0.001). Age was positively correlated with discussion of specific health problems and negatively correlated with discussion of preventive medicine. Consultations are complex with multiple problems frequently discussed, suggesting comorbidity may be common. Future research utilising practice data should consider how much of this complexity needs to be <span class="hlt">captured</span>, and use appropriate methods accordingly. The findings here have implications for directing research and education as well as application in veterinary practice. PMID:25262057</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AAS...22412327P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AAS...22412327P"><span>White-Light <span class="hlt">Observations</span> of Major Flares Compared to Total <span class="hlt">Solar</span> Irradiance and Short-Wavelength <span class="hlt">Observations</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Petrie, Gordon; Kopp, Greg; Harvey, J. W.</p> <p>2014-06-01</p> <p>The NSO’s GONG network produces “white light” (WL) continuum intensity images from one-minute integrations averaged across a 0. Å wide band pass centered at 676 Å at one minute cadence using six sites worldwide. Clear WL signatures of <span class="hlt">solar</span> flares are present in GONG intensity data for only the largest flares because of low spatial resolution (2.5 arcsec pixel size). For six major flares (GOES class X6.5 - X28) <span class="hlt">observed</span> by GONG, we compare integrated GONG full-disk WL intensity curves with SORCE/TIM total <span class="hlt">solar</span> irradiance (TSI) measurements. Distinctive p-mode signatures are evident in both GONG and SORCE time series, though the correlation between GONG and SORCE data varies from flare to flare. In some cases a clear TSI peak and an interruption of the GONG p-mode pattern accompany the flare. The flare signature is generally weaker in the GONG data, suggesting that most of the TIM flare signal arises from wavelengths shorter than the GONG band pass. The flare kernels nevertheless are clear and last many minutes in the spatially resolved GONG image time series. We also compare the GONG active region intensity <span class="hlt">observations</span> with shorter-wavelength data. In one case <span class="hlt">observed</span> by TRACE, the GONG and TRACE WL curves are very similar and the TRACE 160 Å curve shows a significant precursor and a long tail. In most cases the GONG WL and RHESSI 25-100 keV counts appear well correlated in time. This work utilizes GONG data obtained by the NSO Integrated Synoptic Program (NISP), managed by the National <span class="hlt">Solar</span> Observatory, which is operated by AURA, Inc. under a cooperative agreement with the National Science Foundation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22663855-hard-ray-emission-from-partially-occulted-solar-flares-rhessi-observations-two-solar-cycles','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22663855-hard-ray-emission-from-partially-occulted-solar-flares-rhessi-observations-two-solar-cycles"><span>Hard X-Ray Emission from Partially Occulted <span class="hlt">Solar</span> Flares: RHESSI <span class="hlt">Observations</span> in Two <span class="hlt">Solar</span> Cycles</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>Effenberger, Frederic; Costa, Fatima Rubio da; Petrosian, Vahé</p> <p>2017-02-01</p> <p>Flares close to the <span class="hlt">solar</span> limb, where the footpoints are occulted, can reveal the spectrum and structure of the coronal looptop source in X-rays. We aim at studying the properties of the corresponding energetic electrons near their acceleration site, without footpoint contamination. To this end, a statistical study of partially occulted flares <span class="hlt">observed</span> with Reuven Ramaty High-Energy <span class="hlt">Solar</span> Spectroscopic Imager is presented here, covering a large part of <span class="hlt">solar</span> cycles 23 and 24. We perform detailed spectra, imaging, and light curve analyses for 116 flares and include contextual <span class="hlt">observations</span> from SDO and STEREO when available, providing further insights into flaremore » emission that were previously not accessible. We find that most spectra are fitted well with a thermal component plus a broken power-law, non-thermal component. A thin-target kappa distribution model gives satisfactory fits after the addition of a thermal component. X-ray imaging reveals small spatial separation between the thermal and non-thermal components, except for a few flares with a richer coronal source structure. A comprehensive light curve analysis shows a very good correlation between the derivative of the soft X-ray flux (from GOES ) and the hard X-rays for a substantial number of flares, indicative of the Neupert effect. The results confirm that non-thermal particles are accelerated in the corona and estimated timescales support the validity of a thin-target scenario with similar magnitudes of thermal and non-thermal energy fluxes.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/17662653','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/17662653"><span>BioCO2 - a multidisciplinary, biological approach using <span class="hlt">solar</span> energy to <span class="hlt">capture</span> CO2 while producing H2 and high value products.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Skjånes, Kari; Lindblad, Peter; Muller, Jiri</p> <p>2007-10-01</p> <p>Many areas of algae technology have developed over the last decades, and there is an established market for products derived from algae, dominated by health food and aquaculture. In addition, the interest for active biomolecules from algae is increasing rapidly. The need for CO(2) management, in particular <span class="hlt">capture</span> and storage is currently an important technological, economical and global political issue and will continue to be so until alternative energy sources and energy carriers diminish the need for fossil fuels. This review summarizes in an integrated manner different technologies for use of algae, demonstrating the possibility of combining different areas of algae technology to <span class="hlt">capture</span> CO(2) and using the obtained algal biomass for various industrial applications thus bringing added value to the <span class="hlt">capturing</span> and storage processes. Furthermore, we emphasize the use of algae in a novel biological process which produces H(2) directly from <span class="hlt">solar</span> energy in contrast to the conventional CO(2) neutral biological methods. This biological process is a part of the proposed integrated CO(2) management scheme.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AAS...22831105P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AAS...22831105P"><span>First Report on the 2016 March 9 Total <span class="hlt">Solar</span> Eclipse <span class="hlt">Observations</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pasachoff, Jay M.</p> <p>2016-06-01</p> <p>Totality swept across Indonesia and into the Pacific on 2016 March 9, lasting up to 2 min 45 s on Ternate in the Spice Islands (Malukus). I provide a first report on our <span class="hlt">observations</span>. Our scientific goal is to follow changes in the corona over the <span class="hlt">solar</span>-activity cycle, now past its 2012 and 2014 double peak, and to measure temporal changes in the corona on the scale of minutes or hours by comparing eclipse <span class="hlt">observations</span> made at several sites along the path. I also discuss the near-simultaneous coronal <span class="hlt">observations</span> made with SOHO/LASCO, SDO/AIA, STEREO/SECCHI, PROBA2/SWAP, and Hinode XRT.For the forthcoming 2017 eclipse, we acknowledge grants to JMP and Williams College from the <span class="hlt">Solar</span> Terrestrial Program of the Atmospheric and Geospace Sciences Division of the National Science Foundation and from the Committee for Research and Exploration of the National Geographic Society.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20090033109&hterms=atom&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Datom','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20090033109&hterms=atom&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Datom"><span><span class="hlt">Observation</span> and Interpretation of Energetic Neutral Hydrogen Atoms from the December 5, 2006 <span class="hlt">Solar</span> Event</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Mewaldt, R. A.; Leske, R. A.; Stone, E. C.; Barghouty, A. F.; Shih, A. Y.; von Rosenvinge, T. T.; Labrador, A. W.; Cohen, C. M. S.; Cummings, A. C.; Cummings, A. C.</p> <p>2009-01-01</p> <p>We report the first <span class="hlt">observations</span> of energetic neutral atoms (ENAs) from a <span class="hlt">solar</span> flare/coronal mass ejection event. The <span class="hlt">observations</span> were made during the December 5, 2006 X9 <span class="hlt">solar</span> flare, located at E79, by the Low Energy Telescopes (LETs) on the STEREO A and B spacecraft. Within 1-2 hours of the flare onset, both LETs <span class="hlt">observed</span> a sudden burst of 1.6 to 15 MeV protons arriving hours before the onset of the main <span class="hlt">solar</span> energetic particle (SEP) event at Earth. More than 70% of these particles arrived from a longitude within +-10 degrees of the Sun. The derived emission profile at the Sun lasted for more than an hour and had a profile remarkably similar to the GOES soft X-ray profile. The <span class="hlt">observed</span> arrival directions and energy spectrum argue strongly that the particle events <5 MeV were due to energetic neutral hydrogen atoms that were stripped of their electrons upon entering the LET sensor. To our knowledge, this is the first reported <span class="hlt">observation</span> of ENA emission from a <span class="hlt">solar</span> flare/coronal mass ejection. We discuss possible origins for the production of ENAs in <span class="hlt">solar</span> events, including charge-transfer reactions involving both flare and shock-accelerated protons. Assuming isotropic emission, we find that 2 x 10E28 ENAs escaped from the Sun in the upper hemisphere. Based on the 2.2 MeV gamma-ray emission <span class="hlt">observed</span> by RHESSI in this event, and using measured and theoretical cross sections, we estimate that 3 x 10E31 ENAs with 1.8 - 5 MeV could be produced by protons accelerated in the flare. CME-driven shock acceleration is also a possible ENA source, but unfortunately there were no CME <span class="hlt">observations</span> available from this event. Taking into account ENA losses, we conclude that the <span class="hlt">observed</span> ENAs were most likely produced in the high corona at heliocentric distances 1.6 <span class="hlt">solar</span> radii.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMSA41A2360K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMSA41A2360K"><span>Ionospheric Caustics in <span class="hlt">Solar</span> Radio <span class="hlt">Observations</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Koval, A.; Chen, Y.; Stanislavsky, A.</p> <p>2016-12-01</p> <p>The Earth ionosphere possesses by natural focusing and defocusing effects on radio waves due to presence of variable ionospheric irregularities which could act like convergent and divergent lenses on incident radiation. In particular, the focusing of emission from the Sun was firstly detected on the Nançay Decameter Array dynamic spectra in the 1980s. On time-frequency spectrograms the intensity variations form specific structures different from well-known <span class="hlt">solar</span> radio bursts and clearly distinguishing on a background of <span class="hlt">solar</span> radiation. Such structures have been identified as ionospheric caustics (ICs) and considered to be the result of radio waves refraction on medium scale travelling ionospheric disturbances (MSTIDs). Although nowadays the ICs are registered by different radio observatories due to augmentation of low-frequency radio telescopes, the most recent papers devoted to ICs in <span class="hlt">solar</span> radio records date back to the 1980s. In this study, we revisit the ICs issue with some new results by conducting a statistical analysis of occurrence rate of ICs in <span class="hlt">solar</span> dynamic spectra in meter-decameter wavelength range for long continuous period (15 years). The seasonal variations in ICs appearance have been found for the first time. Besides, we report the possible <span class="hlt">solar</span> cycle dependence of ICs emergence. The radio waves propagation in the ionosphere comprising MSTIDs will be considered. The present research renews the subject of ICs in the low-frequency <span class="hlt">solar</span> radio astronomy after about 35-year letup.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010ApJ...719...28D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010ApJ...719...28D"><span>A Model of Magnetic Braking of <span class="hlt">Solar</span> Rotation that Satisfies <span class="hlt">Observational</span> Constraints</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Denissenkov, Pavel A.</p> <p>2010-08-01</p> <p>The model of magnetic braking of <span class="hlt">solar</span> rotation considered by Charbonneau & MacGregor has been modified so that it is able to reproduce for the first time the rotational evolution of both the fastest and slowest rotators among <span class="hlt">solar</span>-type stars in open clusters of different ages, without coming into conflict with other <span class="hlt">observational</span> constraints, such as the time evolution of the atmospheric Li abundance in <span class="hlt">solar</span> twins and the thinness of the <span class="hlt">solar</span> tachocline. This new model assumes that rotation-driven turbulent diffusion, which is thought to amplify the viscosity and magnetic diffusivity in stellar radiative zones, is strongly anisotropic with the horizontal components of the transport coefficients strongly dominating over those in the vertical direction. Also taken into account is the poloidal field decay that helps to confine the width of the tachocline at the <span class="hlt">solar</span> age. The model's properties are investigated by numerically solving the azimuthal components of the coupled momentum and magnetic induction equations in two dimensions using a finite element method.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012ApJ...752L..23S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012ApJ...752L..23S"><span>Simultaneous <span class="hlt">Observations</span> of a Large-scale Wave Event in the <span class="hlt">Solar</span> Atmosphere: From Photosphere to Corona</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Shen, Yuandeng; Liu, Yu</p> <p>2012-06-01</p> <p>For the first time, we report a large-scale wave that was <span class="hlt">observed</span> simultaneously in the photosphere, chromosphere, transition region, and low corona layers of the <span class="hlt">solar</span> atmosphere. Using the high temporal and high spatial resolution <span class="hlt">observations</span> taken by the <span class="hlt">Solar</span> Magnetic Activity Research Telescope at Hida Observatory and the Atmospheric Imaging Assembly (AIA) on board <span class="hlt">Solar</span> Dynamic Observatory, we find that the wave evolved synchronously at different heights of the <span class="hlt">solar</span> atmosphere, and it propagated at a speed of 605 km s-1 and showed a significant deceleration (-424 m s-2) in the extreme-ultraviolet (EUV) <span class="hlt">observations</span>. During the initial stage, the wave speed in the EUV <span class="hlt">observations</span> was 1000 km s-1, similar to those measured from the AIA 1700 Å (967 km s-1) and 1600 Å (893 km s-1) <span class="hlt">observations</span>. The wave was reflected by a remote region with open fields, and a slower wave-like feature at a speed of 220 km s-1 was also identified following the primary fast wave. In addition, a type-II radio burst was <span class="hlt">observed</span> to be associated with the wave. We conclude that this wave should be a fast magnetosonic shock wave, which was first driven by the associated coronal mass ejection and then propagated freely in the corona. As the shock wave propagated, its legs swept the <span class="hlt">solar</span> surface and thereby resulted in the wave signatures <span class="hlt">observed</span> in the lower layers of the <span class="hlt">solar</span> atmosphere. The slower wave-like structure following the primary wave was probably caused by the reconfiguration of the low coronal magnetic fields, as predicted in the field-line stretching model.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017SoPh..292..106M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017SoPh..292..106M"><span>First <span class="hlt">Observations</span> from the Multi-Application <span class="hlt">Solar</span> Telescope (MAST) Narrow-Band Imager</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mathew, Shibu K.; Bayanna, Ankala Raja; Tiwary, Alok Ranjan; Bireddy, Ramya; Venkatakrishnan, Parameswaran</p> <p>2017-08-01</p> <p>The Multi-Application <span class="hlt">Solar</span> Telescope is a 50 cm off-axis Gregorian telescope recently installed at the Udaipur <span class="hlt">Solar</span> Observatory, India. In order to obtain near-simultaneous <span class="hlt">observations</span> at photospheric and chromospheric heights, an imager optimized for two or more wavelengths is being integrated with the telescope. Two voltage-tuneable lithium-niobate Fabry-Perot etalons along with a set of interference blocking filters have been used for developing the imager. Both of the etalons are used in tandem for photospheric <span class="hlt">observations</span> in Fe i 6173 Å and chromospheric <span class="hlt">observation</span> in Hα 6563 Å spectral lines, whereas only one of the etalons is used for the chromospheric Ca II line at 8542 Å. The imager is also being used for spectropolarimetric <span class="hlt">observations</span>. We discuss the characterization of the etalons at the above wavelengths, detail the integration of the imager with the telescope, and present a few sets of <span class="hlt">observations</span> taken with the imager set-up.</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('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4354106','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4354106"><span>Full-Sun <span class="hlt">observations</span> for identifying the source of the slow <span class="hlt">solar</span> wind</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Brooks, David H.; Ugarte-Urra, Ignacio; Warren, Harry P.</p> <p>2015-01-01</p> <p>Fast (>700 km s−1) and slow (~400 km s−1) winds stream from the Sun, permeate the heliosphere and influence the near-Earth environment. While the fast wind is known to emanate primarily from polar coronal holes, the source of the slow wind remains unknown. Here we identify possible sites of origin using a slow <span class="hlt">solar</span> wind source map of the entire Sun, which we construct from specially designed, full-disk <span class="hlt">observations</span> from the Hinode satellite, and a magnetic field model. Our map provides a full-Sun <span class="hlt">observation</span> that combines three key ingredients for identifying the sources: velocity, plasma composition and magnetic topology and shows them as <span class="hlt">solar</span> wind composition plasma outflowing on open magnetic field lines. The area coverage of the identified sources is large enough that the sum of their mass contributions can explain a significant fraction of the mass loss rate of the <span class="hlt">solar</span> wind. PMID:25562705</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015IAUGA..2254684P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015IAUGA..2254684P"><span>Public Education and Outreach for <span class="hlt">Observing</span> <span class="hlt">Solar</span> Eclipses and Transits</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pasachoff, Jay M.</p> <p>2015-08-01</p> <p>The general public is often very interested in <span class="hlt">observing</span> <span class="hlt">solar</span> eclipses, with widespread attention from newspapers and other sources often available only days before the events. Recently, the 2012 eclipse's partial phases in Australia and the 2015 eclipse's partial phases throughout Europe as well as western Asia and northern Africa, were widely viewed. The 21 August 2017 eclipse, whose totality will sweep across the Continental United States from northwest to southeast, will have partial phases visible throughout the U.S., Canada, Mexico, Central America, and into South America. The 2019 and 2020 partial phases of total eclipses will be visible throughout South America, and partial phases from annular eclipses will be visible from other parts of the world. The 9 May 2016 transit of Mercury will be best visible from the Western Hemisphere, Europe, and Africa. Many myths and misunderstandings exist about the safety of <span class="hlt">observing</span> partial phases, and it is our responsibility as astronomers and educators to transmit accurate information and to attempt the widest possible distribution of such information. The Working Group on Public Education at Eclipses and Transits, formerly of Commission 46 on Education and Development and now of New Commission 11, tries to coordinate the distribution of information. In collaboration with the <span class="hlt">Solar</span> Division's Working Group on <span class="hlt">Solar</span> Eclipses, their website at http://eclipses.info is a one-stop shop for accurate information on how to <span class="hlt">observe</span> eclipses, why it is interesting to do so, where they will be visible (with links to online maps and weather statistics), and how encouraging students to <span class="hlt">observe</span> eclipses can be inspirational for them, perhaps even leading them to realize that the Universe can be understood and therefore renewing the strength of their studies. Links to information about transits of Mercury and Venus are also included.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22357004-multi-spacecraft-observations-recurrent-sup-he-rich-solar-energetic-particles','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22357004-multi-spacecraft-observations-recurrent-sup-he-rich-solar-energetic-particles"><span>Multi-spacecraft <span class="hlt">observations</span> of recurrent {sup 3}He-rich <span class="hlt">solar</span> energetic particles</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>Bučík, R.; Innes, D. E.; Mall, U.</p> <p>2014-05-01</p> <p>We study the origin of {sup 3}He-rich <span class="hlt">solar</span> energetic particles (<1 MeV nucleon{sup –1}) that are <span class="hlt">observed</span> consecutively on STEREO-B, Advanced Composition Explorer (ACE), and STEREO-A spacecraft when they are separated in heliolongitude by more than 90°. The {sup 3}He-rich period on STEREO-B and STEREO-A commences on 2011 July 1 and 2011 July 16, respectively. The ACE {sup 3}He-rich period consists of two sub-events starting on 2011 July 7 and 2011 July 9. We associate the STEREO-B July 1 and ACE July 7 {sup 3}He-rich events with the same sizeable active region (AR) producing X-ray flares accompanied by prompt electronmore » events, when it was near the west <span class="hlt">solar</span> limb as seen from the respective spacecraft. The ACE July 9 and STEREO-A July 16 events were dispersionless with enormous {sup 3}He enrichment, lacking <span class="hlt">solar</span> energetic electrons and occurring in corotating interaction regions. We associate these events with a small, recently emerged AR near the border of a low-latitude coronal hole that produced numerous jet-like emissions temporally correlated with type III radio bursts. For the first time we present <span class="hlt">observations</span> of (1) <span class="hlt">solar</span> regions with long-lasting conditions for {sup 3}He acceleration and (2) <span class="hlt">solar</span> energetic {sup 3}He that is temporarily confined/re-accelerated in interplanetary space.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/15767690','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/15767690"><span>Biotechnological storage and utilization of entrapped <span class="hlt">solar</span> energy.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Bhattacharya, Sumana; Schiavone, Marc; Nayak, Amiya; Bhattacharya, Sanjoy K</p> <p>2005-03-01</p> <p>Our laboratory has recently developed a device employing immobilized F0F1 adenosine triphosphatase (ATPase) that allows synthesis of adenosine triphosphate (ATP) from adenosine 5'-diphosphate and inorganic phosphate using <span class="hlt">solar</span> energy. We present estimates of total <span class="hlt">solar</span> energy received by Earth's land area and demonstrate that its efficient <span class="hlt">capture</span> may allow conversion of <span class="hlt">solar</span> energy and storage into bonds of biochemicals using devices harboring either immobilized ATPase or NADH dehydrogenase. <span class="hlt">Capture</span> and storage of <span class="hlt">solar</span> energy into biochemicals may also enable fixation of CO2 emanating from polluting units. The cofactors ATP and NADH synthesized using <span class="hlt">solar</span> energy could be used for regeneration of acceptor D-ribulose-1,5-bisphosphate from 3-phosphoglycerate formed during CO2 fixation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20160012097','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20160012097"><span><span class="hlt">Observations</span> of Transient ISS Floating Potential Variations During High Voltage <span class="hlt">Solar</span> Array Operations</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Willis, Emily M.; Minow, Joseph I.; Parker, Linda N.; Pour, Maria Z. A.; Swenson, Charles; Nishikawa, Ken-ichi; Krause, Linda Habash</p> <p>2016-01-01</p> <p>The International Space Station (ISS) continues to be a world-class space research laboratory after over 15 years of operations, and it has proven to be a fantastic resource for <span class="hlt">observing</span> spacecraft floating potential variations related to high voltage <span class="hlt">solar</span> array operations in Low Earth Orbit (LEO). Measurements of the ionospheric electron density and temperature along the ISS orbit and variations in the ISS floating potential are obtained from the Floating Potential Measurement Unit (FPMU). In particular, rapid variations in ISS floating potential during <span class="hlt">solar</span> array operations on time scales of tens of milliseconds can be recorded due to the 128 Hz sample rate of the Floating Potential Probe (FPP) pro- viding interesting insight into high voltage <span class="hlt">solar</span> array interaction with the space plasma environment. Comparing the FPMU data with the ISS operations timeline and <span class="hlt">solar</span> array data provides a means for correlating some of the more complex and interesting transient floating potential variations with mission operations. These complex variations are not reproduced by current models and require further study to understand the underlying physical processes. In this paper we present some of the floating potential transients <span class="hlt">observed</span> over the past few years along with the relevant space environment parameters and <span class="hlt">solar</span> array operations data.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018ApJ...860..142H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018ApJ...860..142H"><span><span class="hlt">Solar</span> Coronal Jets Extending to High Altitudes <span class="hlt">Observed</span> during the 2017 August 21 Total Eclipse</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hanaoka, Yoichiro; Hasuo, Ryuichi; Hirose, Tsukasa; Ikeda, Akiko C.; Ishibashi, Tsutomu; Manago, Norihiro; Masuda, Yukio; Morita, Sakuhiro; Nakazawa, Jun; Ohgoe, Osamu; Sakai, Yoshiaki; Sasaki, Kazuhiro; Takahashi, Koichi; Toi, Toshiyuki</p> <p>2018-06-01</p> <p>Coronal jets, which extend from the <span class="hlt">solar</span> surface to beyond 2 R ⊙, were <span class="hlt">observed</span> in the polar coronal hole regions during the total <span class="hlt">solar</span> eclipse on 2017 August 21. In a time-series of white-light images of the corona spanning 70 minutes taken with our multi-site <span class="hlt">observations</span> of this eclipse, six jets were found as narrow structures upwardly ejected with an apparent speed of about 450 km s‑1 in polar plumes. On the other hand, extreme-ultraviolet (EUV) images taken with the Atmospheric Image Assembly of the <span class="hlt">Solar</span> Dynamics Observatory show that all of the eclipse jets were preceded by EUV jets. Conversely, all the EUV jets whose brightnesses are comparable to ordinary soft X-ray jets and that occurred in the polar regions near the eclipse period, were <span class="hlt">observed</span> as eclipse jets. These results suggest that ordinary polar jets generally reach high altitudes and escape from the Sun as part of the <span class="hlt">solar</span> wind.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016A%26A...587A.123M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016A%26A...587A.123M"><span>Anomalous temporal behaviour of broadband Lyα <span class="hlt">observations</span> during <span class="hlt">solar</span> flares from SDO/EVE</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Milligan, Ryan O.; Chamberlin, Phillip C.</p> <p>2016-03-01</p> <p>Although it is the most prominent emission line in the <span class="hlt">solar</span> spectrum, there has been a notable lack of studies devoted to variations in Lyα emission during <span class="hlt">solar</span> flares in recent years. However, the few examples that do exist have shown Lyα emission to be a substantial radiator of the total energy budget of <span class="hlt">solar</span> flares (of the order of 10%). It is also a known driver of fluctuations in the Earth's ionosphere. The EUV Variability Experiment (EVE) on board the <span class="hlt">Solar</span> Dynamics Observatory now provides broadband, photometric Lyα data at 10 s cadence with its Multiple EUV Grating Spectrograph-Photometer (MEGS-P) component, and has <span class="hlt">observed</span> scores of <span class="hlt">solar</span> flares in the 5 years since it was launched. However, the MEGS-P time profiles appear to display a rise time of tens of minutes around the time of the flare onset. This is in stark contrast to the rapid, impulsive increase <span class="hlt">observed</span> in other intrinsically chromospheric features (Hα, Lyβ, LyC, C III, etc.). Furthermore, the emission detected by MEGS-P peaks around the time of the peak of thermal soft X-ray emission and not during the impulsive phase when energy deposition in the chromosphere (often assumed to be in the form of non-thermal electrons) is greatest. The time derivative of Lyα lightcurves also appears to resemble that of the time derivative of soft X-rays, reminiscent of the Neupert effect. Given that spectrally-resolved Lyα <span class="hlt">observations</span> during flares from SORCE/SOLSTICE peak during the impulsive phase as expected, this suggests that the atypical behaviour of MEGS-P data is a manifestation of the broadband nature of the <span class="hlt">observations</span>. This could imply that other lines and/or continuum emission that becomes enhanced during flares could be contributing to the passband. Users are hereby urged to exercise caution when interpreting broadband Lyα <span class="hlt">observations</span> of <span class="hlt">solar</span> flares. Comparisons have also been made with other broadband Lyα photometers such as PROBA2/LYRA and GOES/EUVS-E.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20170003779&hterms=hodge&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dhodge','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20170003779&hterms=hodge&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dhodge"><span>The HEXITEC Hard X-Ray Pixelated CdTe Imager for Fast <span class="hlt">Solar</span> <span class="hlt">Observations</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Baumgartner, Wayne H.; Christe, Steven D.; Ryan, Daniel; Inglis, Andrew R.; Shih, Albert Y.; Gregory, Kyle; Wilson, Matt; Seller, Paul; Gaskin, Jessica; Wilson-Hodge, Colleen</p> <p>2016-01-01</p> <p>There is an increasing demand in <span class="hlt">solar</span> and astrophysics for high resolution X-ray spectroscopic imaging. Such <span class="hlt">observations</span> would present ground breaking opportunities to study the poorly understood high energy processes in our <span class="hlt">solar</span> system and beyond, such as <span class="hlt">solar</span> flares, X-ray binaries, and active galactic nuclei. However, such <span class="hlt">observations</span> require a new breed of solid state detectors sensitive to high energy X-rays with fine independent pixels to sub-sample the point spread function (PSF) of the X-ray optics. For <span class="hlt">solar</span> <span class="hlt">observations</span> in particular, they must also be capable of handling very high count rates as photon fluxes from <span class="hlt">solar</span> flares often cause pile up and saturation in present generation detectors. The Rutherford Appleton Laboratory (RAL) has recently developed a new cadmium telluride (CdTe) detector system, called HEXITEC (High Energy X-ray Imaging Technology). It is an 80 x 80 array of 250 micron independent pixels sensitive in the 2-200 keV band and capable of a high full frame read out rate of 10 kHz. HEXITEC provides the smallest independently read out CdTe pixels currently available, and are well matched to the few arcsecond PSF produced by current and next generation hard X-ray focusing optics. NASA's Goddard and Marshall Space Flight Centers are collaborating with RAL to develop these detectors for use on future space borne hard X-ray focusing telescopes. We show the latest results on HEXITEC's imaging capability, energy resolution, high read out rate, and reveal it to be ideal for such future instruments.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMSH21C..05V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMSH21C..05V"><span>Combining Remote and In Situ <span class="hlt">Observations</span> with MHD models to Understand the Formation of the Slow <span class="hlt">Solar</span> Wind</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Viall, N. M.; Kepko, L.; Antiochos, S. K.; Lepri, S. T.; Vourlidas, A.; Linker, J.</p> <p>2017-12-01</p> <p>Connecting the structure and variability in the <span class="hlt">solar</span> corona to the Heliosphere and <span class="hlt">solar</span> wind is one of the main goals of Heliophysics and space weather research. The instrumentation and viewpoints of the Parker <span class="hlt">Solar</span> Probe and <span class="hlt">Solar</span> Orbiter missions will provide an unprecedented opportunity to combine remote sensing with in situ data to determine how the corona drives the Heliosphere, especially as it relates to the origin of the slow <span class="hlt">solar</span> wind. We present analysis of STEREO coronagraph and heliospheric imager <span class="hlt">observations</span> and of in situ ACE and Wind measurements that reveal an important connection between the dynamics of the corona and of the <span class="hlt">solar</span> wind. We show <span class="hlt">observations</span> of quasi-periodic release of plasma into the slow <span class="hlt">solar</span> wind occurring throughout the corona - including regions away from the helmet streamer and heliospheric current sheet - and demonstrate that these <span class="hlt">observations</span> place severe constraints on the origin of the slow <span class="hlt">solar</span> wind. We build a comprehensive picture of the dynamic evolution by combining remote imaging data, in situ composition and magnetic connectivity information, and MHD models of the <span class="hlt">solar</span> wind. Our results have critical implications for the magnetic topology involved in slow <span class="hlt">solar</span> wind formation and magnetic reconnection dynamics. Crucially, this analysis pushes the limits of current instrument resolution and sensitivity, showing the enormous potential science to be accomplished with the Parker <span class="hlt">Solar</span> Probe and <span class="hlt">Solar</span> Orbiter missions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017SpWea..15.1215K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017SpWea..15.1215K"><span>Ms. Hisako Koyama: From Amateur Astronomer to Long-Term <span class="hlt">Solar</span> <span class="hlt">Observer</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Knipp, Delores; Liu, Huixin; Hayakawa, Hisashi</p> <p>2017-10-01</p> <p>The path to science for a girl of any nationality born in the early twentieth century was formidable-to-nonexistent. Yet paths were forged by a few. We present the little-known story of one of Japan's premier <span class="hlt">solar</span> <span class="hlt">observers</span> and her contribution to the world's understanding of sunspots and space weather cycles. Ms. Hisako Koyama, born in Tokyo in 1916, became a passionate amateur astronomer, a dedicated <span class="hlt">solar</span> <span class="hlt">observer</span>, and a long-serving staff member of the National Museum of Nature and Science, Tokyo. As a writer for amateur astronomy journals she advised many on the details and joys of sky viewing. She created a consistent, extended record of sunspots. Her multidecade archive of sunspot drawings is one of the "backbones" for the recent international recalibration of the sunspot record that provides insight into space weather reaching back to the early 1600s. We detail her contributions to the citizens of Japan as an ambassador of astronomy and her international contribution to understanding the symmetries and asymmetries of the <span class="hlt">solar</span> cycle. We comment on the value of her continuous record of sunspots and on her tenacity in promoting a science that links to space weather.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20010032414','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20010032414"><span>High Resolution <span class="hlt">Observations</span> and Modeling of Small-Scale <span class="hlt">Solar</span> Magnetic Elements</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Berger, Thomas E.</p> <p>2001-01-01</p> <p>This research contract investigating the radiative transfer and dynamic physics of the smallest <span class="hlt">observable</span> magnetic structures in the <span class="hlt">solar</span> photosphere. Due to the lack of a high-resolution visible light satellite instrument for <span class="hlt">solar</span> studies, all data were acquired using ground-based instrumentation. The primary goal of the investigation was to understand the formation and evolution of "G-band bright points" in relation to the associated magnetic elements. G-band bright points are small (on the order of 100 kin or less in diameter) bright signatures associated with magnetic flux elements in the photosphere. They are seen in the A2A-X2 4308 A molecular bandhead of the CH radical ill the <span class="hlt">solar</span> spectrum and offer the highest spatial resolution and highest contrast "tracers" of small magnetic structure on the Sun.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018ApJ...857..115Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018ApJ...857..115Y"><span><span class="hlt">Observation</span> of the Kelvin–Helmholtz Instability in a <span class="hlt">Solar</span> Prominence</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yang, Heesu; Xu, Zhi; Lim, Eun-Kyung; Kim, Sujin; Cho, Kyung-Suk; Kim, Yeon-Han; Chae, Jongchul; Cho, Kyuhyoun; Ji, Kaifan</p> <p>2018-04-01</p> <p>Many <span class="hlt">solar</span> prominences end their lives in eruptions or abrupt disappearances that are associated with dynamical or thermal instabilities. Such instabilities are important because they may be responsible for energy transport and conversion. We present a clear <span class="hlt">observation</span> of a streaming kink-mode Kelvin–Helmholtz Instability (KHI) taking place in a <span class="hlt">solar</span> prominence using the Hα Lyot filter installed at the New Vacuum <span class="hlt">Solar</span> Telescope, Fuxian-lake <span class="hlt">Solar</span> Observatory in Yunnan, China. On one side of the prominence, a series of plasma blobs floated up from the chromosphere and streamed parallel to the limb. The plasma stream was accelerated to about 20–60 km s‑1 and then undulated. We found that 2″- and 5″-size vortices formed, floated along the stream, and then broke up. After the 5″-size vortex, a plasma ejection out of the stream was detected in the <span class="hlt">Solar</span> Dynamics Observatory/Atmospheric Imaging Assembly images. Just before the formation of the 5″-size vortex, the stream displayed an oscillatory transverse motion with a period of 255 s with the amplitude growing at the rate of 0.001 s‑1. We attribute this oscillation of the stream and the subsequent formation of the vortex to the KHI triggered by velocity shear between the stream, guided by the magnetic field and the surrounding media. The plasma ejection suggests the transport of prominence material into the upper layer by the KHI in its nonlinear stage.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19950004551&hterms=spices&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dspices','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19950004551&hterms=spices&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dspices"><span>Small Particles Intact <span class="hlt">Capture</span> Experiment (SPICE)</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Nishioka, Ken-Ji; Carle, G. C.; Bunch, T. E.; Mendez, David J.; Ryder, J. T.</p> <p>1994-01-01</p> <p>The Small Particles Intact <span class="hlt">Capture</span> Experiment (SPICE) will develop technologies and engineering techniques necessary to <span class="hlt">capture</span> nearly intact, uncontaminated cosmic and interplanetary dust particles (IDP's). Successful <span class="hlt">capture</span> of such particles will benefit the exobiology and planetary science communities by providing particulate samples that may have survived unaltered since the formation of the <span class="hlt">solar</span> system. Characterization of these particles may contribute fundamental data to our knowledge of how these particles could have formed into our planet Earth and, perhaps, contributed to the beginnings of life. The term 'uncontaminated' means that <span class="hlt">captured</span> cosmic and IDP particles are free of organic contamination from the <span class="hlt">capture</span> process and the term 'nearly intact <span class="hlt">capture</span>' means that their chemical and elemental components are not materially altered during <span class="hlt">capture</span>. The key to <span class="hlt">capturing</span> cosmic and IDP particles that are organic-contamination free and nearly intact is the <span class="hlt">capture</span> medium. Initial screening of <span class="hlt">capture</span> media included organic foams, multiple thin foil layers, and aerogel (a silica gel); but, with the exception of aerogel, the requirements of no contamination or nearly intact <span class="hlt">capture</span> were not met. To ensure no contamination of particles in the <span class="hlt">capture</span> process, high-purity aerogel was chosen. High-purity aerogel results in high clarity (visual clearness), a useful quality in detection and recovery of embedded <span class="hlt">captured</span> particles from the aerogel. P. Tsou at the Jet Propulsion Laboratory (JPL) originally described the use of aerogel for this purpose and reported laboratory test results. He has flown aerogel as a 'GAS-can Lid' payload on STS-47 and is evaluating the results. The Timeband <span class="hlt">Capture</span> Cell Experiment (TICCE), a Eureca 1 experiment, is also flying aerogel and is scheduled for recovery in late April.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22663897-comparison-between-physics-based-polytropic-mhd-models-stellar-coronae-stellar-winds-solar-analogs','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22663897-comparison-between-physics-based-polytropic-mhd-models-stellar-coronae-stellar-winds-solar-analogs"><span>A Comparison between Physics-based and Polytropic MHD Models for Stellar Coronae and Stellar Winds of <span class="hlt">Solar</span> Analogs</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>Cohen, O.</p> <p></p> <p>The development of the Zeeman–Doppler Imaging (ZDI) technique has provided synoptic <span class="hlt">observations</span> of surface magnetic fields of low-mass stars. This led the stellar astrophysics community to adopt modeling techniques that have been used in <span class="hlt">solar</span> physics using <span class="hlt">solar</span> magnetograms. However, many of these techniques have been neglected by the <span class="hlt">solar</span> community due to their failure to reproduce <span class="hlt">solar</span> <span class="hlt">observations</span>. Nevertheless, some of these techniques are still used to simulate the coronae and winds of <span class="hlt">solar</span> analogs. Here we present a comparative study between two MHD models for the <span class="hlt">solar</span> corona and <span class="hlt">solar</span> wind. The first type of model is amore » polytropic wind model, and the second is the physics-based AWSOM model. We show that while the AWSOM model consistently reproduces many <span class="hlt">solar</span> <span class="hlt">observations</span>, the polytropic model fails to reproduce many of them, and in the cases where it does, its solutions are unphysical. Our recommendation is that polytropic models, which are used to estimate mass-loss rates and other parameters of <span class="hlt">solar</span> analogs, must first be calibrated with <span class="hlt">solar</span> <span class="hlt">observations</span>. Alternatively, these models can be calibrated with models that <span class="hlt">capture</span> more detailed physics of the <span class="hlt">solar</span> corona (such as the AWSOM model) and that can reproduce <span class="hlt">solar</span> <span class="hlt">observations</span> in a consistent manner. Without such a calibration, the results of the polytropic models cannot be validated, but they can be wrongly used by others.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018MNRAS.476..868T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018MNRAS.476..868T"><span>Synchronized <span class="hlt">observations</span> of bright points from the <span class="hlt">solar</span> photosphere to the corona</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tavabi, Ehsan</p> <p>2018-05-01</p> <p>One of the most important features in the <span class="hlt">solar</span> atmosphere is the magnetic network and its relationship to the transition region (TR) and coronal brightness. It is important to understand how energy is transported into the corona and how it travels along the magnetic field lines between the deep photosphere and chromosphere through the TR and corona. An excellent proxy for transportation is the Interface Region Imaging Spectrograph (IRIS) raster scans and imaging <span class="hlt">observations</span> in near-ultraviolet (NUV) and far-ultraviolet (FUV) emission channels, which have high time, spectral and spatial resolutions. In this study, we focus on the quiet Sun as <span class="hlt">observed</span> with IRIS. The data with a high signal-to-noise ratio in the Si IV, C II and Mg II k lines and with strong emission intensities show a high correlation with TR bright network points. The results of the IRIS intensity maps and dopplergrams are compared with those of the Atmospheric Imaging Assembly (AIA) and Helioseismic and Magnetic Imager (HMI) instruments onboard the <span class="hlt">Solar</span> Dynamical Observatory (SDO). The average network intensity profiles show a strong correlation with AIA coronal channels. Furthermore, we applied simultaneous <span class="hlt">observations</span> of the magnetic network from HMI and found a strong relationship between the network bright points in all levels of the <span class="hlt">solar</span> atmosphere. These features in the network elements exhibited regions of high Doppler velocity and strong magnetic signatures. Plenty of corona bright points emission, accompanied by the magnetic origins in the photosphere, suggest that magnetic field concentrations in the network rosettes could help to couple the inner and outer <span class="hlt">solar</span> atmosphere.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/4383536-solar-spicules-observed-through-filter','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/4383536-solar-spicules-observed-through-filter"><span><span class="hlt">Solar</span> spicules <span class="hlt">observed</span> through a K-filter</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>Banos, G.</p> <p>1973-10-01</p> <p>Some properties of the <span class="hlt">solar</span> spicules as <span class="hlt">observed</span> outside the limb through a Halle K-filter at the center of the line were investigated. The <span class="hlt">observations</span> were made at the Pic-du-Midi Observatory. The results were as follows: (a) The chromosphere at the limb appears more diffuse in the K line than in the H alpha line, the spicules being not well resolved. (b) The ratio of spicule intensity to the background intensity incrcases with height, as in the case of H alpha spicules, but it is, in every height, smaller than that in H alpha . (c) The spicule mean widthmore » is measured photometrically and found equal to 1900 km. (d) The lifetime is found to be 4.5 min. (e) The mean chromospheric height is estimated to be 6,000 km.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2006IAUSS...5E..29P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006IAUSS...5E..29P"><span><span class="hlt">Observing</span> <span class="hlt">Solar</span> Eclipses in the Developing World</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pasachoff, J. M.</p> <p>2006-08-01</p> <p>The paths of totality of total <span class="hlt">solar</span> eclipses cross the world, with each spot receiving such a view about every 300 years. The areas of the world from which partial eclipses are visible are much wider. For the few days prior to a total eclipse, the attention of a given country is often drawn toward the eclipse, providing a teachable moment that we can use to bring astronomy to the public's attention. Also, it is important to describe how to <span class="hlt">observe</span> the partial phases of the eclipse safely. Further, it is important to describe to those people in the zone of totality that it is not only safe but also interesting to view totality. Those who are misled by false warnings that overstate the hazards of viewing the eclipse, or that fail to distinguish between safe and unsafe times for naked-eye viewing, may well be skeptical when other health warnings--perhaps about AIDS or malaria prevention or polio inoculations--come from the authorities, meaning that the penalties for misunderstanding the astronomical event can be severe. Through the International Astronomical Union's Working Group on <span class="hlt">Solar</span> Eclipses and through the I.A.U.'s Program Group on Public Education at the Times of Eclipses, part of the Commission on Education and Development, we make available information to national authorities, to colleagues in the relevant countries, and to others, through our Websites at http://www.eclipses.info and http://www.totalsolareclipse.net and through personal communication. Among our successes at the 29 March 2006 total <span class="hlt">solar</span> eclipse was the distribution through a colleague in Nigeria of 400,000 eye-protection filters.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AdSpR..60.1585S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AdSpR..60.1585S"><span>Ionospheric winter anomaly and annual anomaly <span class="hlt">observed</span> from Formosat-3/COSMIC Radio Occultation <span class="hlt">observations</span> during the ascending phase of <span class="hlt">solar</span> cycle 24</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sai Gowtam, V.; Tulasi Ram, S.</p> <p>2017-10-01</p> <p>Ionospheric winter and annual anomalies have been investigated during the ascending phase of <span class="hlt">solar</span> cycle 24 using high-resolution global 3D - data of the FORMOSAT - 3/COSMIC (Formosa satellite - 3/Constellation <span class="hlt">Observing</span> System for Meterology, Ionosphere and Climate) radio occultation <span class="hlt">observations</span>. Our detailed analysis shows that the occurrence of winter anomaly at low-latitudes is confined only to the early morning to afternoon hours, whereas, the winter anomaly at mid-latitudes is almost absent at all local times during the ascending phase of <span class="hlt">solar</span> cycle 24. Further, in the topside ionosphere (altitudes of 400 km and above), the winter anomaly is completely absent at all local times. In contrast, the ionospheric annual anomaly is consistently <span class="hlt">observed</span> at all local times and altitudes during this ascending phase of <span class="hlt">solar</span> cycle 24. The annual anomaly exhibits strong enhancements over southern EIA crest latitudes during day time and around Weddle Sea Anomaly (WSA) region during night times. The global mean annual asymmetry index is also computed to understand the altitudinal variation. The global mean AI maximizes around 300-500 km altitudes during the low <span class="hlt">solar</span> active periods (2008-10), whereas it extends up to 600 km during moderate to high (2011) <span class="hlt">solar</span> activity period. These findings from our study provide new insights to the current understanding of the annual anomaly.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/21455040-model-magnetic-braking-solar-rotation-satisfies-observational-constraints','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/21455040-model-magnetic-braking-solar-rotation-satisfies-observational-constraints"><span>A MODEL OF MAGNETIC BRAKING OF <span class="hlt">SOLAR</span> ROTATION THAT SATISFIES <span class="hlt">OBSERVATIONAL</span> CONSTRAINTS</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>Denissenkov, Pavel A., E-mail: pavel.denisenkov@gmail.co</p> <p></p> <p>The model of magnetic braking of <span class="hlt">solar</span> rotation considered by Charbonneau and MacGregor has been modified so that it is able to reproduce for the first time the rotational evolution of both the fastest and slowest rotators among <span class="hlt">solar</span>-type stars in open clusters of different ages, without coming into conflict with other <span class="hlt">observational</span> constraints, such as the time evolution of the atmospheric Li abundance in <span class="hlt">solar</span> twins and the thinness of the <span class="hlt">solar</span> tachocline. This new model assumes that rotation-driven turbulent diffusion, which is thought to amplify the viscosity and magnetic diffusivity in stellar radiative zones, is strongly anisotropic withmore » the horizontal components of the transport coefficients strongly dominating over those in the vertical direction. Also taken into account is the poloidal field decay that helps to confine the width of the tachocline at the <span class="hlt">solar</span> age. The model's properties are investigated by numerically solving the azimuthal components of the coupled momentum and magnetic induction equations in two dimensions using a finite element method.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19840049457&hterms=astronomia+espacio&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dastronomia%2By%2Bespacio','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19840049457&hterms=astronomia+espacio&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dastronomia%2By%2Bespacio"><span>Microwave, soft and hard X-ray imaging <span class="hlt">observations</span> of two <span class="hlt">solar</span> flares</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kundu, M. R.; Erskine, F. T.; Schmahl, E. J.; Machado, M. E.; Rovira, M. G.</p> <p>1984-01-01</p> <p>A set of microwave and hard X-ray <span class="hlt">observations</span> of two flares <span class="hlt">observed</span> simultaneously with the Very Large Array (VLA) and the <span class="hlt">Solar</span> Maximum Mission Hard X-ray Imaging Spectrometer (SMM-HXIS) are presented. The LVA was used at 6 cm to map the slowly varying and burst components in three neighboring <span class="hlt">solar</span> active regions (Boulder Nos. 2522, 2530, and 2519) from approximately 14:00 UT until 01:00 UT on June 24-25, 1980. Six microwave bursts less than 30 sfu were <span class="hlt">observed</span>, and for the strongest of these, two-dimensional 'snapshot' (10 s) maps with spatial resolution of 5 in. were synthesized. HXIS data show clear interconnections between regions 2522 and 2530. The X-ray <span class="hlt">observations</span> present a global picture of flaring activity, while the VLA data show the complexity of the small magnetic structures associated with the impulsive phase phenomena. It is seen that energy release did not occur in a single isolated magnetic structure, but over a large area of intermingled loop structures.</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('http://adsabs.harvard.edu/abs/2006JGRA..11112S01N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006JGRA..11112S01N"><span>Magnetic helicity and flux tube dynamics in the <span class="hlt">solar</span> convection zone: Comparisons between <span class="hlt">observation</span> and theory</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Nandy, Dibyendu</p> <p>2006-12-01</p> <p>Magnetic helicity, a conserved topological parameter in ideal MHD systems, conditions close to which are realized in the <span class="hlt">solar</span> plasma, is intimately connected to the creation and subsequent dynamics of magnetic flux tubes in the <span class="hlt">solar</span> interior. It can therefore be used as a tool to probe such dynamics. In this paper we show how photospheric <span class="hlt">observations</span> of magnetic helicity of isolated magnetic flux tubes, manifested as the twist and writhe of <span class="hlt">solar</span> active regions, can constrain the creation and dynamics of flux tubes in the <span class="hlt">solar</span> convection zone and the nature of convective turbulence itself. We analyze the <span class="hlt">observed</span> latitudinal distribution of twists in photospheric active regions, derived from <span class="hlt">solar</span> vector magnetograms, in the largest such sample studied till-date. We confirm and put additional constraints on the hemispheric twist helicity trend and find that the dispersion in the active region twist distribution is latitude-independent, implying that the amplitude of turbulent fluctuations does not vary with latitude in the convection zone. Our data set also shows that the amplitude and dispersion of twist decreases with increasing magnetic size of active regions, supporting the conclusion that larger flux tubes are less affected by turbulence. Among the various theoretical models that have been proposed till-date to explain the origin of twist, our <span class="hlt">observations</span> best match the Σ effect model, which invokes helical turbulent buffeting of rising flux tubes as the mechanism for twist creation. Finally, we complement our analysis of twists with past <span class="hlt">observations</span> of tilts in <span class="hlt">solar</span> active regions and tie them in with theoretical modeling studies, to build up a comprehensive picture of the dynamics of twisted magnetic flux tubes throughout the <span class="hlt">solar</span> convection zone. This general framework, binding together theory and <span class="hlt">observations</span>, suggests that flux tubes have a wide range of twists in the <span class="hlt">solar</span> convection zone, with some as high as to make them susceptible to the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010SPIE.7732E..0QS','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010SPIE.7732E..0QS"><span>Development of double-sided silicon strip detectors for <span class="hlt">solar</span> hard x-ray <span class="hlt">observation</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Saito, Shinya; Ishikawa, Shin-Nosuke; Watanabe, Shin; Odaka, Hirokazu; Sugimoto, Soichiro; Fukuyama, Taro; Kokubun, Motohide; Takahashi, Tadayuki; Terada, Yukikatsu; Tajima, Hiroyasu; Tanaka, Takaaki; Krucker, Säm; Christe, Steven; McBride, Steve; Glesener, Lindsay</p> <p>2010-07-01</p> <p>The Focusing Optics X-ray <span class="hlt">Solar</span> Imager (FOXSI) is a rocket experiment scheduled for January 2011 launch. FOXSI <span class="hlt">observes</span> 5 - 15 keV hard X-ray emission from quiet-region <span class="hlt">solar</span> flares in order to study the acceleration process of electrons and the mechanism of coronal heating. For <span class="hlt">observing</span> faint hard X-ray emission, FOXSI uses focusing optics for the first time in <span class="hlt">solar</span> hard X-ray <span class="hlt">observation</span>, and attains 100 times higher sensitivity than RHESSI, which is the present <span class="hlt">solar</span> hard X-ray <span class="hlt">observing</span> satellite. Now our group is working on developments of both Double-sided Silicon Strip Detector (DSSD) and read-out analog ASIC "VATA451" used for FOXSI. Our DSSD has a very fine strip pitch of 75 μm, which has sufficient position resolution for FOXSI mirrors with angular resolution (FWHM) of 12 arcseconds. DSSD also has high spectral resolution and efficiency in the FOXSI's energy range of 5 - 15 keV, when it is read out by our 64-channel analog ASIC. In advance of the FOXSI launch, we have established and tested a setup of 75 μm pitch DSSD bonded with "VATA451" ASICs. We successfully read out from almost all the channels of the detector, and proved ability to make a shadow image of tungsten plate. We also confirmed that our DSSD has energy resolution (FWHM) of 0.5 keV, lower threshold of 5 keV, and position resolution less than 63 μm. These performance satisfy FOXSI's requirements.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=solar+AND+energy&pg=2&id=EJ828725','ERIC'); return false;" href="https://eric.ed.gov/?q=solar+AND+energy&pg=2&id=EJ828725"><span>Leaves: Nature's <span class="hlt">Solar</span> Collectors</span></a></p> <p><a target="_blank" href="http://www.eric.ed.gov/ERICWebPortal/search/extended.jsp?_pageLabel=advanced">ERIC Educational Resources Information Center</a></p> <p>Isabelle, Aaron D.; de Groot, Cornelis</p> <p>2009-01-01</p> <p>One of the most captivating things about plants is the way they <span class="hlt">capture</span> the Sun's energy, but this can be a difficult topic to cover with elementary students. Therefore, to help students to make a concrete connection to this abstract concept, this series of <span class="hlt">solar</span>-energy lessons focuses on leaves and how they act as "<span class="hlt">solar</span> collectors." As students…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19900053142&hterms=mahan&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dmahan','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19900053142&hterms=mahan&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dmahan"><span>An improved electrothermal model for the ERBE nonscanning radiometer - Comparison of predicted and measured behavior during <span class="hlt">solar</span> <span class="hlt">observations</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Tira, Nour E.; Mahan, J. R.; Lee, Robert B., III</p> <p>1989-01-01</p> <p>The improved Earth Radiation Budget Experiment nonscanning-channels electrothermal model presented is used to model two types of <span class="hlt">solar</span> <span class="hlt">observations</span>: those obtained through the <span class="hlt">solar</span> port during <span class="hlt">solar</span> calibration, and and those obtained during the satellite pitch-over maneuver, in which the sun is <span class="hlt">observed</span> by the radiometer while it is in earth-viewing configuration. Thermal noise has been separately studied to evaluate its contribution to the radiative energy absorbed by the active cavity. It is found that the scattering of the collimated <span class="hlt">solar</span> radiation contributes an average of 0.071 mW during <span class="hlt">solar</span> calibration.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007BASI...35..709K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007BASI...35..709K"><span>A <span class="hlt">solar</span> <span class="hlt">observing</span> station for education and research in Peru</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kaname, José Iba, Ishitsuka; Ishitsuka, Mutsumi; Trigoso Avilés, Hugo; Takashi, Sakurai; Yohei, Nishino; Miyazaki, Hideaki; Shibata, Kazunari; Ueno, Satoru; Yumoto, Kiyohumi; Maeda, George</p> <p>2007-12-01</p> <p>Since 1937 Carnegie Institution of Washington made <span class="hlt">observations</span> of active regions of the Sun with a Hale type spectro-helioscope in Huancayo observatory of the Instituto Geofísico del Perú (IGP). IGP has contributed significantly to geophysical and <span class="hlt">solar</span> sciences in the last 69 years. Now IGP and the Faculty of Sciences of the Universidad Nacional San Luis Gonzaga de Ica (UNICA) are planning to refurbish the coelostat at the observatory with the support of National Astronomical Observatory of Japan. It is also planned to install a <span class="hlt">solar</span> Flare Monitor Telescope (FMT) at UNICA, from Hida observatory of Kyoto University. Along with the coelostat, the FMT will be useful to improve scientific research and education.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMSH42A..07D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMSH42A..07D"><span><span class="hlt">Solar</span>-Iss a New <span class="hlt">Solar</span> Reference Spectrum Covering the Far UV to the Infrared (165 to 3088 Nm) Based on Reanalyzed <span class="hlt">Solar</span>/solspec Cycle 24 <span class="hlt">Observations</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Damé, L.; Meftah, M.; Irbah, A.; Hauchecorne, A.; Bekki, S.; Bolsée, D.; Pereira, N.; Sluse, D.; Cessateur, G.</p> <p>2017-12-01</p> <p>Since April 5, 2008 and until February 15, 2017, the SOLSPEC (<span class="hlt">SOLar</span> SPECtrometer) spectro-radiometer of the <span class="hlt">SOLAR</span> facility on the International Space Station performed accurate measurements of <span class="hlt">Solar</span> Spectral Irradiance (SSI) from the far ultraviolet to the infrared (165 nm to 3088 nm). These measurements, unique by their large spectral coverage and long time range, are of primary importance for a better understanding of <span class="hlt">solar</span> physics and of the impact of <span class="hlt">solar</span> variability on climate (via Earth's atmospheric photochemistry), noticeably through the "top-down" mechanism amplifying ultraviolet (UV) <span class="hlt">solar</span> forcing effects on the climate (UV affects stratospheric dynamics and temperatures, altering interplanetary waves and weather patterns both poleward and downward to the lower stratosphere and troposphere regions). <span class="hlt">SOLAR</span>/SOLSPEC, with almost 9 years of <span class="hlt">observations</span> covering the essential of the unusual <span class="hlt">solar</span> cycle 24 from minimum in 2008 to maximum, allowed to establish new reference <span class="hlt">solar</span> spectra from UV to IR (165 to 3088 nm) at minimum (beginning of mission) and maximum of activity. The complete reanalysis was possible thanks to revised engineering corrections, improved calibrations and advanced procedures to account for thermal, aging and pointing corrections. The high quality and sensitivity of SOLSPEC data allow to follow temporal variability in UV but also in visible along the cycle. Uncertainties on these measurements are evaluated and results, absolute reference spectra and variability, are compared with other measurements (WHI, ATLAS-3, SCIAMACHY, SORCE/SOLSTICE, SORCE/SIM) and models (SATIRE-S, NRLSSI, NESSY)</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4912660','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4912660"><span><span class="hlt">Observing</span> the release of twist by magnetic reconnection in a <span class="hlt">solar</span> filament eruption</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Xue, Zhike; Yan, Xiaoli; Cheng, Xin; Yang, Liheng; Su, Yingna; Kliem, Bernhard; Zhang, Jun; Liu, Zhong; Bi, Yi; Xiang, Yongyuan; Yang, Kai; Zhao, Li</p> <p>2016-01-01</p> <p>Magnetic reconnection is a fundamental process of topology change and energy release, taking place in plasmas on the Sun, in space, in astrophysical objects and in the laboratory. However, <span class="hlt">observational</span> evidence has been relatively rare and typically only partial. Here we present evidence of fast reconnection in a <span class="hlt">solar</span> filament eruption using high-resolution H-alpha images from the New Vacuum <span class="hlt">Solar</span> Telescope, supplemented by extreme ultraviolet <span class="hlt">observations</span>. The reconnection is seen to occur between a set of ambient chromospheric fibrils and the filament itself. This allows for the relaxation of magnetic tension in the filament by an untwisting motion, demonstrating a flux rope structure. The topology change and untwisting are also found through nonlinear force-free field modelling of the active region in combination with magnetohydrodynamic simulation. These results demonstrate a new role for reconnection in <span class="hlt">solar</span> eruptions: the release of magnetic twist. PMID:27306479</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19860014074','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19860014074"><span><span class="hlt">Solar</span> wind-magnetosphere coupling and the distant magnetotail: ISEE-3 <span class="hlt">observations</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Slavin, J. A.; Smith, E. J.; Sibeck, D. G.; Baker, D. N.; Zwickl, R. D.; Akasofu, S. I.; Lepping, R. P.</p> <p>1985-01-01</p> <p>ISEE-3 Geotail <span class="hlt">observations</span> are used to investigate the relationship between the interplanetary magnetic field, substorm activity, and the distant magnetotail. Magnetic field and plasma <span class="hlt">observations</span> are used to present evidence for the existence of a quasi-permanent, curved reconnection neutral line in the distant tail. The distance to the neutral line varies from absolute value of X = 120 to 140 R/sub e near the center of the tail to beyond absolute value of X = 200 R/sub e at the flanks. Downstream of the neutral line the plasma sheet magnetic field is shown to be negative and directly proportional to negative B/sub z in the <span class="hlt">solar</span> wind as <span class="hlt">observed</span> by IMP-8. V/sub x in the distant plasma sheet is also found to be proportional to IMF B/sub z with southward IMF producing the highest anti-<span class="hlt">solar</span> flow velocities. A global dayside reconnection efficiency of 20 +- 5% is derived from the ISEE-3/IMP-8 magnetic field comparisons. Substorm activity, as measured by the AL index, produces enhanced negative B/sub z and tailward V/sub x in the distant plasma sheet in agreement with the basic predictions of the reconnection-based models of substorms. The rate of magnetic flux transfer out of the tail as a function of AL is found to be consistent with previous near-Earth studies. Similarly, the mass and energy fluxes carried by plasma sheet flow down the tail are consistent with theoretical mass and energy budgets for an open magnetosphere. In summary, the ISEE-3 Geotail <span class="hlt">observations</span> appear to provide good support for reconnection models of <span class="hlt">solar</span> wind-magnetosphere coupling and substorm energy rates.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19990111616&hterms=1756&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3D1756','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19990111616&hterms=1756&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3D1756"><span>A CME-Driven <span class="hlt">Solar</span> Wind Disturbance <span class="hlt">Observed</span> at both Low and High Heliographic Latitudes</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Gosling, J. T.; McComas, D. J.; Phillips, J. L.; Pizzo, V. J.; Goldstein, B. E.; Forsyth, R. J.; Lepping, R. P.</p> <p>1995-01-01</p> <p>A <span class="hlt">solar</span> wind disturbance produced by a fast coronal mass ejection, CME, that departed from the Sun on February 20, 1994 was <span class="hlt">observed</span> in the ecliptic plane at 1 AU by IMP 8 and at high heliographic latitudes at 3.53 AU by Ulysses. In the ecliptic the disturbance included a strong forward shock but no reverse shock, while at high latitudes the disturbance was bounded by a relatively weak forward-reverse shock pair. It is clear that the disturbance in the ecliptic plane was driven primarily by the relative speed between the CME and a slower ambient <span class="hlt">solar</span> wind ahead, whereas at higher latitudes the disturbance was driven by expansion of the CME. The combined IMP 8 and Ulysses <span class="hlt">observations</span> thus provide a graphic illustration of how a single fast CME can produce very different types of <span class="hlt">solar</span> wind disturbances at low and high heliographic latitudes. Simple numerical simulations help explain <span class="hlt">observed</span> differences at the two spacecraft.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008cosp...37..458C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008cosp...37..458C"><span>The MEXART ips <span class="hlt">observations</span> in route to the next <span class="hlt">solar</span> maximum</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Carrillo-Vargas, Armando; Gonzalez-Esparza, Americo; Andrade, Ernesto; Perez-Enriquez, Roman; Aguilar-Rodriguez, Ernesto; Casillas-Perez, Gilberto; Jeyakumar, Solai; Kurtz, Stanley; Sierra, Pablo; Vazquez, Samuel</p> <p></p> <p>We report the status of the Mexican Array Radio Telescope (MEXART) in preparation for the next <span class="hlt">solar</span> maximum. During this epoch, the MEXART will be one of the four dedicated radio telescopes (with the ORT in India; STEL in Japan; and MWA in Australia) to track large-scale structures in the <span class="hlt">solar</span> wind using the interplanetary scintillation (IPS) technique. This network of IPS observatories would produce, for the first time four g maps of the sky showing the size and shape of disturbances between the Sun and the Earth. We describe the operation and current <span class="hlt">observations</span> of the first IPS radio sources at 140 MHz detected by the MEXART. These <span class="hlt">observations</span> use a plane dipole array of 1024 elements (16 lines with 64 dipoles each one), feeding a Butler matrix of 16x16 ports. This system generates a 16 lobes at fixed declinations covering 120 degrees (from 40 degrees South to 80 degrees North). The beam fan uses the Earth's rotation to cover the whole sky. The <span class="hlt">observations</span> that will be made with the network of observatories of interplanetary flashing will complement the <span class="hlt">observations</span> of other observatories, instruments in situ, space probes, satellite, among others.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22663231-nustar-hard-ray-observation-sub-class-solar-flare','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22663231-nustar-hard-ray-observation-sub-class-solar-flare"><span>NuSTAR Hard X-Ray <span class="hlt">Observation</span> of a Sub-A Class <span class="hlt">Solar</span> Flare</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>Glesener, Lindsay; Krucker, Säm; Hudson, Hugh</p> <p></p> <p>We report a Nuclear Spectroscopic Telescope Array ( NuSTAR ) <span class="hlt">observation</span> of a <span class="hlt">solar</span> microflare, SOL2015-09-01T04. Although it was too faint to be <span class="hlt">observed</span> by the GOES X-ray Sensor, we estimate the event to be an A0.1 class flare in brightness. This microflare, with only ∼5 counts s{sup −1} detector{sup −1} <span class="hlt">observed</span> by the Reuven Ramaty High Energy <span class="hlt">Solar</span> Spectroscopic Imager ( RHESSI ), is fainter than any hard X-ray (HXR) flare in the existing literature. The microflare occurred during a <span class="hlt">solar</span> pointing by the highly sensitive NuSTAR astrophysical observatory, which used its direct focusing optics to produce detailed HXRmore » microflare spectra and images. The microflare exhibits HXR properties commonly <span class="hlt">observed</span> in larger flares, including a fast rise and more gradual decay, earlier peak time with higher energy, spatial dimensions similar to the RHESSI microflares, and a high-energy excess beyond an isothermal spectral component during the impulsive phase. The microflare is small in emission measure, temperature, and energy, though not in physical size; <span class="hlt">observations</span> are consistent with an origin via the interaction of at least two magnetic loops. We estimate the increase in thermal energy at the time of the microflare to be 2.4 × 10{sup 27} erg. The <span class="hlt">observation</span> suggests that flares do indeed scale down to extremely small energies and retain what we customarily think of as “flare-like” properties.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19990111714&hterms=solar+radiation&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Dsolar%2Bradiation','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19990111714&hterms=solar+radiation&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Dsolar%2Bradiation"><span>Surface Net <span class="hlt">Solar</span> Radiation Estimated from Satellite Measurements: Comparisons with Tower <span class="hlt">Observations</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Li, Zhanqing; Leighton, H. G.; Cess, Robert D.</p> <p>1993-01-01</p> <p>A parameterization that relates the reflected <span class="hlt">solar</span> flux at the top of the atmosphere to the net <span class="hlt">solar</span> flux at the surface in terms of only the column water vapor amount and the <span class="hlt">solar</span> zenith angle was tested against surface <span class="hlt">observations</span>. Net surface fluxes deduced from coincidental collocated satellite-measured radiances and from measurements from towers in Boulder during summer and near Saskatoon in winter have mean differences of about 2 W/sq m, regardless of whether the sky is clear or cloudy. Furthermore, comparisons between the net fluxes deduced from the parameterization and from surface measurements showed equally good agreement when the data were partitioned into morning and afternoon <span class="hlt">observations</span>. This is in contrast to results from an empirical clear-sky algorithm that is unable to account adequately for the effects of clouds and that shows, at Boulder, a distinct morning to afternoon variation, which is presumably due to the predominance of different cloud types throughout the day. It is also demonstrated that the parameterization may be applied to irradiances at the top of the atmosphere that have been temporally averaged by using the temporally averaged column water vapor amount and the temporally averaged cosine of the <span class="hlt">solar</span> zenith angle. The good agreement between the results of the parameterization and surface measurements suggests that the algorithm is a useful tool for a variety of climate studies.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20140006007','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20140006007"><span>Suzaku <span class="hlt">Observations</span> of Charge Exchange Emission from <span class="hlt">Solar</span> System Objects</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Ezoe, Y.; Fujimoto, R.; Yamasaki, N. Y.; Mitsuda, K.; Ohashi, T.; Ishikawa, K.; Oishi, S.; Miyoshi, Y; Terada, N.; Futaana, Y.; <a style="text-decoration: none; " href="javascript:void(0); " onClick="displayelement('author_20140006007'); toggleEditAbsImage('author_20140006007_show'); toggleEditAbsImage('author_20140006007_hide'); "> <img style="display:inline; width:12px; height:12px; " src="images/arrow-up.gif" width="12" height="12" border="0" alt="hide" id="author_20140006007_show"> <img style="width:12px; height:12px; display:none; " src="images/arrow-down.gif" width="12" height="12" border="0" alt="hide" id="author_20140006007_hide"></p> <p>2012-01-01</p> <p>Recent results of charge exchange emission from <span class="hlt">solar</span> system objects <span class="hlt">observed</span> with the Japanese Suzaku satellite are reviewed. Suzaku is of great importance to investigate diffuse X-ray emission like the charge exchange from planetary exospheres and comets. The Suzaku studies of Earth's exosphere, Martian exosphere, Jupiter's aurorae, and comets are overviewed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19890014028','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19890014028"><span><span class="hlt">Observational</span> techniques for <span class="hlt">solar</span> flare gamma-rays, hard X-rays, and neutrons</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Lin, Robert P.</p> <p>1989-01-01</p> <p>The development of new instrumentation and techniques for <span class="hlt">solar</span> hard X-ray, gamma ray and neutron <span class="hlt">observations</span> from spacecraft and/or balloon-borne platforms is examined. The principal accomplishments are: (1) the development of a two segment germanium detector which is near ideal for <span class="hlt">solar</span> hard X-ray and gamma ray spectroscopy; (2) the development of long duration balloon flight techniques and associated instrumentation; and (3) the development of innovative new position sensitive detectors for hard X-ray and gamma rays.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AAS...22432349S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AAS...22432349S"><span>MESSENGER soft X-ray <span class="hlt">observations</span> of the quiet <span class="hlt">solar</span> corona</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Schwartz, Richard A.; Hudson, Hugh S.; Tolbert, Anne K; Dennis, Brian R.</p> <p>2014-06-01</p> <p>In a remarkable result from their "SphinX" experiment, Sylwester et al. (2012) found a non-varying base level of soft X-ray emission at the quietest times in 2009. We describe comparable data from the soft X-ray monitor on board MESSENGER (en route to Mercury) which had excellent coverage both in 2009 and during the true <span class="hlt">solar</span> minimum of 2008. These <span class="hlt">observations</span> overlap SphinX's and also are often exactly at Sun-MESSENGER-Earth conjunctions. During <span class="hlt">solar</span> minimum the Sun-MESSENGER distance varied substantially, allowing us to use the inverse-square law to help distinguish the aperture flux (ie, <span class="hlt">solar</span> X-rays) from that due to sources of background in the 2-5 keV range. The MESSENGER data show a non-varying background level for many months in 2008 when no active regions were present. We compare these data in detail with those from SphinX. Both sets of data reveal a different behavior when magnetic active regions are present on the Sun, and when they are not.Reference: Sylwester et al., ApJ 751, 111 (2012)</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007AdSpR..39.1451R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007AdSpR..39.1451R"><span>Brazilian Decimetre Array (Phase-1): Initial <span class="hlt">solar</span> <span class="hlt">observations</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ramesh, R.; Sawant, H. S.; Cecatto, J. R.; Faria, C.; Fernandes, F. C. R.; Kathiravan, C.; Suryanarayana, G. S.</p> <p></p> <p>An East-West one-dimensional radio interferometer array consisting of 5 parabolic dish antennas has been set-up at Cachoeira Paulista, Brazil (Longitude: 45°0'20″W, Latitude: 22°41'19″S) for <span class="hlt">observations</span> of Sun and some of the strong sidereal sources by the Instituto Nacional de Pesquisas Espaciais (INPE), Brazil. This is Phase-1 of the proposed Brazilian Decimetre Array (BDA) and can be operated at any frequency in the range 1.2-1.7 GHz. The instrument is functional since November 2004 onwards at 1.6 GHz. The angular and temporal resolution at the above frequency range are ˜3' and 100 ms, respectively. We present here the initial <span class="hlt">solar</span> <span class="hlt">observations</span> carried out with this array.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015JSARA..10...77M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015JSARA..10...77M"><span>33 Years of Continuous <span class="hlt">Solar</span> Radio Flux <span class="hlt">Observations</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Monstein, Christian</p> <p>2015-10-01</p> <p>In 1982, after development and testing of several analog receiver concepts, I started continuous <span class="hlt">solar</span> radio flux <span class="hlt">observations</span> at 230 MHz. My instruments for the <span class="hlt">observations</span> were based on cheap commercial components out of consumer TV electronics. The main components included a TV-tuner (at that time analog), intermediate frequency (IF) amplifier and video-detector taken from used TV sets. The 5.5 MHz wide video signal was fed into an integrating circuit, in fact a low pass filter, followed by dc-offset circuit and dc-amplifier built with four ua741 and CA3140 operational amplifier integrated circuits. At that time the signal was recorded with a Heathkit stripchart recorder and ink pen; an example is shown in figure 1.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20100003420','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20100003420"><span><span class="hlt">Observations</span> and Interpretations of Energetic Neutral Hydrogen Atoms from the December 5, 2006 <span class="hlt">Solar</span> Event</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Mewaldt, R. A.; Leske, R. A.; Shih, A. Y.; Stone, E. C.; Barghouty, A. f.; Cohen, C. M. S.; Cummings, A. c.; Labrador, A. W.; vonRosenvinge, T. T.</p> <p>2009-01-01</p> <p>We discuss recently reported <span class="hlt">observations</span> of energetic neutral hydrogen atoms (ENAs) from an X9 <span class="hlt">solar</span> flare/coronal mass ejection event on 5 December 2006, located at E79. The <span class="hlt">observations</span> were made by the Low Energy Telescopes (LETs) on STEREO A and B. Prior to the arrival of the main <span class="hlt">solar</span> energetic particle (SEP) event at Earth, both LETs <span class="hlt">observed</span> a sudden burst of 1.6 to 15 MeV energetic neutral hydrogen atoms produced by either flare or shock-accelerated protons. RHESSI measurements of the 2.2-MeV gamma-ray line provide an estimate of the number of interacting flare-accelerated protons in this event, which leads to an improved estimate of ENA production by flare-accelerated protons. Taking into account ENA losses, we find that the <span class="hlt">observed</span> ENAs must have been produced in the high corona at heliocentric distances > or equal to 2 <span class="hlt">solar</span> radii. Although there are no CME images from this event, it is shown that CME-shock-accelerated protons can, in principle, produce a time-history consistent with the <span class="hlt">observations</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008P%26SS...56.1562J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008P%26SS...56.1562J"><span>High-frequency Faraday rotation <span class="hlt">observations</span> of the <span class="hlt">solar</span> corona</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jensen, Elizabeth A.; Russell, Christopher T.</p> <p>2008-10-01</p> <p>This thesis, presented on January 31, 2007 under the supervision of Professor Christopher T. Russell, discusses the <span class="hlt">solar</span> coronal magnetic field <span class="hlt">observations</span> that can be obtained using the phenomenon of Faraday rotation. It was defended in the Department of Earth and Space Sciences at the University of California, Los Angeles (595 Charles E. Young, Dr. East, Los Angeles, CA 90095). A resume can be found at http://acs-consulting.com/.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19920035413&hterms=Pleiades&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3DPleiades','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19920035413&hterms=Pleiades&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3DPleiades"><span>IUE <span class="hlt">observations</span> of <span class="hlt">solar</span>-type stars in the Pleiades and the Hyades</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Caillault, Jean-Pierre; Vilhu, Osmi; Linsky, Jeffrey L.</p> <p>1991-01-01</p> <p>An extensive set of IUE <span class="hlt">observations</span> of <span class="hlt">solar</span>-type stars (spectral types F5-G5) in the Pleiades is presented. Spectra were obtained in January and August 1988 for both the transition region and chromospheric emission wavelength regions, respectively. Mg II fluxes were detected for two out of three Pleiades stars and C IV upper limits for two of these stars. Long-wavelength high-resolution spectra were also obtained for previously unobserved <span class="hlt">solar</span>-type stars in the Hyades. With the inclusion of spectra of additional Hyades stars obtained from the IUE archives, surface fluxes and fractional luminosities for both clusters' <span class="hlt">solar</span>-type stars are calculated; these values provide a better estimate for the Mg II saturation line for single stars.</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/2017EGUGA..19..750S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..19..750S"><span>Distributions of <span class="hlt">solar</span> drift-pair bursts in frequency from decameter radio <span class="hlt">observations</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Stanislavsky, Aleksander; Volvach, Yaroslav</p> <p>2017-04-01</p> <p>Statement of the Problem: <span class="hlt">Solar</span> drift-pair (DP) bursts are one of interesting manifestations of <span class="hlt">solar</span> activity. <span class="hlt">Observed</span> during the <span class="hlt">solar</span> storms of type III bursts, they demonstrate a very simple form on dynamic radio spectra as two short components separated in time, often the second component being the full repetition of the first. As is well known, type III bursts are produced by the accelerated electrons propagating along open magnetic field lines in <span class="hlt">solar</span> corona. However, no each storm of type III bursts leads to any DP. The role of electron beams in the generation of DPs remains unclear. <span class="hlt">Solar</span> DPs are detected by ground-based instruments at decameter and meter wavelengths, but each individual DP occupies only a limited bandwidth in the frequency range. The bursts drift in frequency, and their frequency drift rate can be both negative and positive (so-called the forward and reverse DPs), from -2 MHz/s to 6 MHz/s [1]. Besides, there are cases of vertical DPs, which occur simultaneously in all the frequencies within their bandwidth. It is difficult to interpret them by means of a moving source, as any exciting agent responsible for such bursts would travel with velocities faster than velocity of light [2]. Methodology & Experimental Orientation: New features of modern low-frequency radio astronomy allow us to study the empirical properties of DPs more deeply than ever before. Our results are based on the recent radio data (during 10-12 July of 2015) obtained with help of the UTR-2 radio telescope at frequencies 9-33 MHz with the time resolution of 50 ms and the frequency resolution of 4 kHz. We have identified 301 DP bursts in which 209 events were forward (FDP), and the rest were reverse (RDP). Results & Significance: According to the data, the occurrence of FDPs decreased at high frequencies, whereas the number of RDPs had an opposite tendency, they rarely occured at lower frequencies. During the <span class="hlt">observational</span> session, at 20-25 MHz almost the same amount of</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUFMSH41E..06S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUFMSH41E..06S"><span>Relativistic-Electron-Dominated <span class="hlt">Solar</span> Flares <span class="hlt">Observed</span> by Fermi/GBM</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Shih, A. Y.; Schwartz, R. A.; Dennis, B. R.</p> <p>2013-12-01</p> <p>Up to tens of percent of the energy released in <span class="hlt">solar</span> flares goes into accelerating electrons above ~10 keV and ions above ~1 MeV, and the impulsive heating of the ambient <span class="hlt">solar</span> atmosphere by these particles is partially or wholly responsible for the production of hot flare plasmas (up to ~50 MK). Although flares can accelerate electrons to relativistic energies, in even large flares the typical falling power-law energy spectrum means that the plasma is primarily heated by the much larger number of low-energy electrons. However, there have been flares <span class="hlt">observed</span> where the electron energy spectra have high low-energy cutoffs (well above ~100 keV), which significantly changes the electron energies responsible for heating and modifies the usual conception of energy transport in a flare. A systematic study of a range of relativistic-electron-dominated flares can improve our understanding of the relevant acceleration processes and how they may differ from those in "typical" flares. We search the Fermi/GBM data set for such flares based on the electron-associated X-ray/gamma-ray bremsstrahlung emission, making use of an improved background-subtraction approach to improve the ability to detect weaker flares. We present the fitted parameters for the relativistic-electron spectrum and their evolution over time, and compare against RHESSI <span class="hlt">observations</span> and other instruments when available. We also discuss these events in the context of previously <span class="hlt">observed</span> correlations between relativistic-electron acceleration and ion acceleration in flares.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://images.nasa.gov/#/details-GSFC_20171208_Archive_e000963.html','SCIGOVIMAGE-NASA'); return false;" href="https://images.nasa.gov/#/details-GSFC_20171208_Archive_e000963.html"><span>Mid-level <span class="hlt">Solar</span> Flare</span></a></p> <p><a target="_blank" href="https://images.nasa.gov/">NASA Image and Video Library</a></p> <p></p> <p>2017-12-08</p> <p>SDO View of M7.3 Class <span class="hlt">Solar</span> Flare on Oct. 2, 2014 NASA's <span class="hlt">Solar</span> Dynamics Observatory <span class="hlt">captured</span> this image of an M7.3 class <span class="hlt">solar</span> flare on Oct. 2, 2014. The <span class="hlt">solar</span> flare is the bright flash of light on the right limb of the sun. A burst of <span class="hlt">solar</span> material erupting out into space can be seen just below it. Credit: NASA/Goddard/SDO NASA image use policy. NASA Goddard Space Flight Center enables NASA’s mission through four scientific endeavors: Earth Science, Heliophysics, <span class="hlt">Solar</span> System Exploration, and Astrophysics. Goddard plays a leading role in NASA’s accomplishments by contributing compelling scientific knowledge to advance the Agency’s mission. Follow us on Twitter Like us on Facebook Find us on Instagram</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017APS..DPPN11177L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017APS..DPPN11177L"><span><span class="hlt">Observations</span> of magnetic pumping in the <span class="hlt">solar</span> wind using MMS data</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lichko, Emily; Egedal, Jan; Daughton, William; Kasper, Justin</p> <p>2017-10-01</p> <p>The turbulent cascade is believed to play an important role in the energization of the <span class="hlt">solar</span> wind plasma. However, there are characteristics of the <span class="hlt">solar</span> wind that are not readily explained by the cascade, such as the power-law distribution of the <span class="hlt">solar</span> wind speed. Starting from the drift kinetic equation, we have derived a magnetic pumping model, similar to the magnetic pumping well-known in fusion research, that provides an explanation for these features. In this model, particles are heated by the largest scale turbulent fluctuations, providing a complementary heating mechanism to the turbulent cascade. We will present <span class="hlt">observations</span> of this mechanism in the bow shock region using data from the Magnetospheric MultiScale mission. This research was conducted with support from National Defense Science and Engineering Graduate (NDSEG) Fellowship, 32 CFR 168, as well as from NSF Award 1404166 and NASA award NNX15AJ73G.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19890040747&hterms=energy+solar&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Denergy%2Bsolar','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19890040747&hterms=energy+solar&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Denergy%2Bsolar"><span>Multispectral <span class="hlt">observations</span> complementary to the study of high-energy <span class="hlt">solar</span> phenomena</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Walker, Arthur B. C., Jr.</p> <p>1988-01-01</p> <p>Multispectral <span class="hlt">observations</span> of phenomena associated with nonthermal events on the sun and characterized by the transient acceleration of electrons and ions to energies ranging from several keV to tens of GeV are discussed. It is shown that <span class="hlt">observations</span> of the thermal and quasi-thermal phenomena preceeding, coinciding with, and following the impulsive acceleration and heating event itself can be used to study the evolution of magnetic structures in the <span class="hlt">solar</span> convection zone and atmosphere. <span class="hlt">Observational</span> techniques are discussed in detail.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19950058979&hterms=time+series+modeling&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dtime%2Bseries%2Bmodeling','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19950058979&hterms=time+series+modeling&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dtime%2Bseries%2Bmodeling"><span>Recent <span class="hlt">solar</span> extreme ultraviolet irradiance <span class="hlt">observations</span> and modeling: A review</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Tobiska, W. Kent</p> <p>1993-01-01</p> <p>For more than 90 years, <span class="hlt">solar</span> extreme ultraviolet (EUV) irradiance modeling has progressed from empirical blackbody radiation formulations, through fudge factors, to typically measured irradiances and reference spectra was well as time-dependent empirical models representing continua and line emissions. A summary of recent EUV measurements by five rockets and three satellites during the 1980s is presented along with the major modeling efforts. The most significant reference spectra are reviewed and threee independently derived empirical models are described. These include Hinteregger's 1981 SERF1, Nusinov's 1984 two-component, and Tobiska's 1990/1991/SERF2/EUV91 flux models. They each provide daily full-disk broad spectrum flux values from 2 to 105 nm at 1 AU. All the models depend to one degree or another on the long time series of the Atmosphere Explorer E (AE-E) EUV database. Each model uses ground- and/or space-based proxies to create emissions from <span class="hlt">solar</span> atmospheric regions. Future challenges in EUV modeling are summarized including the basic requirements of models, the task of incorporating new <span class="hlt">observations</span> and theory into the models, the task of comparing models with <span class="hlt">solar</span>-terrestrial data sets, and long-term goals and modeling objectives. By the late 1990s, empirical models will potentially be improved through the use of proposed <span class="hlt">solar</span> EUV irradiance measurements and images at selected wavelengths that will greatly enhance modeling and predictive capabilities.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19800000342&hterms=use+solar+panels&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Duse%2Bsolar%2Bpanels','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19800000342&hterms=use+solar+panels&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Duse%2Bsolar%2Bpanels"><span><span class="hlt">Solar</span> heated office complex--Greenwood, South Carolina</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p></p> <p>1981-01-01</p> <p>Report contains thorough docuumentation of project meeting 85 percent of building heat requirements. System uses roof mounted recirculating water <span class="hlt">solar</span> panels and underground hot water energy storage. Aluminum film reflectors increase total <span class="hlt">solar</span> flux <span class="hlt">captured</span> by panels.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMSH51D2610K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMSH51D2610K"><span>Identifying and Characterizing Kinetic Instabilities using <span class="hlt">Solar</span> Wind <span class="hlt">Observations</span> of Non-Maxwellian Plasmas</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Klein, K. G.</p> <p>2016-12-01</p> <p>Weakly collisional plasmas, of the type typically <span class="hlt">observed</span> in the <span class="hlt">solar</span> wind, are commonly in a state other than local thermodynamic equilibrium. This deviation from a Maxwellian velocity distribution can be characterized by pressure anisotropies, disjoint beams streaming at differing speeds, leptokurtic distributions at large energies, and other non-thermal features. As these features may be artifacts of dynamic processes, including the the acceleration and expansion of the <span class="hlt">solar</span> wind, and as the free energy contained in these features can drive kinetic micro-instabilities, accurate measurement and modeling of these features is essential for characterizing the <span class="hlt">solar</span> wind. After a review of these features, a technique is presented for the efficient calculation of kinetic instabilities associated with a general, non-Maxwellian plasma. As a proof of principle, this technique is applied to bi-Maxwellian systems for which kinetic instability thresholds are known, focusing on parameter scans including beams and drifting heavy minor ions. The application of this technique to fits of velocity distribution functions from current, forthcoming, and proposed missions including WIND, DSCOVR, <span class="hlt">Solar</span> Probe Plus, and THOR, as well as the underlying measured distribution functions, is discussed. Particular attention is paid to the effects of instrument pointing and integration time, as well as potential deviation between instabilities associated with the Maxwellian fits and those associated with the <span class="hlt">observed</span>, potentially non-Maxwellian, velocity distribution. Such application may further illuminate the role instabilities play in the evolution of the <span class="hlt">solar</span> wind.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMSH13B2485F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMSH13B2485F"><span>Atmospheric Responses from Radiosonde <span class="hlt">Observations</span> of the 2017 Total <span class="hlt">Solar</span> Eclipse</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Fowler, J.</p> <p>2017-12-01</p> <p>The Atmospheric Responses from Radiosonde <span class="hlt">Observations</span> project during the August 21st, 2017 Total <span class="hlt">Solar</span> Eclipse was to <span class="hlt">observe</span> the atmospheric response under the shadow of the Moon using both research and operational earth science instruments run primarily by undergraduate students not formally trained in atmospheric science. During the eclipse, approximately 15 teams across the path of totality launched radiosonde balloon platforms in very rapid, serial sonde deployment. Our strategy was to combine a dense ground <span class="hlt">observation</span> network with multiple radiosonde sites, located within and along the margins of the path of totality. This can demonstrate how dense <span class="hlt">observation</span> networks leveraged among various programs can "fill the gaps" in data sparse regions allowing research ideas and questions that previously could not be approached with courser resolution data and improving the scientific understanding and prediction of geophysical and hazardous phenomenon. The core scientific objectives are (1) to make high-resolution surface and upper air <span class="hlt">observations</span> in several sites along the eclipse path (2) to quantitatively study atmospheric responses to the rapid disappearance of the Sun across the United States, and (3) to assess the performance of high-resolution weather forecasting models in simulating the <span class="hlt">observed</span> response. Such a scientific campaign, especially unique during a total <span class="hlt">solar</span> eclipse, provides a rare but life-altering opportunity to attract and enable next-generation of <span class="hlt">observational</span> scientists. It was an ideal "laboratory" for graduate, undergraduate, citizen scientists and k-12 students and staff to learn, explore and research in STEM.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018ApJ...860L..25Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018ApJ...860L..25Y"><span>Mini-filament Eruptions Triggering Confined <span class="hlt">Solar</span> Flares <span class="hlt">Observed</span> by ONSET and SDO</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yang, Shuhong; Zhang, Jun</p> <p>2018-06-01</p> <p>Using the <span class="hlt">observations</span> from the Optical and Near-infrared <span class="hlt">Solar</span> Eruption Tracer (ONSET) and the <span class="hlt">Solar</span> Dynamics Observatory (SDO), we study an M5.7 flare in AR 11476 on 2012 May 10 and a micro-flare in the quiet Sun on 2017 March 23. Before the onset of each flare, there is a reverse S-shaped filament above the polarity inversion line, then the filaments become unstable and begin to rise. The rising filaments gain the upper hand over the tension force of the dome-like overlying loops and thus successfully erupt outward. The footpoints of the reconnecting overlying loops successively brighten and are <span class="hlt">observed</span> as two flare ribbons, while the newly formed low-lying loops appear as post-flare loops. These eruptions are similar to the classical model of successful filament eruptions associated with coronal mass ejections (CMEs). However, the erupting filaments in this study move along large-scale lines and eventually reach the remote <span class="hlt">solar</span> surface; i.e., no filament material is ejected into the interplanetary space. Thus, both the flares are confined. These results reveal that some successful filament eruptions can trigger confined flares. Our <span class="hlt">observations</span> also imply that this kind of filament eruption may be ubiquitous on the Sun, from active regions (ARs) with large flares to the quiet Sun with micro-flares.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AAS...22914005K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AAS...22914005K"><span><span class="hlt">Observing</span> the 2017 Total <span class="hlt">Solar</span> Eclipse from the Pisgah Astronomical Research Institute</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kirwan, Sean Matthew; Cline, J. Donald; Krochmal, Mark; Donald Cline, Mark Krochmal</p> <p>2017-01-01</p> <p>The Pisgah Astronomical Research Institute (PARI) is located directly under the path of totality of next year’s <span class="hlt">solar</span> eclipse and possesses two 26m radio telescopes capable of interferometry at simultaneously at 2.3 GHz and 8.4 GHZ. PARI is preparing these radio telescopes for use by the astronomical community to <span class="hlt">observe</span> <span class="hlt">solar</span> eclipse. We will present the status of PARI’s radio telescopes and information on access for the eclipse. We will also present the status and availability of several optical telescopes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016cosp...41E.787H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016cosp...41E.787H"><span><span class="hlt">Observations</span> of a <span class="hlt">solar</span> storm from the stratosphere: The BARREL Mission</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Halford, Alexa</p> <p>2016-07-01</p> <p>During the Balloon Array for Radiation belt Relativistic Electron Losses (BARREL) second campaign, BARREL <span class="hlt">observed</span> with a single primary instrument, a 3"x3" NaI spectrometer measuring 20 keV - 10 MeV X-rays [Woodger et al 2015 JGR], portions of an entire <span class="hlt">solar</span> storm. This very small event, in terms of geomagnetic activity, or one of the largest of the current <span class="hlt">solar</span> cycle, in terms of <span class="hlt">solar</span> energetic particle events, has given us a very clear set of <span class="hlt">observations</span> of the response of the day side magnetosphere to the arrival of an interplanetary coronal mass ejection shock. The BARREL mission of opportunity working in tandem with the Van Allen Probes was designed to study the loss of radiation belt electrons to the ionosphere and upper atmosphere. However BARREL is able to see X-rays from a multitude of sources. During the second campaign, the Sun produced, and BARREL <span class="hlt">observed</span>, an X-class flare [McGregor et al in prep.]. This was followed by BARREL <span class="hlt">observations</span> of X-rays, gamma-rays, and directly injected protons from the <span class="hlt">solar</span> energetic particle (SEP) event associated with the eruption from the Sun while simultaneously the Van Allen Probes <span class="hlt">observed</span> the SEP protons in the inner magnetosphere [Halford et al 2016 submitted JGR]. Two days later the shock generated by the interplanetary coronal mass ejection (ICME-shock) hit the Earth while BARREL was in conjunction with the Van Allen Probes and GOES [Halford et al 2015 JGR]. Although this was a Mars directed CME and the Earth only received a glancing blow [Möstl et al 2015 Nat. Commun., Mays et al 2015 ApJ], the modest compression led to the formation of ultra low frequency (ULF) waves, electromagnetic ion cyclotron (EMIC) waves, and very low frequency (VLF) whistler mode waves [Halford and Mann 2016 submitted to JGR]. The combination of these waves and the enhancement of the local particle population led to precipitation of electrons remotely <span class="hlt">observed</span> by BARREL. This was not a Halloween, Bastille Day, or one of the now</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015JGRD..120.6500W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015JGRD..120.6500W"><span>Decadal variability of surface incident <span class="hlt">solar</span> radiation over China: <span class="hlt">Observations</span>, satellite retrievals, and reanalyses</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wang, Kaicun; Ma, Qian; Li, Zhijun; Wang, Jiankai</p> <p>2015-07-01</p> <p>Existing studies have shown that <span class="hlt">observed</span> surface incident <span class="hlt">solar</span> radiation (Rs) over China may have important inhomogeneity issues. This study provides metadata and reference data to homogenize <span class="hlt">observed</span> Rs, from which the decadal variability of Rs over China can be accurately derived. From 1958 to 1990, diffuse <span class="hlt">solar</span> radiation (Rsdif) and direct <span class="hlt">solar</span> radiation (Rsdir) were measured separately, and Rs was calculated as their sum. The pyranometers used to measure Rsdif had a strong sensitivity drift problem, which introduced a spurious decreasing trend into the <span class="hlt">observed</span> Rsdif and Rs data, whereas the <span class="hlt">observed</span> Rsdir did not suffer from this sensitivity drift problem. From 1990 to 1993, instruments and measurement methods were replaced and measuring stations were restructured in China, which introduced an abrupt increase in the <span class="hlt">observed</span> Rs. Intercomparisons between <span class="hlt">observation</span>-based and model-based Rs performed in this research show that sunshine duration (SunDu)-derived Rs is of high quality and can be used as reference data to homogenize <span class="hlt">observed</span> Rs data. The homogenized and adjusted data of <span class="hlt">observed</span> Rs combines the advantages of <span class="hlt">observed</span> Rs in quantifying hourly to monthly variability and SunDu-derived Rs in depicting decadal variability and trend. Rs averaged over 105 stations in China decreased at -2.9 W m-2 per decade from 1961 to 1990 and remained stable afterward. This decadal variability is confirmed by the <span class="hlt">observed</span> Rsdir and diurnal temperature ranges, and can be reproduced by high-quality Earth System Models. However, neither satellite retrievals nor reanalyses can accurately reproduce such decadal variability over China.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://images.nasa.gov/#/details-GSFC_20171208_Archive_e000962.html','SCIGOVIMAGE-NASA'); return false;" href="https://images.nasa.gov/#/details-GSFC_20171208_Archive_e000962.html"><span>Mid-level <span class="hlt">Solar</span> Flare</span></a></p> <p><a target="_blank" href="https://images.nasa.gov/">NASA Image and Video Library</a></p> <p></p> <p>2014-10-02</p> <p>NASA's <span class="hlt">Solar</span> Dynamics Observatory <span class="hlt">captured</span> these images of a <span class="hlt">solar</span> flare on Oct. 2, 2014. The <span class="hlt">solar</span> flare is the bright flash of light on the right limb of the sun. A burst of <span class="hlt">solar</span> material erupting out into space can be seen just below it. Read more: 1.usa.gov/1mW8rel Credit: NASA/Goddard/SDO NASA image use policy. NASA Goddard Space Flight Center enables NASA’s mission through four scientific endeavors: Earth Science, Heliophysics, <span class="hlt">Solar</span> System Exploration, and Astrophysics. Goddard plays a leading role in NASA’s accomplishments by contributing compelling scientific knowledge to advance the Agency’s mission. Follow us on Twitter Like us on Facebook Find us on Instagram</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011SPD....42.1903C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011SPD....42.1903C"><span>Tiny Pores <span class="hlt">Observed</span> by New <span class="hlt">Solar</span> Telescope and Hinode</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Cho, KyungSuk; Bong, S.; Chae, J.; Kim, Y.; Park, Y.; Ahn, K.; Katsukawa, Y.</p> <p>2011-05-01</p> <p>Seoul National University and Korea Astronomy and Space Science Institute installed Fast Imaging <span class="hlt">Solar</span> Spectrograph (FISS) in the Cude room of the 1.6 m New <span class="hlt">Solar</span> Telescope (NST) at Big Bear <span class="hlt">Solar</span> Observatory on May 14, 2010. FISS is a unique system that can do imaging of H-alpha and Ca II 8542 band simultaneously, which is quite suitable for studying of dynamics of chromosphere. To investigate the relationship between the photospheric and low-chromospheric motions at the pore region, we took a coordinate <span class="hlt">observation</span> with NST/FISS and Hinode/SOT for new emerging active region (AR11117) on October 26, 2010. In the <span class="hlt">observed</span> region, we could find two tiny pores and two small magnetic concentrations (SMCs), which have similar magnetic flux with the pores but do not look dark. Magnetic flux density and Doppler velocities at the photosphere are estimated by applying the center-of-gravity (COG) method to the HINODE/spectropolarimeter (SP) data. The line-of-sight motions above the photosphere are determined by adopting the bisector method to the wing spectra of Ha and CaII 8542 lines. As results, we found the followings. (1)There are upflow motion on the pores and downflow motion on the SMCs. (2)Towards the CaII 8542 line center, upflow motion decrease and turn to downward motion in pores, while the speed of down flow motion increases in the SMCs. (3)There is oscillating motion above pores and the SMCs, and this motion keep its pattern along the height. (4) As height increase, there is a general tendency of the speed shift to downward on pores and the SMCs. In this poster, we will present preliminary understanding of the coupling of pore dynamics between the photosphere and the low-chromosphere.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22167560-stereo-observations-fast-magnetosonic-waves-extended-solar-corona-associated-eit-euv-waves','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22167560-stereo-observations-fast-magnetosonic-waves-extended-solar-corona-associated-eit-euv-waves"><span>STEREO <span class="hlt">OBSERVATIONS</span> OF FAST MAGNETOSONIC WAVES IN THE EXTENDED <span class="hlt">SOLAR</span> CORONA ASSOCIATED WITH EIT/EUV WAVES</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>Kwon, Ryun-Young; Ofman, Leon; Kramar, Maxim</p> <p>2013-03-20</p> <p>We report white-light <span class="hlt">observations</span> of a fast magnetosonic wave associated with a coronal mass ejection <span class="hlt">observed</span> by STEREO/SECCHI/COR1 inner coronagraphs on 2011 August 4. The wave front is <span class="hlt">observed</span> in the form of density compression passing through various coronal regions such as quiet/active corona, coronal holes, and streamers. Together with measured electron densities determined with STEREO COR1 and Extreme UltraViolet Imager (EUVI) data, we use our kinematic measurements of the wave front to calculate coronal magnetic fields and find that the measured speeds are consistent with characteristic fast magnetosonic speeds in the corona. In addition, the wave front turns outmore » to be the upper coronal counterpart of the EIT wave <span class="hlt">observed</span> by STEREO EUVI traveling against the <span class="hlt">solar</span> coronal disk; moreover, stationary fronts of the EIT wave are found to be located at the footpoints of deflected streamers and boundaries of coronal holes, after the wave front in the upper <span class="hlt">solar</span> corona passes through open magnetic field lines in the streamers. Our findings suggest that the <span class="hlt">observed</span> EIT wave should be in fact a fast magnetosonic shock/wave traveling in the inhomogeneous <span class="hlt">solar</span> corona, as part of the fast magnetosonic wave propagating in the extended <span class="hlt">solar</span> corona.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3580320','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3580320"><span>Radioactive Cs <span class="hlt">capture</span> in the early <span class="hlt">solar</span> system</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Hidaka, Hiroshi; Yoneda, Shigekazu</p> <p>2013-01-01</p> <p>Barium isotopic compositions of primitive materials in the <span class="hlt">solar</span> system are generally affected by s- and r-process nucleosynthetic components that hide the contribution of the isotopic excess of 135Ba formed by decay of radioactive 135Cs. However, the Ba isotopic composition of the chemical separates from chondrules in the Sayama CM2 chondrite shows an excess of 135Ba isotopic abundance up to (0.33 ± 0.06)%, which is independent of the isotopic components from s- and r-process nucleosyntheses. The isotopic excesses of 135Ba correlate with the elemental abundance of Ba relative to Cs, providing chemical and isotopic evidence for the existence of the presently extinct radionuclide 135Cs (t1/2 = 2.3 million years) in the early <span class="hlt">solar</span> system. The estimated abundance of 135Cs/133Cs = (6.8 ± 1.9) × 10−4 is more than double that expected from the uniform production model of the short-lived radioisotopes, suggesting remobilization of Cs including 135Cs in the chondrules of the meteorite parent body. PMID:23435551</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMIN43C0090Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMIN43C0090Y"><span>The comparison of SRs' variation affected by <span class="hlt">solar</span> events <span class="hlt">observed</span> in America and in China</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yu, H.; Williams, E.</p> <p>2017-12-01</p> <p>Schumann Resonances(SRs) are the electromagnetic resonance wave propagating in the earth-ionosphere cavity. Its characteristic of propagation are modified by the variation of ionosphere. So SRs can be the tools of monitoring the ionosphere which is often perturbed by <span class="hlt">solar</span> events, x-ray emission and some other space-weather events (Roldugin et.al., 2004, De et al., 2010; Satori et.al., 2015). In present work, the amplitude and intrinsic frequencies of SRs <span class="hlt">observed</span> at RID station in America and YSH station in China are compared. The variation of SRs during the <span class="hlt">solar</span> flare on Feb. 15, 2011 are analyzed. Two-Dimensional Telegraph Equation(TDTE) method is used to simulate the perturbation of ionosphere by <span class="hlt">solar</span> proton events. From the simulation and <span class="hlt">observation</span>, the asymmetric construction of ionoshphere which is perturbed by the <span class="hlt">solar</span> event will affect the amplitudes and frequencies of SRs. Due to the interfere influence of forward and backward propagation of electromagnetic field, the SR amplitude on different station will present different variation. The distance among the lightning source, <span class="hlt">observer</span> and perturbed area will produce the different variation of amplitude and frequency for different station' SR.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19910013648','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19910013648"><span>The properties and environment of primitive <span class="hlt">solar</span> nebulae as deduced from <span class="hlt">observations</span> of <span class="hlt">solar</span>-type pre-main sequence stars</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Strom, Stephen E.; Edwards, Suzan; Strom, Karen M.</p> <p>1991-01-01</p> <p>The following topics were discussed: (1) current <span class="hlt">observation</span> evidence for the presence of circumstellar disks associated with <span class="hlt">solar</span> type pre-main sequence (PMS) stars; (2) the properties of such disks; and (3) the disk environment.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4508929','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4508929"><span>Ensemble downscaling in coupled <span class="hlt">solar</span> wind-magnetosphere modeling for space weather forecasting</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Owens, M J; Horbury, T S; Wicks, R T; McGregor, S L; Savani, N P; Xiong, M</p> <p>2014-01-01</p> <p>Advanced forecasting of space weather requires simulation of the whole Sun-to-Earth system, which necessitates driving magnetospheric models with the outputs from <span class="hlt">solar</span> wind models. This presents a fundamental difficulty, as the magnetosphere is sensitive to both large-scale <span class="hlt">solar</span> wind structures, which can be <span class="hlt">captured</span> by <span class="hlt">solar</span> wind models, and small-scale <span class="hlt">solar</span> wind “noise,” which is far below typical <span class="hlt">solar</span> wind model resolution and results primarily from stochastic processes. Following similar approaches in terrestrial climate modeling, we propose statistical “downscaling” of <span class="hlt">solar</span> wind model results prior to their use as input to a magnetospheric model. As magnetospheric response can be highly nonlinear, this is preferable to downscaling the results of magnetospheric modeling. To demonstrate the benefit of this approach, we first approximate <span class="hlt">solar</span> wind model output by smoothing <span class="hlt">solar</span> wind <span class="hlt">observations</span> with an 8 h filter, then add small-scale structure back in through the addition of random noise with the <span class="hlt">observed</span> spectral characteristics. Here we use a very simple parameterization of noise based upon the <span class="hlt">observed</span> probability distribution functions of <span class="hlt">solar</span> wind parameters, but more sophisticated methods will be developed in the future. An ensemble of results from the simple downscaling scheme are tested using a model-independent method and shown to add value to the magnetospheric forecast, both improving the best estimate and quantifying the uncertainty. We suggest a number of features desirable in an operational <span class="hlt">solar</span> wind downscaling scheme. Key Points <span class="hlt">Solar</span> wind models must be downscaled in order to drive magnetospheric models Ensemble downscaling is more effective than deterministic downscaling The magnetosphere responds nonlinearly to small-scale <span class="hlt">solar</span> wind fluctuations PMID:26213518</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/26213518','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26213518"><span>Ensemble downscaling in coupled <span class="hlt">solar</span> wind-magnetosphere modeling for space weather forecasting.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Owens, M J; Horbury, T S; Wicks, R T; McGregor, S L; Savani, N P; Xiong, M</p> <p>2014-06-01</p> <p>Advanced forecasting of space weather requires simulation of the whole Sun-to-Earth system, which necessitates driving magnetospheric models with the outputs from <span class="hlt">solar</span> wind models. This presents a fundamental difficulty, as the magnetosphere is sensitive to both large-scale <span class="hlt">solar</span> wind structures, which can be <span class="hlt">captured</span> by <span class="hlt">solar</span> wind models, and small-scale <span class="hlt">solar</span> wind "noise," which is far below typical <span class="hlt">solar</span> wind model resolution and results primarily from stochastic processes. Following similar approaches in terrestrial climate modeling, we propose statistical "downscaling" of <span class="hlt">solar</span> wind model results prior to their use as input to a magnetospheric model. As magnetospheric response can be highly nonlinear, this is preferable to downscaling the results of magnetospheric modeling. To demonstrate the benefit of this approach, we first approximate <span class="hlt">solar</span> wind model output by smoothing <span class="hlt">solar</span> wind <span class="hlt">observations</span> with an 8 h filter, then add small-scale structure back in through the addition of random noise with the <span class="hlt">observed</span> spectral characteristics. Here we use a very simple parameterization of noise based upon the <span class="hlt">observed</span> probability distribution functions of <span class="hlt">solar</span> wind parameters, but more sophisticated methods will be developed in the future. An ensemble of results from the simple downscaling scheme are tested using a model-independent method and shown to add value to the magnetospheric forecast, both improving the best estimate and quantifying the uncertainty. We suggest a number of features desirable in an operational <span class="hlt">solar</span> wind downscaling scheme. <span class="hlt">Solar</span> wind models must be downscaled in order to drive magnetospheric models Ensemble downscaling is more effective than deterministic downscaling The magnetosphere responds nonlinearly to small-scale <span class="hlt">solar</span> wind fluctuations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018AAS...23122008G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018AAS...23122008G"><span>Physical Conditions in the <span class="hlt">Solar</span> Corona Derived from the Total <span class="hlt">Solar</span> Eclipse <span class="hlt">Observations</span> obtained on 2017 August 21 Using a Polarization Camera</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gopalswamy, N.; Yashiro, Seiji; Reginald, Nelson; Thakur, Neeharika; Thompson, Barbara J.; Gong, Qian</p> <p>2018-01-01</p> <p>We present preliminary results obtained by <span class="hlt">observing</span> the <span class="hlt">solar</span> corona during the 2017 August 21 total <span class="hlt">solar</span> eclipse using a polarization camera mounted on an eight-inch Schmidt-Cassegrain telescope. The <span class="hlt">observations</span> were made from Madras Oregon during 17:19 to 17:21 UT. Total and polarized brightness images were obtained at four wavelengths (385, 398.5, 410, and 423 nm). The polarization camera had a polarization mask mounted on a 2048x2048 pixel CCD with a pixel size of 7.4 microns. The resulting images had a size of 975x975 pixels because four neighboring pixels were summed to yield the polarization and total brightness images. The ratio of 410 and 385 nm images is a measure of the coronal temperature, while that at 423 and 398.5 nm images is a measure of the coronal flow speed. We compared the temperature map from the eclipse <span class="hlt">observations</span> with that obtained from the <span class="hlt">Solar</span> Dynamics Observatory’s Atmospheric Imaging Assembly images at six EUV wavelengths, yielding consistent temperature information of the corona.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20050210136','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20050210136"><span>Simulation of the October-November 2003 <span class="hlt">solar</span> proton event in the CMAM GCM: Comparison with <span class="hlt">observations</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Semeniuk, K.; McConnell, J. C.; Jackman, C. H.</p> <p>2005-01-01</p> <p>The FTS instrument on SciSat-I <span class="hlt">observed</span> a very large NO(x) anomaly in mid February of 2004 near 80 N in the lower mesosphere. It has been proposed that the most likely origin of the lower mesosphere anomaly in February is transport, from the lower thermosphere or upper mesosphere, of high levels of NO(x) associated with high levels of <span class="hlt">solar</span> activity in 0ct.-Nov. 2003. There was no major <span class="hlt">solar</span> flare activity during January and February to cause ionization in the mesosphere. Using a middle atmosphere GCM we investigate whether the NO(x) produced directly by the 0ct.-Nov. 2003 <span class="hlt">solar</span> flares or indirectly via enhanced auroral ionization as a result of magnetospheric precipitation can explain the ACE <span class="hlt">observations</span>. We find that the <span class="hlt">solar</span> proton events associated with the <span class="hlt">solar</span> explosions in 0ct.-Nov. 2003 produce insufficient amounts of NO(x), in the mesosphere and thermosphere (less than 2 ppm at 90 km) to give rise to the <span class="hlt">observed</span> anomaly. However. there is evidence that intense aurorae caused by the 0ct.-Nov. 2003 <span class="hlt">solar</span> storms produced thermospheric values of NO(x) reaching hundreds of ppm. The NO(x) created by the auroral particles appears to have lasted much longer than the immediate period of the 0ct.-Nov. 2003 <span class="hlt">solar</span> storms. It appears that NO(x) rich air experienced confined polar night descent into the middle mesosphere during November and December, prior to the onset of the strong mesospheric vortex in January 2004.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/17289986','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/17289986"><span>Toward cost-effective <span class="hlt">solar</span> energy use.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Lewis, Nathan S</p> <p>2007-02-09</p> <p>At present, <span class="hlt">solar</span> energy conversion technologies face cost and scalability hurdles in the technologies required for a complete energy system. To provide a truly widespread primary energy source, <span class="hlt">solar</span> energy must be <span class="hlt">captured</span>, converted, and stored in a cost-effective fashion. New developments in nanotechnology, biotechnology, and the materials and physical sciences may enable step-change approaches to cost-effective, globally scalable systems for <span class="hlt">solar</span> energy use.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2005ApJ...627L.145I','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2005ApJ...627L.145I"><span>Near-Ultraviolet <span class="hlt">Observations</span> of CS 29497-030: New Constraints on Neutron-<span class="hlt">Capture</span> Nucleosynthesis Processes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ivans, Inese I.; Sneden, Christopher; Gallino, Roberto; Cowan, John J.; Preston, George W.</p> <p>2005-07-01</p> <p>Employing spectra obtained with the new Keck I HIRES near-UV-sensitive detector, we have performed a comprehensive chemical composition analysis of the binary blue metal-poor star CS 29497-030. Abundances for 29 elements and upper limits for an additional seven have been derived, concentrating on elements largely produced by means of neutron-<span class="hlt">capture</span> nucleosynthesis. Included in our analysis are the two elements that define the termination point of the slow neutron-<span class="hlt">capture</span> process, lead and bismuth. We determine an extremely high value of [Pb/Fe]=+3.65+/-0.07 (σ=0.13) from three features, supporting the single-feature result obtained in previous studies. We detect Bi for the first time in a metal-poor star. Our derived Bi/Pb ratio is in accord with those predicted from the most recent FRANEC calculations of the slow neutron-<span class="hlt">capture</span> process in low-mass asymptotic giant branch (AGB) stars. We find that the neutron-<span class="hlt">capture</span> elemental abundances of CS 29497-030 are best explained by an AGB model that also includes very significant amounts of pre-enrichment of rapid neutron-<span class="hlt">capture</span> process material in the protostellar cloud out of which the CS 29497-030 binary system formed. Mass transfer is consistent with the <span class="hlt">observed</span> [Nb/Zr]~0. Thus, CS 29497-030 is both an r+s and ``extrinsic AGB'' star. Furthermore, we find that the mass of the AGB model can be further constrained by the abundance of the light odd-element Na. The data presented herein were obtained at the W. M. Keck Observatory, which is operated as a scientific partnership among the California Institute of Technology, the University of California, and NASA. The Observatory was made possible by the generous financial support of the W. M. Keck Foundation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016cosp...41E2083Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016cosp...41E2083Y"><span><span class="hlt">Solar</span> neutron <span class="hlt">observations</span> with ChubuSat-2 satellite</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yamaoka, Kazutaka</p> <p>2016-07-01</p> <p><span class="hlt">Solar</span> neutron <span class="hlt">observation</span> is a key in understanding of ion accerelation mechanism in the Sun surface since neutrons are hardly affected by magnetic field around the Sun and intersteller mediums unlike charged particles. However, there was only a few tenth detections so far since its discovery in 1982. Actually SEDA-AP Fiber detector (FIB) onboard the International Space Station (ISS) was suffered from a high neutron background produced by the ISS itself. ChubuSat is a series of 50-kg class microsatellite jointly depeloped by universities (Nagoya university and Daido university) and aerospace companies at the Chubu area of central Japan. The ChubuSat-2 is the second ChubuSat following the ChubuSat-1 which was launched by Russian DNEPR rocket on November 6, 2014. It was selected as one of four piggyback payloads of the X-ray astronomy satellite ASTRO-H in 2014 summer, and will be launched by the H-IIA launch vehcles from from JAXA Tanegashima Space Center (TNSC) in February 2016. The ChubuSat-2 carries a mission instrument, radiation detector (RD). The main mission of ChubuSat-2 is devoted for monitoring neutrons and gamma-rays which can be background source for ASTRO-H celestrial <span class="hlt">observations</span> with the RD. The mission also involves a function of <span class="hlt">solar</span> neutron <span class="hlt">observations</span> which were originally proposed by graduate students who join the leadership development program for space exploration and research, program for leading graduate schools at Nagoya University. The RD has a similar detection area and efficiency to those of the SEDA-AP FIB, but is expected to have lower backgrounthan the ISS thanks to much smaller mass of the micro-satellite. In this paper, we will describe details of ChubuSat-2 satellite and RD, and in-orbit performance of RD.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017nova.pres.2871K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017nova.pres.2871K"><span>Little Eyes on Large <span class="hlt">Solar</span> Motions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kohler, Susanna</p> <p>2017-10-01</p> <p>Images taken during the <span class="hlt">solar</span> eclipse in 2012. The central color composite of the eclipsed <span class="hlt">solar</span> surface was <span class="hlt">captured</span> by SDO, the white-light view of the <span class="hlt">solar</span> corona around it was taken by the authors, and the background, wide-field black-and-white view is from LASCO. The white arrows mark the atypical structure. [Alzate et al. 2017]It seems like science is increasingly being done with advanced detectors on enormous ground- and space-based telescopes. One might wonder: is there anything left to learn from <span class="hlt">observations</span> made with digital cameras mounted on 10-cm telescopes?The answer is yes plenty! Illustrating this point, a new study using such equipment recently reports on the structure and dynamics of the Suns corona during two <span class="hlt">solar</span> eclipses.A Full View of the CoronaThe <span class="hlt">solar</span> corona is the upper part of the Suns atmosphere, extending millions of kilometers into space. This plasma is dynamic, with changing structures that arise in response to activity on the Suns surface such as enormous ejections of energy known as coronal mass ejections (CMEs). Studying the corona is therefore important for understanding what drives its structure and how energy is released from the Sun.Though there exist a number of space-based telescopes that <span class="hlt">observe</span> the Suns corona, they often have limited fields of view. The <span class="hlt">Solar</span> Dynamics Observatory AIA, for instance, has spectacular resolution but only images out to 1/3 of a <span class="hlt">solar</span> radius above the Suns limb. The space-based coronagraph LASCO C2, on the other hand, provides a broad view of the outer regions of the corona, but it only images down to 2.2 <span class="hlt">solar</span> radii above the Suns limb. Piecing together <span class="hlt">observations</span> from these telescopes therefore leaves a gap that prevents a full picture of the large-scale corona and how it connects to activity at the <span class="hlt">solar</span> surface.Same as the previous figure, but for the eclipse in 2013. [Alzate et al. 2017]To provide this broad, continuous picture, a team of scientists used digital cameras mounted on 10</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20000101064&hterms=Physical+Review&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3DPhysical%2BReview','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20000101064&hterms=Physical+Review&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3DPhysical%2BReview"><span><span class="hlt">Solar</span> Spicules: A Review of Recent Models and Targets for Future <span class="hlt">Observations</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Sterling, Alphonse C.; Rose, M. Franklin (Technical Monitor)</p> <p>2000-01-01</p> <p>Since their discovery over 100 years ago, there have been many suggestions for the origin and development of <span class="hlt">solar</span> spicules. Because the velocities of spicules are comparable to the sound and Alfven speeds of the low chromosphere, linear theory cannot fully describe them. Consequently, detailed tests of theoretical ideas had to await the development of computing power that only became available during the 1970s. This work reviews theories for spicules and spicule-like features over approximately the past 25 years, with an emphasis on the models based on nonlinear numerical simulations. These models have given us physical insight into wave propagation in the <span class="hlt">solar</span> atmosphere, and have helped elucidate how such waves, and associated shock waves, may be capable of creating motions and structures on magnetic flux tubes in the lower <span class="hlt">solar</span> atmosphere. So far, however, it has been difficult to reproduce the most- commonly -quoted parameters for spicules with these models, using what appears to be the most suitable input parameters. A key impediment to developing satisfactory models has been the lack of reliable <span class="hlt">observational</span> information, which is a consequence of the small angular size and transient lifetime of spicules. I close with a list of key <span class="hlt">observational</span> questions to be addressed with space-based satellites, such as the currently operating TRACE satellite, and especially the upcoming <span class="hlt">Solar</span>-B mission. Answers to these questions will help determine which, if any, of the current models correctly explains spicules.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20020022839&hterms=Physical+Review&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3DPhysical%2BReview','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20020022839&hterms=Physical+Review&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3DPhysical%2BReview"><span><span class="hlt">Solar</span> Spicules: A Review of Recent Models and Targets for Future <span class="hlt">Observations</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Sterling, Alphonse C.</p> <p>2000-01-01</p> <p>Since their discovery over 100 years ago, there have been many suggestions for the origin and development of <span class="hlt">solar</span> spicules. Because the velocities of spicules are comparable to the sound and Alfven speeds of the low chromosphere, linear theory cannot fully describe them. Consequently, detailed tests of theoretical ideas had to await the development of computing power that only became available during the 1970s. This work reviews theories for spicules and spicule-like features over approximately the past 25 years, with an emphasis an the models based on nonlinear numerical simulations. These models have given us physical insight into wave propagation in the <span class="hlt">solar</span> atmosphere and have helped elucidate how such waves, and associated shock waves, may be capable of creating motions and structures on magnetic flux tubes in the lower <span class="hlt">solar</span> atmosphere. So far, however, it has been difficult to reproduce the most commonly quoted parameters for spicules with these models, using what appears to be the most suitable input parameters. A key impediment to developing satisfactory models has been the lack of reliable <span class="hlt">observational</span> information, which is a consequence of the small angular size and transient lifetime of spicules. I close with a list of key <span class="hlt">observational</span> questions to be addressed with space-based satellites, such as the currently operating Transition Region and Coronal Explorer (TRACE) satellite, and especially the upcoming <span class="hlt">Solar</span>-B mission. Answers to these questions will help determine which, if any, of the current models correctly explains spicules.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19940035657&hterms=solar+radiation&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Dsolar%2Bradiation','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19940035657&hterms=solar+radiation&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Dsolar%2Bradiation"><span>Surface net <span class="hlt">solar</span> radiation estimated from satellite measurements - Comparisons with tower <span class="hlt">observations</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Li, Zhanqing; Leighton, H. G.; Cess, Robert D.</p> <p>1993-01-01</p> <p>A parameterization that relates the reflected <span class="hlt">solar</span> flux at the top of the atmosphere to the net <span class="hlt">solar</span> flux at the surface in terms of only the column water vapor amount and the <span class="hlt">solar</span> zenith angle was tested against surface <span class="hlt">observations</span>. Net surface fluxes deduced from coincidental collocated satellite-measured radiances and from measurements from towers in Boulder during summer and near Saskatoon in winter have mean differences of about 2 W/sq m, regardless of whether the sky is clear or cloudy. Furthermore, comparisons between the net fluxes deduced from the parameterization and from surface measurements showed equally good agreement when the data were partitioned into morning and afternoon <span class="hlt">observations</span>. This is in contrast to results from an empirical clear-sky algorithm that is unable to account adequately for the effects of clouds and that shows, at Boulder, a distinct morning to afternoon variation. It is also demonstrated that the parameterization may be applied to irradiances at the top of the atmosphere that have been temporally averaged. The good agreement between the results of the parameterization and surface measurements suggests that the algorithm is a useful tool for a variety of climate studies.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19890009004','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19890009004"><span>An investigation of ground-based <span class="hlt">observations</span> of <span class="hlt">solar</span> oscillations at Stanford</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Henning, Harald M. J.</p> <p>1987-01-01</p> <p>Data obtained in the last 8 years of <span class="hlt">solar</span> differential Doppler <span class="hlt">observations</span> at Stanford were considered. The four best time series of data were examined in detail. The sources of error in the data were investigated and removed where possible. In particular, the contribution resulting from transparency variations in the sky was examined. Detection method applicable to data with low signal to noise ratio and low filling factor were developed and utilized for the investigation of global <span class="hlt">solar</span> modes of oscillations in the data. The frequencies of p-modes were measured and identified. The presence of g-modes were also determined in the Stanford data.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009SPD....40.0916H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009SPD....40.0916H"><span><span class="hlt">Solar</span> Mean Magnetic Field <span class="hlt">Observed</span> by GONG</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Harvey, J. W.; Petrie, G.; Clark, R.; GONG Team</p> <p>2009-05-01</p> <p>The average line-of-sight (LOS) magnetic field of the Sun has been <span class="hlt">observed</span> for decades, either by measuring the circular polarization across a selected spectrum line using integrated sunlight or by averaging such measurements in spatially resolved images. The GONG instruments produce full-disk LOS magnetic images every minute, which can be averaged to yield the mean magnetic field nearly continuously. Such measurements are well correlated with the heliospheric magnetic field <span class="hlt">observed</span> near Earth about 4 days later. They are also a measure of <span class="hlt">solar</span> activity on long and short time scales. Averaging a GONG magnetogram, with nominal noise of 3 G per pixel, results in a noise level of about 4 mG. This is low enough that flare-related field changes have been seen in the mean field signal with time resolution of 1 minute. Longer time scales readily show variations associated with rotation of magnetic patterns across the <span class="hlt">solar</span> disk. Annual changes due to the varying visibility of the polar magnetic fields may also be seen. Systematic effects associated with modulator non-uniformity require correction and limit the absolute accuracy of the GONG measurements. Comparison of the measurements with those from other instruments shows high correlation but suggest that GONG measurements of field strength are low by a factor of about two. The source of this discrepancy is not clear. Fourier analysis of 2007 and 2008 time series of the GONG mean field measurements shows strong signals at 27.75 and 26.84/2 day (synodic) periods with the later period showing more power. The heliospheric magnetic field near Earth shows the same periods but with reversed power dominance. The Global Oscillation Network Group (GONG) project is managed by NSO, which is operated by AURA, Inc. under a cooperative agreement with the National Science Foundation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19790067720&hterms=Thermal+power+plant&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3DThermal%2Bpower%2Bplant','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19790067720&hterms=Thermal+power+plant&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3DThermal%2Bpower%2Bplant"><span>Projected techno-economic improvements for advanced <span class="hlt">solar</span> thermal power plants</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Fujita, T.; Manvi, R.; Roschke, E. J.</p> <p>1979-01-01</p> <p>The projected characteristics of <span class="hlt">solar</span> thermal power plants (with outputs up to 10 MWe) employing promising advanced technology subsystems/components are compared to current (or pre-1985) steam-Rankine systems. Improvements accruing to advanced technology development options are delineated. The improvements derived from advanced systems result primarily from achieving high efficiencies via <span class="hlt">solar</span> collector systems which (1) <span class="hlt">capture</span> a large portion of the available insolation and (2) concentrate this <span class="hlt">captured</span> <span class="hlt">solar</span> flux to attain high temperatures required for high heat engine/energy conversion performance. The most efficient <span class="hlt">solar</span> collector systems employ two-axis tracking. Attractive systems include the central receiver/heliostat and the parabolic dish.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19930049687&hterms=energy+regions+Remote&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Denergy%2Bregions%2BRemote','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19930049687&hterms=energy+regions+Remote&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Denergy%2Bregions%2BRemote"><span>Remote radio <span class="hlt">observations</span> of <span class="hlt">solar</span> wind parameters upstream of planetary bow shocks</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Macdowall, R. J.; Stone, R. G.; Gaffey, J. D., Jr.</p> <p>1992-01-01</p> <p>Radio emission is frequently produced at twice the electron plasma frequency 2fp in the foreshock region upstream of the terrestrial bow shock. <span class="hlt">Observations</span> of this emission provide a remote diagnostic of <span class="hlt">solar</span> wind parameters in the foreshock. Using ISEE-3 radio data, we present the first evidence that the radio intensity is proportional to the kinetic energy flux and to other parameters correlated with <span class="hlt">solar</span> wind density. We provide a qualitative explanation of this intensity behavior and predict the detection of similar emission at Jupiter by the Ulysses spacecraft.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016ASPC..504..331M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016ASPC..504..331M"><span><span class="hlt">Solar</span> Radio <span class="hlt">Observation</span> using Callisto Spectrometer at Sumedang West Java Indonesia: Current Status and Future Development Plan in Indonesia</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Manik, T.; Sitompul, P.; Batubara, M.; Harjana, T.; Yatini, C. Y.; Monstein, C.</p> <p>2016-04-01</p> <p>Sumedang Observatory (6.91°S, 107,84°E) was established in 1975 and is one of the <span class="hlt">solar</span> <span class="hlt">observation</span> facilities of the Space Science Center of Indonesian National Institute of Aeronautics and Space (LAPAN), located around 40 km, east part of Bandung City, West Java, Indonesia. Several instrumentations for <span class="hlt">solar</span> and space <span class="hlt">observation</span> such as optical telescopes, radio <span class="hlt">solar</span> spectrograph, flux gate magnetometer, etc. are operated there, together with an ionosphere sounding system (ionosonde) that was set up later. In July 2014, a standard Callisto (Compound Astronomical Low-cost Low-frequency Instrument for Spectroscopy and Transportable Observatory) spectrometer was installed at Sumedang Observatory for <span class="hlt">solar</span> radio activity monitoring. Callisto has been developed in the framework of IHY2007 and ISWI, supported by UN and NASA. Callisto spectrometer has <span class="hlt">observation</span> capability in the frequency range of 45-870 MHz. The Callisto spectrometer receives signal by using a set of 21 elements log-periodic antenna, model CLP5130-1N, pointed to the Sun and equipped with a low noise pre-amplifier. With respect to the Radio Frequency Interferences (RFI) measurements, the Callisto spectrometer is operated individually in frequency ranges of 45-80 MHz and 180-450 MHz. <span class="hlt">Observation</span> status and data flow are monitored in on-line from center office located in Bandung. The data was transferred to central database at FHNW (Fachhochschule Nordwestschweiz) server every 15 minutes to appear on e-Callisto network subsequently. A real time data transfer and data processing based on Python software also has been developed successfully to be used as an input for Space Weather Information and Forecasting Services (SWIFtS) provided by LAPAN. On 5th November 2014, Callisto spectrometer at Sumedang <span class="hlt">observed</span> the first clear <span class="hlt">solar</span> radio event, a <span class="hlt">solar</span> radio burst type II corresponding to a coronal mass ejection (CME), indicated by a strong X-ray event of M7.9 that was informed on by Space Weather</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20120012561&hterms=CAPS&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3DCAPS','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20120012561&hterms=CAPS&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3DCAPS"><span>24/7 <span class="hlt">Solar</span> Minimum Polar Cap and Auroral Ion Temperature <span class="hlt">Observations</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Sojka, Jan J.; Nicolls, Michael; van Eyken, Anthony; Heinselman, Craig; Bilitza, Dieter</p> <p>2011-01-01</p> <p>During the International Polar Year (IPY) two Incoherent Scatter Radars (ISRs) achieved close to 24/7 continuous <span class="hlt">observations</span>. This presentation describes their data sets and specifically how they can provide the International Reference Ionosphere (IRI) a fiduciary E- and F-region ionosphere description for <span class="hlt">solar</span> minimum conditions in both the auroral and polar cap regions. The ionospheric description being electron density, ion temperature and electron temperature profiles from as low as 90 km extending to several scale heights above the F-layer peak. The auroral location is Poker Flat in Alaska at 65.1 N latitude, 212.5 E longitude where the NSF s new Poker Flat Incoherent Scatter Radar (PFISR) is located. This location during <span class="hlt">solar</span> minimum conditions is in the auroral region for most of the day but is at midlatitudes, equator ward of the cusp, for about 4-8 h per day dependent upon geomagnetic activity. In contrast the polar location is Svalbard, at 78.2 N latitude, 16.0 E longitude where the EISCAT Svalbard Radar (ESR) is located. For most of the day the ESR is in the Northern Polar Cap with a noon sector passage often through the dayside cusp. Of unique relevance to IRI is that these extended <span class="hlt">observations</span> have enabled the ionospheric morphology to be distinguished between quiet and disturbed geomagnetic conditions. During the IPY year, 1 March 2007 - 29 February 2008, about 50 <span class="hlt">solar</span> wind Corotating Interaction Regions (CIRs) impacted geospace. Each CIR has a two to five day geomagnetic disturbance that is <span class="hlt">observed</span> in the ESR and PFISR <span class="hlt">observations</span>. Hence, this data set also enables the quiet-background ionospheric climatology to be established as a function of season and local time. These two separate climatologies for the ion temperature at an altitude of 300 km are presented and compared with IRI ion temperatures. The IRI ion temperatures are about 200-300 K hotter than the <span class="hlt">observed</span> values. However, the MSIS neutral temperature at 300 km compares favorably</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19930049592&hterms=lazarus&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAuthor-Name%26N%3D0%26No%3D60%26Ntt%3Dlazarus','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19930049592&hterms=lazarus&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAuthor-Name%26N%3D0%26No%3D60%26Ntt%3Dlazarus"><span><span class="hlt">Solar</span> wind temperature <span class="hlt">observations</span> in the outer heliosphere</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Gazis, P. R.; Barnes, A.; Mihalov, J. D.; Lazarus, A. J.</p> <p>1992-01-01</p> <p>The Pioneer 10, Pioneer 11, and Voyager 2 spacecraft are now at heliocentric distances of 50, 32 and 33 AU, and heliographic latitudes of 3.5 deg N, 17 deg N, and 0 deg N, respectively. Pioneer 11 and Voyager 2 are at similar celestial longitudes, while Pioneer l0 is on the opposite side of the sun. The baselines defined by these spacecraft make it possible to resolve radial, longitudinal, and latitudinal variations of <span class="hlt">solar</span> wind parameters. The <span class="hlt">solar</span> wind temperature decreases with increasing heliocentric distance out to a distance of 10-15 AU. At larger heliocentric distances, this gradient disappears. These high <span class="hlt">solar</span> wind temperatures in the outer heliosphere have persisted for at least 10 years, which suggests that they are not a <span class="hlt">solar</span> cycle effect. The <span class="hlt">solar</span> wind temperature varied with heliographic latitude during the most recent <span class="hlt">solar</span> minimum. The <span class="hlt">solar</span> wind temperature at Pioneer 11 and Voyager 2 was higher than that seen at Pioneer 10 for an extended period of time, which suggests the existence of a large-scale variation of temperature with celestial longitude, but the contribution of transient phenomena is yet to be clarified.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMIN43C0092B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMIN43C0092B"><span>Survey of localized <span class="hlt">solar</span> flare signatures in the ionosphere with GNSS, VLF, and GOES <span class="hlt">observations</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Blevins, S. M.; Hayes, L.; Collado-Vega, Y. M.; Michael, B. P.; Noll, C. E.</p> <p>2017-12-01</p> <p>Global navigation satellite system (GNSS) phase measurements of the total electron content (TEC) and ionospheric delay are sensitive to sudden increases in electron density in the layers of the Earth's ionosphere. These sudden ionospheric disruptions, or SIDs, are due to enhanced X-ray and extreme ultraviolet radiation from a <span class="hlt">solar</span> flare that drastically increases the electron density in localized regions. SIDs are <span class="hlt">solar</span> flare signatures in the Earth's ionosphere and can be <span class="hlt">observed</span> with very low frequency (VLF 3-30 kHz) monitors and dual-frequency GNSS (L1 = 1575.42 MHz, L2 = 1227.60 MHz) receivers that probe lower (D-region) to upper (F-region) ionospheric layers, respectively. Data from over 500 <span class="hlt">solar</span> flare events, spanning April 2010 to July 2017, including GOES C-, M-, and X-class <span class="hlt">solar</span> flares at various intensities, were collected from the Space Weather Database Of Notifications, Knowledge, Information (DONKI) developed at the NASA Goddard Space Flight Center (GSFC) Community Coordinated Modeling Center (CCMC). Historical GOES satellite (NOAA) X-ray flux (NASA GSFC CCMC integrated Space Weather Analysis system (iSWA)), and VLF SID (Stanford University <span class="hlt">Solar</span> SID Space Weather Monitor program) time series data are available for all <span class="hlt">solar</span> flare events of the sample set. We use GNSS data archived at the NASA GSFC Crustal Dynamics Data Information System (CDDIS) to characterize the F-region reactions to the increased ionization, complementing the ground-based D-region (VLF), and space-based X-ray <span class="hlt">observations</span> (GOES). CDDIS provides GNSS data with 24-hour coverage at a temporal resolution of 30 seconds from over 500 stations. In our study we choose 63 stations, spanning 23 countries at a variety of geographic locations to provide continuous coverage for all <span class="hlt">solar</span> flare events in the sample. This geographic distribution enables us to explore the effects of different <span class="hlt">solar</span> flare intensities at localized regions in the Earths ionosphere around the globe. The GNSS</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=Solar+AND+system&pg=2&id=EJ977364','ERIC'); return false;" href="https://eric.ed.gov/?q=Solar+AND+system&pg=2&id=EJ977364"><span><span class="hlt">Solar</span> Electricity for Homes</span></a></p> <p><a target="_blank" href="http://www.eric.ed.gov/ERICWebPortal/search/extended.jsp?_pageLabel=advanced">ERIC Educational Resources Information Center</a></p> <p>Roman, Harry T.</p> <p>2012-01-01</p> <p>Every day, the sun showers the Earth with millions of times more energy than its people use. The only problem is that energy is spread out over the entire Earth's surface and must be harvested. Engineers are learning to <span class="hlt">capture</span> and use some of this energy to make electricity for homes. <span class="hlt">Solar</span> panels make up the heart of a <span class="hlt">solar</span> system. They can be…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2004PhDT.........1Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2004PhDT.........1Y"><span>High resolution <span class="hlt">solar</span> <span class="hlt">observations</span> in the context of space weather prediction</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yang, Guo</p> <p></p> <p>Space weather has a great impact on the Earth and human life. It is important to study and monitor active regions on the <span class="hlt">solar</span> surface and ultimately to predict space weather based on the Sun's activity. In this study, a system that uses the full power of speckle masking imaging by parallel processing to obtain high-spatial resolution images of the <span class="hlt">solar</span> surface in near real-time has been developed and built. The application of this system greatly improves the ability to monitor the evolution of <span class="hlt">solar</span> active regions and to predict the adverse effects of space weather. The data obtained by this system have also been used to study fine structures on the <span class="hlt">solar</span> surface and their effects on the upper <span class="hlt">solar</span> atmosphere. A <span class="hlt">solar</span> active region has been studied using high resolution data obtained by speckle masking imaging. Evolution of a pore in an active region presented. Formation of a rudimentary penumbra is studied. The effects of the change of the magnetic fields on the upper level atmosphere is discussed. Coronal Mass Ejections (CMEs) have a great impact on space weather. To study the relationship between CMEs and filament disappearance, a list of 431 filament and prominence disappearance events has been compiled. Comparison of this list with CME data obtained by satellite has shown that most filament disappearances seem to have no corresponding CME events. Even for the limb events, only thirty percent of filament disappearances are associated with CMEs. A CME event that was <span class="hlt">observed</span> on March 20, 2000 has been studied in detail. This event did not show the three-parts structure of typical CMEs. The kinematical and morphological properties of this event were examined.</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('https://www.ncbi.nlm.nih.gov/pubmed/17774043','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/17774043"><span>Neutron <span class="hlt">capture</span> and stellar synthesis of heavy elements.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Gibbons, J H; Macklin, R L</p> <p>1967-05-26</p> <p>The neutron buildup processes of heavy-element synthesis in stars have left us a number of tantalizing nuclear clues to the early history of solarsystem material. Considerable illumination of our past history has been achieved through studying the correlations between abundance and neutroncapture cross section. Measurement of these cross sections required the development of new techniques for measuring time of flight of pulsed neutron beams. A clear conclusion is that many of our heavy elements were produced inside stars, which can be thought of as giant fast reactors. Extensions of these <span class="hlt">capture</span> studies have given a clearer picture of additional. violent processes which produced some heavy elements, particularly thorium and uranium. In addition, the correlations have been used for obtaining an independent measure of the time that has elapsed since the <span class="hlt">solar</span>-system material was synthesized. Finally, data on <span class="hlt">capture</span> cross section relative to abundance will enable us to determine rather accurately the <span class="hlt">solar</span>-system abundances of gaseous, volatile, and highly segregated elements.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20070011610&hterms=lazarus&qs=N%3D0%26Ntk%3DAuthor-Name%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dlazarus','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20070011610&hterms=lazarus&qs=N%3D0%26Ntk%3DAuthor-Name%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dlazarus"><span><span class="hlt">Solar</span> Wind Proton Temperature Anisotropy: Linear Theory and WIND/SWE <span class="hlt">Observations</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Hellinger, P.; Travnicek, P.; Kasper, J. C.; Lazarus, A. J.</p> <p>2006-01-01</p> <p>We present a comparison between WIND/SWE <span class="hlt">observations</span> (Kasper et al., 2006) of beta parallel to p and T perpendicular to p/T parallel to p (where beta parallel to p is the proton parallel beta and T perpendicular to p and T parallel to p are the perpendicular and parallel proton are the perpendicular and parallel proton temperatures, respectively; here parallel and perpendicular indicate directions with respect to the ambient magnetic field) and predictions of the Vlasov linear theory. In the slow <span class="hlt">solar</span> wind, the <span class="hlt">observed</span> proton temperature anisotropy seems to be constrained by oblique instabilities, by the mirror one and the oblique fire hose, contrary to the results of the linear theory which predicts a dominance of the proton cyclotron instability and the parallel fire hose. The fast <span class="hlt">solar</span> wind core protons exhibit an anticorrelation between beta parallel to c and T perpendicular to c/T parallel to c (where beta parallel to c is the core proton parallel beta and T perpendicular to c and T parallel to c are the perpendicular and parallel core proton temperatures, respectively) similar to that <span class="hlt">observed</span> in the HELIOS data (Marsch et al., 2004).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://images.nasa.gov/#/details-GSFC_20171208_Archive_e001746.html','SCIGOVIMAGE-NASA'); return false;" href="https://images.nasa.gov/#/details-GSFC_20171208_Archive_e001746.html"><span>NASA's SDO Satellite <span class="hlt">Captures</span> Venus Transit Approach</span></a></p> <p><a target="_blank" href="https://images.nasa.gov/">NASA Image and Video Library</a></p> <p></p> <p>2012-06-05</p> <p>NASA image <span class="hlt">captured</span> June 5, 2012 at 212357 UTC (about 5:24 p.m. EDT). On June 5-6 2012, SDO is collecting images of one of the rarest predictable <span class="hlt">solar</span> events: the transit of Venus across the face of the sun. This event happens in pairs eight years apart that are separated from each other by 105 or 121 years. The last transit was in 2004 and the next will not happen until 2117. This image was <span class="hlt">captured</span> by SDO's AIA instrument at 193 Angstroms. Credit: NASA/SDO, AIA To read more about the 2012 Venus Transit go to: sunearthday.nasa.gov/transitofvenus Add your photos of the Transit of Venus to our Flickr Group here: www.flickr.com/groups/venustransit/ NASA image use policy. NASA Goddard Space Flight Center enables NASA’s mission through four scientific endeavors: Earth Science, Heliophysics, <span class="hlt">Solar</span> System Exploration, and Astrophysics. Goddard plays a leading role in NASA’s accomplishments by contributing compelling scientific knowledge to advance the Agency’s mission. Follow us on Twitter Like us on Facebook Find us on Instagram</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018AAS...23240503B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018AAS...23240503B"><span>Possible Detection of <span class="hlt">Solar</span> Neutrons from the ISS</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Benker, Nicole; Echeverria-Mora, Elena; Hamblin, Jennifer; Dowben, Peter A.; Enders, Axel; Kananen, Brant; Petrosky, James; McClory, John</p> <p>2018-06-01</p> <p>A low energy steady state <span class="hlt">solar</span> neutron flux has been long predicted [1]. The Detector for the Analysis of <span class="hlt">Solar</span> Neutrons (DANSON), designed to detect this flux, was launched on the OA-5 mission to the International Space Station (ISS) on 17 Oct. 2016, deployed aboard ISS, and returned 19 March 2017. This detector is insensitive to high energy <span class="hlt">solar</span> neutron events associated with <span class="hlt">solar</span> flares, which have now been routinely detected in the range of 40 to 140 MeV, but the lower energy steady state <span class="hlt">solar</span> neutron background has not been thoroughly examined. DANSON is based on boron rich detector elements combined with a plastic moderator to thermalize neutrons at energies above 40 meV, maximizing the B10 <span class="hlt">capture</span> of epithermal neutrons. The detector elements include boron carbide (B10C2HX) heterojunction diodes on silicon and lithium tetraborate (Li2B4O7) single crystals. Three types of lithium tetraborate detector elements are used: crystals with a natural abundance of 10B (approx. 20% 10B, 80% 11B), crystals enriched in 10B, and crystals enriched in 11B. Enrichment in 10B provides a higher cross section for thermal neutron <span class="hlt">capture</span>, while enrichment in 11B results in a negligible cross section for thermal neutron <span class="hlt">capture</span> while maintaining a proton <span class="hlt">capture</span> cross section comparable to that of 10B. The signature of neutron <span class="hlt">capture</span> in the lithium tetraborate samples is evident in the thermoluminescent spectra. In the boron carbide diodes, the signature is measured in the huge decrease in drift carrier lifetimes compared to pre-flight characterization data, corresponding to about 3×109 neutrons/cm2 exposure. Since the estimated total <span class="hlt">solar</span> exposure time for deployment is 8×106 seconds, this amounts to about 250 to 375 neutrons and protons/cm2sec. The detector package shows increased detection on the zenith side of ISS, after subtraction of radiation events from energetic protons and other sources, indicating possible detection of <span class="hlt">solar</span> neutrons. Additionally, detection of</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/21578307-spatially-spectrally-resolved-observations-zebra-pattern-solar-decimetric-radio-burst','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/21578307-spatially-spectrally-resolved-observations-zebra-pattern-solar-decimetric-radio-burst"><span>SPATIALLY AND SPECTRALLY RESOLVED <span class="hlt">OBSERVATIONS</span> OF A ZEBRA PATTERN IN A <span class="hlt">SOLAR</span> DECIMETRIC RADIO BURST</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>Chen Bin; Bastian, T. S.; Gary, D. E.</p> <p>2011-07-20</p> <p>We present the first interferometric <span class="hlt">observation</span> of a zebra-pattern radio burst with simultaneous high spectral ({approx}1 MHz) and high time (20 ms) resolution. The Frequency-Agile <span class="hlt">Solar</span> Radiotelescope Subsystem Testbed (FST) and the Owens Valley <span class="hlt">Solar</span> Array (OVSA) were used in parallel to <span class="hlt">observe</span> the X1.5 flare on 2006 December 14. By using OVSA to calibrate the FST, the source position of the zebra pattern can be located on the <span class="hlt">solar</span> disk. With the help of multi-wavelength <span class="hlt">observations</span> and a nonlinear force-free field extrapolation, the zebra source is explored in relation to the magnetic field configuration. New constraints are placed onmore » the source size and position as a function of frequency and time. We conclude that the zebra burst is consistent with a double-plasma resonance model in which the radio emission occurs in resonance layers where the upper-hybrid frequency is harmonically related to the electron cyclotron frequency in a coronal magnetic loop.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20120010218&hterms=Butterfly&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3DButterfly','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20120010218&hterms=Butterfly&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3DButterfly"><span>Behavior of <span class="hlt">Solar</span> Cycles 23 and 24 Revealed by Microwave <span class="hlt">Observations</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Gopalswamy, N.; Yashiro, S.; Maekelae, P.; Michalek, G.; Shibasaki, K.; Hathaway, D. H.</p> <p>2012-01-01</p> <p>Using magnetic and microwave butterfly diagrams, we compare the behavior of <span class="hlt">solar</span> polar regions to show that (1) the polar magnetic field and the microwave brightness temperature during <span class="hlt">solar</span> minimum substantially diminished during the cycle 23/24 minimum compared to the 22/23 minimum. (2) The polar microwave brightness temperature (Tb) seems to be a good proxy for the underlying magnetic field strength (B). The analysis indicates a relationship, B = 0.0067Tb - 70, where B is in G and Tb in K. (3) Both the brightness temperature and the magnetic field strength show north-south asymmetry most of the time except for a short period during the maximum phase. (4) The rush-to-the-pole phenomenon <span class="hlt">observed</span> in the prominence eruption (PE) activity seems to be complete in the northern hemisphere as of 2012 March. (5) The decline of the microwave brightness temperature in the north polar region to the quiet-Sun levels and the sustained PE activity poleward of 60degN suggest that <span class="hlt">solar</span> maximum conditions have arrived at the northern hemisphere. The southern hemisphere continues to exhibit conditions corresponding to the rise phase of <span class="hlt">solar</span> cycle 24. Key words: Sun: chromosphere Sun: coronal mass ejections (CMEs) Sun: filaments, prominences Sun: photosphere Sun: radio radiation Sun: surface magnetism</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19980018649','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19980018649"><span>Constraints on <span class="hlt">Solar</span> Wind Acceleration Mechanisms from Ulysses Plasma <span class="hlt">Observations</span>: The First Polar Pass</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Barnes, Aaron; Gazis, Paul R.; Phillips, John L.</p> <p>1995-01-01</p> <p>The mass flux density and velocity of the <span class="hlt">solar</span> wind at polar latitudes can provide strong constraints on <span class="hlt">solar</span> wind acceleration mechanisms. We use plasma <span class="hlt">observations</span> from the first polar passage of the Ulysses spacecraft to investigate this question. We find that the mass flux density and velocity are too high to reconcile with acceleration of the <span class="hlt">solar</span> wind by classical thermal conduction alone. Therefore acceleration of the high-speed must involve extended deposition of energy by some other mechanism, either as heat or as a direct effective pressure, due possibly to waves and/or turbulence, or completely non-classical heat transport.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19820036544&hterms=coulomb+law&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Dcoulomb%2Blaw','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19820036544&hterms=coulomb+law&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Dcoulomb%2Blaw"><span><span class="hlt">Solar</span> wind helium ions - <span class="hlt">Observations</span> of the Helios <span class="hlt">solar</span> probes between 0.3 and 1 AU</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Marsch, E.; Rosenbauer, H.; Schwenn, R.; Muehlhaeuser, K.-H.; Neubauer, F. M.</p> <p>1982-01-01</p> <p>A Helios <span class="hlt">solar</span> probe survey of <span class="hlt">solar</span> wind helium ion velocity distributions and derived parameters between 0.3 and 1 AU is presented. Distributions in high-speed wind are found to generally have small total anisotropies, with some indication that, in the core part, the temperatures are greater parallel rather than perpendicular to the magnetic field. The anisotropy tends to increase with heliocentric radial distance, and the average dependence of helium ion temperatures on radial distance from the sun is described by a power law. Differential ion speeds with values of more than 150 km/sec are <span class="hlt">observed</span> near perihelion, or 0.3 AU. The role of Coulomb collisions in limiting differential ion speeds and the ion temperature ratio is investigated, and it is found that collisions play a distinct role in low-speed wind, by limiting both differential ion velocity and temperature.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMSA51B2426D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMSA51B2426D"><span>8 years of <span class="hlt">Solar</span> Spectral Irradiance <span class="hlt">Observations</span> from the ISS with the <span class="hlt">SOLAR</span>/SOLSPEC Instrument</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Damé, L.; Bolsée, D.; Meftah, M.; Irbah, A.; Hauchecorne, A.; Bekki, S.; Pereira, N.; Cessateur, G.; Marchand, M.; Thiéblemont, R.; Foujols, T.</p> <p>2016-12-01</p> <p>Accurate measurements of <span class="hlt">Solar</span> Spectral Irradiance (SSI) are of primary importance for a better understanding of <span class="hlt">solar</span> physics and of the impact of <span class="hlt">solar</span> variability on climate (via Earth's atmospheric photochemistry). The acquisition of a top of atmosphere reference <span class="hlt">solar</span> spectrum and of its temporal and spectral variability during the unusual <span class="hlt">solar</span> cycle 24 is of prime interest for these studies. These measurements are performed since April 2008 with the SOLSPEC spectro-radiometer from the far ultraviolet to the infrared (166 nm to 3088 nm). This instrument, developed under a fruitful LATMOS/BIRA-IASB collaboration, is part of the <span class="hlt">Solar</span> Monitoring Observatory (<span class="hlt">SOLAR</span>) payload, externally mounted on the Columbus module of the International Space Station (ISS). The <span class="hlt">SOLAR</span> mission, with its actual 8 years duration, will cover almost the entire <span class="hlt">solar</span> cycle 24. We present here the in-flight operations and performances of the SOLSPEC instrument, including the engineering corrections, calibrations and improved know-how procedure for aging corrections. Accordingly, a SSI reference spectrum from the UV to the NIR will be presented, together with its UV variability, as measured by <span class="hlt">SOLAR</span>/SOLSPEC. Uncertainties on these measurements and comparisons with other instruments will be briefly discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012AGUFMSM51A2295K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012AGUFMSM51A2295K"><span>Investigation of the <span class="hlt">solar</span> UV/EUV heating effect on the Jovian radiation belt by GMRT-IRTF <span class="hlt">observation</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kita, H.; Misawa, H.; Bhardwaj, A.; Tsuchiya, F.; Tao, C.; Uno, T.; Kondo, T.; Morioka, A.</p> <p>2012-12-01</p> <p>Jupiter's synchrotron radiation (JSR) is the emission from relativistic electrons, and it is the most effective probe for remote sensing of Jupiter's radiation belt from the Earth. Recent intensive <span class="hlt">observations</span> of JSR revealed short term variations of JSR with the time scale of days to weeks. Brice and McDonough (1973) proposed a scenario for the short term variations; i.e, the <span class="hlt">solar</span> UV/EUV heating for Jupiter's upper atmosphere causes enhancement of total flux density. The purpose of this study is to investigate whether sufficient <span class="hlt">solar</span> UV/EUV heating in Jupiter's upper atmosphere can actually causes variation in the JSR total flux and brightness distribution. Previous JSR <span class="hlt">observations</span> using the Giant Metrewave Radio Telescope (GMRT) suggested important characteristics of short term variations; relatively low energy particles are accelerated by some acceleration processes which might be driven by <span class="hlt">solar</span> UV/EUV heating and/or Jupiter's own magnetic activities. In order to evaluate the effect of <span class="hlt">solar</span> UV/EUV heating on JSR variations, we made coordinated <span class="hlt">observations</span> using the GMRT and NASA Infra-Red Telescope Facility (IRTF). By using IRTF, we can estimate the temperature of Jupiter's upper atmosphere from spectroscopic <span class="hlt">observation</span> of H_3^+ infrared emission. Hence, we can evaluate the relationship between variations in Jupiter's upper atmosphere initiated by the <span class="hlt">solar</span> UV/EUV heating and its linkage with the JSR. The GMRT <span class="hlt">observations</span> were made during Nov. 6-17, 2011 at the frequency of 235/610MHz. The H_3^+ 3.953 micron line was <span class="hlt">observed</span> using the IRTF during Nov. 7-12, 2011. During the <span class="hlt">observation</span> period, the <span class="hlt">solar</span> UV/EUV flux variations expected on Jupiter showed monotonic increase. A preliminary analysis of GMRT 610MHz band showed a radio flux variation similar to that in the <span class="hlt">solar</span> UV/EUV. Radio images showed that the emission intensity increased at the outer region and the position of equatorial peak emission moved in the outward direction. If radial diffusion</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016JPhCS.771a2043S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016JPhCS.771a2043S"><span>A perspective about the total <span class="hlt">solar</span> eclipse <span class="hlt">observation</span> from future space settlements and a review of Indonesian space researches</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sastradipradja, D.; Dwivany, F. M.; Swandjaja, L.</p> <p>2016-11-01</p> <p>Viewing astronomy objects from space is superior to that from Earth due to the absence of terrestrial atmospheric disturbances. Since decades ago, there has been an idea of building gigantic spaceships to live in, i.e., low earth orbit (LEO) settlement. In the context of <span class="hlt">solar</span> eclipse, the presuming space settlements will accommodate future <span class="hlt">solar</span> eclipse chasers (amateur or professional astronomers) to <span class="hlt">observe</span> <span class="hlt">solar</span> eclipse from space. Not only for scientific purpose, human personal <span class="hlt">observation</span> from space is also needed for getting aesthetical mental impression. Furthermore, since space science indirectly aids <span class="hlt">solar</span> eclipse <span class="hlt">observation</span>, we will discuss the related history and development of Indonesian space experiments. Space science is an essential knowledge to be mastered by all nations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19730024002','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19730024002"><span>Feasibility study for the use of a YF-12 aircraft as a scientific instrument platform for <span class="hlt">observing</span> the 1970 <span class="hlt">solar</span> eclipse</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Mercer, R. D.</p> <p>1973-01-01</p> <p>The scientific and engineering findings are presented of the feasibility study for the use of a YF-12 aircraft as a scientific instrument platform for <span class="hlt">observing</span> the 1970 <span class="hlt">solar</span> eclipse. Included in the report is the computer program documentation of the <span class="hlt">solar</span> eclipse determination; summary data on SR-71A type aircraft capabilities and limitations as an <span class="hlt">observing</span> platform for <span class="hlt">solar</span> eclipses; and the recordings of an informal conference on <span class="hlt">observations</span> of <span class="hlt">solar</span> eclipses using SR-71A type aircraft.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFMSH33A4124Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFMSH33A4124Y"><span>How Well Does the S-Web Theory Predict In-Situ <span class="hlt">Observations</span> of the Slow <span class="hlt">Solar</span> Wind?</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Young, A. K.; Antiochos, S. K.; Linker, J.; Zurbuchen, T.</p> <p>2014-12-01</p> <p>The S-Web theory provides a physical explanation for the origin and properties of the slow <span class="hlt">solar</span> wind, particularly its composition. The theory proposes that magnetic reconnection along topologically complex boundaries between open and closed magnetic fields on the sun releases plasma from closed magnetic field regions into the <span class="hlt">solar</span> wind at latitudes away from the heliospheric current sheet. Such a wind would have elevated charge states compared to the fast wind and an elemental composition resembling the closed-field corona. This theory is currently being tested using time-dependent, high-resolution, MHD simulations, however comparisons to in-situ <span class="hlt">observations</span> play an essential role in testing and understanding slow-wind release mechanisms. In order to determine the relationship between S-Web signatures and the <span class="hlt">observed</span>, slow <span class="hlt">solar</span> wind, we compare plasma data from the ACE and Ulysses spacecraft to solutions from the steady-state models created at Predictive Science, Inc., which use <span class="hlt">observed</span> magnetic field distributions on the sun as a lower boundary condition. We discuss the S-Web theory in light of our results and the significance of the S-Web for interpreting current and future <span class="hlt">solar</span> wind <span class="hlt">observations</span>. This work was supported, in part, by the NASA TR&T and SR&T programs.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1255080-ion-driven-instabilities-solar-wind-wind-observations-march','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1255080-ion-driven-instabilities-solar-wind-wind-observations-march"><span>Ion-driven instabilities in the <span class="hlt">solar</span> wind: Wind <span class="hlt">observations</span> of 19 March 2005</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Gary, S. Peter; Jian, Lan K.; Broiles, Thomas W.; ...</p> <p>2016-01-16</p> <p>Intervals of enhanced magnetic fluctuations have been frequently <span class="hlt">observed</span> in the <span class="hlt">solar</span> wind. However, it remains an open question as to whether these waves are generated at the Sun and then transported outward by the <span class="hlt">solar</span> wind or generated locally in the interplanetary medium. Magnetic field and plasma measurements from the Wind spacecraft under slow <span class="hlt">solar</span> wind conditions on 19 March 2005 demonstrate seven events of enhanced magnetic fluctuations at spacecraft-frame frequencies somewhat above the proton cyclotron frequency and propagation approximately parallel or antiparallel to the background magnetic field B o. The proton velocity distributions during these events are characterizedmore » by two components: a more dense, slower core and a less dense, faster beam. In conclusion, <span class="hlt">observed</span> plasma parameters are used in a kinetic linear dispersion equation analysis for electromagnetic fluctuations at k x B o = 0; for two events the most unstable mode is the Alfvén-cyclotron instability driven by a proton component temperature anisotropy T ⊥/T || > 1 (where the subscripts denote directions relative to B o), and for three events the most unstable mode is the right-hand polarized magnetosonic instability driven primarily by ion component relative flows. Thus, both types of ion anisotropies and both types of instabilities are likely to be local sources of these enhanced fluctuation events in the <span class="hlt">solar</span> wind.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1255080','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1255080"><span>Ion-driven instabilities in the <span class="hlt">solar</span> wind: Wind <span class="hlt">observations</span> of 19 March 2005</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>Gary, S. Peter; Jian, Lan K.; Broiles, Thomas W.</p> <p></p> <p>Intervals of enhanced magnetic fluctuations have been frequently <span class="hlt">observed</span> in the <span class="hlt">solar</span> wind. However, it remains an open question as to whether these waves are generated at the Sun and then transported outward by the <span class="hlt">solar</span> wind or generated locally in the interplanetary medium. Magnetic field and plasma measurements from the Wind spacecraft under slow <span class="hlt">solar</span> wind conditions on 19 March 2005 demonstrate seven events of enhanced magnetic fluctuations at spacecraft-frame frequencies somewhat above the proton cyclotron frequency and propagation approximately parallel or antiparallel to the background magnetic field B o. The proton velocity distributions during these events are characterizedmore » by two components: a more dense, slower core and a less dense, faster beam. In conclusion, <span class="hlt">observed</span> plasma parameters are used in a kinetic linear dispersion equation analysis for electromagnetic fluctuations at k x B o = 0; for two events the most unstable mode is the Alfvén-cyclotron instability driven by a proton component temperature anisotropy T ⊥/T || > 1 (where the subscripts denote directions relative to B o), and for three events the most unstable mode is the right-hand polarized magnetosonic instability driven primarily by ion component relative flows. Thus, both types of ion anisotropies and both types of instabilities are likely to be local sources of these enhanced fluctuation events in the <span class="hlt">solar</span> wind.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27818854','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27818854"><span>Ion-driven instabilities in the <span class="hlt">solar</span> wind: Wind <span class="hlt">observations</span> of 19 March 2005.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Gary, S Peter; Jian, Lan K; Broiles, Thomas W; Stevens, Michael L; Podesta, John J; Kasper, Justin C</p> <p>2016-01-01</p> <p>Intervals of enhanced magnetic fluctuations have been frequently <span class="hlt">observed</span> in the <span class="hlt">solar</span> wind. But it remains an open question as to whether these waves are generated at the Sun and then transported outward by the <span class="hlt">solar</span> wind or generated locally in the interplanetary medium. Magnetic field and plasma measurements from the Wind spacecraft under slow <span class="hlt">solar</span> wind conditions on 19 March 2005 demonstrate seven events of enhanced magnetic fluctuations at spacecraft-frame frequencies somewhat above the proton cyclotron frequency and propagation approximately parallel or antiparallel to the background magnetic field B o . The proton velocity distributions during these events are characterized by two components: a more dense, slower core and a less dense, faster beam. <span class="hlt">Observed</span> plasma parameters are used in a kinetic linear dispersion equation analysis for electromagnetic fluctuations at k x B o  = 0; for two events the most unstable mode is the Alfvén-cyclotron instability driven by a proton component temperature anisotropy T ⊥ /T ||  > 1 (where the subscripts denote directions relative to B o ), and for three events the most unstable mode is the right-hand polarized magnetosonic instability driven primarily by ion component relative flows. Thus, both types of ion anisotropies and both types of instabilities are likely to be local sources of these enhanced fluctuation events in the <span class="hlt">solar</span> wind.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5070513','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5070513"><span>Ion‐driven instabilities in the <span class="hlt">solar</span> wind: Wind <span class="hlt">observations</span> of 19 March 2005</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Jian, Lan K.; Broiles, Thomas W.; Stevens, Michael L.; Podesta, John J.; Kasper, Justin C.</p> <p>2016-01-01</p> <p>Abstract Intervals of enhanced magnetic fluctuations have been frequently <span class="hlt">observed</span> in the <span class="hlt">solar</span> wind. But it remains an open question as to whether these waves are generated at the Sun and then transported outward by the <span class="hlt">solar</span> wind or generated locally in the interplanetary medium. Magnetic field and plasma measurements from the Wind spacecraft under slow <span class="hlt">solar</span> wind conditions on 19 March 2005 demonstrate seven events of enhanced magnetic fluctuations at spacecraft‐frame frequencies somewhat above the proton cyclotron frequency and propagation approximately parallel or antiparallel to the background magnetic field B o. The proton velocity distributions during these events are characterized by two components: a more dense, slower core and a less dense, faster beam. <span class="hlt">Observed</span> plasma parameters are used in a kinetic linear dispersion equation analysis for electromagnetic fluctuations at k x B o = 0; for two events the most unstable mode is the Alfvén‐cyclotron instability driven by a proton component temperature anisotropy T⊥/T|| > 1 (where the subscripts denote directions relative to B o), and for three events the most unstable mode is the right‐hand polarized magnetosonic instability driven primarily by ion component relative flows. Thus, both types of ion anisotropies and both types of instabilities are likely to be local sources of these enhanced fluctuation events in the <span class="hlt">solar</span> wind. PMID:27818854</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010AGUFMSH13A..02S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010AGUFMSH13A..02S"><span>Multi-thermal <span class="hlt">observations</span> of flares and eruptions with the Atmospheric Imaging Assembly on the <span class="hlt">Solar</span> Dynamics Observatory. (Invited)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Schrijver, C. J.; Aia Science Team</p> <p>2010-12-01</p> <p>The revolutionary advance in <span class="hlt">observational</span> capabilities offered by SDO's AIA offers new views of <span class="hlt">solar</span> flares and eruptions. The high cadence and spatial resolution, the full-Sun coverage, and the variety of thermal responses of the AIA channels from thousands to millions of degrees enable the study the source regions of <span class="hlt">solar</span> explosions, as well as the responses of the <span class="hlt">solar</span> corona from their immediate vicinity to regions over a <span class="hlt">solar</span> radius away. These <span class="hlt">observations</span> emphasize the importance of magnetic connectivity and topology, the frequent occurrence of fast wave-like perturbations, and the contrasts between impulsive compact X-ray-bright flares and long-duration EUV-bright phenomena.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20170003051&hterms=Mysteries&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3DMysteries','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20170003051&hterms=Mysteries&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3DMysteries"><span>Implications of L1 <span class="hlt">Observations</span> for Slow <span class="hlt">Solar</span> Wind Formation by <span class="hlt">Solar</span> Reconnection</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kepko, L.; Viall, N. M.; Antiochos, S. K.; Lepri, S. T.; Kasper, J. C.; Weberg, M.</p> <p>2016-01-01</p> <p>While the source of the fast <span class="hlt">solar</span> wind is known to be coronal holes, the source of the slow <span class="hlt">solar</span> wind has remained a mystery. Long time scale trends in the composition and charge states show strong correlations between <span class="hlt">solar</span> wind velocity and plasma parameters, yet these correlations have proved ineffective in determining the slow wind source. We take advantage of new high time resolution (12 min) measurements of <span class="hlt">solar</span> wind composition and charge state abundances at L1 and previously identified 90 min quasi periodic structures to probe the fundamental timescales of slow wind variability. The combination of new high temporal resolution composition measurements and the clearly identified boundaries of the periodic structures allows us to utilize these distinct <span class="hlt">solar</span> wind parcels as tracers of slowwind origin and acceleration. We find that each 90 min (2000 Mm) parcel of slow wind has near-constant speed yet exhibits repeatable, systematic charge state and composition variations that span the entire range of statistically determined slow <span class="hlt">solar</span> wind values. The classic composition-velocity correlations do not hold on short, approximately hour long, time scales. Furthermore, the data demonstrate that these structures were created by magnetic reconnection. Our results impose severe new constraints on slow <span class="hlt">solar</span> wind origin and provide new, compelling evidence that the slow wind results from the sporadic release of closed field plasma via magnetic reconnection at the boundary between open and closed flux in the Sun's atmosphere.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMSH41B2533S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMSH41B2533S"><span><span class="hlt">Solar</span> Energetic Particle Events and CME Accelerations in the Low Corona: MLSO <span class="hlt">Observations</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>St Cyr, O. C.; Kahler, S. W.; Richardson, I. G.; Cane, H. V.; Xie, H.; Burkepile, J.</p> <p>2016-12-01</p> <p>The low <span class="hlt">solar</span> corona (< 2.5 Rs) is the region in which maximum coronal mass ejection (CME) acceleration occurs and where Type II radio <span class="hlt">observations</span> suggest that shock formation occurs (Mäkelä et al., 2015). It is therefore a key region for investigations of <span class="hlt">solar</span> energetic particle (SEP) acceleration by CME-driven shocks. <span class="hlt">Observations</span> very low in the corona are necessary to detect the rapid CME accelerations leading to shock formation and to assess the speeds of CMEs through the middle corona. However, these <span class="hlt">observations</span> cannot be made by space borne coronagraphs in which CME trajectories above the occulting disk are usually characterized by a single (constant) speed: e.g., 80% of the speeds in the compilation of SMM CMEs (Burkepile and St. Cyr, 1993) and SOHO LASCO CMEs (St. Cyr et al., 2000). The Mk3/Mk4/K-Cor coronameters at the Mauna Loa <span class="hlt">Solar</span> Observatory are able to measure the initial accelerations of CMEs low in the corona (i.e., < 2 Rs). We examine a subset of CMEs that were associated with SEP events between 1980-present. The subset is based on the CME launch occurring between 16 UT - 01 UT - the MLSO <span class="hlt">observing</span> window. In most cases, the CME accelerations are significantly larger than those measured by spaceborne coronagraphs (e.g., SMM, Solwind, LASCO, SECCHI). We will present the preliminary results of a comparison of the SEP parameters with initial CME accelerations in the MLSO coronagraph field of view.</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/2018SpWea..16..245H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018SpWea..16..245H"><span>Onsets of <span class="hlt">Solar</span> Proton Events in Satellite and Ground Level <span class="hlt">Observations</span>: A Comparison</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>He, Jing; Rodriguez, Juan V.</p> <p>2018-03-01</p> <p>The early detection of <span class="hlt">solar</span> proton event onsets is essential for protecting humans and electronics in space, as well as passengers and crew at aviation altitudes. Two commonly compared methods for <span class="hlt">observing</span> <span class="hlt">solar</span> proton events that are sufficiently large and energetic to be detected on the ground through the creation of secondary radiation—known as ground level enhancements (GLEs)—are (1) a network of ground-based neutron monitors (NMs) and (2) satellite-based particle detectors. Until recently, owing to the different time resolution of the two data sets, it has not been feasible to compare these two types of <span class="hlt">observations</span> using the same detection algorithm. This paper presents a comparison between the two <span class="hlt">observational</span> platforms using newly processed >100 MeV 1 min count rates and fluxes from National Oceanic and Atmospheric Administration's Geostationary Operational Environmental Satellite (GOES) 8-12 satellites, and 1 min count rates from the Neutron Monitor Database. We applied the same detection algorithm to each data set (tuned to the different background noise levels of the instrument types). Seventeen SPEs with GLEs were studied: GLEs 55-70 from <span class="hlt">Solar</span> Cycle 23 and GLE 71 from <span class="hlt">Solar</span> Cycle 24. The median difference in the event detection times by GOES and NM data is 0 min, indicating no innate benefit in time of either system. The 10th, 25th, 75th, and 90th percentiles of the onset time differences (GOES minus NMs) are -7.2 min, -1.5 min, 2.5 min, and 4.2 min, respectively. This is in contrast to previous studies in which NM detections led GOES by 8 to 52 min without accounting for different alert protocols.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://images.nasa.gov/#/details-GSFC_20171208_Archive_e001641.html','SCIGOVIMAGE-NASA'); return false;" href="https://images.nasa.gov/#/details-GSFC_20171208_Archive_e001641.html"><span>A New Set of <span class="hlt">Solar</span> Fireworks</span></a></p> <p><a target="_blank" href="https://images.nasa.gov/">NASA Image and Video Library</a></p> <p></p> <p>2017-12-08</p> <p>NASA's <span class="hlt">Solar</span> Dynamics Observatory (SDO) <span class="hlt">captured</span> this image of an M9-class flare on Oct 20, 2012 at 2:14 p.m. EDT. This image shows light at a wavelength of 131 Angstroms, which corresponds to material at 10 million Kelvin, and is a good wavelength for <span class="hlt">observing</span> flares. This wavelength is typically colorized as teal, as shown here. To read more go to: www.nasa.gov/mission_pages/sunearth/news/News102012-m9fla... Credit: NASA/GSFC/SDO NASA image use policy. NASA Goddard Space Flight Center enables NASA’s mission through four scientific endeavors: Earth Science, Heliophysics, <span class="hlt">Solar</span> System Exploration, and Astrophysics. Goddard plays a leading role in NASA’s accomplishments by contributing compelling scientific knowledge to advance the Agency’s mission. Follow us on Twitter Like us on Facebook Find us on Instagram</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018ApJ...856L..39C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018ApJ...856L..39C"><span>Weakened Magnetization and Onset of Large-scale Turbulence in the Young <span class="hlt">Solar</span> Wind—Comparisons of Remote Sensing <span class="hlt">Observations</span> with Simulation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chhiber, Rohit; Usmanov, Arcadi V.; DeForest, Craig E.; Matthaeus, William H.; Parashar, Tulasi N.; Goldstein, Melvyn L.</p> <p>2018-04-01</p> <p>Recent analysis of <span class="hlt">Solar</span>-Terrestrial Relations Observatory (STEREO) imaging <span class="hlt">observations</span> have described the early stages of the development of turbulence in the young <span class="hlt">solar</span> wind in <span class="hlt">solar</span> minimum conditions. Here we extend this analysis to a global magnetohydrodynamic (MHD) simulation of the corona and <span class="hlt">solar</span> wind based on inner boundary conditions, either dipole or magnetogram type, that emulate <span class="hlt">solar</span> minimum. The simulations have been calibrated using Ulysses and 1 au <span class="hlt">observations</span>, and allow, within a well-understood context, a precise determination of the location of the Alfvén critical surfaces and the first plasma beta equals unity surfaces. The compatibility of the the STEREO <span class="hlt">observations</span> and the simulations is revealed by direct comparisons. Computation of the radial evolution of second-order magnetic field structure functions in the simulations indicates a shift toward more isotropic conditions at scales of a few Gm, as seen in the STEREO <span class="hlt">observations</span> in the range 40–60 R ⊙. We affirm that the isotropization occurs in the vicinity of the first beta unity surface. The interpretation based on early stages of in situ <span class="hlt">solar</span> wind turbulence evolution is further elaborated, emphasizing the relationship of the <span class="hlt">observed</span> length scales to the much smaller scales that eventually become the familiar turbulence inertial range cascade. We argue that the <span class="hlt">observed</span> dynamics is the very early manifestation of large-scale in situ nonlinear couplings that drive turbulence and heating in the <span class="hlt">solar</span> wind.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19850059164&hterms=quasi+particle&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3Dquasi%2Bparticle','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19850059164&hterms=quasi+particle&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3Dquasi%2Bparticle"><span>Multispacecraft <span class="hlt">observations</span> of the east-west asymmetry of <span class="hlt">solar</span> energetic storm particle events</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Sarris, E. T.; Krimigis, S. M.</p> <p>1985-01-01</p> <p>Energetic proton <span class="hlt">observations</span> have been obtained by instruments aboard the IMP-7 and -8 spacecraft and Voyager-1 and -2 deep space probes, in order to study the generation of <span class="hlt">solar</span> flare Energetic Storm Particle Events (ESP) events at widely separated locations on the same shock front which are presumably characterized, on average, by different IMF shock front configurations for <span class="hlt">solar</span> flare sites. Energetic proton <span class="hlt">observations</span> indicate that substantial differences in the ESP proton intensity enhancements are detected at these energies for locations on the shock front with wide heliolongitude separations. The present results indicate that acceleration of ESP protons to more than 500 keV takes place at the quasi-perpendicular shock front domain, consistent with the 'shock drift' acceleration mechanism.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JASTP.171..277M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JASTP.171..277M"><span><span class="hlt">Observation</span> of the <span class="hlt">solar</span> eclipse of 20 March 2015 at the Pruhonice station</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mošna, Zbyšek; Boška, Josef; Knížová, Petra Koucká; Šindelářová, Tereza; Kouba, Daniel; Chum, Jaroslav; Rejfek, Luboš; Potužníková, Kateřina; Arikan, Feza; Toker, Cenk</p> <p>2018-06-01</p> <p>Response of the atmosphere to the <span class="hlt">Solar</span> Eclipse on 20 March 2015 is described for mid-latitude region of Czech Republic. For the first time we show join analysis using Digisonde vertical sounding, manually processed Digisonde drift measurement, and Continuous Doppler Sounding for the <span class="hlt">solar</span> eclipse study. The critical frequencies foE, foF1 and foF2 show changes with different time offset connected to the <span class="hlt">solar</span> eclipse. Digisonde drift measurement shows significant vertical plasma drifts in F2 region deviating from daily mean course with amplitudes reaching 15-20 m/s corresponding to the time of <span class="hlt">solar</span> eclipse. Continuous Doppler Sounding shows propagation of waves in the NE direction with velocities between 70 and 100 m/s with a peak 30 min after first contact. We <span class="hlt">observed</span> increased and persistent wave activity at heights between 150 and 250 km at time about 20-40 min after beginning of SE with central period 65 min.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19870067070&hterms=orbiting+wind&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dorbiting%2Bwind','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19870067070&hterms=orbiting+wind&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dorbiting%2Bwind"><span>Simultaneous <span class="hlt">observation</span> of Pc 3-4 pulsations in the <span class="hlt">solar</span> wind and in the earth's magnetosphere</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Engebretson, M. J.; Zanetti, L. J.; Potemra, T. A.; Baumjohann, W.; Luehr, H.; Acuna, M. H.</p> <p>1987-01-01</p> <p>The equatorially orbiting Active Magnetospheric Particle Tracer Explorers CCE and IRM satellites have made numerous <span class="hlt">observations</span> of Pc 3-4 magnetic field pulsations (10-s to 100-s period) simultaneously at locations upstream of the earth's bow shock and inside the magnetosphere. These <span class="hlt">observations</span> show <span class="hlt">solar</span> wind/IMF control of two categories of dayside magnetospheric pulsations. Harmonically structured, azimuthally polarized pulsations are commonly <span class="hlt">observed</span> from L = 4 to 9 in association with upstream waves. More monochromatic compressional pulsations are clearly evident on occasion, with periods identical to those <span class="hlt">observed</span> simultaneously in the <span class="hlt">solar</span> wind. The <span class="hlt">observations</span> reported here are consistent with a high-latitude (cusp) entry mechanism for wave energy related to harmonically structured pulsations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFMSH31C2435R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFMSH31C2435R"><span>Compressive Acceleration of <span class="hlt">Solar</span> Energetic Particles within Coronal Mass Ejections: <span class="hlt">Observations</span> and Theory Relevant to the <span class="hlt">Solar</span> Probe Plus and <span class="hlt">Solar</span> Orbiter Missions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Roelof, E. C.</p> <p>2015-12-01</p> <p><span class="hlt">Observations</span> of <span class="hlt">solar</span> energetic particles (SEPs) over <span class="hlt">Solar</span> Cycles 22-24 included the measurement of their pitch-angle distributions (PADs). When only magnetically "well-connected" SEP events were selected, i.e., with the spacecraft on interplanetary magnetic field (IMF) lines whose coronal foot-points were within about 30 deg of the associated flare site, the PADs were usually "beam-like" during the rise-to-maximum phase (RTM) of the events. This nearly "scatter-free" propagation (due to magnetic focusing of the IMF) revealed that the injection times of the SEPs were delayed up to 10s of minutes after the onset of electromagnetic emissions from the flare. Direct comparison with the flare-associated coronal mass ejections (CMEs) from the western hemisphere indicated that the SEP acceleration/injection was occurring at least 1 Rs into the corona (and often continuing well above that radial distance). Moreover, the RTM profiles exhibited a continuum of shapes, from "spikes" to "pulses" to "ramps", and these shape characterizations ordered the properties of the associated CMEs. Most importantly, when compared at nearly the same near-relativistic velocities, electrons and protons exhibited similar PADs and RTM profiles. Clearly, such orderly patterns in the data call for a single dominant acceleration process that treats all particles of similar velocities the same, regardless of mass and charge. A simple theory that meets all of these requirements, based on nearly scatter-free propagation and energy change within particle "reservoirs" (such as the closed magnetic structure of a CME), has recently been proposed [Roelof, Proc. 14th Ann. Int'l. Astrophys. Conf., IOP, in press, 2015]. The acceleration results from compression (-divV) of the driver plasma, well sunward of the CME shock. Acceleration (e-folding) times of only a few minutes can be obtained from representative parameters of 1000 km/s CMEs. A companion paper [Roelof and Vourlidas, op. cit.], proposed a new</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22654565-observational-evidence-associated-formation-blobs-raining-inflows-solar-corona','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22654565-observational-evidence-associated-formation-blobs-raining-inflows-solar-corona"><span><span class="hlt">Observational</span> Evidence for the Associated Formation of Blobs and Raining Inflows in the <span class="hlt">Solar</span> Corona</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>Sanchez-Diaz, E.; Rouillard, A. P.; Lavraud, B.</p> <p></p> <p>The origin of the slow <span class="hlt">solar</span> wind is still a topic of much debate. The continual emergence of small transient structures from helmet streamers is thought to constitute one of the main sources of the slow wind. Determining the height at which these transients are released is an important factor in determining the conditions under which the slow <span class="hlt">solar</span> wind forms. To this end, we have carried out a multipoint analysis of small transient structures released from a north–south tilted helmet streamer into the slow <span class="hlt">solar</span> wind over a broad range of position angles during Carrington Rotation 2137. Combining themore » remote-sensing <span class="hlt">observations</span> taken by the <span class="hlt">Solar</span>-TErrestrial RElations Observatory ( STEREO ) mission with coronagraphic <span class="hlt">observations</span> from the <span class="hlt">SOlar</span> and Heliospheric Observatory ( SOHO ) spacecraft, we show that the release of such small transient structures (often called blobs), which subsequently move away from the Sun, is associated with the concomitant formation of transient structures collapsing back toward the Sun; the latter have been referred to by previous authors as “raining inflows.” This is the first direct association between outflowing blobs and raining inflows, which locates the formation of blobs above the helmet streamers and gives strong support that the blobs are released by magnetic reconnection.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017ApJ...849...10F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017ApJ...849...10F"><span>A Compressed Sensing-based Image Reconstruction Algorithm for <span class="hlt">Solar</span> Flare X-Ray <span class="hlt">Observations</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Felix, Simon; Bolzern, Roman; Battaglia, Marina</p> <p>2017-11-01</p> <p>One way of imaging X-ray emission from <span class="hlt">solar</span> flares is to measure Fourier components of the spatial X-ray source distribution. We present a new compressed sensing-based algorithm named VIS_CS, which reconstructs the spatial distribution from such Fourier components. We demonstrate the application of the algorithm on synthetic and <span class="hlt">observed</span> <span class="hlt">solar</span> flare X-ray data from the Reuven Ramaty High Energy <span class="hlt">Solar</span> Spectroscopic Imager satellite and compare its performance with existing algorithms. VIS_CS produces competitive results with accurate photometry and morphology, without requiring any algorithm- and X-ray-source-specific parameter tuning. Its robustness and performance make this algorithm ideally suited for the generation of quicklook images or large image cubes without user intervention, such as for imaging spectroscopy analysis.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016cosp...41E1762S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016cosp...41E1762S"><span>Geomagnetic activity during 10 - 11 <span class="hlt">solar</span> cycles that has been <span class="hlt">observed</span> by old Russian observatories.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Seredyn, Tomasz; Wysokinski, Arkadiusz; Kobylinski, Zbigniew; Bialy, Jerzy</p> <p>2016-07-01</p> <p>A good knowledge of <span class="hlt">solar</span>-terrestrial relations during past <span class="hlt">solar</span> activity cycles could give the appropriate tools for a correct space weather forecast. The paper focuses on the analysis of the historical collections of the ground based magnetic <span class="hlt">observations</span> and their operational indices from the period of two sunspot <span class="hlt">solar</span> cycles 10 - 11, period 1856 - 1878 (Bartels rotations 324 - 635). We use hourly <span class="hlt">observations</span> of H and D geomagnetic field components registered at Russian stations: St. Petersburg - Pavlovsk, Barnaul, Ekaterinburg, Nertshinsk, Sitka, and compare them to the data obtained from the Helsinki observatory. We compare directly these records and also calculated from the data of the every above mentioned station IHV indices introduced by Svalgaard (2003), which have been used for further comparisons in epochs of assumed different polarity of the heliospheric magnetic field. We used also local index C9 derived by Zosimovich (1981) from St. Petersburg - Pavlovsk data. <span class="hlt">Solar</span> activity is represented by sunspot numbers. The correlative and continuous wavelet analyses are applied for estimation of the correctness of records from different magnetic stations. We have specially regard to magnetic storms in the investigated period and the special Carrington event of 1-2 Sep 1859. Generally studied magnetic time series correctly show variability of the geomagnetic activity. Geomagnetic activity presents some delay in relation to <span class="hlt">solar</span> one as it is seen especially during descending and minimum phase of the even 11-year cycle. This pattern looks similarly in the case of 16 - 17 <span class="hlt">solar</span> cycles.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20060030172&hterms=corona&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3Dcorona','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20060030172&hterms=corona&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3Dcorona"><span>Ka-band and X-band <span class="hlt">observations</span> of the <span class="hlt">solar</span> corona aquired during the Cassini 2002 superior conjunction</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Morabito, D. D.</p> <p>2002-01-01</p> <p>A superior <span class="hlt">solar</span> conjunction occurs when the sun lies near the signal path of a source as <span class="hlt">observed</span> from the Earth. Interplanetary spacecraft sent to the planets typically encounter one or more <span class="hlt">solar</span> conjunctions during their mission lifetimes. During these periods, the signals sent to and from the spacecraft encounter degradation due to the intervening charged particles of the <span class="hlt">solar</span> corona.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1990A%26A...240..506B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1990A%26A...240..506B"><span><span class="hlt">Solar</span> flare microwave <span class="hlt">observations</span> with high spectral resolution</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bruggmann, G.; Magun, A.; Benz, A. O.; Stehling, W.</p> <p>1990-12-01</p> <p>The <span class="hlt">solar</span> flare radio emission in the 6-8 GHz range was <span class="hlt">observed</span> with a high resolution spectrometer. The <span class="hlt">observed</span> band corresponds to the plasma frequencies and gyrofrequencies of the transition region and the lowest part of the corona in active regions. Most of the emissions were found to be broadbanded, as expected from the gyrosynchrotron mechanism. In eight out of 46 <span class="hlt">observed</span> events, spectral structures of three types were detected: spikes below the time resolution of 100 ms, slowly drifting broadband structures, and a narrow bandwidth patch of continuum emission. These first narrowband bursts spectrally recorded in the 6-8 GHz range are generally weak. Slowly drifting structures are the only type compatible with the gyrosynchrotron emission mechanism. A simple argument based on free-free absorption shows that plasma emission can only be propagated if the radiation originates in a dense region with a small density-scale length. The same holds for maser emission at a low harmonic of the electron gyrofrequency. Possible emission mechanisms and diagnostic capabilities are discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22370548-exploring-prominence-corona-connection-its-expansion-outer-corona-using-total-solar-eclipse-observations','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22370548-exploring-prominence-corona-connection-its-expansion-outer-corona-using-total-solar-eclipse-observations"><span>Exploring the prominence-corona connection and its expansion into the outer corona using total <span class="hlt">solar</span> eclipse <span class="hlt">observations</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>Habbal, Shadia Rifai; Morgan, Huw; Druckmüller, Miloslav, E-mail: shadia@ifa.hawaii.edu</p> <p></p> <p>Prominences constitute the most complex magnetic structures in the <span class="hlt">solar</span> corona. The ubiquitous presence of their seemingly confined dense and cool plasma in an otherwise million-degree environment remains a puzzle. Using a decade of white light total <span class="hlt">solar</span> eclipse <span class="hlt">observations</span>, we show how these images reveal an intricate relationship between prominences and coronal structures both in their immediate vicinity, known as coronal cavities, and in the extended corona out to several <span class="hlt">solar</span> radii. <span class="hlt">Observations</span> of suspended prominences and twisted helical structures spanning several <span class="hlt">solar</span> radii are central to these findings. The different manifestations of the prominence-corona interface that emerge frommore » this study underscore the fundamental role played by prominences in defining and controlling the complex expansion and dynamic behavior of the <span class="hlt">solar</span> magnetic field in the neighborhood of magnetic polarity reversal regions. This study suggests that the unraveling of prominences and the outward expansion of the helical twisted field lines linked to them could be the <span class="hlt">solar</span> origin of twisted magnetic flux ropes detected in interplanetary space, and of the mechanism by which the Sun sheds its magnetic helicity. This work also underscores the likely role of the prominence-corona interface as a source of the slow <span class="hlt">solar</span> wind.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMED11B0896R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMED11B0896R"><span>Demonstrations to Teach Electricity and Safely <span class="hlt">Observe</span> a <span class="hlt">Solar</span> Eclipse</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Reiff, P. H.</p> <p>2016-12-01</p> <p>Electricity and magnetism are often difficult to understand because they are invisible. We will demonstrate various ways to visualize electric fields. We will play music on a plasma discharge from a Tesla coil, create static charge on balloons with hair, and store charge using a Leyden jar. We will also show safe ways to <span class="hlt">observe</span> a <span class="hlt">solar</span> eclipse, which is critical for the upcoming August 21, 2017 eclipse.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017Ge%26Ae..57..798A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017Ge%26Ae..57..798A"><span>Results of Spectral Corona <span class="hlt">Observations</span> in <span class="hlt">Solar</span> Activity Cycles 17-24</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Aliev, A. Kh.; Guseva, S. A.; Tlatov, A. G.</p> <p>2017-12-01</p> <p>The results of the work of the global <span class="hlt">observation</span> network are considered, and a comparative analysis of the data of various coronal observatories is performed. The coronal activity index has been reconstructed for the period 1939-2016 based on the data of various observatories in Kislovodsk system. For this purpose, the corona daily intensity maps from the Sacramento Peak and Lomnický Štít observatories according to the <span class="hlt">Solar</span>-Geophysical Data journal have been digitized; they supplement the data of other observatories. The homogeneity and continuity of the corona <span class="hlt">observations</span> at the Kislovodsk station, including activity cycle 24, is confirmed. Unfortunately, the only observatory at present that continues <span class="hlt">observation</span> of the spectral corona in Fe XIV 5303 Å and Fe XIV 6374 Å lines is the Kislovodsk astronomical station Mountain Astronomical Station (MAS) of the Central Astronomical Observatory, Russian Academy of Sciences (Pulkovo). The data on the combined corona in 5303 Å line are analyzed. It is shown that there is a high correlation of the intensity index of green corona with <span class="hlt">solar</span> radiation measurements in the vacuum UV region. Data on the beginning of the new 25th activity cycle in the corona at high latitudes are presented.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010EGUGA..1214629S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010EGUGA..1214629S"><span>Ground-based <span class="hlt">Observations</span> of Large <span class="hlt">Solar</span> Flares Precursors</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sheyner, Olga; Smirnova, Anna; Snegirev, Sergey</p> <p>2010-05-01</p> <p>The importance problem of <span class="hlt">Solar</span>-terrestrial physics is regular forecasting of <span class="hlt">solar</span> activity phenomena, which negatively influence the human's health, operating safety, communication, radar sets and others. The opportunity of development of short-term forecasting technique of geoeffective <span class="hlt">solar</span> flares is presented in this study. This technique is based on the effect of growth of pulsations of horizontal component of geomagnetic field before the <span class="hlt">solar</span> proton flares. The long-period (30-60 minutes) pulsations of H-component of geomagnetic field are detected for the events of different intensity on March 22, 1991, November 4, 2001, and November 17, 2001 using the method of wavelet-analysis. Amplitudes of fluctuations of horizontal component of geomagnetic field with the 30-60 minute's periods grow at the most of tested stations during 0.5-3.5 days before the <span class="hlt">solar</span> flares. The particularities of spectral component are studied for the stations situated on different latitudes. The assumptions about the reason of such precursors-fluctuations appearance are made.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017ApJ...850..179C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017ApJ...850..179C"><span>The Universality of the Rapid Neutron-<span class="hlt">capture</span> Process Revealed by a Possible Disrupted Dwarf Galaxy Star</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Casey, Andrew R.; Schlaufman, Kevin C.</p> <p>2017-12-01</p> <p>The rapid neutron-<span class="hlt">capture</span> or r-process is thought to produce the majority of the heavy elements (Z> 30) in extremely metal-poor stars. The same process is also responsible for a significant fraction of the heavy elements in the Sun. This universality of the r-process is one of its characteristic features, as well as one of the most important clues to its astrophysical origin. We report the discovery of an extremely metal-poor field giant with [{Sr},{Ba}/{{H}}]≈ -6.0 and [{Sr},{Ba}/{Fe}]≈ -3.0, the lowest abundances of strontium and barium relative to iron ever <span class="hlt">observed</span>. Despite its low abundances, the star 2MASS J151113.24-213003.0 has [{Sr}/{Ba}]=-0.11+/- 0.14, therefore its neutron-<span class="hlt">capture</span> abundances are consistent with the main <span class="hlt">solar</span> r-process pattern that has [{Sr}/{Ba}]=-0.25. It has been suggested that extremely low neutron-<span class="hlt">capture</span> abundances are a characteristic of dwarf galaxies, and we find that this star is on a highly eccentric orbit with an apocenter ≳100 kpc that lies in the disk of satellites in the halo of the Milky Way. We show that other extremely metal-poor stars with low [Sr, Ba/H] and [Sr, Ba/Fe] plus <span class="hlt">solar</span> [Sr/Ba] tend to have orbits with large apocenters, consistent with a dwarf galaxy origin for this class of object. The nucleosynthesis event that produced the neutron-<span class="hlt">capture</span> elements in 2MASS J151113.24-213003.0 must produce both strontium and barium together in the <span class="hlt">solar</span> ratio. We exclude contributions from the s-process in intermediate-mass asymptotic giant branch or fast-rotating massive metal-poor stars, pair-instability supernovae, the weak r-process, and neutron-star mergers. We argue that the event was a Pop III or extreme Pop II core-collapse supernova explosion. This paper includes data gathered with the 6.5 m Magellan Telescopes located at Las Campanas Observatory, Chile.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017Ge%26Ae..57..896P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017Ge%26Ae..57..896P"><span>Cyclotron Line in <span class="hlt">Solar</span> Microwave Radiation by Radio Telescope RATAN-600 <span class="hlt">Observations</span> of the <span class="hlt">Solar</span> Active Region NOAA 12182</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Peterova, N. G.; Topchilo, N. A.</p> <p>2017-12-01</p> <p>This paper presents the results of <span class="hlt">observation</span> of a rare phenomenon—a narrowband increase in the brightness of cyclotron radiation of one of the structural details of a radio source located in the <span class="hlt">solar</span> corona above the <span class="hlt">solar</span> active region NOAA 12182 in October 2014 at a frequency of 4.2 ± 0.1 GHz. The brightness of radiation in the maximum of the phenomenon has reached 10 MK; its duration was equal to 3 s. The exact location of the source of the narrowband cyclotron radiation is indicated: it is a corona above a fragmented (4-nuclear) sunspot, on which a small UV flare loop was closed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20140017392','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20140017392"><span>Atmospheric Mining in the Outer <span class="hlt">Solar</span> System:. [Aerial Vehicle Reconnaissance and Exploration Options</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Palaszewski, Bryan A.</p> <p>2014-01-01</p> <p>Atmospheric mining in the outer <span class="hlt">solar</span> system has been investigated as a means of fuel production for high energy propulsion and power. Fusion fuels such as Helium 3 (3He) and hydrogen can be wrested from the atmospheres of Uranus and Neptune and either returned to Earth or used in-situ for energy production. Helium 3 and hydrogen (deuterium, etc.) were the primary gases of interest with hydrogen being the primary propellant for nuclear thermal solid core and gas core rocket-based atmospheric flight. A series of analyses were undertaken to investigate resource <span class="hlt">capturing</span> aspects of atmospheric mining in the outer <span class="hlt">solar</span> system. This included the gas <span class="hlt">capturing</span> rate, storage options, and different methods of direct use of the <span class="hlt">captured</span> gases. Additional supporting analyses were conducted to illuminate vehicle sizing and orbital transportation issues. While <span class="hlt">capturing</span> 3He, large amounts of hydrogen and 4He are produced. With these two additional gases, the potential for fueling small and large fleets of additional exploration and exploitation vehicles exists. Additional aerospacecraft or other aerial vehicles (UAVs, balloons, rockets, etc.) could fly through the outer planet atmospheres, for global weather <span class="hlt">observations</span>, localized storm or other disturbance investigations, wind speed measurements, polar <span class="hlt">observations</span>, etc. Deep-diving aircraft (built with the strength to withstand many atmospheres of pressure) powered by the excess hydrogen or helium 4 may be designed to probe the higher density regions of the gas giants. Outer planet atmospheric properties, atmospheric storm data, and mission planning for future outer planet UAVs are presented.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19930049596&hterms=background+wind&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3Dbackground%2Bwind','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19930049596&hterms=background+wind&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3Dbackground%2Bwind"><span>Evolution of spatial and temporal correlations in the <span class="hlt">solar</span> wind - <span class="hlt">Observations</span> and interpretation</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Klein, L. W.; Matthaeus, W. H.; Roberts, D. A.; Goldstein, M. L.</p> <p>1992-01-01</p> <p><span class="hlt">Observations</span> of <span class="hlt">solar</span> wind magnetic field spectra from 1-22 AU indicate a distinctive structure in frequency which evolves with increasing heliocentric distance. At 1 AU extremely low frequency correlations are associated with temporal variations at the <span class="hlt">solar</span> period and its first few harmonics. For periods of l2-96 hours, a l/f distribution is <span class="hlt">observed</span>, which we interpret as an aggregate of uncorrelated coronal structures which have not dynamically interacted by 1 AU. At higher frequencies the familiar Kolmogorov-like power law is seen. Farther from the sun the frequency break point between the shallow l/f and the steeper Kolmogorov spectrum evolves systematically towards lower frequencies. We suggest that the Kolmogorov-like spectra emerge due to in situ turbulence that generates spatial correlations associated with the turbulent cascade and that the background l/f noise is a largely temporal phenomenon, not associated with in situ dynamical processes. In this paper we discuss these ideas from the standpoint of <span class="hlt">observations</span> from several interplanetary spacecraft.</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://www.osti.gov/accomplishments/documents/fullText/ACC0196.pdf','DOE-RDACC'); return false;" href="http://www.osti.gov/accomplishments/documents/fullText/ACC0196.pdf"><span>OUT Success Stories: <span class="hlt">Solar</span> Trough Power Plants</span></a></p> <p><a target="_blank" href="http://www.osti.gov/accomplishments/fieldedsearch.html">DOE R&D Accomplishments Database</a></p> <p>Jones, J.</p> <p>2000-08-01</p> <p>The <span class="hlt">Solar</span> Electric Generating System (SEGS) plants use parabolic-trough <span class="hlt">solar</span> collectors to <span class="hlt">capture</span> the sun's energy and convert it to heat. The SEGS plants range in capacity from 13.8 to 80 MW, and they were constructed to meet Southern California Edison Company's periods of peak power demand.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.P13A1901L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.P13A1901L"><span><span class="hlt">Solar</span> Wind Interaction and Crustal Field Influences on Mars' Upper Ionosphere: MAVEN <span class="hlt">Observations</span> Compared to Model Results</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Luhmann, J. G.; Alvarez, K.; Curry, S.; Dong, C.; Ma, Y.; Bougher, S. W.; Benna, M.; Elrod, M. K.; Mahaffy, P. R.; Withers, P.; Girazian, Z.; Connerney, J. E. P.; Brain, D.; Jakosky, B. M.</p> <p>2016-12-01</p> <p>Since the two Viking Landers, progress on improving our global knowledge of the Martian ionosphere's characteristics has been limited by the available instrumentation and sampling geometries. In particular, while remote sensing and the lower energy plasma spectrometer <span class="hlt">observations</span> on missions including MGS and MEX provided insights on the effects of the crustal magnetic fields of Mars and the <span class="hlt">solar</span> wind interaction, these measurements did not allow the broader thermal ion surveys necessary to test our current understanding of the region between the exobase at 200 km altitude and the <span class="hlt">solar</span> wind interaction boundary. In this study we use the MAVEN NGIMS thermal ion mass spectrometer <span class="hlt">observations</span> from the prime mission year 2015 to construct some statistical pictures of the increasingly collisionless region of the ionosphere between 200 and 500 km where crustal field and <span class="hlt">solar</span> wind interaction effects should begin to dominate its behavior. Comparisons with models of the <span class="hlt">solar</span> wind interaction with Mars provide important global context for these <span class="hlt">observations</span>, including the roles of system diversity associated with changing crustal field and interplanetary field orientations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22679727-compressed-sensing-based-image-reconstruction-algorithm-solar-flare-ray-observations','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22679727-compressed-sensing-based-image-reconstruction-algorithm-solar-flare-ray-observations"><span>A Compressed Sensing-based Image Reconstruction Algorithm for <span class="hlt">Solar</span> Flare X-Ray <span class="hlt">Observations</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>Felix, Simon; Bolzern, Roman; Battaglia, Marina, E-mail: simon.felix@fhnw.ch, E-mail: roman.bolzern@fhnw.ch, E-mail: marina.battaglia@fhnw.ch</p> <p></p> <p>One way of imaging X-ray emission from <span class="hlt">solar</span> flares is to measure Fourier components of the spatial X-ray source distribution. We present a new compressed sensing-based algorithm named VIS-CS, which reconstructs the spatial distribution from such Fourier components. We demonstrate the application of the algorithm on synthetic and <span class="hlt">observed</span> <span class="hlt">solar</span> flare X-ray data from the Reuven Ramaty High Energy <span class="hlt">Solar</span> Spectroscopic Imager satellite and compare its performance with existing algorithms. VIS-CS produces competitive results with accurate photometry and morphology, without requiring any algorithm- and X-ray-source-specific parameter tuning. Its robustness and performance make this algorithm ideally suited for the generation ofmore » quicklook images or large image cubes without user intervention, such as for imaging spectroscopy analysis.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22661245-solar-energetic-particle-event-august-connectivity-solar-source-inferred-from-multiple-spacecraft-observations-modeling','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22661245-solar-energetic-particle-event-august-connectivity-solar-source-inferred-from-multiple-spacecraft-observations-modeling"><span>The <span class="hlt">Solar</span> Energetic Particle Event of 2010 August 14: Connectivity with the <span class="hlt">Solar</span> Source Inferred from Multiple Spacecraft <span class="hlt">Observations</span> and Modeling</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>Lario, D.; Kwon, R.-Y.; Raouafi, N. E.</p> <p></p> <p>We analyze one of the first <span class="hlt">solar</span> energetic particle (SEP) events of <span class="hlt">solar</span> cycle 24 <span class="hlt">observed</span> at widely separated spacecraft in order to assess the reliability of models currently used to determine the connectivity between the sources of SEPs at the Sun and spacecraft in the inner heliosphere. This SEP event was <span class="hlt">observed</span> on 2010 August 14 by near-Earth spacecraft, STEREO-A (∼80° west of Earth) and STEREO-B (∼72° east of Earth). In contrast to near-Earth spacecraft, the footpoints of the nominal magnetic field lines connecting STEREO-A and STEREO-B with the Sun were separated from the region where the parent fastmore » halo coronal mass ejection (CME) originated by ∼88° and ∼47° in longitude, respectively. We discuss the properties of the phenomena associated with this <span class="hlt">solar</span> eruption. Extreme ultraviolet and white-light images are used to specify the extent of the associated CME-driven coronal shock. We then assess whether the SEPs <span class="hlt">observed</span> at the three heliospheric locations were accelerated by this shock or whether transport mechanisms in the corona and/or interplanetary space provide an alternative explanation for the arrival of particles at the poorly connected spacecraft. A possible scenario consistent with the <span class="hlt">observations</span> indicates that the <span class="hlt">observation</span> of SEPs at STEREO-B and near Earth resulted from particle injection by the CME shock onto the field lines connecting to these spacecraft, whereas SEPs reached STEREO-A mostly via cross-field diffusive transport processes. The successes, limitations, and uncertainties of the methods used to resolve the connection between the acceleration sites of SEPs and the spacecraft are evaluated.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMSH51D2606P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMSH51D2606P"><span>Kinetic Features <span class="hlt">Observed</span> in the <span class="hlt">Solar</span> Wind Electron Distributions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pierrard, V.; Lazar, M.; Poedts, S.</p> <p>2016-12-01</p> <p>More than 120 000 of velocity distributions measured by Helios, Cluster and Ulysses in the ecliptic have been analyzed within an extended range of heliocentric distances from 0.3 to over 4 AU. The velocity distribution of electrons reveal a dual structure with a thermal (Maxwellian) core and a suprathermal (Kappa) halo. A detailed <span class="hlt">observational</span> analysis of these two components provides estimations of their temperatures and temperature anisotropies, and we decode any potential interdependence that their properties may indicate. The core temperature is found to decrease with the radial distance, while the halo temperature slightly increases, clarifying an apparent contradiction in previous <span class="hlt">observational</span> analysis and providing valuable clues about the temperature of the Kappa-distributed populations. For low values of the power-index kappa, these two components manifest a clear tendency to deviate from isotropy in the same direction, that seems to confirm the existence of mechanisms with similar effects on both components, e.g., the <span class="hlt">solar</span> wind expansion, or the particle heating by the fluctuations. However, the existence of plasma states with anti-correlated anisotropies of the core and halo populations and the increase of their number for high values of the power-index kappa suggest a dynamic interplay of these components, mediated most probably by the anisotropy-driven instabilities. Estimating the temperature of the <span class="hlt">solar</span> wind particles and their anisotropies is particularly important for understanding the origin of these deviations from thermal equilibrium as well as their effects.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://images.nasa.gov/#/details-iss036e047951.html','SCIGOVIMAGE-NASA'); return false;" href="https://images.nasa.gov/#/details-iss036e047951.html"><span><span class="hlt">Solar</span> Array and Earth <span class="hlt">Observation</span></span></a></p> <p><a target="_blank" href="https://images.nasa.gov/">NASA Image and Video Library</a></p> <p></p> <p>2013-09-07</p> <p>ISS036-E-047951 (7 Sept. 2013) --- Backdropped by a blue and white part of Earth and the blackness of space, International Space Station <span class="hlt">solar</span> array panels are featured in this image photographed by an Expedition 36 crew member aboard the station.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008ICRC....1...19W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008ICRC....1...19W"><span>The High Energy Photons Emission from <span class="hlt">Solar</span> Flares <span class="hlt">Observed</span> by SZ2-XD</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wang, Huanyu; Li, Xinqiao; Ma, Yuqian; Zhang, Chengmo; Xu, Yupeng; Wang, Jingzhou; Chen, Guoming</p> <p></p> <p>The spectra and light curve of near a hundred <span class="hlt">Solar</span> X-ray Flare events, which were <span class="hlt">observed</span> by SZ2/XD in the energy band of 10-800 keV during 2001, have been investigated. The events covered from C to X-class flares, which are shown different characters of high energy photons emission. The results will be presented in this paper. The discussions will be made especially for 3 of the brightest X-class <span class="hlt">solar</span> flares SF010402(X20),SF010406(X5.6) and SF010415 (X14.4, a GLE event).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19940024950','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19940024950"><span>Correlative analysis of hard and soft x ray <span class="hlt">observations</span> of <span class="hlt">solar</span> flares</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Zarro, Dominic M.</p> <p>1994-01-01</p> <p>We have developed a promising new technique for jointly analyzing BATSE hard X-ray <span class="hlt">observations</span> of <span class="hlt">solar</span> flares with simultaneous soft X-ray <span class="hlt">observations</span>. The technique is based upon a model in which electric currents and associated electric fields are responsible for the respective heating and particle acceleration that occur in <span class="hlt">solar</span> flares. A useful by-product of this technique is the strength and evolution of the coronal electric field. The latter permits one to derive important flare parameters such as the current density, the number of current filaments composing the loop, and ultimately the hard X-ray spectrum produced by the runaway electrons. We are continuing to explore the technique by applying it to additional flares for which we have joint BATSE/Yohkoh <span class="hlt">observations</span>. A central assumption of our analysis is the constant of proportionality alpha relating the hard X-ray flux above 50 keV and the rate of electron acceleration. For a thick-target model of hard X-ray production, it can be shown that cv is in fact related to the spectral index and low-energy cutoff of precipitating electrons. The next step in our analysis is to place <span class="hlt">observational</span> constraints on the latter parameters using the joint BATSE/Yohkoh data.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19980201314','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19980201314"><span>Seismic Study of the Subsurface Structure and Dynamics of the <span class="hlt">Solar</span> Interior from High Spatial Resolution <span class="hlt">Observations</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Korzennik, Sylvain G.</p> <p>1997-01-01</p> <p>We have carried out the data reduction and analysis of Mt. Wilson 60' <span class="hlt">solar</span> tower high spatial resolution <span class="hlt">observations</span>. The reduction of the 100-day-long summer of 1990 <span class="hlt">observation</span> campaign in terms of rotational splittings was completed leading to an excess of 600,000 splittings. The analysis of these splittings lead to a new inference of the <span class="hlt">solar</span> internal rotation rate as a function of depth and latitude.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22520075-activity-analyses-solar-type-stars-observed-kepler-proxies-magnetic-activity','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22520075-activity-analyses-solar-type-stars-observed-kepler-proxies-magnetic-activity"><span>ACTIVITY ANALYSES FOR <span class="hlt">SOLAR</span>-TYPE STARS <span class="hlt">OBSERVED</span> WITH KEPLER. I. PROXIES OF MAGNETIC ACTIVITY</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>He, Han; Wang, Huaning; Yun, Duo, E-mail: hehan@nao.cas.cn</p> <p>2015-11-15</p> <p>Light curves of <span class="hlt">solar</span>-type stars often show gradual fluctuations due to rotational modulation by magnetic features (starspots and faculae) on stellar surfaces. Two quantitative measures of modulated light curves are employed as the proxies of magnetic activity for <span class="hlt">solar</span>-type stars <span class="hlt">observed</span> with Kepler telescope. The first is named autocorrelation index i{sub AC}, which describes the degree of periodicity of the light curve; the second is the effective fluctuation range of the light curve R{sub eff}, which reflects the depth of rotational modulation. The two measures are complementary and depict different aspects of magnetic activities on <span class="hlt">solar</span>-type stars. By using themore » two proxies i{sub AC} and R{sub eff}, we analyzed activity properties of two carefully selected <span class="hlt">solar</span>-type stars <span class="hlt">observed</span> with Kepler (Kepler ID: 9766237 and 10864581), which have distinct rotational periods (14.7 versus 6.0 days). We also applied the two measures to the Sun for a comparative study. The result shows that both the measures can reveal cyclic activity variations (referred to as i{sub AC}-cycle and R{sub eff}-cycle) on the two Kepler stars and the Sun. For the Kepler star with the faster rotation rate, i{sub AC}-cycle and R{sub eff}-cycle are in the same phase, while for the Sun (slower rotator), they are in the opposite phase. By comparing the <span class="hlt">solar</span> light curve with simultaneous photospheric magnetograms, it is identified that the magnetic feature that causes the periodic light curve during <span class="hlt">solar</span> minima is the faculae of the enhanced network region, which can also be a candidate of magnetic features that dominate the periodic light curves on the two Kepler stars.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://images.nasa.gov/#/details-GSFC_20171208_Archive_e001079.html','SCIGOVIMAGE-NASA'); return false;" href="https://images.nasa.gov/#/details-GSFC_20171208_Archive_e001079.html"><span>A First for NASA's IRIS: <span class="hlt">Observing</span> a Gigantic Eruption of <span class="hlt">Solar</span> Material</span></a></p> <p><a target="_blank" href="https://images.nasa.gov/">NASA Image and Video Library</a></p> <p></p> <p>2014-05-30</p> <p>Watch a video from this event here: www.flickr.com/photos/gsfc/14118958800/ A coronal mass ejection, or CME, surged off the side of the sun on May 9, 2014, and NASA's newest <span class="hlt">solar</span> observatory caught it in extraordinary detail. This was the first CME <span class="hlt">observed</span> by the Interface Region Imaging Spectrograph, or IRIS, which launched in June 2013 to peer into the lowest levels of the sun's atmosphere with better resolution than ever before. Watch the movie to see how a curtain of <span class="hlt">solar</span> material erupts outward at speeds of 1.5 million miles per hour. Read more: 1.usa.gov/1kp7O4F NASA image use policy. NASA Goddard Space Flight Center enables NASA’s mission through four scientific endeavors: Earth Science, Heliophysics, <span class="hlt">Solar</span> System Exploration, and Astrophysics. Goddard plays a leading role in NASA’s accomplishments by contributing compelling scientific knowledge to advance the Agency’s mission. Follow us on Twitter Like us on Facebook Find us on Instagram</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27194964','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27194964"><span><span class="hlt">Solar</span> Adaptive Optics.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Rimmele, Thomas R; Marino, Jose</p> <p></p> <p>Adaptive optics (AO) has become an indispensable tool at ground-based <span class="hlt">solar</span> telescopes. AO enables the ground-based <span class="hlt">observer</span> to overcome the adverse effects of atmospheric seeing and obtain diffraction limited <span class="hlt">observations</span>. Over the last decade adaptive optics systems have been deployed at major ground-based <span class="hlt">solar</span> telescopes and revitalized ground-based <span class="hlt">solar</span> astronomy. The relatively small aperture of <span class="hlt">solar</span> telescopes and the bright source make <span class="hlt">solar</span> AO possible for visible wavelengths where the majority of <span class="hlt">solar</span> <span class="hlt">observations</span> are still performed. <span class="hlt">Solar</span> AO systems enable diffraction limited <span class="hlt">observations</span> of the Sun for a significant fraction of the available <span class="hlt">observing</span> time at ground-based <span class="hlt">solar</span> telescopes, which often have a larger aperture than equivalent space based observatories, such as HINODE. New ground breaking scientific results have been achieved with <span class="hlt">solar</span> adaptive optics and this trend continues. New large aperture telescopes are currently being deployed or are under construction. With the aid of <span class="hlt">solar</span> AO these telescopes will obtain <span class="hlt">observations</span> of the highly structured and dynamic <span class="hlt">solar</span> atmosphere with unprecedented resolution. This paper reviews <span class="hlt">solar</span> adaptive optics techniques and summarizes the recent progress in the field of <span class="hlt">solar</span> adaptive optics. An outlook to future <span class="hlt">solar</span> AO developments, including a discussion of Multi-Conjugate AO (MCAO) and Ground-Layer AO (GLAO) will be given. Supplementary material is available for this article at 10.12942/lrsp-2011-2.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19920036827&hterms=SMM&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3DSMM','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19920036827&hterms=SMM&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3DSMM"><span>Activity associated with coronal mass ejections at <span class="hlt">solar</span> minimum - SMM <span class="hlt">observations</span> from 1984-1986</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>St. Cyr, O. C.; Webb, D. F.</p> <p>1991-01-01</p> <p>Seventy-three coronal mass ejections (CMEs) <span class="hlt">observed</span> by the coronagraph aboard SMM between 1984 and 1986 were examined in order to determine the distribution of various forms of <span class="hlt">solar</span> activity that were spatially and temporally associated with mass ejections during <span class="hlt">solar</span> minimum phase. For each coronal mass ejection a speed was measured, and the departure time of the transient from the lower corona estimated. Other forms of <span class="hlt">solar</span> activity that appeared within 45 deg longitude and 30 deg latitude of the mass ejection and within +/-90 min of its extrapolated departure time were explored. The statistical results of the analysis of these 73 CMEs are presented, and it is found that slightly less than half of them were infrequently associated with other forms of <span class="hlt">solar</span> activity. It is suggested that the distribution of the various forms of activity related to CMEs does not change at different phases of the <span class="hlt">solar</span> cycle. For those CMEs with associations, it is found that eruptive prominences and soft X-rays were the most likely forms of activity to accompany the appearance of mass ejections.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19870052734&hterms=SMM&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3DSMM','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19870052734&hterms=SMM&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3DSMM"><span>Evidence for explosive chromospheric evaporation in a <span class="hlt">solar</span> flare <span class="hlt">observed</span> with SMM</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Zarro, D. M.; Saba, J. L. R.; Strong, K. T.; Canfield, R. C.; Metcalf, T.</p> <p>1986-01-01</p> <p>SMM soft X-ray data and Sacramento Peak Observatory H-alpha <span class="hlt">observations</span> are combined in a study of the impulsive phase of a <span class="hlt">solar</span> flare. A blue asymmetry, indicative of upflow motions, was <span class="hlt">observed</span> in the coronal Ca XIX line during the soft X-ray rise phase. H-alpha redshifts, indicative of downward motions, were <span class="hlt">observed</span> simultaneously in bright flare kernels during the period of hard X-ray emission. It is shown that, to within <span class="hlt">observational</span> errors, the impulsive phase momentum transported by the upflowing soft X-ray plasma is equivalent to that of the downward moving chromospheric material.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26854530','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26854530"><span>The problem of latent attentional <span class="hlt">capture</span>: Easy visual search conceals <span class="hlt">capture</span> by task-irrelevant abrupt onsets.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Gaspelin, Nicholas; Ruthruff, Eric; Lien, Mei-Ching</p> <p>2016-08-01</p> <p>Researchers are sharply divided regarding whether irrelevant abrupt onsets <span class="hlt">capture</span> spatial attention. Numerous studies report that they do and a roughly equal number report that they do not. This puzzle has inspired numerous attempts at reconciliation, none gaining general acceptance. The authors propose that abrupt onsets routinely <span class="hlt">capture</span> attention, but the size of <span class="hlt">observed</span> <span class="hlt">capture</span> effects depends critically on how long attention dwells on distractor items which, in turn, depends critically on search difficulty. In a series of spatial cuing experiments, the authors show that irrelevant abrupt onsets produce robust <span class="hlt">capture</span> effects when visual search is difficult, but not when search is easy. Critically, this effect occurs even when search difficulty varies randomly across trials, preventing any strategic adjustments of the attentional set that could modulate probability of <span class="hlt">capture</span> by the onset cue. The authors argue that easy visual search provides an insensitive test for stimulus-driven <span class="hlt">capture</span> by abrupt onsets: even though onsets truly <span class="hlt">capture</span> attention, the effects of <span class="hlt">capture</span> can be latent. This <span class="hlt">observation</span> helps to explain previous failures to find <span class="hlt">capture</span> by onsets, nearly all of which used an easy visual search. (PsycINFO Database Record (c) 2016 APA, all rights reserved).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4977216','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4977216"><span>The Problem of Latent Attentional <span class="hlt">Capture</span>: Easy Visual Search Conceals <span class="hlt">Capture</span> by Task-Irrelevant Abrupt Onsets</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Gaspelin, Nicholas; Ruthruff, Eric; Lien, Mei-Ching</p> <p>2016-01-01</p> <p>Researchers are sharply divided regarding whether irrelevant abrupt onsets <span class="hlt">capture</span> spatial attention. Numerous studies report that they do and a roughly equal number report that they do not. This puzzle has inspired numerous attempts at reconciliation, none gaining general acceptance. We propose that abrupt onsets routinely <span class="hlt">capture</span> attention, but the size of <span class="hlt">observed</span> <span class="hlt">capture</span> effects depends critically on how long attention dwells on distractor items which, in turn, depends critically on search difficulty. In a series of spatial cuing experiments, we show that irrelevant abrupt onsets produce robust <span class="hlt">capture</span> effects when visual search is difficult, but not when search is easy. Critically, this effect occurs even when search difficulty varies randomly across trials, preventing any strategic adjustments of the attentional set that could modulate probability of <span class="hlt">capture</span> by the onset cue. We argue that easy visual search provides an insensitive test for stimulus-driven <span class="hlt">capture</span> by abrupt onsets: even though onsets truly <span class="hlt">capture</span> attention, the effects of <span class="hlt">capture</span> can be latent. This <span class="hlt">observation</span> helps to explain previous failures to find <span class="hlt">capture</span> by onsets, nearly all of which employed an easy visual search. PMID:26854530</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20140011683','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20140011683"><span>The Substructure of the <span class="hlt">Solar</span> Corona <span class="hlt">Observed</span> in the Hi-C Telescope</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Winebarger, A.; Cirtain, J.; Golub, L.; DeLuca, E.; Savage, S.; Alexander, C.; Schuler, T.</p> <p>2014-01-01</p> <p>In the summer of 2012, the High-resolution Coronal Imager (Hi-C) flew aboard a NASA sounding rocket and collected the highest spatial resolution images ever obtained of the <span class="hlt">solar</span> corona. One of the goals of the Hi-C flight was to characterize the substructure of the <span class="hlt">solar</span> corona. We therefore calculate how the intensity scales from a low-resolution (AIA) pixels to high-resolution (Hi-C) pixels for both the dynamic events and "background" emission (meaning, the steady emission over the 5 minutes of data acquisition time). We find there is no evidence of substructure in the background corona; the intensity scales smoothly from low-resolution to high-resolution Hi-C pixels. In transient events, however, the intensity <span class="hlt">observed</span> with Hi-C is, on average, 2.6 times larger than <span class="hlt">observed</span> with AIA. This increase in intensity suggests that AIA is not resolving these events. This result suggests a finely structured dynamic corona embedded in a smoothly varying background.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018SoPh..293...34S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018SoPh..293...34S"><span>Probing Twisted Magnetic Field Using Microwave <span class="hlt">Observations</span> in an M Class <span class="hlt">Solar</span> Flare on 11 February, 2014</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sharykin, I. N.; Kuznetsov, A. A.; Myshyakov, I. I.</p> <p>2018-02-01</p> <p>This work demonstrates the possibility of magnetic-field topology investigations using microwave polarimetric <span class="hlt">observations</span>. We study a <span class="hlt">solar</span> flare of GOES M1.7 class that occurred on 11 February, 2014. This flare revealed a clear signature of spatial inversion of the radio-emission polarization sign. We show that the <span class="hlt">observed</span> polarization pattern can be explained by nonthermal gyrosynchrotron emission from the twisted magnetic structure. Using <span class="hlt">observations</span> of the Reuven Ramaty High Energy <span class="hlt">Solar</span> Spectroscopic Imager, Nobeyama Radio Observatory, Radio <span class="hlt">Solar</span> Telescope Network, and <span class="hlt">Solar</span> Dynamics Observatory, we have determined the parameters of nonthermal electrons and thermal plasma and identified the magnetic structure where the flare energy release occurred. To reconstruct the coronal magnetic field, we use nonlinear force-free field (NLFFF) and potential magnetic-field approaches. Radio emission of nonthermal electrons is simulated by the GX Simulator code using the extrapolated magnetic field and the parameters of nonthermal electrons and thermal plasma inferred from the <span class="hlt">observations</span>; the model radio maps and spectra are compared with <span class="hlt">observations</span>. We have found that the potential-magnetic-field approach fails to explain the <span class="hlt">observed</span> circular polarization pattern; on the other hand, the Stokes-V map is successfully explained by assuming nonthermal electrons to be distributed along the twisted magnetic structure determined by the NLFFF extrapolation approach. Thus, we show that the radio-polarization maps can be used for diagnosing the topology of the flare magnetic structures where nonthermal electrons are injected.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMSH11B2437J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMSH11B2437J"><span>Digging into the corona: A modeling framework trained with Sun-grazing comet <span class="hlt">observations</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jia, Y. D.; Pesnell, W. D.; Bryans, P.; Downs, C.; Liu, W.; Schwartz, S. J.</p> <p>2017-12-01</p> <p>Images of comets diving into the low corona have been <span class="hlt">captured</span> a few times in the past decade. Structures visible at various wavelengths during these encounters indicate a strong variation of the ambient conditions of the corona. We combine three numerical models: a global coronal model, a particle transportation model, and a cometary plasma interaction model into one framework to model the interaction of such Sun-grazing comets with plasma in the low corona. In our framework, cometary vapors are ionized via multiple channels and then <span class="hlt">captured</span> by the coronal magnetic field. In seconds, these ions are further ionized into their highest charge state, which is revealed by certain coronal emission lines. Constrained by <span class="hlt">observations</span>, we apply our framework to trace back to the local conditions of the ambient corona, and their spatial/time variation over a broad range of scales. Once trained by multiple stages of the comet's journey in the low corona, we illustrate how this framework can leverage these unique <span class="hlt">observations</span> to probe the structure of the <span class="hlt">solar</span> corona and <span class="hlt">solar</span> wind.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018GeoRL..45.2574D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018GeoRL..45.2574D"><span><span class="hlt">Solar</span> Wind Deflection by Mass Loading in the Martian Magnetosheath Based on MAVEN <span class="hlt">Observations</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Dubinin, E.; Fraenz, M.; Pätzold, M.; Halekas, J. S.; Mcfadden, J.; Connerney, J. E. P.; Jakosky, B. M.; Vaisberg, O.; Zelenyi, L.</p> <p>2018-03-01</p> <p>Mars Atmosphere and Volatile EvolutioN <span class="hlt">observations</span> at Mars show clear signatures of the shocked <span class="hlt">solar</span> wind interaction with the extended oxygen atmosphere and hot corona displayed in a lateral deflection of the magnetosheath flow in the direction opposite to the direction of the <span class="hlt">solar</span> wind motional electric field. The value of the velocity deflection reaches ˜50 km/s. The occurrence of such deflection is caused by the "Lorentz-type" force due to a differential streaming of the <span class="hlt">solar</span> wind protons and oxygen ions originating from the extended oxygen corona. The value of the total deceleration of the magnetosheath flow due to mass loading is estimated as ˜40 km/s.</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/2016AGUFMAE23B0428B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMAE23B0428B"><span>Effects of Energetic <span class="hlt">Solar</span> Emissions on the Lower Ionosphere as seen in Ionosonde <span class="hlt">Observations</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Barta, V.; Satori, G.; Williams, E.</p> <p>2016-12-01</p> <p>The sudden increase of X-radiation and EUV emission following <span class="hlt">solar</span> flares causes extra ionization in the sunlit hemisphere in the D- and E-regions of the Earth's ionosphere. In addition, <span class="hlt">solar</span> flares are also accompanied by energetic particles (protons and electrons) with energies from tens of keV to hundreds of MeV result additional ionization. The impact of two exceptional <span class="hlt">solar</span> events - the Bastille Day event (July 14, 2000) and the Halloween event (Oct/Nov2003) on the lowest region of the ionosphere (<100 km) have recently been analyzed with global Schumann resonance measurements (Sátori et al., 2015). The present study is aimed at somewhat higher levels of the ionosphere (90-150 km) accessible with ionosonde <span class="hlt">observations</span>. The variation of two ionospheric parameters, namely the minimum frequency of echoes (fmin) and the critical frequency of the E-layer (foE) were studied to disclose the effect of the <span class="hlt">solar</span> flares on the lower ionosphere. The time series of the fmin and foE parameters recorded at meridionally-distributed stations in Europe were analyzed during these two intense <span class="hlt">solar</span> events. Extreme increases of the fmin values (2-6 MHz) were <span class="hlt">observed</span> at several European stations (Juliusruh, 53.6°N, 13.4°E; Chilton, 51.5°N, 359.4°E; Rome, 41.9°N, 12.5°E; SanVito 40.6°N, 17.8°E) during the Halloween event. This ionosonde response increases with increasing latitude. Simultaneously the absence of the foE parameter was <span class="hlt">observed</span>. The sharply increased values (2-4 MHz) of the fmin parameters and the co-occurring absence of the foE parameters were detected in the case of the Bastille Day event as well, but only at high latitude stations (Loparskaya, 68°N, 33°E; St. Petersburg, 59.9°N, 30.3°E; Juliusruh, 53.6°N, 13.4°E). These results suggest that the latitude-dependent change of the fmin and foE parameters is related to energetic <span class="hlt">solar</span> particles penetrating to the lower ionosphere.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25469229','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25469229"><span><span class="hlt">Observations</span> on spiny dogfish ( Squalus acanthias) <span class="hlt">captured</span> in late spring in a North Carolina estuary.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Bangley, Charles; Rulifson, Roger</p> <p>2014-01-01</p> <p>Five spiny dogfish were <span class="hlt">captured</span> in early-mid May during gillnet and longline sampling targeting juvenile coastal sharks in inshore North Carolina waters.  Dogfish <span class="hlt">captures</span> were made within Back Sound and Core Sound, North Carolina. All dogfish were females measuring 849-905 mm total length, well over the size at 50% maturity. Dogfish were caught at stations 1.8-2.7 m in depth, with temperatures 22.9-24.2 °C, 32.8-33.4 ppt salinity, and 6.9-8.0 mg/L dissolved oxygen. These <span class="hlt">observations</span> are among the latest in the spring for spiny dogfish in the southeastern U.S. and occurred at higher temperatures than previously recorded for this species.  It is unclear whether late-occurring spiny dogfish in this area represent a cryptic late-migrating or resident segment of the Northwest Atlantic population.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4240240','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4240240"><span><span class="hlt">Observations</span> on spiny dogfish ( Squalus acanthias) <span class="hlt">captured</span> in late spring in a North Carolina estuary</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Bangley, Charles; Rulifson, Roger</p> <p>2014-01-01</p> <p>Five spiny dogfish were <span class="hlt">captured</span> in early-mid May during gillnet and longline sampling targeting juvenile coastal sharks in inshore North Carolina waters.  Dogfish <span class="hlt">captures</span> were made within Back Sound and Core Sound, North Carolina. All dogfish were females measuring 849-905 mm total length, well over the size at 50% maturity. Dogfish were caught at stations 1.8-2.7 m in depth, with temperatures 22.9-24.2 °C, 32.8-33.4 ppt salinity, and 6.9-8.0 mg/L dissolved oxygen. These <span class="hlt">observations</span> are among the latest in the spring for spiny dogfish in the southeastern U.S. and occurred at higher temperatures than previously recorded for this species.  It is unclear whether late-occurring spiny dogfish in this area represent a cryptic late-migrating or resident segment of the Northwest Atlantic population. PMID:25469229</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AAS...22915804C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AAS...22915804C"><span>Changes in Latitude, Changes in Attitude: U.S. Naval Observatory <span class="hlt">Observations</span> of <span class="hlt">Solar</span> Eclipses 1869 to the Present</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chizek Frouard, Malynda R.; Towne, Linda; Kaplan, George H.</p> <p>2017-01-01</p> <p>In anticipation of the 2017 August 21 total <span class="hlt">solar</span> eclipse over the continental United States, the history of U.S. Naval Observatory eclipse <span class="hlt">observations</span> illustrates the changes in science, technology, and policy over the past 148 years.USNO eclipse <span class="hlt">observations</span> began in 1869, when staff traveled to Des Moines, Iowa and the Bering Strait to look for intra-mercurial planets and to <span class="hlt">observe</span> the <span class="hlt">solar</span> corona. During the golden age of eclipse expeditions, the USNO officially participated in a dozen expeditions between 1869 and 1929. Seven of these expeditions were to US locations: 1869 in Iowa; 1878 in Colorado, Wyoming, and Texas; 1880 in California; 1900 in Georgia and North Carolina; 1918 in Oregon; 1923 in California; and 1925 in New York. A total <span class="hlt">solar</span> eclipse has not traced a path across the width of the continental US since 1918 although several eclipses have passed over parts of the US since then.A few official expeditions occurred later in the 20th century to measure the <span class="hlt">solar</span> diameter, including a total eclipse in the northwest US in 1979 and an annular eclipse across the southeast in 1984. However, <span class="hlt">observations</span> began transitioning to mostly personal adventures as individual astronomers arranged unofficial trips.Historians can use the USNO Multi-year Interactive Computer Almanac (MICA) to compute local circumstances for <span class="hlt">solar</span> eclipses world-wide starting with the annual eclipse of 1800 April 24, which was visible from Alaska. Those looking to make history in 2017 may consult the USNO 2017 August 21 <span class="hlt">Solar</span> Eclipse Resource page (http://aa.usno.navy.mil/data/docs/Eclipse2017.php).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMSH13B2478G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMSH13B2478G"><span>Measuring <span class="hlt">Solar</span> Coronal Magnetism during the Total <span class="hlt">Solar</span> Eclipse of 2017</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gibson, K. L.; Tomczyk, S.</p> <p>2017-12-01</p> <p>The total <span class="hlt">solar</span> eclipse on August 21, 2017 provided a notable opportunity to measure the <span class="hlt">solar</span> corona at specific emission wavelengths to gain information about coronal magnetic fields. <span class="hlt">Solar</span> magnetic fields are intimately related to the generation of space weather and its effects on the earth, and the infrared imaging and polarization information collected on coronal emission lines here will enhance the scientific value of several other ongoing experiments, as well as benefit the astrophysics and upper atmosphere communities. Coronal measurements were collected during the 2 minute and 24 second totality period from Casper Mountain, WY. Computer-controlled telescopes automatically inserted four different narrow band pass filters to <span class="hlt">capture</span> images in the visible range on a 4D PolCam, and in the infrared range on the FLIR 8501c camera. Each band pass filter selects a specific wavelength range that corresponds to a known coronal emission line possessing magnetic sensitivity. The 4D PolCam incorporated a novel grid of linear polarizers precisely aligned with the micron scale pixels. This allowed for direct measurement of the degree of linear polarization in a very small instrument with no external moving parts as is typically required. The FLIR offers short exposure times to freeze motion and output accurate thermal measurements. This allowed a new <span class="hlt">observation</span> of the sun's corona using thermo infrared technology.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19910038931&hterms=SME&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3DSME','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19910038931&hterms=SME&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3DSME"><span>Satellite <span class="hlt">observations</span> of polar mesospheric clouds by the <span class="hlt">solar</span> backscattered ultraviolet spectral radiometer - Evidence of a <span class="hlt">solar</span> cycle dependence</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Thomas, Gary E.; Mcpeters, Richard D.; Jensen, Eric J.</p> <p>1991-01-01</p> <p>Results are presented on eight years of satellite <span class="hlt">observations</span> of the polar mesospheric clouds (PMCs) by the SBUV spectral radiometer, showing that PMCs occur in the summertime polar cap regions of both hemispheres and that they exhibit year-to-year variability. It was also found that the increase in the PMC occurrence frequency was inversely correlated with <span class="hlt">solar</span> activity. Two kinds of hemispherical asymmetries could be identified: (1) PMCs in the Northern Hemisphere were significantly brighter than in the Southern Hemisphere, in accordance with previous results derived from SME data; and (2) the <span class="hlt">solar</span> cycle response in the south is more pronounced than in the north. The paper also describes the cloud detection algorithm.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19780036136&hterms=Exciter&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3DExciter','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19780036136&hterms=Exciter&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3DExciter"><span>Interplanetary baseline <span class="hlt">observations</span> of type III <span class="hlt">solar</span> radio bursts</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Weber, R. R.; Fitzenreiter, R. J.; Novaco, J. C.; Fainberg, J.</p> <p>1977-01-01</p> <p>Simultaneous <span class="hlt">observations</span> of type III radio bursts from spacecraft separated by 0.43 AU have been made using the <span class="hlt">solar</span> orbiters Helios-A and Helios-B. The burst beginning at 19:22 UT on March 28, 1976, has been located from the intersection of the source directions measured at each spacecraft and from burst arrival-time differences. The source positions range from 0.03 AU from the sun at 3000 kHz to 0.08 AU at 585 kHz. The electron density along the burst trajectory and the exciter velocity (0.13c) were determined directly without the need to assume a density model, as has been done with single-spacecraft <span class="hlt">observations</span>. The separation of Helios-A and -B has also provided measurements of burst directivity at low frequencies. For the March 28 burst the intensity <span class="hlt">observed</span> from near the source longitude (Helios-B) was 3-10dB greater than that from 60 deg west of the source (Helios-A)</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016usc..confE.129D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016usc..confE.129D"><span>8 years of <span class="hlt">Solar</span> Spectral Irradiance Variability <span class="hlt">Observed</span> from the ISS with the <span class="hlt">SOLAR</span>/SOLSPEC Instrument</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Damé, Luc; Bolsée, David; Meftah, Mustapha; Irbah, Abdenour; Hauchecorne, Alain; Bekki, Slimane; Pereira, Nuno; Cessateur, Marchand; Gäel; , Marion; et al.</p> <p>2016-10-01</p> <p>Accurate measurements of <span class="hlt">Solar</span> Spectral Irradiance (SSI) are of primary importance for a better understanding of <span class="hlt">solar</span> physics and of the impact of <span class="hlt">solar</span> variability on climate (via Earth's atmospheric photochemistry). The acquisition of a top of atmosphere reference <span class="hlt">solar</span> spectrum and of its temporal and spectral variability during the unusual <span class="hlt">solar</span> cycle 24 is of prime interest for these studies. These measurements are performed since April 2008 with the SOLSPEC spectro-radiometer from the far ultraviolet to the infrared (166 nm to 3088 nm). This instrument, developed under a fruitful LATMOS/BIRA-IASB collaboration, is part of the <span class="hlt">Solar</span> Monitoring Observatory (<span class="hlt">SOLAR</span>) payload, externally mounted on the Columbus module of the International Space Station (ISS). The <span class="hlt">SOLAR</span> mission, with its actual 8 years duration, will cover almost the entire <span class="hlt">solar</span> cycle 24. We present here the in-flight operations and performances of the SOLSPEC instrument, including the engineering corrections, calibrations and improved know-how procedure for aging corrections. Accordingly, a SSI reference spectrum from the UV to the NIR will be presented, together with its variability in the UV, as measured by <span class="hlt">SOLAR</span>/SOLSPEC for 8 years. Uncertainties on these measurements and comparisons with other instruments will be briefly discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19920017004','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19920017004"><span><span class="hlt">Observational</span> and theoretical investigations in <span class="hlt">solar</span> seismology</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Noyes, Robert W.</p> <p>1992-01-01</p> <p>This is the final report on a project to develop a theoretical basis for interpreting <span class="hlt">solar</span> oscillation data in terms of the interior dynamics and structure of the Sun. The topics covered include the following: (1) studies of the helioseismic signatures of differential rotation and convection in the <span class="hlt">solar</span> interior; (2) wave generation by turbulent convection; and (3) the study of antipodal sunspot imaging of an active region tomography.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19730006113','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19730006113"><span>Analyses of <span class="hlt">solar</span> viewing time, beta angle, and doppler shift for <span class="hlt">solar</span> <span class="hlt">observations</span> from the space shuttle</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Brandon, J. P.</p> <p>1972-01-01</p> <p>Studies of <span class="hlt">solar</span> physics phenomena are aided by the ability to <span class="hlt">observe</span> the sun from earth orbit without periodic occultation. Charts are presented for the selection of suitable orbits about the earth at which a spacecraft is continuously illuminated through a period of a few days. Selection of the orbits considers the reduction of Doppler shift and wavefront attenuation due to relative orbital velocity and residual earth atmosphere.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/11543411','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/11543411"><span>High-performance, low-cost <span class="hlt">solar</span> collectors for disinfection of contaminated water.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Vidal, A; Diaz, A I</p> <p>2000-01-01</p> <p>Although the germicidal action of sunlight has long been recognized, its potential for practical applications has to be researched more thoroughly. This paper summarizes the progress made toward a commercially practical collector for <span class="hlt">solar</span> disinfection applications. Nontracking compound parabolic collectors (CPCs), developed originally for <span class="hlt">capturing</span> <span class="hlt">solar</span> photons for thermal energy applications, were examined as potential <span class="hlt">solar</span> photoreactors. A field demonstration of <span class="hlt">solar</span> disinfection treatment using commercially manufactured <span class="hlt">solar</span> reactors was conducted. Field tests showed successful destruction of Escherichia coli and Enterococcus faecalis and have provided data for full-scale design of water treatment systems. From above <span class="hlt">observations</span>, a throughput value of 50 L/m2 h for the low-cost CPC reactor tested was estimated. For a 190 m3/d (0.05 MGD) facility, the estimated total costs for disinfection using UV-A is U.S. $0.19/m3 ($0.70/1000 gal). The use of near-UV sunlight to disinfect water supplies seems promising in rural communities of developing countries where treated water is unavailable.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://images.nasa.gov/#/details-s93-48707.html','SCIGOVIMAGE-NASA'); return false;" href="https://images.nasa.gov/#/details-s93-48707.html"><span>Computer-generated scenes depicting the HST <span class="hlt">capture</span> and EVA repair mission</span></a></p> <p><a target="_blank" href="https://images.nasa.gov/">NASA Image and Video Library</a></p> <p></p> <p>1993-11-12</p> <p>Computer generated scenes depicting the Hubble Space Telescope <span class="hlt">capture</span> and a sequence of planned events on the planned extravehicular activity (EVA). Scenes include the Remote Manipulator System (RMS) arm assisting two astronauts changing out the Wide Field/Planetary Camera (WF/PC) (48699); RMS arm assisting in the temporary mating of the orbiting telescope to the flight support system in Endeavour's cargo bay (48700); Endeavour's RMS arm assisting in the "<span class="hlt">capture</span>" of the orbiting telescope (48701); Two astronauts changing out the telescope's coprocessor (48702); RMS arm assistign two astronauts replacing one of the telescope's electronic control units (48703); RMS assisting two astronauts replacing the fuse plugs on the telescope's Power Distribution Unit (PDU) (48704); The telescope's High Resolution Spectrograph (HRS) kit is depicted in this scene (48705); Two astronauts during the removal of the high speed photometer and the installation of the COSTAR instrument (48706); Two astronauts, standing on the RMS, during installation of one of the Magnetic Sensing System (MSS) (48707); High angle view of the orbiting Space Shuttle Endeavour with its cargo bay doors open, revealing the bay's pre-<span class="hlt">capture</span> configuration. Seen are, from the left, the <span class="hlt">Solar</span> Array Carrier, the ORU Carrier and the flight support system (48708); Two astronauts performing the replacement of HST's Rate Sensor Units (RSU) (48709); The RMS arm assisting two astronauts with the replacement of the telescope's <span class="hlt">solar</span> array panels (48710); Two astronauts replacing the telescope's <span class="hlt">Solar</span> Array Drive Electronics (SADE) (48711).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016cosp...41E..77H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016cosp...41E..77H"><span>42 years of continuous <span class="hlt">observations</span> of the <span class="hlt">Solar</span> 1 diameter from 1974 to 2015 - What do they forecast.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Humberto Andrei, Alexandre; Penna, Jucira; Boscardin, Sergio; Papa, Andres R. R.; Garcia, Marcos Antonio; Sigismondi, Costantino</p> <p>2016-07-01</p> <p>Several research groups in the world developed <span class="hlt">observational</span> programs for the Sun in order to measure its apparent diameter over time with dedicated instruments, called <span class="hlt">solar</span> astrolabes, since 1974. Their data have been gathered in several <span class="hlt">observing</span> stations connected in the R2S3 (Réseau de Suivi au Sol du Rayon Solaire) network and through reciprocal visits and exchanges: Nice/Calern Observatoire/France, Rio de Janeiro Observatório Nacional/Brazil, Observatório de São Paulo IAGUSP/Brazil, Observatório Abrahão de Moraes IAGUSP/Brazil, Antalya Observatory/Turkey, San Fernando/Spain. Since all the optics and data treatment of the <span class="hlt">solar</span> astrolabes was the same, from the oldest, with a single fixed objective prism, to the newest, with an angle variable objective prism and digital image acquisition, their results could be put together. Each instrument had its own density filter with a prismatic effect responsible for a particular shift. Thus, identical data gathering and just a different prismatic shift, enabled to reconcile all those series by using the common stretches and derive a single additive constant to place each one onto a common average. By doing so, although the value itself of the ground <span class="hlt">observed</span> <span class="hlt">solar</span> diameter is lost, its variations are determined over 35 years. On the combined series of the ground <span class="hlt">observed</span> <span class="hlt">solar</span> diameter a modulation with the 11 years main <span class="hlt">solar</span> cycle is evident. However when such modulation is removed, both from the <span class="hlt">solar</span> diameter compound series and from the <span class="hlt">solar</span> activity series (as given by the sunspots count), a very strong anticorrelation is revealed. This suggested a larger diameter for the forthcoming cycles. This was very well verified for <span class="hlt">solar</span> cycle 23, and correctly forecasted for cycle 24,in a behavior similar to that on the Minima of Dalton and Maunder. The ground monitoring keeps being routinely followed at Observatório Nacional in Rio de Janeiro, now using the <span class="hlt">Solar</span> Heliometer, specially built to this end . The</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMSA54A..03W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMSA54A..03W"><span>Comparison of Model and <span class="hlt">Observations</span> of Middle Atmospheric HOx Response to <span class="hlt">Solar</span> 27-day Cycles: Quantifying Model Uncertainties due to Photochemistry</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wang, S.; Li, K. F.; Shia, R. L.; Yung, Y. L.; Sander, S. P.</p> <p>2016-12-01</p> <p>HO2 and OH (known as odd oxygen HOx), play an important role in middle atmospheric chemistry, in particular, O3 destruction through catalytic HOx reaction cycles. Due to their photochemical production and short chemical lifetimes, HOx species response rapidly to <span class="hlt">solar</span> UV irradiance changes during <span class="hlt">solar</span> cycles, resulting in variability in the corresponding O3 chemistry. <span class="hlt">Observational</span> evidences for both OH and HO2 variability due to <span class="hlt">solar</span> cycles have been reported. However, puzzling discrepancies remain. In particular, the large discrepancy between model and <span class="hlt">observations</span> of <span class="hlt">solar</span> 11-year cycle signal in OH and the significantly different model results when adopting different <span class="hlt">solar</span> spectral irradiance (SSI) [Wang et al., 2013] suggest that both uncertainties in SSI variability and uncertainties in our current understanding of HOx-O3 chemistry could contribute to the discrepancy. Since the short-term SSI variability (e.g. changes during <span class="hlt">solar</span> 27-day cycles) has little uncertainty, investigating 27-day <span class="hlt">solar</span> cycle signals in HOx allows us to simplify the complex problem and to focus on the uncertainties in chemistry alone. We use the Caltech-JPL photochemical model to simulate <span class="hlt">observed</span> HOx variability during 27-day cycles. The comparison between Aura Microwave Limb Sounder (MLS) <span class="hlt">observations</span> and our model results (using standard chemistry and "adjusted chemistry", respectively) will be discussed. A better understanding of uncertainties in chemistry will eventually help us separate the contribution of chemistry from contributions of SSI uncertainties to the complex discrepancy between model and <span class="hlt">observations</span> of OH responses to <span class="hlt">solar</span> 11-year cycles.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017SoPh..292..151B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017SoPh..292..151B"><span><span class="hlt">Observations</span> of a Radio-Quiet <span class="hlt">Solar</span> Preflare</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Benz, Arnold O.; Battaglia, Marina; Güdel, Manuel</p> <p>2017-10-01</p> <p>The preflare phase of the flare SOL2011-08-09T03:52 is unique in its long duration, in that it was covered by the Reuven Ramaty High Energy <span class="hlt">Solar</span> Spectroscopic Imager (RHESSI) and the Nobeyama Radioheliograph, and because it showed three well-developed soft X-ray (SXR) peaks. No hard X-rays (HXR) are <span class="hlt">observed</span> in the preflare phase. Here we report that no associated radio emission at 17 GHz was found either, despite the higher sensitivity of the radio instrument. The ratio between the SXR peaks and the upper limit of the radio peaks is higher by more than one order of magnitude than the ratio in regular flares. The result suggests that the ratio between acceleration and heating in the preflare phase was different than in regular flares. Acceleration to relativistic energies, if any, occurred with lower efficiency.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PhDT........49O','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PhDT........49O"><span>Spectroscopic Analyses of Neutron <span class="hlt">Capture</span> Elements in Open Clusters</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>O'Connell, Julia E.</p> <p></p> <p>The evolution of elements as a function or age throughout the Milky Way disk provides strong constraints for galaxy evolution models, and on star formation epochs. In an effort to provide such constraints, we conducted an investigation into r- and s-process elemental abundances for a large sample of open clusters as part of an optical follow-up to the SDSS-III/APOGEE-1 near infrared survey. To obtain data for neutron <span class="hlt">capture</span> abundance analysis, we conducted a long-term <span class="hlt">observing</span> campaign spanning three years (2013-2016) using the McDonald Observatory Otto Struve 2.1-meter telescope and Sandiford Cass Echelle Spectrograph (SES, R(lambda/Deltalambda) ˜60,000). The SES provides a wavelength range of ˜1400 A, making it uniquely suited to investigate a number of other important chemical abundances as well as the neutron <span class="hlt">capture</span> elements. For this study, we derive abundances for 18 elements covering four nucleosynthetic families- light, iron-peak, neutron <span class="hlt">capture</span> and alpha-elements- for ˜30 open clusters within 6 kpc of the Sun with ages ranging from ˜80 Myr to ˜10 Gyr. Both equivalent width (EW) measurements and spectral synthesis methods were employed to derive abundances for all elements. Initial estimates for model stellar atmospheres- effective temperature and surface gravity- were provided by the APOGEE data set, and then re-derived for our optical spectra by removing abundance trends as a function of excitation potential and reduced width log(EW/lambda). With the exception of Ba II and Zr I, abundance analyses for all neutron <span class="hlt">capture</span> elements were performed by generating synthetic spectra from the new stellar parameters. In order to remove molecular contamination, or blending from nearby atomic features, the synthetic spectra were modeled by a best-fit Gaussian to the <span class="hlt">observed</span> data. Nd II shows a slight enhancement in all cluster stars, while other neutron <span class="hlt">capture</span> elements follow <span class="hlt">solar</span> abundance trends. Ba II shows a large cluster-to-cluster abundance spread</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19970005325','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19970005325"><span>Direct <span class="hlt">Observations</span> of Excess <span class="hlt">Solar</span> Absorption by Clouds</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Pilewskie, Peter; Valero, Francisco P. J.</p> <p>1995-01-01</p> <p>Aircraft measurements of <span class="hlt">solar</span> flux in the cloudy tropical atmosphere reveal that <span class="hlt">solar</span> absorption by clouds is anomalously large when compared to theoretical estimates. The ratio of cloud forcing at an altitude of 20 kilometers to that at the surface is 1.58 rather than 1.0 as predicted by models. These results were derived from a cloud radiation experiment in which identical instrumentation was deployed on coordinated stacked aircraft. These findings indicate a significant difference between measurements and theory and imply that the interaction between clouds and <span class="hlt">solar</span> radiation is poorly understood.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013cctp.book..539H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013cctp.book..539H"><span><span class="hlt">Solar</span> Irradiance Variability and Its Impacts on the Earth Climate System</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Harder, J. W.; Woods, T. N.</p> <p></p> <p>The Sun plays a vital role in the evolution of the climates of terrestrial planets. <span class="hlt">Observations</span> of the <span class="hlt">solar</span> spectrum are now routinely made that span the wavelength range from the X-ray portion of the spectrum (5 nm) into the infrared to about 2400 nm. Over this very broad wavelength range, accounting for about 97% of the total <span class="hlt">solar</span> irradiance, the intensity varies by more than 6 orders of magnitude, requiring a suite of very different and innovative instruments to determine both the spectral irradiance and its variability. The origins of <span class="hlt">solar</span> variability are strongly linked to surface magnetic field changes, and analysis of <span class="hlt">solar</span> images and magnetograms show that the intensity of emitted radiation from <span class="hlt">solar</span> surface features in active regions has a very strong wavelength and magnetic field strength dependence. These magnetic fields produce <span class="hlt">observable</span> <span class="hlt">solar</span> surface features such as sunspots, faculae, and network structures that contribute in different ways to the radiated output. Semi-empirical models of <span class="hlt">solar</span> spectral irradiance are able to <span class="hlt">capture</span> much of the Sun's output, but this topic remains an active area of research. Studies of <span class="hlt">solar</span> structures in both high spectral and spatial resolution are refining this understanding. Advances in Earth <span class="hlt">observation</span> systems and high-quality three-dimensional chemical climate models provide a sound methodology to study the mechanisms of the interaction between Earth's atmosphere and the incoming <span class="hlt">solar</span> radiation. Energetic photons have a profound effect on the chemistry and dynamics of the thermosphere and ionosphere, and these processes are now well represented in upper atmospheric models. In the middle and lower atmosphere the effects of <span class="hlt">solar</span> variability enter the climate system through two nonexclusive pathways referred to as the top-down and bottom-up mechanisms. The top-down mechanism proceeds through the alteration of the photochemical rates that establish the middle atmospheric temperature structure and</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1433310-maximizing-tandem-solar-cell-power-extraction-using-three-terminal-design','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1433310-maximizing-tandem-solar-cell-power-extraction-using-three-terminal-design"><span>Maximizing tandem <span class="hlt">solar</span> cell power extraction using a three-terminal design</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Warren, Emily L.; Deceglie, Michael G.; Rienacker, Michael; ...</p> <p>2018-04-09</p> <p>Three-terminal tandem <span class="hlt">solar</span> cells can provide a robust operating mechanism to efficiently <span class="hlt">capture</span> the <span class="hlt">solar</span> spectrum without the need to current match sub-cells or fabricate complicated metal interconnects.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1434122-maximizing-tandem-solar-cell-power-extraction-using-three-terminal-design','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1434122-maximizing-tandem-solar-cell-power-extraction-using-three-terminal-design"><span>Maximizing tandem <span class="hlt">solar</span> cell power extraction using a three-terminal design</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Warren, Emily L.; Deceglie, Michael G.; Rienäcker, Michael; ...</p> <p>2018-01-01</p> <p>Three-terminal tandem <span class="hlt">solar</span> cells can provide a robust operating mechanism to efficiently <span class="hlt">capture</span> the <span class="hlt">solar</span> spectrum without the need to current match sub-cells or fabricate complicated metal interconnects.</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://hdl.handle.net/2060/19920012697','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19920012697"><span>Stereoscopic <span class="hlt">observations</span> of hard x ray sources in <span class="hlt">solar</span> flares made with GRO and other spacecraft</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kane, S. R.; Hurley, K.; Mctiernan, J. M.; Laros, J. G.</p> <p>1992-01-01</p> <p>Since the launch of the Gamma Ray Observatory (GRO) in Apr. 1991, the Burst and Transient Source Experiment (BATSE) instrument on GRO has recorded a large number of <span class="hlt">solar</span> flares. Some of these flares have also been <span class="hlt">observed</span> by the Gamma-Ray Burst Detector on the Pioneer Venus Orbiter (PVO) and/or by the <span class="hlt">Solar</span> X-Ray/Cosmic Gamma-Ray Burst Experiment on the Ulysses spacecraft. A preliminary list of common flares <span class="hlt">observed</span> during the period May-Jun. 1991 is presented and the possible joint studies are indicated.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20120013207','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20120013207"><span>Thermal Evolution and Radiative Output of <span class="hlt">Solar</span> Flares <span class="hlt">Observed</span> by the EUV Variability Experiment (EVE)</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Chamberlin, P. C.; Milligan, R. O.; Woods, T. N.</p> <p>2012-01-01</p> <p>This paper describes the methods used to obtain the thermal evolution and radiative output during <span class="hlt">solar</span> flares as <span class="hlt">observed</span> by the Extreme u ltraviolet Variability Experiment (EVE) onboard the <span class="hlt">Solar</span> Dynamics Ob servatory (SDO). Presented and discussed in detail are how EVE measur ements, due to its temporal cadence, spectral resolution and spectral range, can be used to determine how the thermal plasma radiates at v arious temperatures throughout the impulsive and gradual phase of fla res. EVE can very accurately determine the radiative output of flares due to pre- and in-flight calibrations. Events are presented that sh ow the total radiated output of flares depends more on the flare duration than the typical GOES X-ray peak magnitude classification. With S DO <span class="hlt">observing</span> every flare throughout its entire duration and over a la rge temperature range, new insights into flare heating and cooling as well as the radiative energy release in EUV wavelengths support exis ting research into understanding the evolution of <span class="hlt">solar</span> flares.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013ASPC..478..145S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013ASPC..478..145S"><span>Differences of the <span class="hlt">Solar</span> Magnetic Activity Signature in Velocity and Intensity Helioseismic <span class="hlt">Observations</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Salabert, D.; García, R. A.; Jiménez, A.</p> <p>2013-12-01</p> <p>The high-quality, full-disk helioseismic <span class="hlt">observations</span> continuously collected by the spectrophotometer GOLF and the three photometers VIRGO/SPMs onboard the SoHO spacecraft for 17 years now (since April 11, 1996, apart from the SoHO “vacations”) are absolutely unique for the study of the interior of the Sun and its variability with magnetic activity. Here, we look at the differences in the low-degree oscillation p-mode frequencies between radial velocity and intensity measurements taking into account all the known features of the p-mode profiles (e.g., the opposite peak asymmetry), and of the power spectrum (e.g., the presence of the higher degrees ℓ = 4 and 5 in the signal). We show that the intensity frequencies are higher than the velocity frequencies during the <span class="hlt">solar</span> cycle with a clear temporal dependence. The response between the individual angular degrees is also different. Time delays are <span class="hlt">observed</span> between the temporal variations in GOLF and VIRGO frequencies. Such analysis is important in order to put new constraints and to better understand the mechanisms responsible for the temporal variations of the oscillation frequencies with the <span class="hlt">solar</span> magnetic activity as well as their height dependences in the <span class="hlt">solar</span> atmosphere. It is also important for the study of the stellar magnetic activity using asteroseismic data.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20000114830','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20000114830"><span>Corongraphic <span class="hlt">Observations</span> and Analyses of The Ultraviolet <span class="hlt">Solar</span> Corona</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kohl, John L.</p> <p>2000-01-01</p> <p>The activities supported under NASA Grant NAG5-613 included the following: 1) reduction and scientific analysis of data from three sounding rocket flights of the Rocket Ultraviolet Coronagraph Spectrometer, 2) development of ultraviolet spectroscopic diagnostic techniques to provide a detailed empirical description of the extended <span class="hlt">solar</span> corona, 3) extensive upgrade of the rocket instrument to become the Ultraviolet Coronal Spectrometer (UVCS) for Spartan 201,4) instrument scientific calibration and characterization, 5) <span class="hlt">observation</span> planning and mission support for a series of five Spartan 201 missions (fully successful except for STS 87 where the Spartan spacecraft was not successfully deployed and the instruments were not activated), and 6) reduction and scientific analysis of the UVCS/Spartan 201 <span class="hlt">observational</span> data. The Ultraviolet Coronal Spectrometer for Spartan 201 was one unit of a joint payload and the other unit was a White Light Coronagraph (WLC) provided by the High Altitude Observatory and the Goddard Space Flight Center. The two instruments were used in concert to determine plasma parameters describing structures in the extended <span class="hlt">solar</span> corona. They provided data that could be used individually or jointly in scientific analyses. The WLC provided electron column densities in high spatial resolution and high time resolution. UVCS/Spartan provided hydrogen velocity distributions, and line of sight hydrogen velocities. The hydrogen intensities from UVCS together with the electron densities from WLC were used to determine hydrogen outflow velocities. The UVCS also provided O VI intensities which were used to develop diagnostics for velocity distributions and outflow velocities of minor ions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19780024031&hterms=Experimental+design&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3DExperimental%2Bdesign','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19780024031&hterms=Experimental+design&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3DExperimental%2Bdesign"><span>A hard X-ray and gamma ray <span class="hlt">observation</span> of the 22 November 1977 <span class="hlt">solar</span> flare. [experimental design</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Chambon, G.; Hurley, K.; Niel, M.; Talon, R.; Vedrenne, G.; Likine, O. B.; Kouznetsov, A. V.; Estouline, I. V.</p> <p>1978-01-01</p> <p>The Franco-Soviet experiment package Signe 2 MP for <span class="hlt">solar</span> and cosmic X and gamma ray <span class="hlt">observations</span>, launched aboard a Soviet Prognoz satellite into a highly eccentric earth orbit is described. An uncollimated NaI detector 37 mm thick by 90 mm diameter, placed on the upper surface of the satellite faced the sun. A collimated lateral NaI detector 14 mm thick by 38 mm diameter also faced the sun, and a similar lateral detector faced the anti-<span class="hlt">solar</span> direction. Data tapes reveal an intense <span class="hlt">solar</span> flare up to energies of up to 5 MeV, with evidence for line emission at 2.23 MeV and possibly 4.4 MeV. The event <span class="hlt">observed</span> was associated with the Mc Math Plage Region 15031, and an H-alpha flare of importance 2B. It is not yet clear what radio emission is associated with the X-ray <span class="hlt">observation</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19990080908&hterms=theory+building&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dtheory%2Bbuilding','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19990080908&hterms=theory+building&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dtheory%2Bbuilding"><span>Update of the ISTP <span class="hlt">Solar</span> Maximum Mission: ISTP Project Scientist for Theory and Ground-Based <span class="hlt">Observations</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Curtis, Steve</p> <p>1999-01-01</p> <p>Building upon the numerous successes of the pre-<span class="hlt">solar</span> maximum International <span class="hlt">Solar</span> Terrestrial Physics (ISTP) mission, the ISTP <span class="hlt">Solar</span> Maximum Mission is expected to produce new insights into global flow of energy, momentum, and mass, from the Sun, through the heliosphere, into the magnetosphere and to their final deposition in the terrestrial upper atmosphere/ionosphere system. Of particular interest is the determination of the geo-effectiveness of <span class="hlt">solar</span> events, principally Coronal Mass Ejections (CMEs). Given the expected increased frequency and strength of CMEs during the <span class="hlt">Solar</span> Maximum period, a major advance in our understanding of nature of the coupling of CMEs to the magnetosphere-ionosphere-atmosphere system is expected. The roles during this time of the various ISTP assets will be discussed. These assets will include the SOHO, Wind, Polar, and Geotail spacecraft, the ground-based <span class="hlt">observing</span> networks and the theory tools.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JGRA..123..848L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JGRA..123..848L"><span>The 11 Year <span class="hlt">Solar</span> Cycle Response of the Equatorial Ionization Anomaly <span class="hlt">Observed</span> by GPS Radio Occultation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Li, King-Fai; Lin, Li-Ching; Bui, Xuan-Hien; Liang, Mao-Chang</p> <p>2018-01-01</p> <p>We have retrieved the latitudinal and vertical structures of the 11 year <span class="hlt">solar</span> cycle modulation on ionospheric electron density using 14 years of satellite-based radio occultation measurements utilizing the Global Positioning System. The densities at the crests of the equatorial ionization anomaly (EIA) in the subtropics near 300 km in 2003 and 2014 (high <span class="hlt">solar</span> activity with <span class="hlt">solar</span> 10.7 cm flux, <fi>F</fi>10.7 ≈ 140 <span class="hlt">solar</span> flux unit (sfu)) were 3 times higher than that in 2009 (low <span class="hlt">solar</span> activity <fi>F</fi>10.7 ≈ 70 sfu). The higher density is attributed to the elevated <span class="hlt">solar</span> extreme ultraviolet and geomagnetic activity during high <span class="hlt">solar</span> activity periods. The location of the EIA crests moved 50 km upward and 10° poleward, because of the enhanced E × B force. The EIA in the northern hemisphere was more pronounced than that in the southern hemisphere. This interhemispheric asymmetry is consistent with the effect of enhanced transequatorial neutral wind. The above <span class="hlt">observations</span> were reproduced qualitatively by the two benchmark runs of the Thermosphere-Ionosphere-Electrodynamics General Circulation Model. In addition, we have studied the impact of the 11 year <span class="hlt">solar</span> cycle on the 27 day <span class="hlt">solar</span> cycle response of the ionospheric electron density. Beside the expected modulation on the amplitude of the 27 day <span class="hlt">solar</span> variation due to the 11 year <span class="hlt">solar</span> cycle, we find that the altitude of the maximal 27 day <span class="hlt">solar</span> response is unexpectedly 50 km higher than that of the 11 year <span class="hlt">solar</span> response. This is the first time that a vertical dependence of the <span class="hlt">solar</span> responses on different time scales is reported.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1992lest.rept....3K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1992lest.rept....3K"><span>GAP: yet another image processing system for <span class="hlt">solar</span> <span class="hlt">observations</span>.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Keller, C. U.</p> <p></p> <p>GAP is a versatile, interactive image processing system for analyzing <span class="hlt">solar</span> <span class="hlt">observations</span>, in particular extended time sequences, and for preparing publication quality figures. It consists of an interpreter that is based on a language with a control flow similar to PASCAL and C. The interpreter may be accessed from a command line editor and from user-supplied functions, procedures, and command scripts. GAP is easily expandable via external FORTRAN programs that are linked to the GAP interface routines. The current version of GAP runs on VAX, DECstation, Sun, and Apollo computers. Versions for MS-DOS and OS/2 are in preparation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19910051714&hterms=solar+intensity+measurement&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3Dsolar%2Bintensity%2Bmeasurement','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19910051714&hterms=solar+intensity+measurement&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3Dsolar%2Bintensity%2Bmeasurement"><span>A simple method for correcting spatially resolved <span class="hlt">solar</span> intensity oscillation <span class="hlt">observations</span> for variations in scattered light</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Jefferies, S. M.; Duvall, T. L., Jr.</p> <p>1991-01-01</p> <p>A measurement of the intensity distribution in an image of the <span class="hlt">solar</span> disk will be corrupted by a spatial redistribution of the light that is caused by the earth's atmosphere and the <span class="hlt">observing</span> instrument. A simple correction method is introduced here that is applicable for <span class="hlt">solar</span> p-mode intensity <span class="hlt">observations</span> obtained over a period of time in which there is a significant change in the scattering component of the point spread function. The method circumvents the problems incurred with an accurate determination of the spatial point spread function and its subsequent deconvolution from the <span class="hlt">observations</span>. The method only corrects the spherical harmonic coefficients that represent the spatial frequencies present in the image and does not correct the image itself.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20150007948','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20150007948"><span>Correlations Between Variations in <span class="hlt">Solar</span> EUV and Soft X-Ray Irradiance and Photoelectron Energy Spectra <span class="hlt">Observed</span> on Mars and Earth</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Peterson, W. K.; Brain, D. A.; Mitchell, D. L.; Bailey, S. M.; Chamberlin, P. C.</p> <p>2013-01-01</p> <p><span class="hlt">Solar</span> extreme ultraviolet (EUV; 10-120 nm) and soft X-ray (XUV; 0-10 nm) radiation are major heat sources for the Mars thermosphere as well as the primary source of ionization that creates the ionosphere. In investigations of Mars thermospheric chemistry and dynamics, <span class="hlt">solar</span> irradiance models are used to account for variations in this radiation. Because of limited proxies, irradiance models do a poor job of tracking the significant variations in irradiance intensity in the EUV and XUV ranges over <span class="hlt">solar</span> rotation time scales when the Mars-Sun-Earth angle is large. Recent results from Earth <span class="hlt">observations</span> show that variations in photoelectron energy spectra are useful monitors of EUV and XUV irradiance variability. Here we investigate photoelectron energy spectra <span class="hlt">observed</span> by the Mars Global Surveyor (MGS) Electron Reflectometer (ER) and the FAST satellite during the interval in 2005 when Earth, Mars, and the Sun were aligned. The Earth photoelectron data in selected bands correlate well with calculations based on 1 nm resolution <span class="hlt">observations</span> above 27 nm supplemented by broadband <span class="hlt">observations</span> and a <span class="hlt">solar</span> model in the 0-27 nm range. At Mars, we find that instrumental and orbital limitations to the identifications of photoelectron energy spectra in MGS/ER data preclude their use as a monitor of <span class="hlt">solar</span> EUV and XUV variability. However, <span class="hlt">observations</span> with higher temporal and energy resolution obtained at lower altitudes on Mars might allow the separation of the <span class="hlt">solar</span> wind and ionospheric components of electron energy spectra so that they could be used as reliable monitors of variations in <span class="hlt">solar</span> EUV and XUV irradiance than the time shifted, Earth-based, F(10.7) index currently used.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19900003993','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19900003993"><span>EIT: <span class="hlt">Solar</span> corona synoptic <span class="hlt">observations</span> from SOHO with an Extreme-ultraviolet Imaging Telescope</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Delaboudiniere, J. P.; Gabriel, A. H.; Artzner, G. E.; Michels, D. J.; Dere, K. P.; Howard, R. A.; Catura, R.; Stern, R.; Lemen, J.; Neupert, W.</p> <p>1988-01-01</p> <p>The Extreme-ultraviolet Imaging Telescope (EIT) of SOHO (<span class="hlt">solar</span> and heliospheric observatory) will provide full disk images in emission lines formed at temperatures that map <span class="hlt">solar</span> structures ranging from the chromospheric network to the hot magnetically confined plasma in the corona. Images in four narrow bandpasses will be obtained using normal incidence multilayered optics deposited on quadrants of a Ritchey-Chretien telescope. The EIT is capable of providing a uniform one arc second resolution over its entire 50 by 50 arc min field of view. Data from the EIT will be extremely valuable for identifying and interpreting the spatial and temperature fine structures of the <span class="hlt">solar</span> atmosphere. Temporal analysis will provide information on the stability of these structures and identify dynamical processes. EIT images, issued daily, will provide the global corona context for aid in unifying the investigations and in forming the <span class="hlt">observing</span> plans for SOHO coronal instruments.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1326029-time-dependent-mhd-simulations-solar-wind-outflow-using-interplanetary-scintillation-observations','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1326029-time-dependent-mhd-simulations-solar-wind-outflow-using-interplanetary-scintillation-observations"><span>Time-dependent MHD simulations of the <span class="hlt">solar</span> wind outflow using interplanetary scintillation <span class="hlt">observations</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Kim, Tae K.; Pogorelov, Nikolai V.; Borovikov, Sergey N.; ...</p> <p>2012-11-20</p> <p>Numerical modeling of the heliosphere is a critical component of space weather forecasting. The accuracy of heliospheric models can be improved by using realistic boundary conditions and confirming the results with in situ spacecraft measurements. To accurately reproduce the <span class="hlt">solar</span> wind (SW) plasma flow near Earth, we need realistic, time-dependent boundary conditions at a fixed distance from the Sun. We may prepare such boundary conditions using SW speed and density determined from interplanetary scintillation (IPS) <span class="hlt">observations</span>, magnetic field derived from photospheric magnetograms, and temperature estimated from its correlation with SW speed. In conclusion, we present here the time-dependent MHD simulationmore » results obtained by using the 2011 IPS data from the <span class="hlt">Solar</span>-Terrestrial Environment Laboratory as time-varying inner boundary conditions and compare the simulated data at Earth with OMNI data (spacecraft-interspersed, near-Earth <span class="hlt">solar</span> wind data).« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19960021432&hterms=geofisica&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dgeofisica','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19960021432&hterms=geofisica&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dgeofisica"><span>The effects of 8 Helios <span class="hlt">observed</span> <span class="hlt">solar</span> proton events of interplanetary magnetic field fluctuations</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>ValdezGalicia, J. F.; Alexander, P.; Otaola, J. A.</p> <p>1995-01-01</p> <p>There have been recent suggestions that large fluxes during <span class="hlt">solar</span> energetic particle events may produce their own turbulence. To verify this argument it becomes essential to find out whether these flows cause an enhancement of interplanetary magnetic field fluctuations. In the present work, power and helicity spectra of the IMF before, during and after 8 Helios-<span class="hlt">observed</span> <span class="hlt">solar</span> proton events in the range 0.3 - 1 AU are analyzed. In order to detect proton self generated waves, the time evolution of spectra are followed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25104382','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25104382"><span>Early <span class="hlt">solar</span> system. Stellar origin of the ¹⁸²Hf cosmochronometer and the presolar history of <span class="hlt">solar</span> system matter.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Lugaro, Maria; Heger, Alexander; Osrin, Dean; Goriely, Stephane; Zuber, Kai; Karakas, Amanda I; Gibson, Brad K; Doherty, Carolyn L; Lattanzio, John C; Ott, Ulrich</p> <p>2014-08-08</p> <p>Among the short-lived radioactive nuclei inferred to be present in the early <span class="hlt">solar</span> system via meteoritic analyses, there are several heavier than iron whose stellar origin has been poorly understood. In particular, the abundances inferred for (182)Hf (half-life = 8.9 million years) and (129)I (half-life = 15.7 million years) are in disagreement with each other if both nuclei are produced by the rapid neutron-<span class="hlt">capture</span> process. Here, we demonstrate that contrary to previous assumption, the slow neutron-<span class="hlt">capture</span> process in asymptotic giant branch stars produces (182)Hf. This has allowed us to date the last rapid and slow neutron-<span class="hlt">capture</span> events that contaminated the <span class="hlt">solar</span> system material at ~100 million years and ~30 million years, respectively, before the formation of the Sun. Copyright © 2014, American Association for the Advancement of Science.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22518823-new-observations-solar-kev-soft-ray-spectrum','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22518823-new-observations-solar-kev-soft-ray-spectrum"><span>NEW <span class="hlt">OBSERVATIONS</span> OF THE <span class="hlt">SOLAR</span> 0.5–5 KEV SOFT X-RAY SPECTRUM</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>Caspi, Amir; Woods, Thomas N.; Warren, Harry P.</p> <p>2015-03-20</p> <p>The <span class="hlt">solar</span> corona is orders of magnitude hotter than the underlying photosphere, but how the corona attains such high temperatures is still not understood. Soft X-ray (SXR) emission provides important diagnostics for thermal processes in the high-temperature corona, and is also an important driver of ionospheric dynamics at Earth. There is a crucial <span class="hlt">observational</span> gap between ∼0.2 and ∼4 keV, outside the ranges of existing spectrometers. We present <span class="hlt">observations</span> from a new SXR spectrometer, the Amptek X123-SDD, which measured the spatially integrated <span class="hlt">solar</span> spectral irradiance from ∼0.5 to ∼5 keV, with ∼0.15 keV FWHM resolution, during sounding rocket flights onmore » 2012 June 23 and 2013 October 21. These measurements show that the highly variable SXR emission is orders of magnitude greater than that during the deep minimum of 2009, even with only weak activity. The <span class="hlt">observed</span> spectra show significant high-temperature (5–10 MK) emission and are well fit by simple power-law temperature distributions with indices of ∼6, close to the predictions of nanoflare models of coronal heating. <span class="hlt">Observations</span> during the more active 2013 flight indicate an enrichment of low first-ionization potential elements of only ∼1.6, below the usually <span class="hlt">observed</span> value of ∼4, suggesting that abundance variations may be related to coronal heating processes. The XUV Photometer System Level 4 data product, a spectral irradiance model derived from integrated broadband measurements, significantly overestimates the spectra from both flights, suggesting a need for revision of its non-flare reference spectra, with important implications for studies of Earth ionospheric dynamics driven by <span class="hlt">solar</span> SXRs.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19800017743','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19800017743"><span>Rocket <span class="hlt">observations</span> of <span class="hlt">solar</span> radiation during the eclipse of 26 February 1979</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Bliss, H. M.; Smith, L. G.</p> <p>1980-01-01</p> <p>Three Nike Tomahawk rockets were launched in Red Lake, Ontario, one previous to, and two during, the total eclipse of the Sun, for the purpose of studying the atmosphere and its interaction with <span class="hlt">solar</span> radiation. The method and preliminary results of three experiments that were used to measure <span class="hlt">solar</span> radiation in the X-ray, Lyman-alpha, and visible parts of the spectrum are described. The instrumentation designed for this investigation is discussed as well as post-flight data processing techniques. The retrieved data were processed to some extent to verify that a valid representation of the <span class="hlt">solar</span> radiation was obtained. The Lyman-alpha experiment yielded very good results, and preliminary data are included. The visible radiation experiment served as support for the other experiments and also functioned well. Due to a high level of energetic particles during the eclipse, the X-ray data were contaminated and are not presented. However, satellite <span class="hlt">observations</span> indicate no appreciable level of X-rays from the Sun during the time of the eclipse.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMSA21B2513S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMSA21B2513S"><span>On the Importance of <span class="hlt">Solar</span> Eclipse Geometry in the Interpretation of Ionospheric <span class="hlt">Observations</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Stankov, S.; Verhulst, T. G. W.</p> <p>2017-12-01</p> <p>A reliable interpretation of <span class="hlt">solar</span> eclipse effects on the geospace environment, and on the ionosphere in particular, necessitates a careful consideration of the so-called eclipse geometry. A <span class="hlt">solar</span> eclipse is a relatively rare astronomical phenomenon, which geometry is rather complex, specific for each event, and fast changing in time. The standard, most popular way to look at the eclipse geometry is via the two-dimensional representation (map) of the <span class="hlt">solar</span> obscuration on the Earth's surface, in which the path of eclipse totality is drawn together with isolines of the gradually-decreasing eclipse magnitude farther away from this path. Such "surface maps" are widely used to readily explain some of the <span class="hlt">solar</span> eclipse effects including, for example, the well-known decrease in total ionisation (due to the substantial decrease in <span class="hlt">solar</span> irradiation), usually presented by the popular and easy to understand ionospheric characteristic of Total Electron Content (TEC). However, many other effects, especially those taking place at higher altitudes, cannot be explained in this fashion. Instead, a complete, four-dimensional (4D) description of the umbra (and penumbra), would be required. This presentation will address the issue of eclipse geometry effects on various ionospheric <span class="hlt">observations</span> carried out during the total <span class="hlt">solar</span> eclipse of August 21, 2017. In particular, GPS-based TEC and ionosonde measurements will be analysed and the eclipse effects on the ionosphere will be interpreted with respect to the actual eclipse geometry at ionospheric heights. Whenever possible, a comparison will be made with results from previous events, such as the ones from March 20, 2015 and October 3, 2005.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007AAS...210.7203H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007AAS...210.7203H"><span>An <span class="hlt">Observation</span> Knowledgebase for Hinode Data</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hurlburt, Neal E.; Freeland, S.; Green, S.; Schiff, D.; Seguin, R.; Slater, G.; Cirtain, J.</p> <p>2007-05-01</p> <p>We have developed a standards-based system for the <span class="hlt">Solar</span> Optical and X Ray Telescopes on the Hinode orbiting <span class="hlt">solar</span> observatory which can serve as part of a developing Heliophysics informatics system. Our goal is to make the scientific data acquired by Hinode more accessible and useful to scientists by allowing them to do reasoning and flexible searches on <span class="hlt">observation</span> metadata and to ask higher-level questions of the system than previously allowed. The Hinode <span class="hlt">Observation</span> Knowledgebase relates the intentions and goals of the <span class="hlt">observation</span> planners (as-planned metadata) with actual <span class="hlt">observational</span> data (as-run metadata), along with connections to related models, data products and identified features (follow-up metadata) through a citation system. Summaries of the data (both as image thumbnails and short "film strips") serve to guide researchers to the <span class="hlt">observations</span> appropriate for their research, and these are linked directly to the data catalog for easy extraction and delivery. The semantic information of the <span class="hlt">observation</span> (Field of view, wavelength, type of <span class="hlt">observable</span>, average cadence etc.) is <span class="hlt">captured</span> through simple user interfaces and encoded using the VOEvent XML standard (with the addition of some <span class="hlt">solar</span>-related extensions). These interfaces merge metadata acquired automatically during both mission planning and an data analysis (see Seguin et. al. 2007 at this meeting) phases with that obtained directly from the planner/analyst and send them to be incorporated into the knowledgebase. The resulting information is automatically rendered into standard categories based on planned and recent <span class="hlt">observations</span>, as well as by popularity and recommendations by the science team. They are also directly searchable through both and web-based searches and direct calls to the API. <span class="hlt">Observations</span> details can also be rendered as RSS, iTunes and Google Earth interfaces. The resulting system provides a useful tool to researchers and can act as a demonstration for larger, more complex systems.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFMSH43A4181V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFMSH43A4181V"><span>The Propagation of <span class="hlt">Solar</span> Energetic Particles as <span class="hlt">Observed</span> by the Stereo Spacecraft and Near Earth</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>von Rosenvinge, T. T.; Richardson, I. G.; Cane, H. V.; Christian, E. R.; Cummings, A. C.; Cohen, C. M.; Leske, R. A.; Mewaldt, R. A.; Stone, E. C.; Wiedenbeck, M. E.</p> <p>2014-12-01</p> <p>Over 200 <span class="hlt">Solar</span> Energetic Particle Events (SEPs) with protons > 25 MeV have been identified using data from the IMPACT HET telescopes on the STEREO A and B spacecraft and similar data from SoHO near Earth. The properties of these events are tabulated in a recent publication in <span class="hlt">Solar</span> Physics (Richardson, et al., 2014). One of the goals of the Stereo Mission is to better understand the propagation of SEPs. The properties of events <span class="hlt">observed</span> by multiple spacecraft on average are well-organized by the distance of the footpoints of the nominal Parker Spiral magnetic field lines passing the <span class="hlt">observing</span> spacecraft from the parent active regions. However, some events deviate significantly from this pattern. For example, in events <span class="hlt">observed</span> by three spacecraft, the spacecraft with the best nominal connection does not necessarily <span class="hlt">observe</span> the highest intensity or earliest particle arrival time. We will search for such events and try to relate their behavior to non-nominal magnetic field patterns. We will look, for example, for the effects of the interplanetary current sheet, the influence of magnetic clouds which are thought to contain large magnetic loops with both ends connected to the sun (a large departure from the Parker spiral), and also whether particle propagation can be disrupted by the presence of interplanetary shocks. Reference: Richardson et al., <span class="hlt">Solar</span> Phys. 289, 3059, 2014</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015APS..DPP.M9004E','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015APS..DPP.M9004E"><span>Magnetic pumping of the <span class="hlt">solar</span> wind</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Egedal, Jan; Lichko, Emily; Daughton, William</p> <p>2015-11-01</p> <p>The transport of matter and radiation in the <span class="hlt">solar</span> wind and terrestrial magnetosphere is a complicated problem involving competing processes of charged particles interacting with electric and magnetic fields. Given the rapid expansion of the <span class="hlt">solar</span> wind, it would be expected that superthermal electrons originating in the corona would cool rapidly as a function of distance to the Sun. However, this is not <span class="hlt">observed</span>, and various models have been proposed as candidates for heating the <span class="hlt">solar</span> wind. In the compressional pumping mechanism explored by Fisk and Gloeckler particles are accelerated by random compressions by the interplanetary wave turbulence. This theory explores diffusion due to spatial non-uniformities and provides a mechanism for redistributing particle. For investigation of a related but different heating mechanism, magnetic pumping, in our work we include diffusion of anisotropic features that develops in velocity space. The mechanism allows energy to be transferred to the particles directly from the turbulence. Guided by kinetic simulations a theory is derived for magnetic pumping. At the heart of this work is a generalization of the Parker Equation to <span class="hlt">capture</span> the role of the pressure anisotropy during the pumping process. Supported by NASA grant NNX15AJ73G.</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://hdl.handle.net/2060/19790022944','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19790022944"><span>The shape and location of the sector boundary surface in the inner <span class="hlt">solar</span> system. [Helios <span class="hlt">observations</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Villante, U.; Bruno, R.; Mariani, F.; Burlaga, L. F.; Ness, N. F.</p> <p>1979-01-01</p> <p>Simultaneous <span class="hlt">observations</span> by Helios-1 and Helios-2 over four <span class="hlt">solar</span> rotations were used to determine the latitudinal dependence of the polarity of the interplanetary magnetic field within plus or minus 7.23 deg of the <span class="hlt">solar</span> equator and within 1 AU. The longitudinal and latitudinal positions of the sector boundary crossing are consistent with a warped sector boundary which extended from the sun to 1 AU and was inclined approximately 10 deg with respect to the heliographic equator. This is consistent with simultaneous Pioneer 11 <span class="hlt">observations</span>, which showed unipolar fields at latitude approximately 16 deg at heliocentric distances greater than 3.5 AU. Two sectors were <span class="hlt">observed</span> at southern latitudes; however, four sectors were <span class="hlt">observed</span> at northern latitudes on two rotations, indicating a distortion from planarity of the sectory boundary surface.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMSH43C..01S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMSH43C..01S"><span>Multi-wavelength <span class="hlt">Observations</span> and Modeling of <span class="hlt">Solar</span> Flares: Magnetic Structures</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Su, Y.</p> <p>2017-12-01</p> <p>We present a review of our recent investigations on multi-wavelength <span class="hlt">observations</span> and magnetic field modeling of <span class="hlt">solar</span> flares. High-resolution <span class="hlt">observations</span> taken by NVST and BBSO/NST reveal unprecedented fine structures of the flaring regions. <span class="hlt">Observations</span> by SDO, IRIS, and GOES provide the complementary information. The magnetic field models are constructed using either non-linear force free field extrapolations or flux rope insertion method. Our studies have shown that the flaring regions often consist of double or multiple flux ropes, which often exist at different heights. The fine flare ribbon structures may be due to the magnetic reconnection in the complex quasi separatrix layers. The magnetic field modeling of several large flares suggests that the so called hot-channel structure is corresponding to the erupting flux rope above the X-point in a magnetic configuration with Hyperbolic Flux Tube.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22654348-stereoscopic-observation-slipping-reconnection-double-candle-flame-shaped-solar-flare','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22654348-stereoscopic-observation-slipping-reconnection-double-candle-flame-shaped-solar-flare"><span>STEREOSCOPIC <span class="hlt">OBSERVATION</span> OF SLIPPING RECONNECTION IN A DOUBLE CANDLE-FLAME-SHAPED <span class="hlt">SOLAR</span> FLARE</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>Gou, Tingyu; Liu, Rui; Wang, Yuming</p> <p>2016-04-20</p> <p>The 2011 January 28 M1.4 flare exhibits two side-by-side candle-flame-shaped flare loop systems underneath a larger cusp-shaped structure during the decay phase, as <span class="hlt">observed</span> at the northwestern <span class="hlt">solar</span> limb by the <span class="hlt">Solar</span> Dynamics Observatory . The northern loop system brightens following the initiation of the flare within the southern loop system, but all three cusp-shaped structures are characterized by ∼10 MK temperatures, hotter than the arch-shaped loops underneath. The “Ahead” satellite of the <span class="hlt">Solar</span> Terrestrial Relations Observatory provides a top view, in which the post-flare loops brighten sequentially, with one end fixed while the other apparently slipping eastward. By performingmore » stereoscopic reconstruction of the post-flare loops in EUV and mapping out magnetic connectivities, we found that the footpoints of the post-flare loops are slipping along the footprint of a hyperbolic flux tube (HFT) separating the two loop systems and that the reconstructed loops share similarity with the magnetic field lines that are traced starting from the same HFT footprint, where the field lines are relatively flexible. These results argue strongly in favor of slipping magnetic reconnection at the HFT. The slipping reconnection was likely triggered by the flare and manifested as propagative dimmings before the loop slippage is <span class="hlt">observed</span>. It may contribute to the late-phase peak in Fe xvi 33.5 nm, which is even higher than its main-phase counterpart, and may also play a role in the density and temperature asymmetry <span class="hlt">observed</span> in the northern loop system through heat conduction.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014ApJ...792L..40S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014ApJ...792L..40S"><span>Direct <span class="hlt">Observations</span> of Magnetic Flux Rope Formation during a <span class="hlt">Solar</span> Coronal Mass Ejection</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Song, H. Q.; Zhang, J.; Chen, Y.; Cheng, X.</p> <p>2014-09-01</p> <p>Coronal mass ejections (CMEs) are the most spectacular eruptive phenomena in the <span class="hlt">solar</span> atmosphere. It is generally accepted that CMEs are the results of eruptions of magnetic flux ropes (MFRs). However, there is heated debate on whether MFRs exist prior to the eruptions or if they are formed during the eruptions. Several coronal signatures, e.g., filaments, coronal cavities, sigmoid structures, and hot channels (or hot blobs), are proposed as MFRs and <span class="hlt">observed</span> before the eruption, which support the pre-existing MFR scenario. There is almost no reported <span class="hlt">observation</span> of MFR formation during the eruption. In this Letter, we present an intriguing <span class="hlt">observation</span> of a <span class="hlt">solar</span> eruptive event that occurred on 2013 November 21 with the Atmospheric Imaging Assembly on board the <span class="hlt">Solar</span> Dynamic Observatory, which shows the formation process of the MFR during the eruption in detail. The process began with the expansion of a low-lying coronal arcade, possibly caused by the flare magnetic reconnection underneath. The newly formed ascending loops from below further pushed the arcade upward, stretching the surrounding magnetic field. The arcade and stretched magnetic field lines then curved in just below the arcade vertex, forming an X-point. The field lines near the X-point continued to approach each other and a second magnetic reconnection was induced. It is this high-lying magnetic reconnection that led to the formation and eruption of a hot blob (~10 MK), presumably an MFR, producing a CME. We suggest that two spatially separated magnetic reconnections occurred in this event, which were responsible for producing the flare and the hot blob (CME).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFMSH43B4203S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFMSH43B4203S"><span>Direct <span class="hlt">Observations</span> of Magnetic Flux Rope Formation during a <span class="hlt">Solar</span> Coronal Mass Ejection</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Song, H.; Zhang, J.; Chen, Y.; Cheng, X.</p> <p>2014-12-01</p> <p>Coronal mass ejections (CMEs) are the most spectacular eruptive phenomena in the <span class="hlt">solar</span> atmosphere. It is generally accepted that CMEs are results of eruptions of magnetic flux ropes (MFRs). However, a heated debate is on whether MFRs pre-exist before the eruptions or they are formed during the eruptions. Several coronal signatures, e.g., filaments, coronal cavities, sigmoid structures and hot channels (or hot blobs), are proposed as MFRs and <span class="hlt">observed</span> before the eruption, which support the pre existing MFR scenario. There is almost no reported <span class="hlt">observation</span> about MFR formation during the eruption. In this presentation, we present an intriguing <span class="hlt">observation</span> of a <span class="hlt">solar</span> eruptive event with the Atmospheric Imaging Assembly on board the <span class="hlt">Solar</span> Dynamic Observatory, which shows a detailed formation process of the MFR during the eruption. The process started with the expansion of a low lying coronal arcade, possibly caused by the flare magnetic reconnection underneath. The newly-formed ascending loops from below further pushed the arcade upward, stretching the surrounding magnetic field. The arcade and stretched magnetic field lines then curved-in just below the arcade vertex, forming an X-point. The field lines near the X-point continued to approach each other and a second magnetic reconnection was induced. It is this high-lying magnetic reconnection that led to the formation and eruption of a hot blob (~ 10 MK), presumably a MFR, producing a CME. We suggest that two spatially-separated magnetic reconnections occurred in this event, responsible for producing the flare and the hot blob (CME), respectively.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JSWSC...8A...4R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JSWSC...8A...4R"><span>Two <span class="hlt">solar</span> proton fluence models based on ground level enhancement <span class="hlt">observations</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Raukunen, Osku; Vainio, Rami; Tylka, Allan J.; Dietrich, William F.; Jiggens, Piers; Heynderickx, Daniel; Dierckxsens, Mark; Crosby, Norma; Ganse, Urs; Siipola, Robert</p> <p>2018-01-01</p> <p><span class="hlt">Solar</span> energetic particles (SEPs) constitute an important component of the radiation environment in interplanetary space. Accurate modeling of SEP events is crucial for the mitigation of radiation hazards in spacecraft design. In this study we present two new statistical models of high energy <span class="hlt">solar</span> proton fluences based on ground level enhancement (GLE) <span class="hlt">observations</span> during <span class="hlt">solar</span> cycles 19-24. As the basis of our modeling, we utilize a four parameter double power law function (known as the Band function) fits to integral GLE fluence spectra in rigidity. In the first model, the integral and differential fluences for protons with energies between 10 MeV and 1 GeV are calculated using the fits, and the distributions of the fluences at certain energies are modeled with an exponentially cut-off power law function. In the second model, we use a more advanced methodology: by investigating the distributions and relationships of the spectral fit parameters we find that they can be modeled as two independent and two dependent variables. Therefore, instead of modeling the fluences separately at different energies, we can model the shape of the fluence spectrum. We present examples of modeling results and show that the two methodologies agree well except for a short mission duration (1 year) at low confidence level. We also show that there is a reasonable agreement between our models and three well-known <span class="hlt">solar</span> proton models (JPL, ESP and SEPEM), despite the differences in both the modeling methodologies and the data used to construct the models.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMIN43D..04F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMIN43D..04F"><span>Enhancing the Value of Sensor-based <span class="hlt">Observations</span> by <span class="hlt">Capturing</span> the Knowledge of How An <span class="hlt">Observation</span> Came to Be</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Fredericks, J.; Rueda-Velasquez, C. A.</p> <p>2016-12-01</p> <p>As we move from keeping data on our disks to sharing it with the world, often in real-time, we are obligated to also tell an unknown user about how our <span class="hlt">observations</span> were made. Data that are shared must not only have ownership metadata, unit descriptions and content formatting information. The provider must also share information that is needed to assess the data as it relates to potential re-use. A user must be able to assess the limitations and capabilities of the sensor, as it is configured, to understand its value. For example, when an instrument is configured, it typically affects the data accuracy and operational limits of the sensor. An operator may sacrifice data accuracy to achieve a broader operational range and visa versa. If you are looking at newly discovered data, it is important to be able to find all of the information that relates to assessing the data quality for your particular application. Traditionally, metadata are <span class="hlt">captured</span> by data managers who usually do not know how the data are collected. By the time data are distributed, this knowledge is often gone, buried within notebooks or hidden in documents that are not machine-harvestable and often not human-readable. In a recently funded NSF EarthCube Integrative Activity called X-DOMES (Cross-Domain <span class="hlt">Observational</span> Metadata in EnviroSensing), mechanisms are underway to enable the <span class="hlt">capture</span> of sensor and deployment metadata by sensor manufacturers and field operators. The support has enabled the development of a community ontology repository (COR) within the Earth Science Information Partnership (ESIP) community, fostering easy creation of resolvable terms for the broader community. This tool enables non-experts to easily develop W3C standards-based content, promoting the implementation of Semantic Web technologies for enhanced discovery of content and interoperability in workflows. The X-DOMES project is also developing a SensorML Viewer/Editor to provide an easy interface for sensor manufacturers and</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24676389','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24676389"><span>Video surveillance <span class="hlt">captures</span> student hand hygiene behavior, reactivity to <span class="hlt">observation</span>, and peer influence in Kenyan primary schools.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Pickering, Amy J; Blum, Annalise G; Breiman, Robert F; Ram, Pavani K; Davis, Jennifer</p> <p>2014-01-01</p> <p>In-person structured <span class="hlt">observation</span> is considered the best approach for measuring hand hygiene behavior, yet is expensive, time consuming, and may alter behavior. Video surveillance could be a useful tool for objectively monitoring hand hygiene behavior if validated against current methods. Student hand cleaning behavior was monitored with video surveillance and in-person structured <span class="hlt">observation</span>, both simultaneously and separately, at four primary schools in urban Kenya over a study period of 8 weeks. Video surveillance and in-person <span class="hlt">observation</span> <span class="hlt">captured</span> similar rates of hand cleaning (absolute difference <5%, p = 0.74). Video surveillance documented higher hand cleaning rates (71%) when at least one other person was present at the hand cleaning station, compared to when a student was alone (48%; rate ratio  = 1.14 [95% CI 1.01-1.28]). Students increased hand cleaning rates during simultaneous video and in-person monitoring as compared to single-method monitoring, suggesting reactivity to each method of monitoring. This trend was documented at schools receiving a handwashing with soap intervention, but not at schools receiving a sanitizer intervention. Video surveillance of hand hygiene behavior yields results comparable to in-person <span class="hlt">observation</span> among schools in a resource-constrained setting. Video surveillance also has certain advantages over in-person <span class="hlt">observation</span>, including rapid data processing and the capability to <span class="hlt">capture</span> new behavioral insights. Peer influence can significantly improve student hand cleaning behavior and, when possible, should be exploited in the design and implementation of school hand hygiene programs.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/21665982','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/21665982"><span>Determination of inadvertent atrial <span class="hlt">capture</span> during para-Hisian pacing.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Obeyesekere, Manoj; Leong-Sit, Peter; Skanes, Allan; Krahn, Andrew; Yee, Raymond; Gula, Lorne J; Bennett, Matthew; Klein, George J</p> <p>2011-08-01</p> <p>Inadvertent <span class="hlt">capture</span> of the atrium will lead to spurious results during para-Hisian pacing. We sought to establish whether the stimulation-to-atrial electrogram interval at the proximal coronary sinus (stim-PCS) or high right atrium (stim-HRA) could signal inadvertent atrial <span class="hlt">capture</span>. Para-Hisian pacing with and without intentional atrial <span class="hlt">capture</span> was performed in 31 patients. Stim-HRA and stim-PCS intervals were measured with atrial <span class="hlt">capture</span>, His plus para-Hisian ventricular (H+V) <span class="hlt">capture</span>, and para-Hisian ventricular (V) <span class="hlt">capture</span> alone. The mean stim-HRA interval was significantly shorter with atrial <span class="hlt">capture</span> (66 ± 18 ms) than with H+V (121 ± 27 ms, P < 0.001) or V <span class="hlt">capture</span> alone (174 ± 38 ms, P < 0.001). The mean stim-PCS interval was significantly shorter with atrial <span class="hlt">capture</span> (51 ± 16 ms) than with H+V (92 ± 22 ms, P<0.001) or V <span class="hlt">capture</span> alone (146 ± 33 ms, P < 0.001). A stim-PCS < 60 ms (stim-HRA < 70 ms) was <span class="hlt">observed</span> only with atrial <span class="hlt">capture</span>. A stim-PCS >90 ms (stim-HRA >100 ms) was <span class="hlt">observed</span> only in the absence of atrial <span class="hlt">capture</span>. A stim-HRA of < 85 ms was highly specific and stim-PCS of < 85 ms highly sensitive at identifying atrial <span class="hlt">capture</span>. Stim-HRA intervals of 75 to 97 ms and stim-PCS intervals of 65 to 88 ms were <span class="hlt">observed</span> with either atrial, His, or para-Hisian ventricular <span class="hlt">capture</span> without atrial <span class="hlt">capture</span>. In this overlap zone, all patients demonstrated a stim-PCS or stim-HRA interval prolongation of at least 20 ms when the catheter was advanced to avoid deliberate atrial pacing. The QRS morphology was of limited value in distinguishing atrial <span class="hlt">capture</span> due to concurrent ventricular or H+V <span class="hlt">capture</span>, as <span class="hlt">observed</span> in 20 of 31 (65%) patients. Stim-PCS and stim-HRA intervals can be used to monitor for inadvertent atrial <span class="hlt">capture</span> during para-Hisian pacing. A stim-PCS < 60 ms (or stim-HRA < 70 ms) and stim-PCS > 90 ms (or stim-HRA > 100 ms) were <span class="hlt">observed</span> only with and without atrial <span class="hlt">capture</span>, respectively, but there was significant overlap between these values. Deliberate</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015PhPro..74..274T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015PhPro..74..274T"><span>About 3He Ions Predominant Acceleration During the January 20, 2005 <span class="hlt">Solar</span> Flare</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Troitskaya, E. V.; Arkhangelskaja, I. V.; Arkhangelskiy, A. I.</p> <p></p> <p>We have studied some properties of the powerful <span class="hlt">solar</span> flare of January 20, 2005 by methods of nuclear lines analysis. The results of temporal profiles investigation in corresponding to neutron <span class="hlt">capture</span> energy bands allow the supposition about predominant acceleration of 3He ions in the corona, their subsequent propagation to the low chromosphere and the photosphere where the area of 2.223 MeV γ-line effective productions is located. The characteristics of accelerated 3He ions propagation processes and the basic explanation of <span class="hlt">observable</span> properties of this <span class="hlt">solar</span> flare due to the variations of 3He content are discussed in the presented article.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19820009149','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19820009149"><span><span class="hlt">Observed</span> variability in the Fraunhofer line spectrum of <span class="hlt">solar</span> flux, 1975 - 1980</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Livingston, W.; Holweger, H.; White, O. R.</p> <p>1981-01-01</p> <p>Over the five years double-pass spectrometer <span class="hlt">observations</span> of the Sun-as-a-star revealed significant changes in line intensities. The photospheric component weakened linearly with time 0 to 2.3%. From a lack of correlation between these line weakenings and <span class="hlt">solar</span> activity indicators like sunspots and plage, a global variation of surface properties is inferred. Model-atmosphere analysis suggests a slight reduction in the lower-photospheric temperature gradient corresponding to a 15% increase in the mixing length within the granulation layer. Chromospheric lines such as Ca II H and K, Ca II 8543 and the CN band head weaken synchronously with <span class="hlt">solar</span> activity. Thus, the behavior of photospheric and chromospheric lines is markedly different, with the possibility of secular change for the former.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/21169574','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/21169574"><span>Attentional <span class="hlt">capture</span> under high perceptual load.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Cosman, Joshua D; Vecera, Shaun P</p> <p>2010-12-01</p> <p>Attentional <span class="hlt">capture</span> by abrupt onsets can be modulated by several factors, including the complexity, or perceptual load, of a scene. We have recently demonstrated that <span class="hlt">observers</span> are less likely to be <span class="hlt">captured</span> by abruptly appearing, task-irrelevant stimuli when they perform a search that is high, as opposed to low, in perceptual load (Cosman & Vecera, 2009), consistent with perceptual load theory. However, recent results indicate that onset frequency can influence stimulus-driven <span class="hlt">capture</span>, with infrequent onsets <span class="hlt">capturing</span> attention more often than did frequent onsets. Importantly, in our previous task, an abrupt onset was present on every trial, and consequently, attentional <span class="hlt">capture</span> might have been affected by both onset frequency and perceptual load. In the present experiment, we examined whether onset frequency influences attentional <span class="hlt">capture</span> under conditions of high perceptual load. When onsets were presented frequently, we replicated our earlier results; attentional <span class="hlt">capture</span> by onsets was modulated under conditions of high perceptual load. Importantly, however, when onsets were presented infrequently, we <span class="hlt">observed</span> robust <span class="hlt">capture</span> effects. These results conflict with a strong form of load theory and, instead, suggest that exposure to the elements of a task (e.g., abrupt onsets) combines with high perceptual load to modulate attentional <span class="hlt">capture</span> by task-irrelevant information.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19800060994&hterms=thermal+noise&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dthermal%2Bnoise','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19800060994&hterms=thermal+noise&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dthermal%2Bnoise"><span>The low-frequency continuum as <span class="hlt">observed</span> in the <span class="hlt">solar</span> wind from ISEE 3 - Thermal electrostatic noise</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Hoang, S.; Steinberg, J.-L.; Epstein, G.; Tilloles, P.; Fainberg, J.; Stone, R. G.</p> <p>1980-01-01</p> <p>The low frequency continuum (LFC) noise between 30 and 200 kHz has been investigated from the ISEE 3 spacecraft in the <span class="hlt">solar</span> wind by means of a radio astronomy experiment more sensitive than previously available. It is demonstrated that the LFC radiation <span class="hlt">observed</span> in the <span class="hlt">solar</span> wind is in the form of longitudinal plasma waves rather than transverse electromagnetic waves. The <span class="hlt">observed</span> spectral characteristics are found to be a function of antenna length. In addition, both the absence of antenna spin modulation and the fact that these plasma waves do not propagate to large distances imply a local origin for the LFC.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20050182112','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20050182112"><span><span class="hlt">Solar</span> System <span class="hlt">Observations</span> with Spitzer Space Telescope: Preliminary Results</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Cruikshank, Dale P.</p> <p>2005-01-01</p> <p>The programs of <span class="hlt">observations</span> of <span class="hlt">Solar</span> System bodies conducted in the first year of the operation of the Spitzer Space Telescope as part of the Guaranteed <span class="hlt">Observing</span> Time allocations are described. Initial results include the determination of the albedos of a number of Kuiper Belt objects and Centaurs from <span class="hlt">observations</span> of their flux densities at 24 and 70 microns, and the detection of emission bands in the spectra of several distant asteroids (Trojans) around 10 and 25 microns. The 10 Kuiper Belt objects <span class="hlt">observed</span> to date have albedos in the range 0.08 - 0.15, significantly higher than the earlier estimated 0.04. An additional KBO [(55565) 2002 AW(sub l97)] has an albedo of 0.17 plus or minus 0.03. The emission bands in the asteroid spectra are indicative of silicates, but specific minerals have not yet been identified. The Centaur/comet 29P/Schwassmann-Wachmann 1 has a nucleus surface albedo of 0.025 plus or minus 0.01, and its dust production rate was calculated from the properties of the coma. Several other investigations are in progress as the incoming data are processed and analyzed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20170004957&hterms=K2&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3DK2','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20170004957&hterms=K2&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3DK2"><span>A Distant Mirror: <span class="hlt">Solar</span> Oscillations <span class="hlt">Observed</span> on Neptune by the Kepler K2 Mission</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Gaulme, P.; Rowe, J. F.; Bedding, T. R.; Benomar, O.; Corsaro, E.; Davies, G. R.; Hale, S. J.; Howe, R.; Garcia, R. A.; Huber, D.; <a style="text-decoration: none; " href="javascript:void(0); " onClick="displayelement('author_20170004957'); toggleEditAbsImage('author_20170004957_show'); toggleEditAbsImage('author_20170004957_hide'); "> <img style="display:inline; width:12px; height:12px; " src="images/arrow-up.gif" width="12" height="12" border="0" alt="hide" id="author_20170004957_show"> <img style="width:12px; height:12px; display:none; " src="images/arrow-down.gif" width="12" height="12" border="0" alt="hide" id="author_20170004957_hide"></p> <p>2016-01-01</p> <p>Starting in 2014 December, Kepler (K2) <span class="hlt">observed</span> Neptune continuously for 49 days at a 1-minute cadence. The goals consisted of studying its atmospheric dynamics, detecting its global acoustic oscillations, and those of the Sun, which we report on here. We present the first indirect detection of <span class="hlt">solar</span> oscillations in intensity measurements. Beyond the remarkable technical performance, it indicates how Kepler would see a star like the Sun. The result from the global asteroseismic approach, which consists of measuring the oscillation frequency at maximum amplitude max velocity and the mean frequency separation between mode overtones delta velocity, is surprising as the max velocity measured from Neptune photometry is larger than the accepted value. Compared to the usual reference max velocity of the sun equal to 3100 microhertz, the asteroseismic scaling relations therefore make the <span class="hlt">solar</span> mass and radius appear larger by 13.8 plus or minus 5.8 percent and 4.3 plus or minus 1.9 percent, respectively. The higher max velocity is caused by a combination of the value of max velocity of the sun, being larger at the time of <span class="hlt">observations</span> than the usual reference from SOHO/VIRGO/SPM (Variability of <span class="hlt">solar</span> IRradiance and Gravity Oscillations / on board SOHO (<span class="hlt">Solar</span> and Heliospheric Observatory) / Sun PhotoMeters) data (3160 plus or minus 10 microhertz), and the noise level of the K2 time series, being 10 times larger than VIRGO's. The peak-bagging method provides more consistent results: despite a low signal-to-noise ratio (S/N), we model 10 overtones for degrees iota equal 0, 1, 2. We compare the K2 data with simultaneous SOHO/VIRGO/SPM photometry and Bison (Birmingham <span class="hlt">Solar</span>-Oscillations Network) velocity measurements. The individual frequencies, widths, and amplitudes mostly match those from VIRGO and BiSON within 1 sigma, except for the few peaks with the lowest S/N.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26502060','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26502060"><span>Tandem <span class="hlt">Solar</span> Cells Using GaAs Nanowires on Si: Design, Fabrication, and <span class="hlt">Observation</span> of Voltage Addition.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Yao, Maoqing; Cong, Sen; Arab, Shermin; Huang, Ningfeng; Povinelli, Michelle L; Cronin, Stephen B; Dapkus, P Daniel; Zhou, Chongwu</p> <p>2015-11-11</p> <p>Multijunction <span class="hlt">solar</span> cells provide us a viable approach to achieve efficiencies higher than the Shockley-Queisser limit. Due to their unique optical, electrical, and crystallographic features, semiconductor nanowires are good candidates to achieve monolithic integration of <span class="hlt">solar</span> cell materials that are not lattice-matched. Here, we report the first realization of nanowire-on-Si tandem cells with the <span class="hlt">observation</span> of voltage addition of the GaAs nanowire top cell and the Si bottom cell with an open circuit voltage of 0.956 V and an efficiency of 11.4%. Our simulation showed that the current-matching condition plays an important role in the overall efficiency. Furthermore, we characterized GaAs nanowire arrays grown on lattice-mismatched Si substrates and estimated the carrier density using photoluminescence. A low-resistance connecting junction was obtained using n(+)-GaAs/p(+)-Si heterojunction. Finally, we demonstrated tandem <span class="hlt">solar</span> cells based on top GaAs nanowire array <span class="hlt">solar</span> cells grown on bottom planar Si <span class="hlt">solar</span> cells. The reported nanowire-on-Si tandem cell opens up great opportunities for high-efficiency, low-cost multijunction <span class="hlt">solar</span> cells.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFMSM43A..07E','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFMSM43A..07E"><span>Sub-<span class="hlt">solar</span> Magnetopause <span class="hlt">Observation</span> and Simulation of a Tripolar Guide-Magnetic Field Perturbation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Eriksson, S.; Cassak, P.; Retino, A.; Mozer, F.</p> <p>2015-12-01</p> <p>The Polar satellite recorded two reconnection exhausts within 6 min on 1 April 2001 at a rather symmetric sub-<span class="hlt">solar</span> magnetopause that displayed different out-of-plane signatures for similar <span class="hlt">solar</span> wind conditions. The first case was reported by Mozer et al. [2002] and displayed a bipolar guide field supporting a quadrupole Hall field consistent with a single X-line. The second case, however, shows the first known example of a tripolar guide-field perturbation at Earth's magnetopause reminiscent of the types of <span class="hlt">solar</span> wind exhausts that Eriksson et al. [2014; 2015] have reported to be in agreement with multiple X-lines. A dedicated particle-in-cell simulation is performed for the prevailing conditions across the magnetopause. We propose an explanation in terms of asymmetric Hall magnetic fields due to a presence of a magnetic island between two X-lines, and discuss how higher resolution MMS <span class="hlt">observations</span> can be used to further study this problem at the magnetopause.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19810038514&hterms=1587&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3D%2526%25231587','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19810038514&hterms=1587&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3D%2526%25231587"><span>Latitude dependence of <span class="hlt">solar</span> wind velocity <span class="hlt">observed</span> at not less than 1 AU</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Mitchell, D. G.; Roelof, E. C.; Wolfe, J. H.</p> <p>1981-01-01</p> <p>The large-scale <span class="hlt">solar</span> wind velocity structure in the outer heliosphere has been systematically analyzed for Carrington rotations 1587-1541 (March 1972 to April 1976). Spacecraft data were taken from Imp 7/8 at earth, Pioneer 6, 8, and 9 near 1 AU, and Pioneer 10 and 11 between 1.6 and 5 AU. Using the constant radial velocity <span class="hlt">solar</span> wind approximation to map all of the velocity data to its high coronal emission heliolongitude, the velocity structure <span class="hlt">observed</span> at different spacecraft was examined for latitudinal dependence and compared with coronal structure in soft X-rays and H-alpha absorption features. The constant radial velocity approximation usually remains self-consistent in decreasing or constant velocity <span class="hlt">solar</span> wind out to 5 AU, enabling us to separate radial from latitudinal propagation effects. Several examples of sharp nonmeridional stream boundaries in interplanetary space (about 5 deg latitude in width), often directly associated with features in coronal X-rays and H-alpha were found.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5159890','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5159890"><span><span class="hlt">Observation</span> of a reversal of rotation in a sunspot during a <span class="hlt">solar</span> flare</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Bi, Yi; Jiang, Yunchun; Yang, Jiayan; Hong, Junchao; Li, Haidong; Yang, Bo; Xu, Zhe</p> <p>2016-01-01</p> <p>The abrupt motion of the photospheric flux during a <span class="hlt">solar</span> flare is thought to be a back reaction caused by the coronal field reconfiguration. However, the type of motion pattern and the physical mechanism responsible for the back reaction has been uncertain. Here we show that the direction of a sunspot's rotation is reversed during an X1.6 flare using <span class="hlt">observations</span> from the Helioseismic and Magnetic Imager. A magnetic field extrapolation model shows that the corresponding coronal magnetic field shrinks with increasing magnetic twist density. This suggests that the abrupt reversal of rotation in the sunspot may be driven by a Lorentz torque that is produced by the gradient of twist density from the <span class="hlt">solar</span> corona to the <span class="hlt">solar</span> interior. These results support the view that the abrupt reversal in the rotation of the sunspot is a dynamic process responding to shrinkage of the coronal magnetic field during the flare. PMID:27958266</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017ApJ...848...84A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017ApJ...848...84A"><span>Dynamics of Large-scale Coronal Structures as Imaged during the 2012 and 2013 Total <span class="hlt">Solar</span> Eclipses</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Alzate, Nathalia; Habbal, Shadia R.; Druckmüller, Miloslav; Emmanouilidis, Constantinos; Morgan, Huw</p> <p>2017-10-01</p> <p>White light images acquired at the peak of <span class="hlt">solar</span> activity cycle 24, during the total <span class="hlt">solar</span> eclipses of 2012 November 13 and 2013 November 3, serendipitously <span class="hlt">captured</span> erupting prominences accompanied by CMEs. Application of state-of-the-art image processing techniques revealed the intricate details of two “atypical” large-scale structures, with strikingly sharp boundaries. By complementing the processed white light eclipse images with processed images from co-temporal <span class="hlt">Solar</span> Dynamics Observatory/AIA and SOHO/LASCO <span class="hlt">observations</span>, we show how the shape of these atypical structures matches the shape of faint CME shock fronts, which traversed the inner corona a few hours prior to the eclipse <span class="hlt">observations</span>. The two events were not associated with any prominence eruption but were triggered by sudden brightening events on the <span class="hlt">solar</span> surface accompanied by sprays and jets. The discovery of the indelible impact that frequent and innocuous transient events in the low corona can have on large-scale coronal structures was enabled by the radial span of the high-resolution white light eclipse images, starting from the <span class="hlt">solar</span> surface out to several <span class="hlt">solar</span> radii, currently unmatched by any coronagraphic instrumentation. These findings raise the interesting question as to whether large-scale coronal structures can ever be considered stationary. They also point to the existence of a much larger number of CMEs that goes undetected from the suite of instrumentation currently <span class="hlt">observing</span> the Sun.</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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