Quality, Quantity, And Surprise! Trade-Offs In X-Raser ASAT Attrition
NASA Astrophysics Data System (ADS)
Callaham, Michael B.; Scibilia, Frank M.
1984-08-01
In order to characterize the effects of technological superiority, numerical superiority, and pre-emption on space battle outcomes, we have constructed a battle simulation in which "Red" and "Blue" ASATs, each armed with a specified number of x-ray lasers of specified range, move along specified orbits and fire on one another according to a pair of battle management algorithms. The simulated battle proceeds until apparent steady-state force levels are reached. Battle outcomes are characterized by terminal force ratio and by terminal force-exchange ratio as effective weapon range, multiplicity (x-rasers per ASAT), and pre-emptive role are varied parametrically. A major conclusion is that pre-emptive advantage increases with increasing x-raser range and multiplicity (x-rasers per ASAT) and with increasing force size. That is, the "use 'em or lose 'em" dilemma will become more stark as such weapons are refined and proliferated.
Para-hydrogen raser delivers sub-millihertz resolution in nuclear magnetic resonance
NASA Astrophysics Data System (ADS)
Suefke, Martin; Lehmkuhl, Sören; Liebisch, Alexander; Blümich, Bernhard; Appelt, Stephan
2017-06-01
The precision of nuclear magnetic resonance spectroscopy (NMR) is limited by the signal-to-noise ratio, the measurement time Tm and the linewidth Δν = 1/(πT2). Overcoming the T 2 limit is possible if the nuclear spins of a molecule emit continuous radio waves. Lasers and masers are self-organized systems which emit coherent radiation in the optical and micro-wave regime. Both are based on creating a population inversion of specific energy states. Here we show continuous oscillations of proton spins of organic molecules in the radiofrequency regime (raser). We achieve this by coupling a population inversion created through signal amplification by reversible exchange (SABRE) to a high-quality-factor resonator. For the case of 15N labelled molecules, we observe multi-mode raser activity, which reports different spin quantum states. The corresponding 1H-15N J-coupled NMR spectra exhibit unprecedented sub-millihertz resolution and can be explained assuming two-spin ordered quantum states. Our findings demonstrate a substantial improvement in the frequency resolution of NMR.
2009-04-01
ii-iii. 50 Rumsfeld, ―Nuclear Posture Review Report: Forward.‖ 51 DOD, ―Findings of the Nuclear Posture Review,‖ 9. 52 Pilat , ―The end of the...28 Pilat , Joseph F. ―The end of the NPT regime?‖ International Affairs 83:3 (2007): 469-482. Raser, John R. ―Deterrence Research: Past
Noise Measurements of the VAIIPR Fan
NASA Technical Reports Server (NTRS)
Mendoza, Jeff; Weir, Don
2012-01-01
This final report has been prepared by Honeywell Aerospace, Phoenix, Arizona, a unit of Honeywell International, Inc., documenting work performed during the period September 2004 through November 2005 for the National Aeronautics and Space Administration (NASA) Glenn Research Center, Cleveland, Ohio, under the Revolutionary Aero-Space Engine Research (RASER) Program, Contract No. NAS3- 01136, Task Order 6, Noise Measurements of the VAIIPR Fan. The NASA Task Manager was Dr. Joe Grady, NASA Glenn Research Center, Mail Code 60-6, Cleveland, Ohio 44135. The NASA Contract Officer was Mr. Albert Spence, NASA Glenn Research Center, Mail Code 60-6, Cleveland, Ohio 44135. This report focuses on the evaluation of internal fan noise as generated from various inflow disturbances based on measurements made from a circumferential array of sensors located near the fan and sensors upstream of a serpentine inlet.
Fuel Cell Auxiliary Power Study Volume 1: RASER Task Order 5
NASA Technical Reports Server (NTRS)
Mak, Audie; Meier, John
2007-01-01
This study evaluated the feasibility of a hybrid solid oxide fuel cell (SOFC) auxiliary power unit (APU) and the impact in a 90-passenger More-Electric Regional Jet application. The study established realistic hybrid SOFC APU system weight and system efficiencies, and evaluated the impact on the aircraft total weight, fuel burn, and emissions from the main engine and the APU during cruise, landing and take-off (LTO) cycle, and at the gate. Although the SOFC APU may be heavier than the current conventional APU, its weight disadvantage can be offset by fuel savings in the higher SOFC APU system efficiencies against the main engine bleed and extraction during cruise. The higher SOFC APU system efficiency compared to the conventional APU on the ground can also provide considerable fuel saving and emissions reduction, particularly at the gate, but is limited by the fuel cell stack thermal fatigue characteristic.
Coronary Intervention with the Excimer Laser: Review of the Technology and Outcome Data
Rawlins, John; Din, Jehangir N; Talwar, Suneel
2016-01-01
Excimer laser coronary atherectomy (ELCA) is a long-established adjunctive therapy that can be applied during percutaneous coronary intervention (PCI). Technical aspects have evolved and there is an established safety and efficacy record across a number of clinical indications in contemporary interventional practice where complex lesions are routinely encountered. The role of ELCA during PCI for thrombus, non-crossable or non-expandable lesions, chronic occlusions and stent under-expansion are discussed in this review. The key advantage of ELCA over alternative atherectomy interventions is delivery on a standard 0.014-inch guidewire. Additionally, the technique can be mastered by any operator after a short period of training. The major limitation is presence of heavy calcification although when rotational atherectomy (RA) is required but cannot be applied due to inability to deliver the dedicated RotaWireTM (Boston Scientific), ELCA can create an upstream channel to permit RotaWire passage and complete the case with RA – the RASER technique. PMID:29588701
Spatial Specificity in Spatiotemporal Encoding and Fourier Imaging
Goerke, Ute
2015-01-01
Purpose Ultrafast imaging techniques based on spatiotemporal-encoding (SPEN), such as RASER (rapid acquisition with sequential excitation and refocusing), is a promising new class of sequences since they are largely insensitive to magnetic field variations which cause signal loss and geometric distortion in EPI. So far, attempts to theoretically describe the point-spread-function (PSF) for the original SPEN-imaging techniques have yielded limited success. To fill this gap a novel definition for an apparent PSF is proposed. Theory Spatial resolution in SPEN-imaging is determined by the spatial phase dispersion imprinted on the acquired signal by a frequency-swept excitation or refocusing pulse. The resulting signal attenuation increases with larger distance from the vertex of the quadratic phase profile. Methods Bloch simulations and experiments were performed to validate theoretical derivations. Results The apparent PSF quantifies the fractional contribution of magnetization to a voxel’s signal as a function of distance to the voxel. In contrast, the conventional PSF represents the signal intensity at various locations. Conclusion The definition of the conventional PSF fails for SPEN-imaging since only the phase of isochromats, but not the amplitude of the signal varies. The concept of the apparent PSF is shown to be generalizable to conventional Fourier- imaging techniques. PMID:26712657
Ultra-efficient Engine Diameter Study
NASA Technical Reports Server (NTRS)
Daggett, David L.; Brown, Stephen T.; Kawai, Ron T.
2003-01-01
Engine fan diameter and Bypass Ratio (BPR) optimization studies have been conducted since the beginning of the turbofan age with the recognition that reducing the engine core jet velocity and increasing fan mass flow rate generally increases propulsive efficiency. However, performance tradeoffs limit the amount of fan flow achievable without reducing airplane efficiency. This study identifies the optimum engine fan diameter and BPR, given the advanced Ultra-Efficient Engine Technology (UEET) powerplant efficiencies, for use on an advanced subsonic airframe. Engine diameter studies have historically focused on specific engine size options, and were limited by existing technology and transportation infrastructure (e.g., ability to fit bare engines through aircraft doors and into cargo holds). This study is unique in defining the optimum fan diameter and drivers for future 2015 (UEET) powerplants while not limiting engine fan diameter by external constraints. This report follows on to a study identifying the system integration issues of UEET engines. This Engine Diameter study was managed by Boeing Phantom Works, Seattle, Washington through the NASA Glenn Revolutionary Aero Space Engine Research (RASER) contract under task order 10. Boeing Phantom Works, Huntington Beach, completed the engine/airplane sizing optimization, while the Boeing Commercial Airplane group (BCA) provided design oversight. A separate subcontract to support the overall project was issued to Tuskegee University.
Engine Validation of Noise and Emission Reduction Technology Phase I
NASA Technical Reports Server (NTRS)
Weir, Don (Editor)
2008-01-01
This final report has been prepared by Honeywell Aerospace, Phoenix, Arizona, a unit of Honeywell International, Inc., documenting work performed during the period December 2004 through August 2007 for the NASA Glenn Research Center, Cleveland, Ohio, under the Revolutionary Aero-Space Engine Research (RASER) Program, Contract No. NAS3-01136, Task Order 8, Engine Validation of Noise and Emission Reduction Technology Phase I. The NASA Task Manager was Dr. Joe Grady of the NASA Glenn Research Center. The NASA Contract Officer was Mr. Albert Spence of the NASA Glenn Research Center. This report is for a test program in which NASA funded engine validations of integrated technologies that reduce aircraft engine noise. These technologies address the reduction of engine fan and jet noise, and noise associated with propulsion/airframe integration. The results of these tests will be used by NASA to identify the engineering tradeoffs associated with the technologies that are needed to enable advanced engine systems to meet stringent goals for the reduction of noise. The objectives of this program are to (1) conduct system engineering and integration efforts to define the engine test-bed configuration; (2) develop selected noise reduction technologies to a technical maturity sufficient to enable engine testing and validation of those technologies in the FY06-07 time frame; (3) conduct engine tests designed to gain insight into the sources, mechanisms and characteristics of noise in the engines; and (4) establish baseline engine noise measurements for subsequent use in the evaluation of noise reduction.
The life RASER and "Okkam's Razor"
NASA Astrophysics Data System (ADS)
Perov, Stanislav P.; Perov, Alexander S.
2013-04-01
A hypothesis of origin of life on the our planet must meet the conditions for well known principles of physics which are summarized in the main principle of the Science - "Okkam`s razor". It is stating: the simplest hypothesis which is accounted for the most facts is most likely to be correct. It must be furthermore attractive and extravagant. Key words: strong non-equilibrium processes, coherent-resonance structures, water plus some chemical elements (H, O, N, Ph, C ...) and resonance system (RASOR see below). The thermodynamic approach to the analysis of irreversible open non-equilibrium systems that interact with electromagnetic radiation is given. The theory of such systems has been created in USSR/Russia in the late twentieth century [2]. It applies to the living and non-living systems as in the macro and micro/nano scales. By entering into system flow of e/m radiation (i.e. absorbed power) and coming out of it, as well as included to the corresponding flow of entropy as well as included in the system of internal energy flow of reagents and out of the products, as well as to relevant incoming and outgoing flow of entropy in our scheme added integration of the external magnetic and electrical fields and gravity factor. In the scheme of power remains outgoing thermal flux and entropy, calculated by the absolute temperature of the system, and the rate of entropy generation in the system (by Ilya Prigozhin). R3+1AS3OR3 (Resonance (1/usual, 2/parametric, 3/stochastic/ 4/diversity) Amplification Stimulated (Stochastically and Synergetically ) by Outside (External) Radiation (1/electromagnetic, 2/corpuscular, 3/gravitational) [3]. Such RASOR arises very often when any comet enters an atmosphere of a planet. And forms shock layer before ice surface of the comet body. For explanation of chirality of arises life structures we use idea of gashydrats in [4] REFERENCES: 1. Chukova Yu.P. The Weber-Fechner Law.- Moscow.-2009.- 143 p 2. Perov S.P., Perov A.S. New physical approach to the analysis of cardiovascular system (CVS) and its interaction with the external factors. Scientific Education Bulletin #4 2012. Moscow. 3. Perov S., Subbaraya B.H.. Offermann D. Kruchenitsky G., Ermakov V. et al., Okkam`s Razor, Solar-Terrestrial Resonances and Global Change. Fluxes and Structures in Fluids, Int. Conf., Abstracts, Moscow.-2001.- p. 164-166 4. Ostrovskii V.E., Kadyshevich E.A. Mitosis and DNA Replication and Life Origination Hydrate Hypothesis: Common Physical and Chemical Grounds. DNA Replication - Current Advances; Ed. by Herve Seligmann. - (first publ. July, 2011. - INTECHWEB.ORG. www.intechopen.com p. 75- 114
46 CFR 11.920 - Subjects for MODU endorsements.
Code of Federal Regulations, 2014 CFR
2014-10-01
... engineering terminology X X X X X X X Engineering equipment, operations and failures X X X X X X Offshore... X X X X X Mooring equipment X X X X X X Crane use procedures and inspections X X X X X X Medical care: Knowledge and use of: First aid X X X X X X X First response medical action X X X X X X X...
15 CFR Supplement No. 1 to Part 740 - Country Groups
Code of Federal Regulations, 2014 CFR
2014-01-01
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15 CFR Supplement No. 1 to Part 740 - Country Groups
Code of Federal Regulations, 2013 CFR
2013-01-01
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15 CFR Supplement No. 1 to Part 740 - Country Groups
Code of Federal Regulations, 2012 CFR
2012-01-01
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15 CFR Supplement No. 1 to Part 740 - Country Groups
Code of Federal Regulations, 2010 CFR
2010-01-01
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15 CFR Supplement No. 1 to Part 740 - Country Groups
Code of Federal Regulations, 2011 CFR
2011-01-01
... X X X New Zealand 1 X X X Norway X X X X Poland X X X Portugal X X X X Romania X X Russia X X... Qatar X X Russia X X Saudi Arabia X X Syria X X Taiwan X Tajikstan X X Turkmenistan X X Ukraine X United...
2012-05-16
Fred Dini, SC, USN, JSF Japan Comptroller, May 2011 Explosion at Unit 4 at Fukushima Daiichi Stand-off area set at 30km radius USS Tortuga offloads...X X X X X X X X X X X X X X X X X X X X X O USNS TORTUGA LSD U U U X X X X X X X X X X X X X X X X X X X X X X X X X O USNS BLUE RIDGE LCC U U U U U
46 CFR 12.505 - Examination requirements.
Code of Federal Regulations, 2014 CFR
2014-10-01
... X X X X Properties of fuel X X X Pumps, fans, and blowers X X X Refrigeration principles X X X... X X X Lubrication X X X X Potable water X X Refrigeration X X X Sanitary/sewage X X Steering X X X...
Advanced Composite Air Frame Life Cycle Cost Estimating
2014-06-19
Kilic, H., et al x Klumpp, Joseph J. x Koury, Jennifer x Kutner, M.,et al Lambert , Daniel x x x x x x x x x x x x x x x Methodology Areas...Joseph J. x x x x x x x Koury, Jennifer x Kutner, M.,et al x x x x x x x x Lambert , Daniel x x x x x x...Company, Houston, TX., 1996. 5. Beer , F., and E. Jr. Johnston. Mechanics of Materials. McGraw-Hill. New York, 1981. 6. Bock, D. Cost Effectiveness
Cedar River and Tributaries, Black Hawk County, Iowa, and Vicinity
1992-07-01
Camp Cabins and Dormitories x Dining Hall x Infirmaries x Amphitheaters x x Caretaker Quarters x Outdoor Cooking x x Beaches x x Docks x x Camping pads...x x Swimming Beaches x x Visitor Center xZ/ x Nature Center x Historical Centers x Archeological Centers x Environmental - Education Centers x Lodges...Benches x x Camping Pads x x Flag Poles x Lantern Hangers x x VI. Play Facilities Courts Multiple Use x7/ x Tennis x Basketball x Handball x
46 CFR 11.910 - Subjects for deck officer endorsements.
Code of Federal Regulations, 2013 CFR
2013-10-01
... Procedures X X X X X X X X X X X X X X X X X X X X X X Emergency Towing X X X X X Medical Care: Knowledge and use of: Int'l. Medical Guide for Ships X X Ship Med. Chest and Med. Aid at Sea X X Medical Sec., Inter... terminology. Applicants for sail/auxiliary sail endorsements to master, mate or operator of uninspected...
46 CFR 11.910 - Subjects for deck officer endorsements.
Code of Federal Regulations, 2012 CFR
2012-10-01
... Procedures X X X X X X X X X X X X X X X X X X X X X X Emergency Towing X X X X X Medical Care: Knowledge and use of: Int'l. Medical Guide for Ships X X Ship Med. Chest and Med. Aid at Sea X X Medical Sec., Inter... terminology. Applicants for sail/auxiliary sail endorsements to master, mate or operator of uninspected...
46 CFR 11.910 - Subjects for deck officer endorsements.
Code of Federal Regulations, 2011 CFR
2011-10-01
... Procedures X X X X X X X X X X X X X X X X X X X X X X Emergency Towing X X X X X Medical Care: Knowledge and use of: Int'l. Medical Guide for Ships X X Ship Med. Chest and Med. Aid at Sea X X Medical Sec., Inter... terminology. Applicants for sail/auxiliary sail endorsements to master, mate or operator of uninspected...
46 CFR 11.910 - Subjects for deck officer endorsements.
Code of Federal Regulations, 2010 CFR
2010-10-01
... Procedures X X X X X X X X X X X X X X X X X X X X X X Emergency Towing X X X X X Medical Care: Knowledge and use of: Int'l. Medical Guide for Ships X X Ship Med. Chest and Med. Aid at Sea X X Medical Sec., Inter... terminology. Applicants for sail/auxiliary sail endorsements to master, mate or operator of uninspected...
17 CFR 229.601 - (Item 601) Exhibits.
Code of Federal Regulations, 2010 CFR
2010-04-01
... accountant regarding non-reliance on a previously issued audit report or completed interim review X (8) Opinion re tax matters X X X X X X X (9) Voting trust agreement X X X X X X X (10) Material contracts X X... X X X X X X (16) Letter re change in certifying accountant 4 X X X X X X (17) Correspondence on...
Marine Ecological Index Survey of San Diego Bay
2013-03-01
Ascidia zara Thermal DO Chordata Botrylloides violaceus Thermal DO Chordata Diplosoma listerianum Thermal DO Annelida Brania complex Thermal DO Annelida...x x Ascidia Zara x? x? x x Ascidia sp x? x x x x Styela canopus x x x x x Styela clava x x x x x Styela plicata x x x x x Polyandrocarpa zorritensis...Estuarine Marine Seasonally Hypersaline Thermal Native Pre ID Region(a) Aplidium californicum x x x Ascidia ceratodes x x Ascidia zara x Estuarine
1981-08-01
pinnata X K CACTACEAE Coryphantha vivipara x Opuntia echinocarpa K 0 x K K K 5putaerinacea K Op’untia sp. x X -12- TABLE 3-1 (Cont.) Shelter site...pilosus x Lepidium montanun X CACTACEAE Opuntia echinocarpa x x Opuntia erinacea X X X CHENOPODIACEAE Atriplex canescens X X X Ceratoides lanata X X X X...Stanleya pinnata X CACTACEAE Coryphantha vivipara var. rosea X Echinocereus engelmannii X opuntia echinocarpa X X X X X X X X Opuntia erinacea XX X X X X x
AM2 Modified 2-1 Lay Pattern Evaluation under F-15E Traffic
2015-08-01
trafficking was completed, posttest forensics were conducted at the same locations to determine the depth of subgrade that might have undergone gradual drying...X X X X 240 X X X X 496 X X X X 1008 X X X X 1520 X X X X 1728 X X X 2032 X X X X 2850 X X X X Posttest Subgrade X X 3.4.1 Centerline...profile Elevation data collected along the traffic centerline on the pretest subgrade, on the mat at scheduled pass levels, and on the posttest
2013-09-01
Ethical hacking & penetration testing,” University of Waterloo, Waterloo, Canada, 2011. [2] B. Jurjonas, “Smart selection and configuration of...Ettercap (XP) X X X X Wireshark X tshark X X Tethereal (XP) *Command line version of Ethereal * X X X X tcpdump X NetStumbler ( Wifi ) X X...Ethereal X X X dsniff X X X X Kismet ( Wifi ) X X X EtherApe X X X Netcat X X X X 2. Robustness Due to the limitations of the operating
46 CFR 11.920 - Subjects for MODU endorsements.
Code of Federal Regulations, 2011 CFR
2011-10-01
... systems: Marine engineering terminology X X X X X X X Engineering equipment, operations and failures X X X... X X Medical care: Knowledge and use of: First aid X X X X X X X First response medical action X X X...
46 CFR 11.920 - Subjects for MODU endorsements.
Code of Federal Regulations, 2013 CFR
2013-10-01
... systems: Marine engineering terminology X X X X X X X Engineering equipment, operations and failures X X X... X X Medical care: Knowledge and use of: First aid X X X X X X X First response medical action X X X...
46 CFR 11.920 - Subjects for MODU endorsements.
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2012-10-01
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46 CFR 11.920 - Subjects for MODU endorsements.
Code of Federal Regulations, 2010 CFR
2010-10-01
... systems: Marine engineering terminology X X X X X X X Engineering equipment, operations and failures X X X... X X Medical care: Knowledge and use of: First aid X X X X X X X First response medical action X X X...
Natural Exposure versus Chamber Simulation.
1984-09-01
Phoma) or at the Forested sites ( Trichoderma , Fusarum and Cephalosporium). -tNtter genera occured only once or twice out of eig-htfungal examinations...APR CURVULARIA x PENICILLIUM X X x X X FUSARIUM CLADOSPORIUM X PHOIAA X ASPERGILLUS X CEPHALOSPORIUM X X TRICHODERMA X PESTALOTIA GL TOCLADIUM...X x x * CLADOSPORIUM PHOMA x ASPERGILLUS. CEPHALOSPORI’JM X x x TRICHODERMA X X X X X X X PESTALOTIA x GLIOCLADIUM NIGROSPORA STEMPHYLIUM ALTERNARIA
36 CFR 294.29 - List of designated Idaho Roadless Areas.
Code of Federal Regulations, 2013 CFR
2013-07-01
...-Spring Creek 111 X X X X Caribou Gibson 181 X X Caribou Hell Hole 168 X X Caribou Huckleberry Basin 165 X... Mink 151 X X X Caribou Williams Creek 174 X X X Caribou Worm Creek 170 X X X Challis Blue Bunch... Creek 509 X X Salmon South Panther 504 X Salmon Taylor Mountain 902 X Salmon West Big Hole 943 X X X X...
36 CFR 294.29 - List of designated Idaho Roadless Areas.
Code of Federal Regulations, 2014 CFR
2014-07-01
...-Spring Creek 111 X X X X Caribou Gibson 181 X X Caribou Hell Hole 168 X X Caribou Huckleberry Basin 165 X... Mink 151 X X X Caribou Williams Creek 174 X X X Caribou Worm Creek 170 X X X Challis Blue Bunch... Mountain 902 X Salmon West Big Hole 943 X X X X Salmon West Panther Creek 504 X Sawtooth Black Pine 003 X X...
36 CFR 294.29 - List of designated Idaho Roadless Areas.
Code of Federal Regulations, 2012 CFR
2012-07-01
...-Spring Creek 111 X X X X Caribou Gibson 181 X X Caribou Hell Hole 168 X X Caribou Huckleberry Basin 165 X... Mink 151 X X X Caribou Williams Creek 174 X X X Caribou Worm Creek 170 X X X Challis Blue Bunch... Creek 509 X X Salmon South Panther 504 X Salmon Taylor Mountain 902 X Salmon West Big Hole 943 X X X X...
1992-06-01
Administration, Legal Principles, Ethics in Government or Public Administration courses in the NPS curriculum. These courses, however, are found in more...Other X Other: Legal Aspects X X X Ethics in Government X X X Public Administration X X 2 X Admin Theory/Policy X X X 2 X Degree Offered: 1)MPA 2 3 2 1 1...Other Other: Legal Aspects X X X Ethics in Government X X X Public Administration X X X X X X X X Admin Theory/Policy X X X X Degree Offered: 1)MPA 1 1
36 CFR 294.29 - List of designated Idaho Roadless Areas.
Code of Federal Regulations, 2011 CFR
2011-07-01
... 019 X X Boise Bear Wallow 125 X X Boise Bernard 029 X X Boise Black Lake 036 X X Boise Blue Bunch 923... Meadows 027 X X Boise Ten Mile/Black Warrior 013 X X X X Boise Tennessee 033 X X Boise Whiskey 031 X Boise...-Spring Creek 111 X X X X Caribou Gibson 181 X X Caribou Hell Hole 168 X X Caribou Huckleberry Basin 165 X...
High Level Design for Distributed Application Instrumentation.
1992-09-01
true branch ,TRUE DD-path5 FALSE false branch SEXI .__T DECISION-TO-DECISION PATH EXAMPLE FIGURE 2 4.0 AUTOMATED TESTING TOOLS Manually testing...I I x l- I lE-4 I XX I WI I x I IH I E- 1>4 I IZI X XX I Z ~It X X XX w 1 0 1 XXX x X Il- I E-4l XXW x x X I c)l I XX x x X I4 l l XXX I X x ( l...I I lC1l XXX x X III xXX X x x X I WI rXX X X x X I I II xXX X X x I i 111 I 1W 0~l XXX X X XX X I1 10.01 XXXX x X XX x I HI0 IW 01 XXXX x Xx XX X X I
1979-11-01
Aspergillus spp. X X Penicillium spp. X X X X Cunninghamella spp. X X Zygorhynchus sp . X X Alternaria sp . X X Mycelial Molds X X Candida spp. X X...itermined if a technique could he used t dtrmn , ’ old s 1 from new sp i 11 . 12 it was not leaving the base and most likely was being held in the bottom...Rhodotorula sp . X X X Geotrichum sp . X X Trichoderma spp. X X X Mucor spp. X X X Rhizopus sp . X X Absidia sp . X X aMicrobial analyses conducted by Department
Federal Register 2010, 2011, 2012, 2013, 2014
2012-07-12
..., and Sulfur Recovery Units. VVV Publicly Owned X X X X Treatment Works. XXX Ferroalloys X X X X... Ceramics X X X X Manufacturing. LLLLL Asphalt Roofing X X X X and Processing. MMMMM Flexible X X X X... Source X Standards for Aluminum, Copper, and Other Nonferrous Foundries. AAAAAAA Asphalt X Processing and...
Inflight Evaluation of an Acoustic Orientation Instrument
1992-12-01
othoienwma noted. mu wwTI DATA OUT DATA VAUID Figure 11-9. Porn Write or Timor Output Compare E:WU READ DATA M* PORTS A. C. 0 DAT VLI DATA Ill PORT fDATA...9* 9* WATCH DOG TIMER x x X x X X X X X X RS-232 CONVERSION X X x X X X X X RS-232 DB25 CONN. X X X X X X X RESET BUTTON X X X X X X X RS-422/485...calanOs. Tfle b.A.1t-in skivmter and us~ dog timrm, rrnm it the natural dmie fo real tire g’~ t~man and sacung also ca benit fr= it’s feture. frv F68MC is
14 CFR Appendix O to Part 121 - Hazardous Materials Training Requirements For Certificate Holders
Code of Federal Regulations, 2011 CFR
2011-01-01
... plannersWill-carry Crew members(other than flight crew members) Will-carry General philosophy X X X X X X... General philosophy X X X X X X Limitations X X X X X X General requirements for shippers X Classification...
14 CFR Appendix O to Part 121 - Hazardous Materials Training Requirements For Certificate Holders
Code of Federal Regulations, 2013 CFR
2013-01-01
... plannersWill-carry Crew members(other than flight crew members) Will-carry General philosophy X X X X X X... General philosophy X X X X X X Limitations X X X X X X General requirements for shippers X Classification...
14 CFR Appendix O to Part 121 - Hazardous Materials Training Requirements For Certificate Holders
Code of Federal Regulations, 2014 CFR
2014-01-01
... plannersWill-carry Crew members(other than flight crew members) Will-carry General philosophy X X X X X X... General philosophy X X X X X X Limitations X X X X X X General requirements for shippers X Classification...
14 CFR Appendix O to Part 121 - Hazardous Materials Training Requirements For Certificate Holders
Code of Federal Regulations, 2012 CFR
2012-01-01
... plannersWill-carry Crew members(other than flight crew members) Will-carry General philosophy X X X X X X... General philosophy X X X X X X Limitations X X X X X X General requirements for shippers X Classification...
14 CFR Appendix O to Part 121 - Hazardous Materials Training Requirements For Certificate Holders
Code of Federal Regulations, 2010 CFR
2010-01-01
... plannersWill-carry Crew members(other than flight crew members) Will-carry General philosophy X X X X X X... General philosophy X X X X X X Limitations X X X X X X General requirements for shippers X Classification...
REACH Compliant Hexavalent Chrome Replacement for Corrosion Protection (HITEA)
2014-11-01
3 The Role of the AAD and Materials KTNs • A joint AAD and Materials KTN workshop in 2011 resulted in: - Definition of the hexavalent chromium ...Alloy Nimonic alloy Hard chrome plating x x x TiN x x CrN x x DLC x WC/C x x x PEO x x Co-P x x x x x x Trivalent Cr x x x x x x Filled ENP x x 8...aims to establish a fast, inexpensive and robust testing methodology for selecting the most promising chromium -free alternatives. • Creation of a
BIT/External Test Figures of Merit and Demonstration Techniques
1979-12-01
affecti1ve Implementation of the defined maintenance concept, The buiit-In-test capability &hall consist of the followingý to) Sul f test provislons: Self...COMBAT GRANDE X x x X X x 4. AN/TPQ-36 x X 5. AN/TrPQ-37 X x ei JOB x x x x 7. AN/PRC-104 x x 6. RADEK x X X x g. MIFAIS x X X X X 10, HADR X X X 114...FFP). FPR,(or FFP) is defined ast FPR- The rate at which good RIs (ie., RIo with no Actual tailure within it) are removed from a system duo to the
Requirements Management for Net-Centric Enterprises. Phase 2
2011-12-31
BusinessWor ks X X X X X Talend Integration Suite – Enterprise Edition X X X X X X X Informatica Data Integration Product Suite...UNCLASSIFIED 83 TIBCO ActiveMatrix BusinessWor ks X NS Talend Integration Suite – Enterprise Edition X X X X X X NS Informatica Data
2014-01-01
kW) and Energy (kWh) Charges, Including Time-of-Use Energy Charges X X X X X Power Factor Improvement X X Emergency Demand Response... Capacity Market) X X X X X Other Capacity Sales X X X Frequency Regulation X X X X Spinning/Synchronous Reserve X X Blackstart Capacity X X X...Policy, Organizational, and Other Factors that can Accelerate Prudent Electricity Security Asset Investments and Uses 0% 2% 4% 6% 8% 10% 12% 14% 16
1990-08-09
Table 2) Yes No Other Alabama X Alaska X Arizona X Arkansas X * California X Colorado X Connecticut X Delaware X Florida X Georgia X Hawaii X I daho ...California X Colorado X Connecticut X Delaware X Florida X Georgia X Hawaii X I daho X Illinois Indiana X Iowa X Kansas X Kentucky X * Louisiana X Maine X...0 Connecticut 1 0 Delaware 1 0 Florida 1 0 Georgia 1 0 Hawaii 10 I daho 10 Illinois 1 0 Indiana 1 0 Iowa X Kansas 10 Kentucky 1 0 * Louisiana 1 0
Code of Federal Regulations, 2010 CFR
2010-07-01
... Fertilizer Industry: Wet Process Phosphoric Acid Plants X X X X U Phosphate Fertilizer Industry: Superphosphoric Acid Plants X X X X V Phosphate Fertilizer Industry: Diammonium Phosphate Plants X X X X W Phosphate Fertilizer Industry: Triple Superphosphate Plants X X X X X Phosphate Fertilizer Industry...
50 CFR Table 15 to Part 679 - Gear Codes, Descriptions, and Use
Code of Federal Regulations, 2011 CFR
2011-10-01
..., power gurdy TROLL X X 15 X X All other gear types OTH X X ADF&G GEAR CODES Diving 11 X X Dredge 22 X X Dredge, hydro/mechanical 23 X X Fish ladder/raceway 77 X X Fish wheel 08 X X Gillnet, drift 03 X X...
1986-03-01
investigations and site preservation Continuous hiking/biking path from Hwy. 20 to Hwy. 92 Soil erosion structures Access roads Skating pond Beach area on...Group Camp Cabins and Dormitories x Dining Hall x Infirmaries x Amphitheaters x x Caretaker Quarters x Outdoor Cooking x x Beaches x x Docks x x Tent pads...x x Swimming Beaches x x Visitor Center x2/ x Nature Center x Historical Centers x Archeological Centers x Environmental-Education Centers x Lodges
49 CFR 178.803 - Testing and certification of IBCs.
Code of Federal Regulations, 2014 CFR
2014-10-01
... Vibration 6 X 6 X 6 X 6 X 6 X 1.5 X Bottom lift 2 X X X X X Top lift 2 X 2 X 2 X 2 5 X Stacking 7 X 7 X 7 X... X Righting 2 5 X Tear 5 X 1 Flexible IBCs must be capable of withstanding the vibration test. 2 This... each test. 6 The vibration test may be performed in another order for IBCs manufactured and tested...
49 CFR 178.803 - Testing and certification of IBCs.
Code of Federal Regulations, 2012 CFR
2012-10-01
... Vibration 6 X 6 X 6 X 6 X 6 X 1.5 X Bottom lift 2 X X X X X Top lift 2 X 2 X 2 X 2,5 X Stacking 7 X 7 X 7 X... X Righting 2,5 X Tear 5 X 1 Flexible IBCs must be capable of withstanding the vibration test. 2 This... each test. 6 The vibration test may be performed in another order for IBCs manufactured and tested...
49 CFR 178.803 - Testing and certification of IBCs.
Code of Federal Regulations, 2013 CFR
2013-10-01
... Vibration 6 X 6 X 6 X 6 X 6 X 1.5 X Bottom lift 2 X X X X X Top lift 2 X 2 X 2 X 2 5 X Stacking 7 X 7 X 7 X... X Righting 2 5 X Tear 5 X 1 Flexible IBCs must be capable of withstanding the vibration test. 2 This... each test. 6 The vibration test may be performed in another order for IBCs manufactured and tested...
Evaluation of the Total Petroleum Hydrocarbon Standard for Cleanup of Petroleum Contaminated Sites
1993-09-01
100-500 20-100 Hawaii .05-1.7 10-21 1.4-7 Idaho 40-200 Illinois 11.705 0.005 Indiana X 20 Iowa 100 Kansas 100 1.4 XXX Kentucky 1 Louisiana X * * Maine...100 Hawaii 0.5-1.7 10-20 1.4-7 XXX Idaho 100 llinois 11.705 0.005 XXX Indiana X 20 Iowa 100 Kansas 100 1.4 XXX Kentucky XXX Louisiana X Maine X FIELD...Alaska X X Arizona X X Arkansas X X California X X X Colorado X X Connecticut (I) Delaware X X lorida X Georstia, X IX I Hawaii X X Idaho X X illinois X X
49 CFR 178.803 - Testing and certification of IBCs.
Code of Federal Regulations, 2011 CFR
2011-10-01
... Vibration 6 X 6 X 6 X 6 X 6 X 1.5 X Bottom lift 2 X X X X X Top lift 2 X 2 X 2 X 2,5 X Stacking 7 X 7 X 7 X... of the bottom lift or top lift tests must be performed. 3 The leakproofness and hydrostatic pressure...
Special Inspector General for Iraq Reconstruction
2013-04-30
budget for gasoline. As a result, they were putting in cheap, contaminated gas that quickly broke all the genera- tors. Then some of the aircraft, the T ...2012 x x x Jill Charpia Providing false statements to a government agency 1/24/2013 x x x Richard Evick Bribery, money laundering 1/28/2013 x x x x x...12/17/2012 x x x x Ulysses Hicks Conspiracy to accept illegal gratuities 1/3/2013 x x x Ramy Elmery Making false statements 4/12/2013 x x x x Richard
33 CFR 160.206 - Information required in an NOA.
Code of Federal Regulations, 2010 CFR
2010-07-01
... CDC (1) Vessel Information: (i) Name; X X X (ii) Name of the registered owner; X X X (iii) Country of registry; X X X (iv) Call sign; X X X (v) International Maritime Organization (IMO) international number or... (vi) Name of the operator; X X X (vii) Name of the charterer; and X X X (viii) Name of classification...
Sacramento River, Chico Landing to Red Bluff, California Bank Protection Project
1975-01-01
Spizella passerina ) White-crowned sparrow Common-Nationwide X X X X X X X (Zonotrichia leucophrys) Fox sparrow Common-Nationwide X X X X... throated swift Common- X X X X (Aeronautes saxatalis) Southwest U.S. Black -chinned hummingbird Occas ional-Southwest X X X X (Archilochus...fishery consisting of black bass, crappie, white catfish, channel catfish, bluegill, and other nongame species. 2.26. Archeological and Historical
Quality of Information Assurance - Assessment, Management and Use (QIAAMU)
2013-04-01
106 4.7.3.1 University authentication infrastructure ...Authentication infrastructure ..................................................................................... 107 Figure 49: Complementary...X X X X Architecture & Infrastructure Quality AIQ X X X X X X Deviation from Configuration (Services) SERV STAT X X X X X Deviation from
Neural Networks and Their Application to Air Force Personnel Modeling
1991-11-01
specifications of the error function ( Chauvin , 1990; Hanson & Pratt, 1989) and found that out-of-sample performance can be improved by this modification...X X Black X X X X Hispanic X X - White & female X Black & male X Female X X X X Xŕ] Single or married indicator X X X X X X Age less than or equal 17...administration, female in unknown specialty, and black male in support and administration. 7Five dummies: TOE 4 and YOS 2. TOE 6 and YOS 1. TOE 6 and
40 CFR 81.322 - Massachusetts.
Code of Federal Regulations, 2010 CFR
2010-07-01
... River X Attleboro X New Bedford X Taunton X All other cities and towns X Metropolitan Boston AQCR... Pittsfield X All other cities and towns X Central Massachusetts AQCR: Worcester X Athol X Gardner X Grafton X Leominster X Millbury X Shrewsbury X All other cities and towns X Merrimack Valley AQCR: Haverhill X Lawrence...
15 CFR Supplement No. 1 to Part 738 - Commerce Country Chart
Code of Federal Regulations, 2010 CFR
2010-01-01
... X X X X X Kiribati X X X X X X X X X X Korea, North See Sections 742.19 and 746.4 of the EAR to determine whether a license is required in order to export or reexport to this destination. Korea, South 3 4...
2009-09-01
Peruvian Navy Peru X X X X VADM Andrzej Karweta Commander-in-Chief, Polish Navy Poland X X ADM Fernando Jose Ribeiro de Melo Gomes...Chief of Naval Staff, Portuguese Navy Portugal X X X X X VADM J. Mudimu Chief, South African Navy South Africa X X X X X ADM Manuel Rebollo
Federal Register 2010, 2011, 2012, 2013, 2014
2013-04-30
..., Reconstruction, or Modification Commenced After May 18, 1978, and Prior to July 23, 1984. Kb Volatile Organic... Primary Lead Smelters X X X X S Primary Aluminum Reduction Plants.... X X X X T Phosphate Fertilizer Industry: Wet X X X X Process Phosphoric Acid Plants. U Phosphate Fertilizer Industry: X X X X...
49 CFR 177.848 - Segregation of hazardous materials.
Code of Federal Regulations, 2010 CFR
2010-10-01
... materials 4.3 X X X X O X O Oxidizers 5.1 A X X X X O O X O Organic peroxides 5.2 X X X X O X O Poisonous...”, ammonium nitrate (UN 1942) and ammonium nitrate fertilizer may be loaded or stored with Division 1.1...
49 CFR 174.81 - Segregation of hazardous materials.
Code of Federal Regulations, 2010 CFR
2010-10-01
... X O O X O Organic peroxides 5.2 X X X X O X O Poisonous liquids PG I Zone A 6.1 X X O X O X X X X X... fertilizer may be loaded or stored with Division 1.1 (explosive) or Division 1.5 materials. (6) When the...
49 CFR 178.803 - Testing and certification of IBCs.
Code of Federal Regulations, 2010 CFR
2010-10-01
... IBCs Vibration 6 X 6 X 6 X 6 X 6 X 1.5 X Bottom lift 2 X X X X X Top lift 2 X 2 X 2 X 2,5 X Stacking 7... one of the bottom lift or top lift tests must be performed. 3 The leakproofness and hydrostatic...
1990-11-01
NY X X x x x X Lockheed. CA X Lockheed, GA X ’ x MCO, TX X X X X TxX Martin Marietta. LA X X X x x x MDDonnell Douglas Astro , CA x GcDonel1 Douglas...LI 4%.0000-00 L -ft L0 v I0U UV~o W N fp F.I w0 !; g 2 CL. cO .01 w C fxC T3 00 6 .- t-63 a wwWWW WWW6WWWIOW6WWWww rnrnrnrnrnrnmn4 Z NNNMW W.rN
48 CFR 25.002 - Applicability of subparts.
Code of Federal Regulations, 2010 CFR
2010-10-01
... Evaluating Foreign Offers—Supply Contracts X X 25.6 American Recovery and Reinvestment Act—Buy American Act... Coordination X X X X 25.9 Customs and Duties X 25.10 Additional Foreign Acquisition Regulations X X X X X X 25...
Water Quality Management Studies, Lake Seminole, February-December 1979. Phase II.
1982-12-01
Carbon, Dissolved Organtc X X X X X X X Carbon. Total Organic I I X I X X" X Carbon Dioxide I X X X X X X I trogen. Total Amonia I X I X X X I Nitrogen...were less than 1 mg S04/1. During Phase I and Phase II there were no distinctive trends in measured carbon dioxide levels. However, there was a tendency...6. so 0 To CARSON DIOXIDE (MG C02.01. 0 1.3 Re 1. Re 0. 2* 0 NITROGEN. TOTAL AMMONIA IMG N/’LI 0.02 < 0.02 < 0.02 CO (002 ’ NITROG01. NITPATE.NITT2lYE
39 CFR 3060. 30 - Statement of allocated assets and liabilities for competitive products.
Code of Federal Regulations, 2012 CFR
2012-07-01
... on basis of: Total net assets Cash and Cash Equivalents $x,xxx $x,xxx $x,xxx Net Accounts Receivable x,xxx x,xxx x,xxx Supplies, Advances and Prepayments x,xxx x,xxx x,xxx Appropriations Receivable—Revenue Forgone x,xxx x,xxx x,xxx Total Current Assets x,xxx x,xxx x,xxx Property and Equipment: Buildings...
39 CFR 3060. 30 - Statement of allocated assets and liabilities for competitive products.
Code of Federal Regulations, 2013 CFR
2013-07-01
... on basis of: Total net assets Cash and Cash Equivalents $x,xxx $x,xxx $x,xxx Net Accounts Receivable x,xxx x,xxx x,xxx Supplies, Advances and Prepayments x,xxx x,xxx x,xxx Appropriations Receivable—Revenue Forgone x,xxx x,xxx x,xxx Total Current Assets x,xxx x,xxx x,xxx Property and Equipment: Buildings...
39 CFR 3060. 30 - Statement of allocated assets and liabilities for competitive products.
Code of Federal Regulations, 2014 CFR
2014-07-01
... on basis of: Total net assets Cash and Cash Equivalents $x,xxx $x,xxx $x,xxx Net Accounts Receivable x,xxx x,xxx x,xxx Supplies, Advances and Prepayments x,xxx x,xxx x,xxx Appropriations Receivable—Revenue Forgone x,xxx x,xxx x,xxx Total Current Assets x,xxx x,xxx x,xxx Property and Equipment: Buildings...
39 CFR 3060. 30 - Statement of allocated assets and liabilities for competitive products.
Code of Federal Regulations, 2011 CFR
2011-07-01
... on basis of: Total net assets Cash and Cash Equivalents $x,xxx $x,xxx $x,xxx Net Accounts Receivable x,xxx x,xxx x,xxx Supplies, Advances and Prepayments x,xxx x,xxx x,xxx Appropriations Receivable—Revenue Forgone x,xxx x,xxx x,xxx Total Current Assets x,xxx x,xxx x,xxx Property and Equipment: Buildings...
39 CFR 3060. 30 - Statement of allocated assets and liabilities for competitive products.
Code of Federal Regulations, 2010 CFR
2010-07-01
... on basis of: Total net assets Cash and Cash Equivalents $x,xxx $x,xxx $x,xxx Net Accounts Receivable x,xxx x,xxx x,xxx Supplies, Advances and Prepayments x,xxx x,xxx x,xxx Appropriations Receivable—Revenue Forgone x,xxx x,xxx x,xxx Total Current Assets x,xxx x,xxx x,xxx Property and Equipment: Buildings...
46 CFR 13.121 - Courses for tankerman endorsements.
Code of Federal Regulations, 2014 CFR
2014-10-01
... during repair and maintenance work X X safety measures for hot and cold work X X electrical safety X X... X X X X Construction, materials, coating, & insulation of cargo tanks X X General arrangement of..., carbon dioxide (CO2), foam * * * X Pressure-water spray system in special-category spaces X Automatic...
Code of Federal Regulations, 2011 CFR
2011-07-01
... County X Cherokee County X Cheyenne County X Clark County X Clay County X Cloud County X Coffey County X... Chautauqua County X Cherokee County X Cheyenne County X Clark County X Clay County X Cloud County X Coffey.../Attainment Cherokee County Unclassifiable/Attainment Cheyenne County Unclassifiable/Attainment Clark County...
Code of Federal Regulations, 2010 CFR
2010-07-01
... County X Cherokee County X Cheyenne County X Clark County X Clay County X Cloud County X Coffey County X... Chautauqua County X Cherokee County X Cheyenne County X Clark County X Clay County X Cloud County X Coffey.../Attainment Cherokee County Unclassifiable/Attainment Cheyenne County Unclassifiable/Attainment Clark County...
Code of Federal Regulations, 2013 CFR
2013-07-01
... County X Cherokee County X Cheyenne County X Clark County X Clay County X Cloud County X Coffey County X... Chautauqua County X Cherokee County X Cheyenne County X Clark County X Clay County X Cloud County X Coffey... Unclassifiable/Attainment Clay County Unclassifiable/Attainment Cloud County Unclassifiable/Attainment Coffey...
Code of Federal Regulations, 2012 CFR
2012-07-01
... County X Cherokee County X Cheyenne County X Clark County X Clay County X Cloud County X Coffey County X... Chautauqua County X Cherokee County X Cheyenne County X Clark County X Clay County X Cloud County X Coffey... Unclassifiable/Attainment Clay County Unclassifiable/Attainment Cloud County Unclassifiable/Attainment Coffey...
Code of Federal Regulations, 2014 CFR
2014-07-01
... County X Cherokee County X Cheyenne County X Clark County X Clay County X Cloud County X Coffey County X... Clark County X Clay County X Cloud County X Coffey County X Comanche County X Cowley County X Crawford.../Attainment Cloud County Unclassifiable/Attainment Coffey County Unclassifiable/Attainment Comanche County...
Federal Register 2010, 2011, 2012, 2013, 2014
2012-02-27
... Tanks. O Ethylene Oxide X X X Sterilization Facilities. Q Industrial Process Cooling X X Towers. R... Organic-Water Separators. WW Storage Vessels (Tanks)-- X X Control Level 2. XX Ethylene Manufacturing X X... Refractory Products X X Manufacturing. TTTTT Primary Magnesium Refining. X WWWWW Hospital Ethylene Oxide X X...
Evaporation of a Thickened Agent Simulant from Oak and Hickory Leaves
1990-12-01
162.5625 1 162.5625 0.591 ------------------- I---------------- ------------------------------ 1x2x3 22.5625 11x2x4 33.0625 1Ix3x4 18.0625 1 2x3x4 1,278.0625...F,513,0625- 1 5,513.0625 10.952 * 1x2x3 r 3.062$ 1 1x2x4 410, 062! Ix3x4 85,562, 2 2x3x4 7,958i.06?21 ], 2x3x4 62 06. . 2,516.8125 5 503.36125...0.0 0.0 1x2 1.0 I 1.0 0.4 1x3 0.25 1. 0. t5 lx4 0X 1 0.0 0.0 2x3 6.25 1 6.25 15.625 ** 32x4 0.0 1 0.0 MS3x4 0. 25 1 0O1: 0.6- 1x2x3 0.25 1 lx2x4 1.00
1990-09-01
Initially, cuttings from the borings and wells will be placed on plastic sheeting, covered, and left at the drilling site until a determination can be...Spwmxds Solids (K160.2) X X X X X Nitrate - Nitrate (PE3M.1) X X X X X tPhysical Caracteristics : Soil Enginering Classificatim X X X X X X X X (MQ8-84...site, soil cuttings from drilling the borings and wells will be placed on a plastic tarp and covered until samples of the soil have been screened using
Gannu, Ramesh; Yamsani, Vamshi Vishnu; Palem, Chinna Reddy; Yamsani, Shravan Kumar; Yamsani, Madhusudan Rao
2010-01-01
The objective of the investigation was to optimize the iontophoresis process parameters of lisinopril (LSP) by 3 x 3 factorial design, Box-Behnken statistical design. LSP is an ideal candidate for iontophoretic delivery to avoid the incomplete absorption problem associated after its oral administration. Independent variables selected were current (X(1)), salt (sodium chloride) concentration (X(2)) and medium/pH (X(3)). The dependent variables studied were amount of LSP permeated in 4 h (Y(1): Q(4)), 24 h (Y(2): Q(24)) and lag time (Y(3)). Mathematical equations and response surface plots were used to relate the dependent and independent variables. The regression equation generated for the iontophoretic permeation was Y(1) = 1.98 + 1.23X(1) - 0.49X(2) + 0.025X(3) - 0.49X(1)X(2) + 0.040X(1)X(3) - 0.010X(2)X(3) + 0.58X(1)(2) - 0.17X(2)(2) - 0.18X(3)(2); Y(2) = 7.28 + 3.32X(1) - 1.52X(2) + 0.22X(3) - 1.30X(1)X(2) + 0.49X(1)X(3) - 0.090X(2)X(3) + 0.79X(1)(2) - 0.62X(2)(2) - 0.33X(3)(2) and Y(3) = 0.60 + 0.0038X(1) + 0.12X(2) - 0.011X(3) + 0.005X(1)X(2) - 0.018X(1)X(3) - 0.015X(2)X(3) - 0.00075X(1)(2) + 0.017X(2)(2) - 0.11X(3)(2). The statistical validity of the polynomials was established and optimized process parameters were selected by feasibility and grid search. Validation of the optimization study with 8 confirmatory runs indicated high degree of prognostic ability of response surface methodology. The use of Box-Behnken design approach helped in identifying the critical process parameters in the iontophoretic delivery of lisinopril.
Code of Federal Regulations, 2011 CFR
2011-07-01
... Wythe County X City of Bristol X City of Galax X City of Norton X Valley of Virginia Intrastate AQCR... City of Buena Vista X City of Clifton Forge X City of Covington X City of Harrisonburg X City of Lexington X City of Radford X City of Roanoke X City of Salem X City of Staunton X City of Waynesboro X City...
Code of Federal Regulations, 2010 CFR
2010-07-01
... Wythe County X City of Bristol X City of Galax X City of Norton X Valley of Virginia Intrastate AQCR... City of Buena Vista X City of Clifton Forge X City of Covington X City of Harrisonburg X City of Lexington X City of Radford X City of Roanoke X City of Salem X City of Staunton X City of Waynesboro X City...
17 CFR 229.601 - (Item 601) Exhibits.
Code of Federal Regulations, 2011 CFR
2011-04-01
... accountant regarding non-reliance on a previously issued audit report or completed interim review X (8... X X X X X X (16) Letter re change in certifying accountant 4 X X X X X X (17) Correspondence on... Form. (6) [Reserved] (7) Correspondence from an independent accountant regarding non-reliance on a...
40 CFR 81.341 - South Carolina.
Code of Federal Regulations, 2012 CFR
2012-07-01
... County X Anderson County X Bamberg County X Barnwell County X Beaufort County X Berkeley County X Calhoun... County X Bamberg County X Barnwell County X Beaufort County X Berkeley County X Calhoun County X... Calhoun County Charleston County Cherokee County Chester County Chesterfield County Clarendon County...
40 CFR 81.341 - South Carolina.
Code of Federal Regulations, 2013 CFR
2013-07-01
... County X Anderson County X Bamberg County X Barnwell County X Beaufort County X Berkeley County X Calhoun... County X Bamberg County X Barnwell County X Beaufort County X Berkeley County X Calhoun County X... Calhoun County Charleston County Cherokee County Chester County Chesterfield County Clarendon County...
40 CFR 81.341 - South Carolina.
Code of Federal Regulations, 2014 CFR
2014-07-01
... County X Anderson County X Bamberg County X Barnwell County X Beaufort County X Berkeley County X Calhoun... County X Berkeley County X Calhoun County X Charleston County X Cherokee County X Chester County X... Beaufort County Berkeley County Calhoun County Charleston County Cherokee County Chester County...
Code of Federal Regulations, 2010 CFR
2010-07-01
... Lee County X Leslie County X Letcher County X Lewis County X Lincoln County X Livingston County X... Lawrence County X Lee County X Leslie County X Letcher County X Lewis County X Lincoln County X Livingston... County Unclassifiable/Attainment Lawrence County Unclassifiable/Attainment Lee County Unclassifiable...
Code of Federal Regulations, 2011 CFR
2011-07-01
... Lee County X Leslie County X Letcher County X Lewis County X Lincoln County X Livingston County X... Lawrence County X Lee County X Leslie County X Letcher County X Lewis County X Lincoln County X Livingston... County Unclassifiable/Attainment Lawrence County Unclassifiable/Attainment Lee County Unclassifiable...
Stream and Aquifer Biology of South-Central Texas - A Literature Review, 1973-97
2000-01-01
Unit, Report IS–37, 42 p. Findeisen , J.A., 1997, An assessment of fishes, biotic integrity, and fish habitat utilization in the lower San Antonio...Epperson and Short, 1987 X 23 Espey, Huston and Associates, Inc., 1983 X X X X X 24 Ezell, 1982 X X X X 25 Findeisen , 1997 X X X X 26 Garrett, 1991
1982-09-01
FQRMAT(/7H FRAME,IX,4HTRIP,3X,4HTYPE,5X,2HAO,9X,24AI,8X, IHQ , I IOX,IHM,6X,2HRE,8X,IHK,8X,4HFREQ) 2002 FORMAT(2X,15,2X,LI,3X,8H STEADY,2X,2(F5.1,4H DEG...C-,FIO.6) 7 2007 FORMAT(1l,EVH ALPHA,3X, IHQ ,3X,13C2X,2HCP,I2,X),4X,2C.,, I 5X,2RCD,5X,2HCM). 2008 FORMIAT(14X,13(2X32HCP,12,1X)//) 2009 FORMAT(2X...4 - .. ~ 4I. * ’~ -~ 4. A 441 4 * * 4.. 9 S ) td " p.- j ~-- -~ "U ".4 1: U, lk~ 0~ .4 0" A, 9 (9 0U 9? 0 ~ V ~ - 0 * qI; ow.. * 00 - . **. 4
Code of Federal Regulations, 2012 CFR
2012-07-01
... Madison Co. in Richmond X Rest of Madison Co X Magoffin County X Marion County X Marshall County X Martin... X Magoffin County X Marion County X Marshall County X Martin County X Mason County X Meade County X... Marshall County Unclassifiable/Attainment Martin County Unclassifiable/Attainment Mason County...
Code of Federal Regulations, 2012 CFR
2012-07-01
... Benton County X Bolivar County X Calhoun County X Carroll County X Chickasaw County X Choctaw County X... Benton County X Bolivar County X Calhoun County X Carroll County X Chickasaw County X Choctaw County X... Calhoun County Carroll County Chickasaw County Choctaw County Claiborne County Clarke County Clay County...
Code of Federal Regulations, 2013 CFR
2013-07-01
... Benton County X Bolivar County X Calhoun County X Carroll County X Chickasaw County X Choctaw County X... Benton County X Bolivar County X Calhoun County X Carroll County X Chickasaw County X Choctaw County X... Calhoun County Carroll County Chickasaw County Choctaw County Claiborne County Clarke County Clay County...
Code of Federal Regulations, 2010 CFR
2010-07-01
... Lee County X Leflore County X Lincoln County X Lowndes County X Madison County X Marion County X... Lee County X Leflore County X Lincoln County X Lowndes County X Madison County X Marion County X... County Kemper County Lafayette County Lamar County Lauderdale County Lawrence County Leake County Lee...
Code of Federal Regulations, 2011 CFR
2011-07-01
... Lee County X Leflore County X Lincoln County X Lowndes County X Madison County X Marion County X... Lee County X Leflore County X Lincoln County X Lowndes County X Madison County X Marion County X... County Kemper County Lafayette County Lamar County Lauderdale County Lawrence County Leake County Lee...
Study of Increasing Lead Times in Major Weapon Systems Acquisition.
1982-07-31
Conduit Covers X X X Connectors, Electrical X X X X X Control Systems (Auto- mated, Boiler) X Davit, Boat, Power- Opera.ted X Diodes X X X X A iX...tubes. Other end uses include washers in computer equipment, electrical insulators in motors and generators, and retardation plates in lasers . Supply...relays, electron tubes, printed circuits, and resistors. Platinum is also used in dentistry and for jewelry. Supply, A small amount of platinum (less
Code of Federal Regulations, 2014 CFR
2014-07-01
... Benton County X Bolivar County X Calhoun County X Carroll County X Chickasaw County X Choctaw County X... Alcorn County X Amite County X Attala County X Benton County X Bolivar County X Calhoun County X Carroll... County Attala County Benton County Bolivar County Calhoun County Carroll County Chickasaw County Choctaw...
Code of Federal Regulations, 2010 CFR
2010-07-01
... Lamar County X Lanier County X Laurens County X Lee County X Liberty County X Lincoln County X Long... Lamar County X Lanier County X Laurens County X Lee County X Liberty County X Lincoln County X Long... County Jenkins County Johnson County Jones County Lamar County Lanier County Laurens County Lee County...
40 CFR 81.341 - South Carolina.
Code of Federal Regulations, 2011 CFR
2011-07-01
... County X Laurens County X Lee County X Lexington County X McCormick County X Marion County X Marlboro... X Jasper County X Kershaw County X Lancaster County X Laurens County X Lee County X Lexington County... County Kershaw County Lancaster County Laurens County Lee County Lexington County Marion County Marlboro...
40 CFR 81.341 - South Carolina.
Code of Federal Regulations, 2010 CFR
2010-07-01
... County X Laurens County X Lee County X Lexington County X McCormick County X Marion County X Marlboro... X Jasper County X Kershaw County X Lancaster County X Laurens County X Lee County X Lexington County... County Kershaw County Lancaster County Laurens County Lee County Lexington County Marion County Marlboro...
Code of Federal Regulations, 2011 CFR
2011-07-01
... Lamar County X Lanier County X Laurens County X Lee County X Liberty County X Lincoln County X Long... Lamar County X Lanier County X Laurens County X Lee County X Liberty County X Lincoln County X Long... County Jenkins County Johnson County Jones County Lamar County Lanier County Laurens County Lee County...
Code of Federal Regulations, 2012 CFR
2012-07-01
... Jasper County X Jeff Davis County X Jefferson County X Jenkins County X Johnson County X Jones County X... Jasper County X Jeff Davis County X Jefferson County X Jenkins County X Johnson County X Jones County X... County Jenkins County Johnson County Jones County Lamar County Lanier County Laurens County Lee County...
Code of Federal Regulations, 2014 CFR
2014-07-01
... Jasper County X Jeff Davis County X Jefferson County X Jenkins County X Johnson County X Jones County X... Jenkins County X Johnson County X Jones County X Lamar County X Lanier County X Laurens County X Lee... County Jasper County Jeff Davis County Jefferson County Jenkins County Johnson County Jones County Lamar...
Code of Federal Regulations, 2013 CFR
2013-07-01
... Jasper County X Jeff Davis County X Jefferson County X Jenkins County X Johnson County X Jones County X... Jasper County X Jeff Davis County X Jefferson County X Jenkins County X Johnson County X Jones County X... County Jenkins County Johnson County Jones County Lamar County Lanier County Laurens County Lee County...
Middle-Term Loss Prediction Models for the Air Force’s Enlisted Force Management System
1987-12-01
326XOD .056152 2C7X2 .0481661 27ZZZ .100352 306X0 .032463 326X3A .075909 20700 .0562272 271X1 .086368 306X1 .045301 326X3B .041313 20799 .0562272...5836 32199 .6233 341X7 .5067 20700 .5134 296X0 .58:36 322X2A .6233 341ZZ .5067 20799 .5134 297X0 .5836 322X2B .6662 34100 .5067 208X0 .5134 30100 .5947...3206 302X0 .276323 :325X1 .372328 362X1 .3467,19 20799 .313206 302X1 .376280 32599 379938 362X3 .362314 208X0 .314906 30299 .376280 326X0C .379938
Reasoning about Human Participation in Self-Adaptive Systems
2015-01-16
Cheng et al. [19] X X X X Oreizy et al. [25] X X Dorn & Taylor [14] X X X Business Process BPMN [27] X X Modelling WSBPEL4People [13] X X Cyber-Human...ter Hofstede, and N. Russell. On the suitability of BPMN for business process modelling. In S. Dustdar, J. L. Fiadeiro, and A. P. Sheth, editors
36 CFR 294.29 - List of designated Idaho Roadless Areas.
Code of Federal Regulations, 2010 CFR
2010-07-01
... Perce Rapid River 922 X X Nez Perce Salmon Face 855 X Nez Perce Selway Bitterroot X Nez Perce Silver... Payette Snowbank 924 X Payette Sugar Mountain 014 X Salmon Agency Creek 512 X X Salmon Allan Mountain 946 X X Salmon Anderson Mountain 942 X Salmon Blue Joint Mountain 941 X Salmon Camas Creek 901 X Salmon...
40 CFR 81.334 - North Carolina.
Code of Federal Regulations, 2012 CFR
2012-07-01
... Lee County X Lenoir County X Lincoln County X McDowell County X Macon County X Madison County X Martin... Lee County X Lenoir County X Lincoln County X McDowell County X Macon County X Madison County X Martin... County Lenoir County Lincoln County Macon County Madison County Martin County McDowell County Mecklenburg...
40 CFR 81.334 - North Carolina.
Code of Federal Regulations, 2010 CFR
2010-07-01
... Lee County X Lenoir County X Lincoln County X McDowell County X Macon County X Madison County X Martin... Lee County X Lenoir County X Lincoln County X McDowell County X Macon County X Madison County X Martin... Hertford County Hoke County Hyde County Iredell County Jackson County Johnston County Jones County Lee...
40 CFR 81.334 - North Carolina.
Code of Federal Regulations, 2011 CFR
2011-07-01
... Lee County X Lenoir County X Lincoln County X McDowell County X Macon County X Madison County X Martin... Lee County X Lenoir County X Lincoln County X McDowell County X Macon County X Madison County X Martin... Hertford County Hoke County Hyde County Iredell County Jackson County Johnston County Jones County Lee...
Finite parametrization of solutions of equations in a free monoid. II
NASA Astrophysics Data System (ADS)
Makanin, G. S.
2004-04-01
In the preceding paper of the author parametrizing functions Fi, Th, Ro were introduced depending on word variables, positive-integer variables, and variables whose values are finite sequences of positive-integer variables. With the help of the parametrizing functions Fi, Th, Ro finite formulae are written out for the family of solutions of every equation of the form \\varphi(x_1,x_2,x_3) x_4=\\psi(x_1,x_2,x_3) x_5, where \\varphi(x_1,x_2,x_3) and \\psi(x_1,x_2,x_3) are arbitrary words in the alphabet x_1, x_2, x_3 in a free monoid.
21 CFR 1002.1 - Applicability.
Code of Federal Regulations, 2011 CFR
2011-04-01
... (1050.10) X X X X X X Diagnostic ultrasound X Medical ultrasound other than therapy or diagnostic X X Nonmedical ultrasound X 1However, authority to inspect all appropriate documents supporting the adequacy of a...
21 CFR 1002.1 - Applicability.
Code of Federal Regulations, 2013 CFR
2013-04-01
... (1050.10) X X X X X X Diagnostic ultrasound X Medical ultrasound other than therapy or diagnostic X X Nonmedical ultrasound X 1However, authority to inspect all appropriate documents supporting the adequacy of a...
21 CFR 1002.1 - Applicability.
Code of Federal Regulations, 2012 CFR
2012-04-01
... (1050.10) X X X X X X Diagnostic ultrasound X Medical ultrasound other than therapy or diagnostic X X Nonmedical ultrasound X 1However, authority to inspect all appropriate documents supporting the adequacy of a...
21 CFR 1002.1 - Applicability.
Code of Federal Regulations, 2010 CFR
2010-04-01
... (1050.10) X X X X X X Diagnostic ultrasound X Medical ultrasound other than therapy or diagnostic X X Nonmedical ultrasound X 1However, authority to inspect all appropriate documents supporting the adequacy of a...
21 CFR 1002.1 - Applicability.
Code of Federal Regulations, 2014 CFR
2014-04-01
... (1050.10) X X X X X X Diagnostic ultrasound X Medical ultrasound other than therapy or diagnostic X X Nonmedical ultrasound X 1However, authority to inspect all appropriate documents supporting the adequacy of a...
Federal Register 2010, 2011, 2012, 2013, 2014
2010-02-26
.... JJJJ Paper and Other Web X X X Coating. KKKK Surface Coating of X X X Metal Cans. MMMM Miscellaneous... X X Facilities. S Pulp and Paper X T Halogenated Solvent Cleaning.. X X U Group I Polymers and... Automobiles X and Light-Duty Trucks. JJJJ Paper and Other Web Coating... X KKKK Surface Coating of Metal Cans...
Differintegration: The One Branch of Calculus
ERIC Educational Resources Information Center
Berry, Andrew J.
2007-01-01
How might one define a functional operator D[superscript I]f(x), say for f(x) = 1 + x[superscript 2] + sin x, such that D[superscript +1](1 + x[superscript 2] + sin x) = 2x + cos x and D[superscript -1](1 + x[superscript 2] + sin x) = x + x[superscript 3]/3 - cos x? Our task in this article is to describe such an operator using a single formula…
Burkholderia pseudomallei Data Gap Analysis
2015-11-01
000 x E -10 1.013 25 x E +2 1.000 000 x E +2 1.000 000 x E -28 1.054 350 x E +3 4.184 000 4.184 000 x E -2 3.700 000 x E +1...1.745 329 x E -2 t = (t f + 459.67)/1.8 1.602 19 x E -19 1.000 000 x E -7 1.000 000 x E -7 3.048 000 x E -1 1.355 818 3.785 412 x E -3 2.540... 000 x E -2 1.000 000 x E +9 1.000 000 4.183 4.448 222 x E +3 6.894 757 x E +3 1.000 000 x E +2 1.000
Code of Federal Regulations, 2014 CFR
2014-07-01
...: Carroll County X Henry County X Mercer County X Rock Island County X Whiteside County X AQCR 70: Madison... X AQCR 72: Massac County X Alexander County X Johnson County X Pope County X Pulaski County X Union... Unclassifiable/Attainment Johnson County Unclassifiable/Attainment Kane County Unclassifiable/Attainment Kankakee...
Walia, Abhishek; Mehta, Preeti; Guleria, Shiwani; Shirkot, Chand Karan
2015-12-01
The effects of yeast extract (X 1 ), NH 4 NO 3 (X 2 ), peptone (X 3 ), urea (X 4 ), CMC (X 5 ), Tween 20 (X 6 ), MgSO 4 (X 7 ), and CaCO 3 (X 8 ) on production of xylanase from Cellulosimicrobium cellulans CKMX1 were optimized by statistical analysis using response surface methodology (RSM). The RSM was used to optimize xylanase production by implementing the Central composite design. Statistical analysis of the results showed that the linear, interaction and quadric terms of these variables had significant effects. However, only the linear effect of X 4 , X 5 , interaction effect of X 1 X 7 , X 1 X 8 , X 2 X 3 , X 2 X 8 , X 3 X 6 , X 3 X 8 , X 4 X 6 , X 4 X 7 , X 5 X 7 , X 5 X 8 and quadratic effect of X 3 2 , X 5 2 and X 7 2 found to be insignificant terms in the quadratic model and had no response at significant level. The minimum and maximum xylanase production obtained was 331.50 U/g DBP and 1027.65 U/g DBP, respectively. The highest xylanase activity was obtained from Run No. 30, which consisted of yeast extract (X 1 ), 1.00 g (%); NH 4 NO 3 (X 2 ), 0.20 g (%); peptone (X 3 ), 1.00 g (%); urea (X 4 ), 10 mg (%); CMC (X 5 ), 1.00 g (%); Tween 20 (X 6 ), 0.02 mL (%); CaCO 3 (X 7 ), 0.50 g (%) and MgSO 4 (X 8 ), 9.0 g (%). The optimization resulted in 3.1-fold increase of xylanase production, compared with the lowest xylanase production of 331.50 U/g DBP after 72 h of incubation in stationary flask experiment. Application of cellulase-free xylanase in pulp biobleaching from C. cellulans CKMX1 under C-E P -D sequence has been shown to bring about a 12.5 % reduction of chlorine, decrease of 0.8 kappa points (40 %), and gain in brightness was 1.42 % ISO points in 0.5 % enzyme treated pulp as compared to control.
Software and the Virus Threat: Providing Authenticity in Distribution
1991-03-01
Classification) SOFTWARE A" D THE VIRUS THREAT: PROVIDING AUTHENTICITY IN DISTRIBUTION 12. PERSONAL AUTHOR( S ) LAVUNTURE, GEORGE M. 13&. TYPE OF REPORT 1 3b...swapping open the code ampering. Re -authentication would then be required prior to regaining ;ntrol. 30 V . AUTHENTICATION MIRTHODS This section examines...x. n/a v mis 15) .. . ... x x ... .074 I .r ..... x . . x x x.x. 3880 S amno 3) . • ..... .. . I. ... 2000 .d0O (3) x x x x I . . . x x
Federal Register 2010, 2011, 2012, 2013, 2014
2013-04-04
... Gasoline R X X Distribution (stage 1). 9 Pulp & Paper I. S X X 10 Halogenated T X X Solvent Cleaning. 11... Fiberglass. 56 Auto & Light IIII X X Duty Truck (coating). 57 Paper & Other JJJJ X X Webs. 58 Metal Can KKKK... & Paper MACT I X T Halogenated Solvent X U Polymers & Resins/Group I...... X W Epoxy Resins and Non-Nylon...
14 CFR Section 22 - General Reporting Instructions
Code of Federal Regulations, 2014 CFR
2014-01-01
... aircraft engines A X X X P-1.1 Statement of operations SA (2) NA NA P-1.2 Statement of operations Q (1) X X P-1(a) Interim operations report M X X X P-2 Notes to RSPA Form 41 report Q (1) X X P-5.1 Aircraft operating expenses Q(1), SA(2) X NA NA P-5.2 Aircraft operating expenses Q NA X X P-6 Operating expenses by...
14 CFR Section 22 - General Reporting Instructions
Code of Federal Regulations, 2011 CFR
2011-01-01
... aircraft engines A X X X P-1.1 Statement of operations SA (2) NA NA P-1.2 Statement of operations Q (1) X X P-1(a) Interim operations report M X X X P-2 Notes to RSPA Form 41 report Q (1) X X P-5.1 Aircraft operating expenses Q(1), SA(2) X NA NA P-5.2 Aircraft operating expenses Q NA X X P-6 Operating expenses by...
14 CFR Section 22 - General Reporting Instructions
Code of Federal Regulations, 2013 CFR
2013-01-01
... aircraft engines A X X X P-1.1 Statement of operations SA (2) NA NA P-1.2 Statement of operations Q (1) X X P-1(a) Interim operations report M X X X P-2 Notes to RSPA Form 41 report Q (1) X X P-5.1 Aircraft operating expenses Q(1), SA(2) X NA NA P-5.2 Aircraft operating expenses Q NA X X P-6 Operating expenses by...
14 CFR 22 - General Reporting Instructions
Code of Federal Regulations, 2012 CFR
2012-01-01
... aircraft engines A X X X P-1.1 Statement of operations SA (2) NA NA P-1.2 Statement of operations Q (1) X X P-1(a) Interim operations report M X X X P-2 Notes to RSPA Form 41 report Q (1) X X P-5.1 Aircraft operating expenses Q(1), SA(2) X NA NA P-5.2 Aircraft operating expenses Q NA X X P-6 Operating expenses by...
Code of Federal Regulations, 2013 CFR
2013-07-01
... Protection of Environment ENVIRONMENTAL PROTECTION AGENCY (CONTINUED) AIR PROGRAMS (CONTINUED) DESIGNATION OF... Chesapeake X City of Franklin X City of Hampton X City of Newport News X City of Norfolk X City of Poquoson X... York County X City of Chesapeake X City of Franklin X City of Hampton X City of Newport News X City of...
Code of Federal Regulations, 2014 CFR
2014-07-01
... Protection of Environment ENVIRONMENTAL PROTECTION AGENCY (CONTINUED) AIR PROGRAMS (CONTINUED) DESIGNATION OF... Chesapeake X City of Franklin X City of Hampton X City of Newport News X City of Norfolk X City of Poquoson X... Hampton X City of Newport News X City of Norfolk X City of Poquoson X City of Portsmouth X City of Suffolk...
Code of Federal Regulations, 2012 CFR
2012-07-01
... Protection of Environment ENVIRONMENTAL PROTECTION AGENCY (CONTINUED) AIR PROGRAMS (CONTINUED) DESIGNATION OF... Chesapeake X City of Franklin X City of Hampton X City of Newport News X City of Norfolk X City of Poquoson X... York County X City of Chesapeake X City of Franklin X City of Hampton X City of Newport News X City of...
DOE Office of Scientific and Technical Information (OSTI.GOV)
Jaya Shankar Tumuluru; Shahab Sokhansanj; Sukumar Bandyopadhyay
Changes in proximate composition of fish and rice flour coextrudates like moisture, protein, and fat content were studied with respect to extrusion process v ariables like barrel temperature, x1 (100–200 degrees C); screw speed, x2 (70–110 rpm); fish content of the feed, x3 (5–45 percent); and feed moisture content, x4 (20–60 percent). Experiments were conducted at five levels of the process variables based on rotatable experimental design. Response surface models (RSM) were developed that adequately described the changes in moisture, protein, and fat content of the extrudates based on the coeff icient of determination (R2) values of 0.95, 0.99, andmore » 0.94. ANOVA analysis indicated that extrudate moisture content was influenced by x4, protein content by x1 and x3, and fat content by x3 and x4 at P < 0.001. Trends based on response surf ace plots indicated that the x1 of about 200 degrees C, x2 of about 90 rpm, x3 of about 25%, and x4 of about 20% minimized the moisture in the extrudates. Protein content was maximized at x1 of 100 degrees C, x2 > 80 rpm, x3 of about 45 percent, and x4 > 50 percent, and fat content was minimized at x1 of about 200 degrees C, x2 of about 85–95 rpm, x3 < 15 percent, and x4 of about >50 percent. Optimized process variables based on a genetic algorithm (GA) for minimum moisture and fat content and maximum protein content were x1 = 199.86, x2 = 109.86, x3 = 32.45, x4 = 20.03; x1 = 199.71, x2 = 90.09, x3 = 15.27, x4 = 58.47; and x1 = 102.97, x2 = 107.67, x3 = 44.56, x4 = 59.54. The predicted values were 17.52 percent, 0.57 percent, and 46.65 percent. Based on the RSM and GA analy sis, extrudate moisture and protein content was influenced by x1, x3, and x4 and fat content by x2, x3, and x4.« less
Thin film dielectric composite materials
Jia, Quanxi; Gibbons, Brady J.; Findikoglu, Alp T.; Park, Bae Ho
2002-01-01
A dielectric composite material comprising at least two crystal phases of different components with TiO.sub.2 as a first component and a material selected from the group consisting of Ba.sub.1-x Sr.sub.x TiO.sub.3 where x is from 0.3 to 0.7, Pb.sub.1-x Ca.sub.x TiO.sub.3 where x is from 0.4 to 0.7, Sr.sub.1-x Pb.sub.x TiO.sub.3 where x is from 0.2 to 0.4, Ba.sub.1-x Cd.sub.x TiO.sub.3 where x is from 0.02 to 0.1, BaTi.sub.1-x Zr.sub.x O.sub.3 where x is from 0.2 to 0.3, BaTi.sub.1-x Sn.sub.x O.sub.3 where x is from 0.15 to 0.3, BaTi.sub.1-x Hf.sub.x O.sub.3 where x is from 0.24 to 0.3, Pb.sub.1-1.3x La.sub.x TiO.sub.3+0.2x where x is from 0.23 to 0.3, (BaTiO.sub.3).sub.x (PbFeo.sub.0.5 Nb.sub.0.5 O.sub.3).sub.1-x where x is from 0.75 to 0.9, (PbTiO.sub.3).sub.- (PbCo.sub.0.5 W.sub.0.5 O.sub.3).sub.1-x where x is from 0.1 to 0.45, (PbTiO.sub.3).sub.x (PbMg.sub.0.5 W.sub.0.5 O.sub.3).sub.1-x where x is from 0.2 to 0.4, and (PbTiO.sub.3).sub.x (PbFe.sub.0.5 Ta.sub.0.5 O.sub.3).sub.1-x where x is from 0 to 0.2, as the second component is described. The dielectric composite material can be formed as a thin film upon suitable substrates.
Pre-vector variational inequality
DOE Office of Scientific and Technical Information (OSTI.GOV)
Lin, Lai-Jiu
1994-12-31
Let X be a Hausdorff topological vector space, (Y, D) be an ordered Hausdorff topological vector space ordered by convex cone D. Let L(X, Y) be the space of all bounded linear operator, E {improper_subset} X be a nonempty set, T : E {yields} L(X, Y), {eta} : E {times} E {yields} E be functions. For x, y {element_of} Y, we denote x {not_lt} y if y - x intD, where intD is the interior of D. We consider the following two problems: Find x {element_of} E such that < T(x), {eta}(y, x) > {not_lt} 0 for all y {element_of}more » E and find x {element_of} E, < T(x), {eta}(y, x) > {not_gt} 0 for all y {element_of} E and < T(x), {eta}(y, x) >{element_of} C{sub p}{sup w+} = {l_brace} {element_of} L(X, Y) {vert_bar}< l, {eta}(x, 0) >{not_lt} 0 for all x {element_of} E{r_brace} where < T(x), y > denotes linear operator T(x) at y, that is T(x), (y). We called Pre-VVIP the Pre-vector variational inequality problem and Pre-VCP complementary problem. If X = R{sup n}, Y = R, D = R{sub +} {eta}(y, x) = y - x, then our problem is the well-known variational inequality first studies by Hartman and Stampacchia. If Y = R, D = R{sub +}, {eta}(y, x) = y - x, our problem is the variational problem in infinite dimensional space. In this research, we impose different condition on T(x), {eta}, X, and < T(x), {eta}(y, x) > and investigate the existences theorem of these problems. As an application of one of our results, we establish the existence theorem of weak minimum of the problem. (P) V - min f(x) subject to x {element_of} E where f : X {yields} Y si a Frechet differentiable invex function.« less
Superfund Reauthorization 1994: DoD’s Opportunity to Clean Up Its Hazardous Waste Act
1994-04-01
AFB AR x Edwards AFB CA x Eielson AFB AK x Ellsworth AFB SD x Elmendorf AFB AK x England AFB LA x Fairchild AFB WA x F.E. Warren AFB WY x George AFB CA...amount of toxins produced, substances such as PCBs, dioxins , cyanides, heavy metals, pesticides, residues, alkalines, and acids have been emitted into...4 TX x *AFP 144 AZ x AFP PKUS CO x Andersen AFB GU x Bergstrom AFB TX x Carswell AFB TX x Castle AFB
2014-12-01
X Establish the limits of the areas of interest X X Determine intelligence and information gaps X X X Describe the impact of the battlespace on...X X X Identify critical gaps X X X X X DRDC-RDDC-2014-R136 9 Table 2: Mapping tools and functionalities. Looking at Table 1 and...it would seem that taking on requirements from IPB/IPOE Steps 3 and 4, although possibly much more challenging, is likely to yield more useful results
Surface-Finish Measurement with Interference Microscopes,
1977-02-01
Microscope 17 Multiple-Beam Interference Microscope .. 25 Fringes of Equal Chromatic Order 27 Nomarski Polarization-Contrast Technique 33...characteristics of each instrument: the double and multiple-beam interferometer, the FECO fringe interferometer, and the Nomarski polarization contrast...328X Beam Reichert 8X 0.15 2.22 87 33X Nomarski 16X 0.25 1.33 52 55X 203X Technique 32X 0.40 0.83 33 87X 395X 45 X 0.65 0.51 20 142X 567 X 80X
Code of Federal Regulations, 2011 CFR
2011-07-01
... X Coffee County X Crockett County X Cumberland County X Those portions of Davidson County within a... Clay County X Cocke County X Coffee County X Crockett County X Cumberland County X Davidson County X... County Claiborne County Clay County Cocke County Coffee County Crockett County Cumberland County Davidson...
Code of Federal Regulations, 2010 CFR
2010-07-01
... X Coffee County X Crockett County X Cumberland County X Those portions of Davidson County within a... Clay County X Cocke County X Coffee County X Crockett County X Cumberland County X Davidson County X... County Claiborne County Clay County Cocke County Coffee County Crockett County Cumberland County Davidson...
Code of Federal Regulations, 2012 CFR
2012-07-01
... Rock Island County X Whiteside County X AQCR 70: Madison County: Wood River Twp X Alton Twp X All other... Johnson County X Pope County X Pulaski County X Union County X AQCR 73 Boone County X De Kalb County X... Jersey County Unclassifiable/Attainment Jo Daviess County Unclassifiable/Attainment Johnson County...
Code of Federal Regulations, 2013 CFR
2013-07-01
... Rock Island County X Whiteside County X AQCR 70: Madison County: Wood River Twp X Alton Twp X All other... Johnson County X Pope County X Pulaski County X Union County X AQCR 73 Boone County X De Kalb County X... Jersey County Unclassifiable/Attainment Jo Daviess County Unclassifiable/Attainment Johnson County...
Code of Federal Regulations, 2014 CFR
2014-07-01
... Stationary Combustion Turbines X X LLLL New Sewage Sludge Incineration Units OOOO Crude Oil and Natural Gas... Dakota, South Dakota, Utah, Wyoming) Director, Air and Toxics Technical Enforcement Program, Office of... Gas Turbines X X X HH Lime Plants X X X KK Lead Acid Battery Manufacturing Plants X X LL Metallic...
Code of Federal Regulations, 2013 CFR
2013-07-01
... Stationary Combustion Turbines X X LLLL New Sewage Sludge Incineration Units OOOO Crude Oil and Natural Gas... Dakota, South Dakota, Utah, Wyoming) Director, Air and Toxics Technical Enforcement Program, Office of... Gas Turbines X X X HH Lime Plants X X X KK Lead Acid Battery Manufacturing Plants X X LL Metallic...
Code of Federal Regulations, 2010 CFR
2010-07-01
... County X Woodford County X Lee County X AQCR 66: Champaign County X Clark County X Coles County X... Washington County X AQCR 71: Bureau County: Shelby Twp X All other Bureau twps X La Salle County X Lee County.../Attainment La Salle County Unclassifiable/Attainment Lawrence County Unclassifiable/Attainment Lee County...
Code of Federal Regulations, 2011 CFR
2011-07-01
... County X Woodford County X Lee County X AQCR 66: Champaign County X Clark County X Coles County X... Washington County X AQCR 71: Bureau County: Shelby Twp X All other Bureau twps X La Salle County X Lee County.../Attainment La Salle County Unclassifiable/Attainment Lawrence County Unclassifiable/Attainment Lee County...
40 CFR 63.99 - Delegated Federal authorities.
Code of Federal Regulations, 2010 CFR
2010-07-01
... (stage 1) R X 9 Pulp & Paper I S X 10 Halogenated Solvent Cleaning T X 11 Polymer & Resins 1 U X 12... Sterilization O X 7 Chromium Cooling Towers Q X 8 Gasoline Distribution (stage 1) R X 9 Pulp & Paper I S X 10... R Gasoline Distribution X S Pulp & Paper MACT I X T Halogenated Solvent X U Polymers & Resins/Group...
Technologies for Energy from Biomass by Direct Combustion, Gasification, and Liquefaction.
1981-05-01
1980 1982 1984 Development Alberta Industrial Dev. X American Fyr. Feeder X Andco, Inc. X Applied Engineering Co., Inc. X Biomass Corp. X Bio-Solar x...Feeder ANDCO, Inc. Applied Engineering Company Biomass Corporation Bio-Solar Research and Development Corporation Combustion Power Company, Inc. Davy...Andco. Inc. X Applied Engineering Co., Inc. X Biomass Corp. X , Big-Solar .X I Combustion Power .. XI Davy Powergas X j Dekalb Acresearch, Inc.- x Duvant
Federal Laws Relating to Cybersecurity: Overview and Discussion of Proposed Revisions
2013-06-20
originally introduced in March.19 Several other Senate bills would have addressed specific aspects of cybersecurity, such as data breaches of personal...H.R. 3674)c X X X Public awareness H.R. 756 X X X X Cybercrime law X X X Data breach notification X X Internet security...Revisions Congressional Research Service 20 Data Breach Notification. The White House Proposal and the Task Force Report would also both have set
1989-11-26
e(rrors.only x - F(ie..only -.errs x -f(ormat x -G(raph x x -g(eierate..ofr x -l(nline x -i(nhibit x -k(eep x x -L( ist x -M(ap x -m(airi x -N(ame x...erbose -e(rrors-.only C -CmIe to object -c/pu.type 20 -d(ebug -kieep -O(ptiznize <key+,> - S(ource..asm -u(pdate-lib <key.-> -x(ecution-.profile -L( ist ...generate execution-profile code. 2.1.12 Listing options: -C(ontext <value> Include 1 line of context with error 2.1.13.1 message. -L( ist Do not
Properties of Riesz fractional derivatives for Korteweg-de Vries solitons
NASA Astrophysics Data System (ADS)
Varlamov, Vladimir
2010-12-01
Riesz fractional derivatives are defined as fractional powers of the Laplacian, D α = (-Δ) α/2 for {α in mathbb{R}}. For the soliton solution of the Korteweg-de Vries equation, u 0( X) with X = x - 4 t, these derivatives, u α ( X) = D α u 0( X), and their Hilbert transforms, v α ( X) = - HD α u 0( X), can be expressed in terms of the full range Hurwitz Zeta functions ζ+( s, a) and ζ-( s, a), respectively. New properties are established for u α ( X) and v α ( X). It is proved that the functions w α ( X) = u α ( X) + iv α ( X) with α > -1 are solutions of the differential equation -fracd{dX}left(P_{α}(X)dw/dXright)+Q_{α}(X)w = λρ_{α}(X)w,qquad X in mathbb{R}, for λ = 1. Here P α ( X), ρ α ( X) > 0 and Q α ( X) is real. The Wronskian W[ u α , v α ] is proved to be positive for all α > -1 and {X in mathbb{R}}. An estimate is given of the number of zeros of u α ( X) and v α ( X) on any finite interval. The fact that W[ u α , v α ] > 0 leads to a new inequality for the Hurwitz Zeta functions.
2012-12-01
of MARSEC 2 13 Causing a fire or explosion, conducting blasting or setting off fireworks , including setting a flare or other signalling device...or explosion, conducting blasting or setting off fireworks , including setting a flare or other signalling device without port approval X X X X X X...explosion, conducting blasting or setting off fireworks , including setting a flare or other signalling device without port approval X X X X X X X Non
Federal Register 2010, 2011, 2012, 2013, 2014
2010-11-03
... Paper X X T Halogenated Solvent X X X Cleaning. U Group I Polymers and Resins X X W Epoxy Resins... Trucks. JJJJ Paper and Other Web Coating X X KKKK Surface Coating of Metal X X Cans. MMMM Miscellaneous...,'' ``us,'' and ``our'' refer to EPA. Table of Contents I. Background A. Delegation of NESHAP B. Clark...
2007-09-01
The Pattern Understood in Terms of Tactics 44 13.4 Variants 44 14 Microkernel Pattern 45 14.1 Problem 45 14.2 Solution 45 14.3 The Pattern...Figure 12: Model-View-Controller Pattern Structure 42 Figure 13: Presentation-Abstraction-Control Pattern Structure 43 Figure 14: Microkernel ...Presentation- Abstraction- Control X X X X Microkernel X X X X X Reflection X X Each pattern is described in more detail in the
14 CFR 139.203 - Contents of Airport Certification Manual.
Code of Federal Regulations, 2014 CFR
2014-01-01
... serving facilities or NAVAIDS that support air carrier operations X X X 8. A description of the system for.... Procedures for maintaining the safety areas, as required under § 139.309 X X X X 13. A plan showing the... accordance with §§ 139.315, 139.317 and 139.319 X X X X 17. A description of any approved exemption to...
14 CFR 139.203 - Contents of Airport Certification Manual.
Code of Federal Regulations, 2013 CFR
2013-01-01
... serving facilities or NAVAIDS that support air carrier operations X X X 8. A description of the system for.... Procedures for maintaining the safety areas, as required under § 139.309 X X X X 13. A plan showing the... accordance with §§ 139.315, 139.317 and 139.319 X X X X 17. A description of any approved exemption to...
14 CFR 139.203 - Contents of Airport Certification Manual.
Code of Federal Regulations, 2012 CFR
2012-01-01
... serving facilities or NAVAIDS that support air carrier operations X X X 8. A description of the system for.... Procedures for maintaining the safety areas, as required under § 139.309 X X X X 13. A plan showing the... accordance with §§ 139.315, 139.317 and 139.319 X X X X 17. A description of any approved exemption to...
14 CFR 139.203 - Contents of Airport Certification Manual.
Code of Federal Regulations, 2010 CFR
2010-01-01
... serving facilities or NAVAIDS that support air carrier operations X X X 8. A description of the system for.... Procedures for maintaining the safety areas, as required under § 139.309 X X X X 13. A plan showing the... accordance with §§ 139.315, 139.317 and 139.319 X X X X 17. A description of any approved exemption to...
14 CFR 139.203 - Contents of Airport Certification Manual.
Code of Federal Regulations, 2011 CFR
2011-01-01
... serving facilities or NAVAIDS that support air carrier operations X X X 8. A description of the system for.... Procedures for maintaining the safety areas, as required under § 139.309 X X X X 13. A plan showing the... accordance with §§ 139.315, 139.317 and 139.319 X X X X 17. A description of any approved exemption to...
Federal Register 2010, 2011, 2012, 2013, 2014
2011-03-18
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Structural and magnetic phase transitions in CeCu 6-xT x (T = Ag,Pd)
DOE Office of Scientific and Technical Information (OSTI.GOV)
Poudel, Lekhanath N.; De la cruz, Clarina; Payzant, E. Andrew
The structural and the magnetic properties of CeCu 6-xAg x (0 ≤ x ≤ 0.85) and CeCu 6-xPd x (0 ≤ x ≤ 0.4) have been studied using neutron diffraction, resonant ultrasound spectroscopy (RUS), x-ray diffraction measurements, and first principles calculations. The structural and magnetic phase diagrams of CeCu 6-xAg x and CeCu 6-xPd x as a function of Ag/Pd composition are reported. The end member, CeCu 6, undergoes a structural phase transition from an orthorhombic ( Pnma) to a monoclinic (P2 1/c) phase at 240 K. In CeCu 6-xAg x, the structural phase transition temperature (T s) decreases linearlymore » with Ag concentration and extrapolates to zero at x S ≈ 0.1. The structural transition in CeCu 6-xPd x remains unperturbed with Pd substitution within the range of our study. The lattice constant b slightly decreases with Ag/Pd doping, whereas a and c increase with an overall increase in the unit cell volume. Both systems, CeCu 6-xAg x and CeCu 6-xPd x, exhibit a magnetic quantum critical point (QCP), at x ≈ 0.2 and x ≈ 0.05, respectively. Near the QCP, long range antiferromagnetic ordering takes place at an incommensurate wave vector (δ 1 0 δ 2), where δ 1 ~ 0.62, δ 2 ~ 0.25, x = 0.125 for CeCu 6-xPd x and δ 1 ~ 0.64, δ 2 ~ 0.3, x = 0.3 for CeCu 6-xAg x. As a result, the magnetic structure consists of an amplitude modulation of the Ce moments which are aligned along the c axis of the orthorhombic unit cell.« less
Structural and magnetic phase transitions in CeCu 6-xT x (T = Ag,Pd)
Poudel, Lekhanath N.; De la cruz, Clarina; Payzant, E. Andrew; ...
2015-12-15
The structural and the magnetic properties of CeCu 6-xAg x (0 ≤ x ≤ 0.85) and CeCu 6-xPd x (0 ≤ x ≤ 0.4) have been studied using neutron diffraction, resonant ultrasound spectroscopy (RUS), x-ray diffraction measurements, and first principles calculations. The structural and magnetic phase diagrams of CeCu 6-xAg x and CeCu 6-xPd x as a function of Ag/Pd composition are reported. The end member, CeCu 6, undergoes a structural phase transition from an orthorhombic ( Pnma) to a monoclinic (P2 1/c) phase at 240 K. In CeCu 6-xAg x, the structural phase transition temperature (T s) decreases linearlymore » with Ag concentration and extrapolates to zero at x S ≈ 0.1. The structural transition in CeCu 6-xPd x remains unperturbed with Pd substitution within the range of our study. The lattice constant b slightly decreases with Ag/Pd doping, whereas a and c increase with an overall increase in the unit cell volume. Both systems, CeCu 6-xAg x and CeCu 6-xPd x, exhibit a magnetic quantum critical point (QCP), at x ≈ 0.2 and x ≈ 0.05, respectively. Near the QCP, long range antiferromagnetic ordering takes place at an incommensurate wave vector (δ 1 0 δ 2), where δ 1 ~ 0.62, δ 2 ~ 0.25, x = 0.125 for CeCu 6-xPd x and δ 1 ~ 0.64, δ 2 ~ 0.3, x = 0.3 for CeCu 6-xAg x. As a result, the magnetic structure consists of an amplitude modulation of the Ce moments which are aligned along the c axis of the orthorhombic unit cell.« less
NASA Astrophysics Data System (ADS)
Chen, Xiuli; Li, Xiaoxia; Yan, Xiao; Liu, Gaofeng; Zhou, Huanfu
2018-06-01
Perovskite solid solution ceramics of (Ba1- x Bi0.33 x Sr0.67 x )(Ti1- x Bi0.67 x V0.33 x )O3 and (Ba1- x Bi0.5 x Sr0.5 x )(Ti1- x Bi0.5 x Ti0.5 x )O3 (BBSTBV, BBSTBT, 0.02 ≤ x ≤ 0.2) were prepared by the traditional solid state reaction technique. The phase evolution, microstructure and dielectric properties of BBSTBV and BBSTBT ceramics were researched. X-Ray diffraction results illustrated that both BBSTBV and BBSTBT could form a homogenous solid solution which has a similar structure with BaTiO3. The optimized properties of (Ba0.8Bi0.1Sr0.1)(Ti0.8Bi0.1Ti0.1)O3 ceramics with stable ɛ r ( 1769-2293), small Δ ɛ/ ɛ 25 °C values (± 15%) over a broad temperature range from - 58 to 151 °C and low tan δ ≤ 0.03 from - 11 to 131 °C were obtained. In the high-temperature region, the relaxation and conduction process are attributed to the thermal activation and the oxygen vacancies may be the ionic charge carriers in perovskite ferroelectrics.
Robotic Vehicle Communications Interoperability
1988-08-01
starter (cold start) X X Fire suppression X Fording control X Fuel control X Fuel tank selector X Garage toggle X Gear selector X X X X Hazard warning...optic Sensors Sensor switch Video Radar IR Thermal imaging system Image intensifier Laser ranger Video camera selector Forward Stereo Rear Sensor control...optic sensors Sensor switch Video Radar IR Thermal imaging system Image intensifier Laser ranger Video camera selector Forward Stereo Rear Sensor
DOE Office of Scientific and Technical Information (OSTI.GOV)
Saeed, Y., E-mail: yasir_saeed54321@yahoo.co; Shaukat, A., E-mail: schaukat@gmail.co; Nazir, S., E-mail: nazirsafdar@gmail.co
2010-01-15
First principles calculations based on the density functional theory (DFT) within the local spin density approximation are performed to investigate the electronic structure and magnetic properties of Cr-based zinc blende diluted magnetic semiconductors Al{sub 1-x}Cr{sub x}X (X=N, P, As, Sb) for 0<=x<=0.50.The behaviour of magnetic moment of Al{sub 1-x}Cr{sub x}X at each Cr site as well as the change in the band gap value due to spin down electrons has been studied by increasing the concentration of Cr atom and through changing X from N to Sb. Furthermore, the role of p-d hybridization is analyzed in the electronic band structuremore » and exchange splitting of d-dominated bands. The interaction strength is stronger in Al{sub 1-x}Cr{sub x}N and becomes weaker in Al{sub 1-x}Cr{sub x}Sb. The band gap due to the spin down electrons decreases with the increased concentration of Cr in Al{sub 1-x}Cr{sub x}X, and as one moves down along the isoelectronic series in the group V from N to Sb. Our calculations also verify the half-metallic ferromagnetic character in Cr doped AlX. - Graphical abstract: The prototype structures of Cr doped AlX (X=N, P, As, Sb) compounds: (A) zinc blende AlP for x=0, (B) Cr{sub 1}Al{sub 7}P{sub 8} for x=0.125, (C) Cr{sub 1}Al{sub 3}P{sub 4} for x=0.25, (D) Cr{sub 1}Al{sub 1}P{sub 2} for x=0.5.« less
Martin, Elliot; Shreim, Amer; Paczuski, Maya
2010-01-01
We define an activity-dependent branching ratio that allows comparison of different time series X(t). The branching ratio b(x) is defined as b(x)=E[xi(x)/x]. The random variable xi(x) is the value of the next signal given that the previous one is equal to x, so xi(x)=[X(t+1) | X(t)=x]. If b(x)>1, the process is on average supercritical when the signal is equal to x, while if b(x)<1, it is subcritical. For stock prices we find b(x)=1 within statistical uncertainty, for all x, consistent with an "efficient market hypothesis." For stock volumes, solar x-ray flux intensities, and the Bak-Tang-Wiesenfeld (BTW) sandpile model, b(x) is supercritical for small values of activity and subcritical for the largest ones, indicating a tendency to return to a typical value. For stock volumes this tendency has an approximate power-law behavior. For solar x-ray flux and the BTW model, there is a broad regime of activity where b(x) approximately equal 1, which we interpret as an indicator of critical behavior. This is true despite different underlying probability distributions for X(t) and for xi(x). For the BTW model the distribution of xi(x) is Gaussian, for x sufficiently larger than 1, and its variance grows linearly with x. Hence, the activity in the BTW model obeys a central limit theorem when sampling over past histories. The broad region of activity where b(x) is close to one disappears once bulk dissipation is introduced in the BTW model-supporting our hypothesis that it is an indicator of criticality.
ACTDs: Management Plans as Predictors of Transition
2007-12-01
phase. Figure 2 shows the current ACTD funding model in place today and highlights the challenges involved in the process. Current ACTD Funding ... Model All other Sources (~70%) OSD AS&C Cash Resources (~30%) Army PE x PE x PE x PE x Navy PE x PE x PE x PE x USAF PE x PE x
Quadruples in the Four-Number Game with Large Termination Times
ERIC Educational Resources Information Center
Yueh, Wen-Chyuan; Cheng, Sui Sun
2002-01-01
The discrete dynamical system of absolute differences defined by the map [psi]( x[subscript 1] , x[subscript 2] , x[subscript 3] , x[subscript 4] ) = ([vertical line] x[subscript 2] - x[subscript 1] [vertical line], [vertical line] x[subscript 3] - x[subscript 2] [vertical line], [vertical line] x[subscript 4] - x[subscript 3] [vertical line],…
Video-Text Processing by Using Motorola 68020 CPU and its Environment
1991-03-01
x I x K x I I x 0 MUMC)I DUARTWE K I I 1 0 K x K x 0 M(DWE)II CRTCS 1 I x 1 0 x x x x x x 0 £RT x . 1 0 x 0 K K K 20 Table 3. THE SELECTION OF THE BUS...Appendix IV). When AS=O, A20=0, ROMCS= 1 , DUDCS=1I CRTCS =l1, the both of the DSACKO and DSACK1 outputs are asserted as seen in Figure 16. In this...Output h. Verifiation of CRTCS (CRT CONTROLLER Chip Select signal) Output In order to assert CRTCS , A21= 1 , A6=0, AS=0, as according to PALSELIN
Seebeck Coefficient of Cation-Substituted Disulfides CuCr1-x Fe x S2 and Cu1-x Fe x CrS2
NASA Astrophysics Data System (ADS)
Korotaev, Evgeniy V.; Syrokvashin, Mikhail M.; Filatova, Irina Yu.; Pelmenev, Konstantin G.; Zvereva, Valentina V.; Peregudova, Natalya N.
2018-03-01
The effect of cation substitution on the Seebeck coefficient of CuCr1-x Fe x S2 (x = 0 to 0.30) and Cu1-x Fe x CrS2 (x = 0 to 0.03) in the temperature range of 100 K to 450 K has been investigated. Increasing iron concentration led to a metal-insulator transition which suppressed the thermoelectric power. However, for low iron concentration (x < 0.03), the Seebeck coefficient of CuCr1-x Fe x S2 and Cu1-x Fe x CrS2 exceeded the values for the undoped copper-chromium disulfide matrix CuCrS2 at temperature below 300 K.
Oliveira, Luiz Fernando M; Brescovit, Antonio D
2015-06-29
The genus Xiruana Brescovit, 1997 is currently composed of four South American species: X. gracilipes (Keyserling) from Brazil, Bolivia and Argentina, X. affinis (Mello-Leitão) from Brazil, X. hirsuta (Mello-Leitão) from Venezuela, Brazil, Paraguay, Argentina and Uruguay, and X. tetraseta (Mello-Leitão) from Venezuela, Brazil and Paraguay. Of these, the last three are redescribed in this paper, including the first description of the females of X. hirsuta and X. tetraseta. Additionally, we describe thirteen new species: Xiruana pocone n. sp. from Brazil, Paraguay and Argentina; X. bifida n. sp. from Brazil and Paraguay; X. aymara n. sp. from Bolivia; X. cocha n. sp. from Peru; X. fiebrigi n. sp. from Paraguay, and X. ajuricaba n. sp., X. tribarrense n. sp., X. guaia n. sp., X. jaboticabal n. sp., X. minacu n. sp., X. tapirape n. sp., X. lusitania n. sp., X. silarae n. sp., all endemic to Brazil. The known geographical distribution of all species here presented is mapped.
DOE Office of Scientific and Technical Information (OSTI.GOV)
Haider, Ali, E-mail: ali.haider@bilkent.edu.tr, E-mail: biyikli@unam.bilkent.edu.tr; Kizir, Seda; Ozgit-Akgun, Cagla
In this work, the authors have performed sequential pulsed chemical vapor deposition of ternary B{sub x}Ga{sub 1-x}N and B{sub x}In{sub 1-x}N alloys at a growth temperature of 450 °C. Triethylboron, triethylgallium, trimethylindium, and N{sub 2} or N{sub 2}/H{sub 2} plasma have been utilized as boron, gallium, indium, and nitrogen precursors, respectively. The authors have studied the compositional dependence of structural, optical, and morphological properties of B{sub x}Ga{sub 1-x}N and B{sub x}In{sub 1-x}N ternary thin film alloys. Grazing incidence X-ray diffraction measurements showed that boron incorporation in wurtzite lattice of GaN and InN diminishes the crystallinity of B{sub x}Ga{sub 1-x}N and B{submore » x}In{sub 1-x}N sample. Refractive index decreased from 2.24 to 1.65 as the B concentration of B{sub x}Ga{sub 1-x}N increased from 35% to 88%. Similarly, refractive index of B{sub x}In{sub 1-x}N changed from 1.98 to 1.74 for increase in B concentration value from 32% to 87%, respectively. Optical transmission band edge values of the B{sub x}Ga{sub 1-x}N and B{sub x}In{sub 1-x}N films shifted to lower wavelengths with increasing boron content, indicating the tunability of energy band gap with alloy composition. Atomic force microscopy measurements revealed an increase in surface roughness with boron concentration of B{sub x}Ga{sub 1-x}N, while an opposite trend was observed for B{sub x}In{sub 1-x}N thin films.« less
1976-10-01
X> X ^^ X X E o lmm X X X X X > J Ä2 NX x xs 10 n N(P) X...to the cell through a stainless steel valve. The crystals and sample cylinder were repeatedly allowed to outgas at room temperature (under vacuum... 350 (1975). 3. J.J. Ewing and C.A. Brau, Appl. Phys. Lett. 27, 557(1975). 4. J.J. Ewing and C.A. Brau, Phys. Rev. A12, 129(1975). 5
Data Association Algorithms for Tracking Satellites
2008-02-05
series of (I) about the current estimate: x{k — l|fc — 1) x-(fc) = f[k, x{k - l\\k - 1)] + fx {k - l)[x{k - 1) - x{k - l\\k - 1)] + l/2^el[x(fc - 1) - x(A...l|ik - 1)]’ i=l ■ fxx{k - l)[x{k - 1) - x{k - l\\k - 1)] + higher-order terms + v(k - 1) (5) where e; is the ith Cartesian basis vector and fx ...34x x{k\\k - 1) = fx {k - l)x(fc - l|fc - 1) + l/2^e!;[x /(fc - l|fc - l)/^{fc - l)x(fc - l|fc - 1) t=l - TvifUk - l)P{k - l\\k - I)
39 CFR 3060.21 - Income report.
Code of Federal Regulations, 2014 CFR
2014-07-01
... 000s] FY 20xx FY 20xx-1 Percent change fromSPLY Percent change fromSPLY Revenue: $x,xxx $x,xxx xxx xx.x (1) Mail and Services Revenues xxx xxx xx xx.x (2) Investment Income x,xx x,xxx xxx xx.x (3) Total Competitive Products Revenue Expenses: (4) Volume-Variable Costs x,xxx x,xxx xxx xx.x (5) Product Specific...
39 CFR 3060.21 - Income report.
Code of Federal Regulations, 2012 CFR
2012-07-01
... 000s] FY 20xx FY 20xx-1 Percent change fromSPLY Percent change fromSPLY Revenue: $x,xxx $x,xxx xxx xx.x (1) Mail and Services Revenues xxx xxx xx xx.x (2) Investment Income x,xx x,xxx xxx xx.x (3) Total Competitive Products Revenue Expenses: (4) Volume-Variable Costs x,xxx x,xxx xxx xx.x (5) Product Specific...
39 CFR 3060.21 - Income report.
Code of Federal Regulations, 2013 CFR
2013-07-01
... 000s] FY 20xx FY 20xx-1 Percent change fromSPLY Percent change fromSPLY Revenue: $x,xxx $x,xxx xxx xx.x (1) Mail and Services Revenues xxx xxx xx xx.x (2) Investment Income x,xx x,xxx xxx xx.x (3) Total Competitive Products Revenue Expenses: (4) Volume-Variable Costs x,xxx x,xxx xxx xx.x (5) Product Specific...
39 CFR 3060.21 - Income report.
Code of Federal Regulations, 2011 CFR
2011-07-01
... 000s] FY 20xx FY 20xx-1 Percent change fromSPLY Percent change fromSPLY Revenue: $x,xxx $x,xxx xxx xx.x (1) Mail and Services Revenues xxx xxx xx xx.x (2) Investment Income x,xx x,xxx xxx xx.x (3) Total Competitive Products Revenue Expenses: (4) Volume-Variable Costs x,xxx x,xxx xxx xx.x (5) Product Specific...
46 CFR 199.10 - Applicability.
Code of Federal Regulations, 2010 CFR
2010-10-01
... provided otherwise in this Chapter, this part applies to all vessels inspected under U.S. law as set out in... 46 CFR 117 L Offshore Supply All 46 CFR 133 R—Part 167 Public Nautical School International voyage 3 X X X 4 X 5 R—Part 167 Public Nautical School All other services X X X 4 X 5 X X R—Part 168 Civilian...
39 CFR 3060.21 - Income report.
Code of Federal Regulations, 2010 CFR
2010-07-01
... 000s] FY 20xx FY 20xx-1 Percent change fromSPLY Percent change fromSPLY Revenue: $x,xxx $x,xxx xxx xx.x (1) Mail and Services Revenues xxx xxx xx xx.x (2) Investment Income x,xx x,xxx xxx xx.x (3) Total Competitive Products Revenue Expenses: (4) Volume-Variable Costs x,xxx x,xxx xxx xx.x (5) Product Specific...
Migeon, B R; Jeppesen, P; Torchia, B S; Fu, S; Dunn, M A; Axelman, J; Schmeckpeper, B J; Fantes, J; Zori, R T; Driscoll, D J
1996-01-01
We have previously reported functional disomy for X-linked genes in females with tiny ring X chromosomes and a phenotype significantly more abnormal than Turner syndrome. In such cases the disomy results from failure of these X chromosomes to inactivate because they lack DNA sequences essential for cis X inactivation. Here we describe a novel molecular mechanism for functional X disomy that is associated with maternal isodisomy. In this case, the severe mental retardation and multiple congenital abnormalities in a female with a mosaic 45,X/ 46,X,del(X)(q21.3-qter)/ 46X,r(X) karyotype are associated with overexpression of the genes within Xpter to Xq21.31 in many of her cells. Her normal X, ring X, and deleted linear X chromosomes originate from the same maternal X chromosome, and all are transcriptionally active. None expresses X inactive specific transcript (XIST), although the locus and region of the putative X inactivation center (XIC) are present on both normal and linear deleted X chromosomes. To our knowledge, this is the first report of a functional maternal X isodisomy, and the largest X chromosome to escape inactivation. In addition, these results (1) show that cis inactivation does not invariably occur in human females with two X chromosomes, even when the XIC region is present on both of them; (2) provide evidence for a critical time prior to the visible onset of X inactivation in the embryo when decisions about X inactivation are made; and (3) support the hypothesis that the X chromosome counting mechanism involves chromosomal imprinting, occurs prior to the onset of random inactivation, and is required for subsequent inactivation of the chromosome.
76 FR 38024 - Standards of Performance for New Stationary Sources
Federal Register 2010, 2011, 2012, 2013, 2014
2011-06-29
..., and Prior to July 23, 1984. Kb Volatile Organic Liquid Storage X Vessels (Including Petroleum Liquid... R Primary Lead Smelters X X S Primary Aluminum Reduction Plants X X T Phosphate Fertilizer Industry: X X Wet Process Phosphoric Acid Plants. U Phosphate Fertilizer Industry: X X Superphosphoric Acid...
The Xylaria names proposed by C. G. Lloyd
USDA-ARS?s Scientific Manuscript database
Seventy-one new Xylaria names that C. G. Lloyd proposed are annotated herein. Type and/or authentic materials of these names, when available, were studied. Twenty-four of these, including X. beccarii, X. brasiliensis, X. chordaeformis, X. cuneata, X. divisa, X. fimbriata, X. humosa, X. kedahae, X. l...
Balance times of multidimensional quasi-additive potentials for a measure-preserving semiflow
NASA Astrophysics Data System (ADS)
Dai, Xiongping
2013-12-01
Let \\theta\\colon X\\times{T}\\rightarrow X;\\ (x,t)\\mapsto{x{\\boldsymbol\\cdot} t} , where {T}={Z}_+ or {R}_+ , be a measure-preserving semiflow on a probability space (X,\\mathscr{F},\\mu) and given a d-dimensional measurable potential p\\colon X\\times{T}\\rightarrow{R}^d which is δ-quasi-additive with respect to θ, where δ ⩾ 0 namely, for μ-a.e. x ∈ X and for all s,t\\in{T} , \\begin{equation*}|p(x,t+s)-(p(x,t)+p(x{\\boldsymbol\\cdot} t,s))|\\le\\delta. \\end{equation*} We prove that if there exists a measurable {R}^d -valued function p*(x) such that \\begin{equation*}\\lim_{t\\to\\infty}\\frac{1}{t}p(x,t)=p^*(x)\\tqs for~\\mu-a.e.\\, x\\in X, \\end{equation*} then for μ-a.e. x ∈ X and any ε > 0, there holds the following tight control by p*(x): \\begin{equation*}{\\bf mes}\\left\\{t\\in{T}\\colon|p(x,t)-p^*(x)t|\\le\\varepsilon+ \\delta\\right\\}=\\infty, \\end{equation*} where mes{·} stands for the Lebesgue measure in the real line {R} or the counting measure in {Z} . This can be applied to the study of ergodic forced monotonic circle maps and of the normal numbers.
NASA Astrophysics Data System (ADS)
Ali, Rajjab; Gilani, Zaheer Abbas; Shahzad Shifa, Muhammad; Asghar, H. M. Noor Ul Huda Khan; Azhar Khan, Muhammad; Naeem Anjum, Muhammad; Nauman Usmani, Muhammad; Farooq Warsi, Muhammad; Khawaja, Imtiaz U.
2017-11-01
Four series nanocrystalline ferrites with nominal composition, NiZr x Co x Fe2-2x O4 (x = 0.0, 0.2, 0.4, 0.6, 0.8) Ni0.5Sn0.5Co x Mn x Fe2-2x O4 (x = 0.0, 0.2, 0.4, 0.6, 0.8), Mg1-x Ca x Ni y Fe2-y O4 (x = 0.0, 0.2, 0.4, 0.6, 0.8; y = 0, 04, 0.8, 1.2, 1.6) and Mg1-x Ni x Co y Fe2-y O4 (x,y = 0.0, 0.2, 0.4, 0.6, 0.8) have been fabricated using the microemulsion synthesis route. The synthesized materials are investigated for dc electrical resistivity measurements. The variation of dc electrical resistivity of these materials has been explainedon the basis of hopping mechanism of both holes and electrons.
A concatenated coding scheme for error control
NASA Technical Reports Server (NTRS)
Lin, S.
1985-01-01
A concatenated coding scheme for error control in data communications is analyzed. The inner code is used for both error correction and detection, however the outer code is used only for error detection. A retransmission is requested if the outer code detects the presence of errors after the inner code decoding. The probability of undetected error of the above error control scheme is derived and upper bounded. Two specific exmaples are analyzed. In the first example, the inner code is a distance-4 shortened Hamming code with generator polynomial (X+1)(X(6)+X+1) = X(7)+X(6)+X(2)+1 and the outer code is a distance-4 shortened Hamming code with generator polynomial (X+1)X(15+X(14)+X(13)+X(12)+X(4)+X(3)+X(2)+X+1) = X(16)+X(12)+X(5)+1 which is the X.25 standard for packet-switched data network. This example is proposed for error control on NASA telecommand links. In the second example, the inner code is the same as that in the first example but the outer code is a shortened Reed-Solomon code with symbols from GF(2(8)) and generator polynomial (X+1)(X+alpha) where alpha is a primitive element in GF(z(8)).
NASA Astrophysics Data System (ADS)
Pyt'ev, Yu. P.
2018-01-01
mathematical formalism for subjective modeling, based on modelling of uncertainty, reflecting unreliability of subjective information and fuzziness that is common for its content. The model of subjective judgments on values of an unknown parameter x ∈ X of the model M( x) of a research object is defined by the researcher-modeler as a space1 ( X, p( X), P{I^{\\bar x}}, Be{l^{\\bar x}}) with plausibility P{I^{\\bar x}} and believability Be{l^{\\bar x}} measures, where x is an uncertain element taking values in X that models researcher—modeler's uncertain propositions about an unknown x ∈ X, measures P{I^{\\bar x}}, Be{l^{\\bar x}} model modalities of a researcher-modeler's subjective judgments on the validity of each x ∈ X: the value of P{I^{\\bar x}}(\\tilde x = x) determines how relatively plausible, in his opinion, the equality (\\tilde x = x) is, while the value of Be{l^{\\bar x}}(\\tilde x = x) determines how the inequality (\\tilde x = x) should be relatively believed in. Versions of plausibility Pl and believability Bel measures and pl- and bel-integrals that inherit some traits of probabilities, psychophysics and take into account interests of researcher-modeler groups are considered. It is shown that the mathematical formalism of subjective modeling, unlike "standard" mathematical modeling, •enables a researcher-modeler to model both precise formalized knowledge and non-formalized unreliable knowledge, from complete ignorance to precise knowledge of the model of a research object, to calculate relative plausibilities and believabilities of any features of a research object that are specified by its subjective model M(\\tilde x), and if the data on observations of a research object is available, then it: •enables him to estimate the adequacy of subjective model to the research objective, to correct it by combining subjective ideas and the observation data after testing their consistency, and, finally, to empirically recover the model of a research object.
2012-01-01
were modified slightly for use in the study, including linking the widely used PTSD Checklist, Peritraumatic Dissociative Experiences Questionnaire...duration of unconsciousness, and altered mental state (AMS) (eg, confusion or dazed feeling or posttraumatic amnesia ). To ensure interrater...X X Dissociative Experiences Scale (DES) X — — X Janoff-Bulman World Assumptions Scale (WAS) X X X — Psychiatric symptoms PTSD Checklist (PCL) X X X X
Dispersal and spatial heterogeneity: Single species
DeAngelis, Donald L.; Ni, Wei-Ming; Zhang, Bo
2016-01-01
A recent result for a reaction-diffusion equation is that a population diffusing at any rate in an environment in which resources vary spatially will reach a higher total equilibrium biomass than the population in an environment in which the same total resources are distributed homogeneously. This has so far been proven by Lou for the case in which the reaction term has only one parameter, m(x)">m(x)m(x), varying with spatial location x">xx, which serves as both the intrinsic growth rate coefficient and carrying capacity of the population. However, this striking result seems rather limited when applies to real populations. In order to make the model more relevant for ecologists, we consider a logistic reaction term, with two parameters, r(x)">r(x)r(x) for intrinsic growth rate, and K(x)">K(x)K(x) for carrying capacity. When r(x)">r(x)r(x) and K(x)">K(x)K(x) are proportional, the logistic equation takes a particularly simple form, and the earlier result still holds. In this paper we have established the result for the more general case of a positive correlation between r(x)">r(x)r(x) and K(x)">K(x)K(x) when dispersal rate is small. We review natural and laboratory systems to which these results are relevant and discuss the implications of the results to population theory and conservation ecology.
Density of a semigroup in a Banach space
NASA Astrophysics Data System (ADS)
Borodin, P. A.
2014-12-01
We study conditions on a set M in a Banach space X which are necessary or sufficient for the set R(M) of all sums x_1+\\dots+x_n, x_k\\in M, to be dense in X. We distinguish conditions under which the closure \\overline{R(M)} is an additive subgroup of X, and conditions under which this additive subgroup is dense in X. In particular, we prove that if M is a closed rectifiable curve in a uniformly convex and uniformly smooth Banach space X, and does not lie in a closed half-space \\{x\\in X\\colon f(x)≥0\\}, f\\in X^*, and is minimal in the sense that every proper subarc of M lies in an open half-space \\{x\\in X\\colon f(x)>0\\}, then \\overline{R(M)}=X. We apply our results to questions of approximation in various function spaces.
NASA Astrophysics Data System (ADS)
Fedorov, V. A.; Karimov, D. N.; Komar'kova, O. N.; Krivandina, E. A.; Zhmurova, Z. I.; Sobolev, B. P.
2010-01-01
Transmission spectra of two-component crystals of Sr1- x R x F2+ x ( R = Y, La-Lu; 0 ≤ x ≤ 0.5) in the 1-17-μm wavelength range were studied. The spectral characteristics of these crystals and of single-component crystals of MF2 ( M = Ca, Sr, or Ba) and RF3 ( R = La-Nd) were compared. The transmission cutoff of Sr1- x R x F2+ x crystals is shifted to shorter wavelengths with increasing x. The same tendency is observed with the increasing atomic number R of rare-earth elements for two isoconcentration series of Sr1- x R x F2+ x ( x ˜ 0.10 and 0.28). This tendency is pronounced at large x. The transmission cutoff of Sr1- x R x F2+ x crystals can be varied in the range of from 10.7 to 12.2 μm by changing their qualitative ( R) and quantitative ( x) composition. Hence, these crystals can be assigned to multicomponent fluoride optical materials with controlled optical characteristics. The Sr1- x R x F2+ x crystals, where R = Ce-Sm, were shown to be promising materials for the design of selective optical filters in the 2-10-μm spectral range.
DOE Office of Scientific and Technical Information (OSTI.GOV)
Gopalakrishnan, J.; Uma, S.; Bhat, V.
1993-01-01
Layered perovskite oxides of the formula ACa[sub 2-x]La[sub x]Nb[sub 3-x]Ti[sub x]O[sub 10] (A = K, Rb, Cs and 0 , x [le] 2) have been prepared. The members adopt the structures of the parent ACa[sub 2]Nb[sub 3]O[sub 10]. Interlayer alkali cations in the niobium-titanium oxide series can be ion-exchanged with Li[sup +], Na[sup +], NG[sub 4][sup +], of H[sup +] to give new derivatives. Intercalation of the protonated derivatives with organic bases reveals that the Bronsted acidity of the solid solution series, HCa[sub 2-x]La[sub x]Nb[sub 3-x]Ti[sub x]O[sub 10], depends on the titanium content. While the x = 1 member (HCaLaNb[submore » 2]TiO[sub 10]) is nearly as acidic as the parent HCa[sub 2]Nb[sub 3]O[sub 10], the x = 2 member (HLA[sub 2]NbTi[sub 2]O[sub 10]) is a weak acid hardly intercalating organic bases with pK[sub a] [approximately] 11.3. The variation of acidity is probably due to an ordering of Nb/Ti atoms in the triple octahedral perovskite slabs, [Ca[sub 2-x]La[sub x]Nb[sub 3-x]Ti[sub x]O[sub 10
A Note on Separation of Variables
ERIC Educational Resources Information Center
Cherniavsky, Yonah
2011-01-01
We write down very simple, necessary and sufficient conditions for the additive and multiplicative separability of variables: v(x[subscript 1], x[subscript 2],..., x[subscript n]) = g[subscript 1](x[subscript 1]) + g[subscript 2](x[subscript 2]) +...+ g[subscript n](x[subscript n]) or u(x[subscript 1], x[subscript 2],..., x[subscript n]) =…
Maeda, Kazuhiko; Teramura, Kentaro; Takata, Tsuyoshi; Hara, Michikazu; Saito, Nobuo; Toda, Kenji; Inoue, Yasunobu; Kobayashi, Hisayoshi; Domen, Kazunari
2005-11-03
The physical and photocatalytic properties of a novel solid solution between GaN and ZnO, (Ga(1-x)Zn(x))(N(1-x)O(x)), are investigated. Nitridation of a mixture of Ga(2)O(3) and ZnO at 1123 K for 5-30 h under NH(3) flow results in the formation of a (Ga(1-x)Zn(x))(N(1-x)O(x)) solid solution with x = 0.05-0.22. With increasing nitridation time, the zinc and oxygen concentrations decrease due to reduction of ZnO and volatilization of zinc, and the crystallinity and band gap energy of the product increase. The highest activity for overall water splitting is obtained for (Ga(1-x)Zn(x))(N(1-x)O(x)) with x = 0.12 after nitridation for 15 h. The crystallinity of the catalyst is also found to increase with increasing the ratio of ZnO to Ga(2)O(3) in the starting material, resulting in an increase in activity.
ACOSS Fifteen (Active Control of Space Structures).
1982-10-01
185680. The three uniform beams are com - bined through the process of modal synthesis to form the equipment section model. This results in mass and...review and com - -_ ment by the VCOSS contractors and others. The data can be quickly changed to emphasize characteristics of LSS that are not sufficiently...JOINT 42 JOINT 46 JOINT 47 ACTUATOR SENSOR MODE = N FREG = X.XXXX HZ X Translation Xnxx :<x:...... . N...X.X....... Y Tr3rslat ior ::. >X .x:x : x ::x;: X
The Spanish Emergency Military Unit: Military Capabilities in a Civilian Environment
2015-05-23
of Weapons of Mass Destruction X X X Irregular Immigration X X X Espionage X Disasters and Emergencies X X X Maritime Vulnerability X...needs. The magnitude of the disaster, and the mishandling of the initial response, forced the governor of Florida, Mr. Lawton Chiles , to request for...Cruz Roja en el envío de ayuda a Haití y Chile .” 6 October 2010. Accessed 3 December 2014. http://www.defensa.gob.es/ gabinete/notasPrensa/2010/06
Construction, Analysis, and Data-Driven Augmentation of Supersaturated Designs
2013-09-01
guidelines and considerations. 27 Table 7. Supersaturated Design Example with 8 Runs and 14 Factors Design Factors Run x1 x2 x3 x4 x5 x6 x7 x8 x9 x10 x11...much larger than the guidelines proposed by Marley 55 and Woods (2010). They recommend the factor-to-run ratio should be less than 2. Because our ratio...established approach in experimental design: Box (1992) provided general guidelines to consider, and traditional augmentation strategies like fold-over
Cockayne, Debra A; Dunn, Philip M; Zhong, Yu; Rong, Weifang; Hamilton, Sara G; Knight, Gillian E; Ruan, Huai-Zhen; Ma, Bei; Yip, Ping; Nunn, Philip; McMahon, Stephen B; Burnstock, Geoffrey; Ford, Anthony PDW
2005-01-01
Extracellular ATP plays a role in nociceptive signalling and sensory regulation of visceral function through ionotropic receptors variably composed of P2X2 and P2X3 subunits. P2X2 and P2X3 subunits can form homomultimeric P2X2, homomultimeric P2X3, or heteromultimeric P2X2/3 receptors. However, the relative contribution of these receptor subtypes to afferent functions of ATP in vivo is poorly understood. Here we describe null mutant mice lacking the P2X2 receptor subunit (P2X2−/−) and double mutant mice lacking both P2X2 and P2X3 subunits (P2X2/P2X3Dbl−/−), and compare these with previously characterized P2X3−/− mice. In patch-clamp studies, nodose, coeliac and superior cervical ganglia (SCG) neurones from wild-type mice responded to ATP with sustained inward currents, while dorsal root ganglia (DRG) neurones gave predominantly transient currents. Sensory neurones from P2X2−/− mice responded to ATP with only transient inward currents, while sympathetic neurones had barely detectable responses. Neurones from P2X2/P2X3Dbl−/− mice had minimal to no response to ATP. These data indicate that P2X receptors on sensory and sympathetic ganglion neurones involve almost exclusively P2X2 and P2X3 subunits. P2X2−/− and P2X2/P2X3Dbl−/− mice had reduced pain-related behaviours in response to intraplantar injection of formalin. Significantly, P2X3−/−, P2X2−/−, and P2X2/P2X3Dbl−/− mice had reduced urinary bladder reflexes and decreased pelvic afferent nerve activity in response to bladder distension. No deficits in a wide variety of CNS behavioural tests were observed in P2X2−/− mice. Taken together, these data extend our findings for P2X3−/− mice, and reveal an important contribution of heteromeric P2X2/3 receptors to nociceptive responses and mechanosensory transduction within the urinary bladder. PMID:15961431
DOE Office of Scientific and Technical Information (OSTI.GOV)
Habu, Daiki; Masubuchi, Yuji; Torii, Shuki
As is the case with SrTaO{sub 2}N, both cis-ordering of nitride anions and octahedral titling are also preferable in La{sub 1−x}Sr{sub x}TiO{sub 2+x}N{sub 1−x} (x=0, 0.2) oxynitride perovskites. A larger dielectric constant of ε{sub r}≈5.0×10{sup 3} was estimated for the pure oxynitride with x=0.2, compared with ε{sub r}≈750 for the product with x=0, by extrapolating the ε{sub r} values obtained from powders mixed with paraffin at various mixing ratios. The crystal structure of x=0.2 with larger tolerance factor than x=0 increased the octahedral tilting, which contributes to the increased dielectric constant. The increased dielectric constant supports the exchange mechanism formore » the dielectric property between two kinds of –Ti–N– helical coils (clockwise and anticlockwise) derived from the above cis-ordering of nitride anions. - Graphical abstract: Very large dielectric constant values were estimated for La{sub 1−x}Sr{sub x}TiO{sub 2+x}N{sub 1−x}; ε{sub r}≈5.0×10{sup 3} in x=0.2 and ε{sub r}≈750 in x=0. - Highlights: • Cis-configuration of nitride anions was confirmed in La{sub 1−x}Sr{sub x}TiO{sub 2+x}N{sub 1−x} (x=0, 0.2). • Dielectric constant values were estimated to be 750 for x=0 and 5.0×10{sup 3} for x=0.2, respectively. • The large dielectric property is to the exchange mechanism between clockwise and anticlockwise –Ti–N– coil motifs.« less
1987-03-01
some general results and definitions from robust statistics (see Hampel et. al.. 1986). The influence function of an M-Lstimator is IC (y.x.0) = D_...estimator is (4,T T T (\\cond(YXGB) . Yx(x,O.B) ) . where X~xO.) =x T T8 xT-lx 1/2 = x x v(x . b/(x B x) ) - B. The influence function of this...the influence function for (3.7) and (3.8) is equal to -. Eo[\\Pcond(y.X.,B)] -1 cond(Yx. ,B). (4.3) On the other hand, the influence function for the
Energetic Materials Optimization via Constrained Search
2015-06-01
steps. 3. Optimization Methodology Our optimization problem is formulated as a constrained maximization: max x∈CCS P (x) s.t. : TED ( x )− 9.75 ≥ 0 SV (x)− 9...0 5− SA(x) ≥ 0, (1) where TED ( x ) is the total energy of detonation (TED) of compound x from the chosen chemical subspace (CCS) of chemical compound...max problem, max x∈CCS min λ∈R3+ P (x)− λTC(x), (2) where C(x) is the vector of constraint violations, i.e., η(9.75 − TED ( x )), η(9 − SV (x)), η(SA(x
1991-07-01
urnessible ID I I X I X I X I x I Inails (undor taib), seal I I IIII Ih~.e with plastic o’ement, I I I I I I land renai3. in new iii-tion.1 B52 -n BREAKAGE...required: I I I I I I I ITighten bolts or secure ID/P/RI I X I X I I I Inails I RI I I I X I X I I RI X I X I X I X I IReplace member if insect ID/P
Composite-Nanoparticles Thermal History Sensors
2012-06-01
E -1 4. 214 011 X E - 2 1. 601 846 X E +1 1.000 000 X E - 2 2. 579 760 X E - 4 1 .000 000 x E - 8 1.459 390 x E +1 1. 333 22 X E -1 met ers...000 X E +1 1. 745 329 X E - 2 tk = (t0 f + 459.67)/1.8 1. 602 19 X E -19 1. 000 000 X E - 7 1. 000 000 X E - 7 3. 048 000 X E - 1 1. 355 818...ELEMENT NUMBER 5d. PROJECT NUMBER 5e. TASK NUMBER 5f. WORK UNIT NUMBER 8 . PERFORMING ORGANIZATION REPORT NUMBER 10. SPONSOR/MONITOR’S ACRONYM(S
NASA Astrophysics Data System (ADS)
Wang, Ding; Zhang, Minglu; Zhuang, Huaijuan; Chen, Xu; Wang, Xianying; Zheng, Xuejun; Yang, Junhe
2017-02-01
(GaN)1-x(ZnO)x composite nanofibers with hollow structure were prepared by initial electrospinning, and the subsequent calcination and nitridation. The structure and morphology characteristics of samples were investigated by X-ray diffraction (XRD), field-emission scanning electron microscopy (FE-SEM), energy dispersive X-ray spectroscopy (EDS) and transmission electron microscopy (TEM). The characterization results showed the phase transition from ZnGa2O4 to (GaN)1-x(ZnO)x solid-solution under ammonia atmosphere. The preparation conditions were explored and the optimum nitridation temperature and holding time are 750 °C and 2 h, respectively. The photocatalytic properties of (GaN)1-x(ZnO)x with different Ga:Zn atomic ratios were investigated by degrading Rhodamine B under the visible light irradiation. The photocatalytic activity sequence is (GaN)1-x(ZnO)x (Ga:Zn = 1:2) > (GaN)1-x(ZnO)x (Ga:Zn = 1:3) > ZnO nanofibers > (GaN)1-x(ZnO)x (Ga:Zn = 1:4) > (GaN)1-x(ZnO)x (Ga:Zn = 1:1). The photocatalytic mechanism of the (GaN)1-x(ZnO)x hollow nanofibers was further studied by UV-vis diffuse reflectance spectra. The excellent photocatalytic performance of (GaN)1-x(ZnO)x hollow nanofibers was attributed to the narrow band gap and high surface area of porous nanofibers with hollow structure.
Comparing hard and soft prior bounds in geophysical inverse problems
NASA Technical Reports Server (NTRS)
Backus, George E.
1988-01-01
In linear inversion of a finite-dimensional data vector y to estimate a finite-dimensional prediction vector z, prior information about X sub E is essential if y is to supply useful limits for z. The one exception occurs when all the prediction functionals are linear combinations of the data functionals. Two forms of prior information are compared: a soft bound on X sub E is a probability distribution p sub x on X which describes the observer's opinion about where X sub E is likely to be in X; a hard bound on X sub E is an inequality Q sub x(X sub E, X sub E) is equal to or less than 1, where Q sub x is a positive definite quadratic form on X. A hard bound Q sub x can be softened to many different probability distributions p sub x, but all these p sub x's carry much new information about X sub E which is absent from Q sub x, and some information which contradicts Q sub x. Both stochastic inversion (SI) and Bayesian inference (BI) estimate z from y and a soft prior bound p sub x. If that probability distribution was obtained by softening a hard prior bound Q sub x, rather than by objective statistical inference independent of y, then p sub x contains so much unsupported new information absent from Q sub x that conclusions about z obtained with SI or BI would seen to be suspect.
Comparing hard and soft prior bounds in geophysical inverse problems
NASA Technical Reports Server (NTRS)
Backus, George E.
1987-01-01
In linear inversion of a finite-dimensional data vector y to estimate a finite-dimensional prediction vector z, prior information about X sub E is essential if y is to supply useful limits for z. The one exception occurs when all the prediction functionals are linear combinations of the data functionals. Two forms of prior information are compared: a soft bound on X sub E is a probability distribution p sub x on X which describeds the observer's opinion about where X sub E is likely to be in X; a hard bound on X sub E is an inequality Q sub x(X sub E, X sub E) is equal to or less than 1, where Q sub x is a positive definite quadratic form on X. A hard bound Q sub x can be softened to many different probability distributions p sub x, but all these p sub x's carry much new information about X sub E which is absent from Q sub x, and some information which contradicts Q sub x. Both stochastic inversion (SI) and Bayesian inference (BI) estimate z from y and a soft prior bound p sub x. If that probability distribution was obtained by softening a hard prior bound Q sub x, rather than by objective statistical inference independent of y, then p sub x contains so much unsupported new information absent from Q sub x that conclusions about z obtained with SI or BI would seen to be suspect.
40 CFR 63.99 - Delegated Federal authorities.
Code of Federal Regulations, 2011 CFR
2011-07-01
... delegated to the air pollution control agencies in each State under the procedures described in this subpart... (Combustion sources) MM X X X 27 Generic MACT: Control Devices SS X X X Eq. Leaks—Level 1 TT X X X Eq. Leaks... of 40 CFR Part 63 General Provisions Authorities to State and Local Air Pollution Control Agencies...
40 CFR 63.99 - Delegated Federal authorities.
Code of Federal Regulations, 2014 CFR
2014-07-01
... lists the specific source categories that have been delegated to the air pollution control agencies in... Generic MACT: Control Devices SS X X X Eq. Leaks—Level 1 TT X X X Eq. Leaks—Level 2 UU X X X Tanks—Level 2... General Provisions Authorities to State and Local Air Pollution Control Agencies.” 2 Alaska received...
40 CFR 63.99 - Delegated Federal authorities.
Code of Federal Regulations, 2013 CFR
2013-07-01
... lists the specific source categories that have been delegated to the air pollution control agencies in... Generic MACT: Control Devices SS X X X Eq. Leaks—Level 1 TT X X X Eq. Leaks—Level 2 UU X X X Tanks—Level 2... General Provisions Authorities to State and Local Air Pollution Control Agencies.” 2 Alaska received...
The Future of Architecture Collaborative Information Sharing: DoDAF Version 2.03 Updates
2012-04-30
Salamander x Select Solution Factory Select Business Solutions BPMN , UML x SimonTool Simon Labs x SimProcess CACI BPMN x System Architecture Management...for DoDAF Mega UML x Metastorm ProVision Metastorm BPMN x Naval Simulation System - 4 Aces METRON x NetViz CA x OPNET OPNET x Tool Name Vendor Primary
Search for charmonium and charmoniumlike states in {Upsilon}(2S) radiative decays
DOE Office of Scientific and Technical Information (OSTI.GOV)
Wang, X. L.; Yuan, C. Z.; Wang, P.
2011-10-01
Using a sample of 158x10{sup 6} {Upsilon}(2S) events collected with the Belle detector, charmonium and charmoniumlike states with even charge parity are searched for in {Upsilon}(2S) radiative decays. No significant {chi}{sub cJ} or {eta}{sub c} signal is observed, and the following upper limits at 90% confidence level (C. L.) are obtained: B({Upsilon}(2S){yields}{gamma}{chi}{sub c0})<1.0x10{sup -4}, B({Upsilon}(2S){yields}{gamma}{chi}{sub c1})<3.6x10{sup -6}, B({Upsilon}(2S){yields}{gamma}{chi}{sub c2})<1.5x10{sup -5}, and B({Upsilon}(2S){yields}{gamma}{eta}{sub c})<2.7x10{sup -5}. No significant signal of any charmoniumlike state is observed, and we obtain the limits B({Upsilon}(2S){yields}{gamma}X(3872))xB(X(3872){yields}{pi}{sup +}{pi}{sup -}J/{psi})<0.8x10{sup -6}, B({Upsilon}(2S){yields}{gamma}X(3872))x B(X(3872){yields}{pi}{sup +}{pi}{sup -}{pi}{sup 0}J/{psi})<2.4x10{sup -6}, B({Upsilon}(2S){yields}{gamma}X(3915))xB(X(3915){yields}{omega}J/{psi})<2.8x10{sup -6}, B({Upsilon}(2S){yields}{gamma}Y(4140))xB(Y(4140){yields}{phi}J/{psi}))<1.2x10{sup -6}, and B({Upsilon}(2S){yields}{gamma}X(4350))xB(X(4350){yields}{phi}J/{psi}))<1.3x10{sup -6} at 90% C. L.
Chase, C C; Riley, D G; Olson, T A; Coleman, S W; Hammond, A C
2004-09-01
To determine the maternal and reproductive performance of F1 cows in the subtropics, 42 Brahman x Angus, 34 Senepol x Angus, and 50 Tuli x Angus cows were bred to Angus bulls to calve first and subsequently bred to Charolais bulls to calve as 3- to 8-yr-olds. Age at first calving did not differ among crossbred cows. Angus-sired calf birth weights were heavier (P < 0.01) from Senepol x Angus than either Brahman x Angus or Tuli x Angus cows. Weaning weights of Angus-sired calves were heavier (P < 0.01) from Brahman x Angus (213.5 kg) than either Senepol x Angus (194.9 kg) or Tuli x Angus (191.5 kg) cows. As 3- to 8-yr-old cows, calf birth weights were heavier (P < 0.05) from Senepol x Angus compared with Brahman x Angus but not Tuli x Angus cows. Weaning weights of Charolais-sired calves were heaviest (P < 0.05) from Brahman x Angus cows (268.9 kg), lightest from Tuli x Angus cows (233.4 kg), and intermediate from Senepol x Angus cows (245.0 kg). Calf crop born and calf crop weaned were lowest (P < 0.05) for Senepol x Angus cows (76.9 and 70.2%) and did not differ between Brahman x Angus (89.0 and 86.1%) and Tuli x Angus (94.7 and 86.5%) cows. Tuli x Angus cows tended (P < 0.10) to have a lower percentage of unassisted births and lower (P < 0.10) calf survival to weaning than Brahman x Angus cows but not Senepol x Angus cows. As 3- to 8-yr-olds, weaning weight per cow exposed was greatest (P < 0.05) for Brahman x Angus (234.2 kg), least (P < 0.05) for Senepol x Angus (173.0 kg), and intermediate (P < 0.05) for Tuli x Angus (209.1 kg) cows. Also as 3- to 8-yr-olds, efficiency (205-d calf weight per 100 kg of cow exposed) was similar for Brahman x Angus (42.2) and Tuli x Angus cows (40.7), and both were greater (P < 0.01) than for Senepol x Angus cows (33.8). These data indicate that, in the subtropics, maternal and reproductive performance of Tuli x Angus cows, but not Senepol x Angus cows, was comparable to Brahman x Angus cows, except for lower calf survivability and weaning weight.
Ouyang, Ping; Zhang, He; Fan, Zhaolan; Wei, Pei; Huang, Zhigang; Wang, Sen; Li, Tao
2016-11-05
NKX2.5 plays important roles in heart development. Being a transcription factor, NKX2.5 exerts its biological functions in nucleus. However, the sequence motif that localize NKX2.5 into nucleus is still not clear. Here, we found a R/K-rich sequence motif from Q187 to R197 (QNRRYKCKRQR) was required for exclusive nuclear localization of NKX2.5. Eight truncated plasmids (E109X, Q149X, Q170X, Q187X, Q198X, Y256X, Y259X, and C264X) which were associated with congenital heart disease (CHD) were constructed. Compared with the wild type NKX2.5, the proteins E109X, Q149X, Q170X, Q187X without intact homeodomain (HD) showed no transcriptional activity while Q198X, Y256X, Y259X and C264X with intact HD showed 50 to 66% transcriptional activity. E109X, Q149X, Q170X, Q187X without intact HD localized in the cytoplasm and nucleus simultaneously and Q198X, Y256X, Y259X and C264X with intact HD localized completely in nucleus. These results inferred the indispensability of 187QNRRYKCKRQR197 in exclusive nucleus localization. Additionally, this sequence motif was very conservative among human, mouse and rat, indicating this motif was important for NKX2.5 function. Thus, we concluded that R/K-rich sequence motif 187QNRRYKCKRQR197 played a central role for NKX2.5 nuclear localization. Our findings provided a clue to understand the mechanisms between the truncated NKX2.5 mutants and CHD. Copyright © 2016 Elsevier B.V. All rights reserved.
Carbonitride based phosphors and light emitting devices using the same
Li, Yuanqiang; Tian, Yongchi; Romanelli, Michael Dennis
2013-08-20
Disclosed herein is a novel group of carbidonitride phosphors and light emitting devices which utilize these phosphors. In certain embodiments, the present invention is directed to a novel family of carbidonitride-based phosphors expressed as follows: Ca.sub.1-xAl.sub.x-xySi.sub.1-x+xyN.sub.2-x-xyC.sub.xy:A; (1) Ca.sub.1-x-zNa.sub.zM(III).sub.x-xy-zSi.sub.1-x+xy+zN.sub.2-x-xyC.sub.xy:- A; (2) M(II).sub.1-x-zM(I).sub.zM(III).sub.x-xy-zSi.sub.1-x+xy+zN.sub.2-x- -xyC.sub.xy:A; (3) M(II).sub.1-x-zM(I).sub.zM(III).sub.x-xy-zSi.sub.1-x+xy+zN.sub.2-x-xy-2w/- 3C.sub.xyO.sub.w-v/2H.sub.v:A; and (4) M(II).sub.1-x-zM(I).sub.zM(III).sub.x-xy-zSi.sub.1-x+xy+zN.sub.2-x-xy-2w/- 3-v/3C.sub.xyO.sub.wH.sub.v:A, (4a) wherein 0
Standards for Prognostics and Health Management (PHM) Techniques within Manufacturing Operations
2014-10-02
SOCIETY 2014 3 International Organization for Standardization (ISO), the Machinery Information Management Open Standards Alliance ( MIMOSA ), SAE...X X X X ISO TC 184/SC 4 X ISO TC 184/SC 5 X X ISO/IEC JTC 1/SC 7 X MIMOSA —— X SAE International AQPIC X SAE...THE PROGNOSTICS AND HEALTH MANAGEMENT SOCIETY 2014 4 HDBK is supported by the Machinery Information Management Open Standards Alliance ( MIMOSA ), a
2016-12-01
five lower-order factors representing verbal, math , spatial, perceptual speed, and aviation knowledge, and a hierarchical general factor showed the...Academic Aptitude Verbal Quant. Verbal Analogies 25 X X X Arithmetic Reasoning 25 X X Word Knowledge 25 X X X Math Knowledge 25 X X...Reasoning (AR) uses word problems to assess the ability to understand arithmetic relations. Math Knowledge (MK) assesses the ability to use
Code of Federal Regulations, 2014 CFR
2014-10-01
... in the BSAI Longline Catcher/Processor Subsector, Column A. X Indicates Whether Column B or Column C... the BSAI Longline Catcher/Processor Subsector, Column A. X Indicates Whether Column B or Column C...)(D)(2) LLG 4508 X LLG 1785 X LLG 3681 X LLG 3676 X LLG 3609 X LLG 1400 X LLG 1401 X LLG 3617 X LLG...
NASA Technical Reports Server (NTRS)
Weisskopf, M. C.; Darbro, W. A.; Elsner, R. F.; Williams, A. C.; Kahn, S. M.; Grindlay, J. E.; Naranan, S.; Sutherland, P. G.
1983-01-01
A comparison is presented of the black hole candidates LMC X-3 and Cygnus X-1 based on Einstein observations of LMC X-3 with the monitor proportional counter. A spectral analysis shows LMC X-3 to be more like the typical bright galactic X-ray source than Cygnus X-1. A search for periodic pulsations over a period range from 0.2 ms to over 1000 s set upper limits at the 90 percent confidence level of the order of 10 percent. An analysis of the aperiodic variability of LMC X-3 shows none of the shot noise behavior characteristic of Cygnus X-1. The absence of distinctive X-ray properties common to both sources suggests that the identification of black hole candidates on the basis of X-ray properties similar to Cygnus X-1 (or LMC X-3) is not reliable.
1996-12-01
ORGANIZATION NAME(S) AND ADDRESS(ES) Centro Nacional de Metrologia , Cenam,Time and Frequency Division,Apdo. Postal 1-100 Centro,C.P. 76900, Queretaro...5.39 x10-" 5.89 x10-" 3.93 x10-" 2.15 x10-l1 1.17 x10-" 7.27 xl0- la MVAR 852 x10-" 8.67 x10-" 9.46 x10-" 1.23 x10-lo x10-lo 1.95 x10-lo
[Characteristics of specifications of transportable inverter-type X-ray equipment].
Yamamoto, Keiichi; Miyazaki, Shigeru; Asano, Hiroshi; Shinohara, Fuminori; Ishikawa, Mitsuo; Ide, Toshinori; Abe, Shinji; Negishi, Toru; Miyake, Hiroyuki; Imai, Yoshio; Okuaki, Tomoyuki
2003-07-01
Our X-ray systems study group measured and examined the characteristics of four transportable inverter-type X-ray equipments. X-ray tube voltage and X-ray tube current were measured with the X-ray tube voltage and the X-ray tube current measurement terminals provided with the equipment. X-ray tube voltage, irradiation time, and dose were measured with a non-invasive X-ray tube voltage-measuring device, and X-ray output was measured by fluorescence meter. The items investigated were the reproducibility and linearity of X-ray output, error of pre-set X-ray tube voltage and X-ray tube current, and X-ray tube voltage ripple percentage. The waveforms of X-ray tube voltage, the X-ray tube current, and fluorescence intensity draw were analyzed using the oscilloscope gram and a personal computer. All of the equipment had a preset error of X-ray tube voltage and X-ray tube current that met JIS standards. The X-ray tube voltage ripple percentage of each equipment conformed to the tendency to decrease when X-ray tube voltage increased. Although the X-ray output reproducibility of system A exceeded the JIS standard, the other systems were within the JIS standard. Equipment A required 40 ms for X-ray tube current to reach the target value, and there was some X-ray output loss because of a trough in X-ray tube current. Owing to the influence of the ripple in X-ray tube current, the strength of the fluorescence waveform rippled in equipments B and C. Waveform analysis could not be done by aliasing of the recording device in equipment D. The maximum X-ray tube current of transportable inverter-type X-ray equipment is as low as 10-20 mA, and the irradiation time of chest X-ray photography exceeds 0.1 sec. However, improvement of the radiophotographic technique is required for patients who cannot move their bodies or halt respiration. It is necessary to make the irradiation time of the equipments shorter for remote medical treatment.
NASA Astrophysics Data System (ADS)
Kitô, Hijiri; Yanagi, Yousuke; Ishida, Shigeyuki; Oka, Kunihiko; Gotoh, Yoshito; Fujihisa, Hiroshi; Yoshida, Yoshiyuki; Iyo, Akira; Eisaki, Hiroshi
2014-07-01
We have synthesized a series of intermetallic ternary phosphide chalcogenide superconductors, AP2-xXx (A = Zr, Hf; X = S, Se), using the high-pressure synthesis technique. These materials have a PbFCl-type crystal structure (space group P4/nmm) when x is greater than 0.3. The superconducting transition temperature Tc changes systematically with x, yielding dome-like phase diagrams. The maximum Tc is achieved at approximately x = 0.7, at which point the Tc is 6.3 K for ZrP2-xSex (x = 0.75), 5.5 K for HfP2-xSex (x = 0.7), 5.0 K for ZrP2-xSx (x = 0.675), and 4.6 K for Hfp2-xSx (x = 0.5). They are typical type-II superconductors and the upper and lower critical fields are estimated to be 2.92 T at 0 K and 0.021 T at 2 K for ZrP2-xSex (x = 0.75), respectively.
Aviation Medicine Research: A Historical Review.
1992-11-18
Laboratory Determinations b/ / / Pulmonary and Metabolic Spirometry / / / Basal Metabolic Rate / Other / / Anthropometry Somatotype...ELECTROCARDIOGRAMS x routine fasting x x treadmill stress (Bruce protocol) X x *VECTORCARDIOGRAM 1974-1977 x BALLISTOCARDIOGRAM X PULMONARY FUNCTION STUDIES X x...few occasions when we went in to pick up MEDCAP, there was a tremendous incidence of tuberculosis . We casualties that were the result of a firefight
Cultural Resource Survey Report. Hildebrand Ranch Area: Proposed Chatfield Arboretum.
1981-05-01
stabilization and attic re- pair General Purpose Shed X X Chicken Coop X X Carriage Shed X x Corrals and Fences X X Grape Arbor x Inventory of Buildings and Fact...area of about 350 acres and included the en- tire ranch except for the areas of ground occupied by buildings and parking lots. The area along Deer
Human Factors Engineering. Part 1. Test Procedures
1990-05-15
b, given to offset mem ’,ry effects, and all participants should begin the test at the same i~erneral level of familiarity with the item. The HFE...Pop ohp l _________________________ CL PUWH p@e flpSI _____________ o AwjiqjIsA poonpojj x x x x x x P L)56MIS P*otnpo8 LIJ U Alijoixec3 poonpoW x x x
Code of Federal Regulations, 2010 CFR
2010-07-01
...′ 111°29.0min; 1 X San Manuel: T10S, R16E X T10S, R17E X Morenci: T4S, R29E 1 X Rest of State 1 X 1 EPA... x T4S, R28E 2 x T4S, R29E x T4S, R30E x T5S, R28E 2 x T5S, R29E 2 x T5S, R30E x San Manuel: T8S... outside Tucson Area: Pinal County Santa Cruz County Yavapai County Yuma County 1 This date is November 15...
Search for Hard X-Ray Emission from the Soft X-Ray Transient Aquila X-1
NASA Astrophysics Data System (ADS)
Harmon, B. A.; Zhang, S. N.; Paciesas, W. S.; Tavani, M.; Kaaret, P.; Ford, E.
1994-12-01
We are investigating the possibility of hard x-ray emission from the recurrent soft x-ray transient and x-ray burst source Aquila X-1 (Aql X-1). Outbursts of this source are relatively frequent with a spacing of ~ 4-10 months (Kitamoto, S. et al. 1993, ApJ, 403, 315). The recent detections of hard tails (\\(>\\)20 keV) in low luminosity x-ray bursters (Barret, D. & Vedrenne, G. 1994, ApJ Supp. S. 92, 505) suggest that neutron star transient systems such as Aql X-1 can produce hard x-ray emission which is detectable by BATSE. We are correlating reported optical and soft x-ray observations since 1991 of Aql X-1 with BATSE observations in order to search for hard x-ray emission episodes, and to study their temporal and spectral evolution. We will present preliminary results of this search in the 20-1000 keV band using the Earth occultation technique applied to the large area detectors. If this work is successful, we hope to alert the astronomical community for the next Aql X-1 outburst expected in 1995. Simultaneous x-ray/hard x-ray and optical observations of Aql X-1 during outburst would be of great importance for the modeling of soft x-ray transients and related systems.
NASA Astrophysics Data System (ADS)
Yu, Guo-Liang; Wang, Zhi-Gang; Li, Zhen-Yu
2018-04-01
Inspired by the newly observed state X*(3860), we analyze the strong decay behaviors of some charmonium-like states, X*(3860), X(3872), X(3915), X(3930) and X(3940), with the 3 P 0 model. We carry out our work based on the hypothesis that all of these states are charmonium systems. Our analysis indicates that, as a 0++ charmonium state, X*(3860) can reproduce the experimental data. As for X(3872), it can tentatively be interpreted as the mixture of a {{c}}\\bar{{{c}}} system and a {\\overline{{{D}}}}{{* 0}}{{{D}}}{{0}} molecular state. If we consider X(3940) as a 31 S 0 state, its total width in the present work is much lower than the experimental result. Thus, the 31 S 0 charmonium state seems not to be a good candidate for X(3940). Furthermore, our analysis implies that it is reasonable to assign X(3915) and X(3930) to be the same state, 2++. However, combining our analysis with that in Refs.[14, 71], we speculate that X(3915)/X(3930) might also be the mixture of a {{c}}\\bar{{{c}}} system and a molecular state. Supported by the Fundamental Research Funds for the Central Universities (2016MS133)
Habitat Value of Man-Made Coastal Marshes in Florida
1991-09-01
extraneous material as possible, and preserved in plastic bags. All cores were taken directly over a culm of Spartina that had been clipped at ground...spoonbill Ajaia ajaja x Wood stork Mycteri.a .ne:-. ana X Mottled duck Anas tulvigula x Black rail Lateral/us jamaici-,A,. X Clapper rail Rat/us...erythrophthalmus X X LeConte’s or sharp-tailed sparrow Ammodramus spp. X X Seaside sparrow Ammodramus maritimus X X Red- winged blackbird Agelaius
Growth and applications of GeSn-related group-IV semiconductor materials.
Zaima, Shigeaki; Nakatsuka, Osamu; Taoka, Noriyuki; Kurosawa, Masashi; Takeuchi, Wakana; Sakashita, Mitsuo
2015-08-01
We review the technology of Ge 1- x Sn x -related group-IV semiconductor materials for developing Si-based nanoelectronics. Ge 1- x Sn x -related materials provide novel engineering of the crystal growth, strain structure, and energy band alignment for realising various applications not only in electronics, but also in optoelectronics. We introduce our recent achievements in the crystal growth of Ge 1- x Sn x -related material thin films and the studies of the electronic properties of thin films, metals/Ge 1- x Sn x , and insulators/Ge 1- x Sn x interfaces. We also review recent studies related to the crystal growth, energy band engineering, and device applications of Ge 1- x Sn x -related materials, as well as the reported performances of electronic devices using Ge 1- x Sn x related materials.
Combined Functional and Immunochemical Analysis of Normal and Abnormal Human Factor X
Fair, Daryl S.; Plow, Edward F.; Edgington, Thomas S.
1979-01-01
Human Factor X was isolated from Cohn fraction III and characterized by polyacrylamide gel electrophoresis, amino acid composition, and isoelectric focusing. Two molecular forms with biological activity were observed at isoelectric points of 4.8 and 5.0. Antisera generated to Factor X was monospecific and used to establish an equilibrium competitive inhibition radioimmunoassay. This assay was specific for human Factor X and did not cross-react with human prothrombin or bovine Factor X within the sensitivity range of 6-300 ng Factor X antigen/ml. The mean concentration of Factor X based on the antigen was 11.9 μg/ml, whereas concentration values based on coagulant activity was 7.8 μg/ml. This 30% difference in measurement appears to result from the presence of a subpopulation of Factor X molecules devoid of coagulant activity. The radioimmunoassay was used to qualitatively and quantitatively compare purified Factor X to plasmic Factor X obtained from normal, warfarintreated, acquired Factor X-deficient, and congenitaldeficient patients. In all but one case, the Factor X present in these plasmas was immunochemically identical to the purified Factor X and permitted precise quantitation of these abnormal Factor X molecules. Factor X procoagulant activity was analyzed relative to Factor X antigen and the specific activities were used to characterize normal and abnormal Factor X molecules. Reduced Factor X activity in plasmas from warfarin-treated and acquired Factor X-deficient patients was attributed to both decreases in Factor X antigen and decreased function of the Factor X molecules. Congenitally deficient patients, in general, showed a reduction in Factor X antigen in parallel with Factor X procoagulant activities resulting from comparable decreases in specific biological activity of the molecules. Images PMID:90058
Low-temperature glasslike properties in (NaCl)1-x(NaCN)x
NASA Astrophysics Data System (ADS)
Watson, Susan K.; Pohl, R. O.
1995-04-01
Thermal conductivity, internal friction, transverse sound velocity (60 mK to 300 K), and specific-heat data (100 mK to 40 K) for (NaCl)1-x(NaCN)x (x=0, 0.025, 0.05, 0.1, 0.76, 1) show a progression from crystalline to glasslike behavior as the CN- concentration is increased from 0 to 76 %. The evolution of glasslike properties is compared to that in other crystals in which glasslike properties evolve with increasing disorder, e.g., (KBr)1-x(KCN)x and Ba1-xLaxF2-x. For (KBr)1-x(KCN)x, Sethna and Chow have shown that as the concentration of the almost freely rotating CN- ions is increased the average potential barrier for CN- reorientation also increases through elastic quadrupolar interactions. For x~0.5, only a small density of low-energy states is left, which equals that observed in structural glasses. In Ba1-xLaxF2-x, on the other hand, the crystal field for small doping x is so large that no atomic motion occurs at low temperatures. (NaCl)1-x(NaCN)x is shown to represent an intermediate case, in that the crystal field is non-negligible at small x, yet glasslike low-energy excitations indicative of very small potential barrier heights evolve with increasing x. It is argued that random internal strains cause a decrease of the barrier heights in these crystals, which lead to the low-energy excitations. It is proposed that random strains have a similar effect in other disordered crystals as in Ba1-xLaxF2-x, which for small x show no low-energy mobile states, yet which for large x become glasslike.
Segregation at the surfaces of CuxPd1-x alloys in the presence of adsorbed S
DOE Office of Scientific and Technical Information (OSTI.GOV)
Miller, James B.; Priyadarshini, Deepika; Gellman, Andrew J.
2012-10-01
The influence of adsorbed S on surface segregation in Cu{sub x}Pd{sub 1 - x} alloys (S/Cu{sub x}Pd{sub 1 - x)} was characterized over a wide range of bulk alloy compositions (x = 0.05 to 0.95) using high-throughput Composition Spread Alloy Film (CSAF) sample libraries. Top-surface and near-surface compositions of the CSAFs were measured as functions of bulk Cu composition, x, and temperature using spatially resolved low energy ion scattering spectroscopy (LEISS) and X-ray photoemission spectroscopy (XPS). Preferential segregation of Cu to the top-surface of the S/Cu{sub x}Pd{sub 1 - x} CSAF was observed at all bulk compositions, x, but themore » extent of Cu segregation to the S/Cu{sub x}Pd{sub 1 - x} surface was lower than the Cu segregation to the surface of a clean Cu{sub x}Pd{sub 1 - x} CSAF, clear evidence of an S-induced “segregation reversal.” The Langmuir–McLean formulation of the Gibbs isotherm was used to estimate the enthalpy and entropy of Cu segregation to the top-surface, ΔH{sub seg}(x) and ΔS{sub seg}(x), at saturation sulfur coverages. While Cu segregation to the top-surface of the clean Cu{sub x}Pd{sub 1 - x} is exothermic (ΔH{sub seg} < 0) for all bulk Cu compositions, it is endothermic (ΔH{sub seg} > 0) for S/Cu{sub x}Pd{sub 1 - x}. Segregation to the S/Cu{sub x}Pd{sub 1 - x} surface is driven by entropy. Changes in segregation patterns that occur upon adsorption of S onto Cu{sub x}Pd{sub 1 - x} appear to be related to formation of energetically favored Pd{single bond}S bonds at the surface, which counterbalance the enthalpic driving forces for Cu segregation to the clean surface.« less
The Phase Relations in the In 2O 3-Al 2ZnO 4-ZnO System at 1350°C
NASA Astrophysics Data System (ADS)
Nakamura, Masaki; Kimizuka, Noboru; Mohri, Takahiko; Isobe, Mitsumasa
1993-08-01
Phase relations in the In 2O 3-Al 2ZnO 4-ZnO system at 1350°C are determined by a classical quenching method. This system consists of In 2O 3, Al 2ZnO 4, ZnO, and homologous phases InAlO 3(ZnO) m ( m = 2, 3, …) having solid solutions with LuFeO 3(ZnO) m-type crystal structures. These solid solution ranges are as follows: In 1+ x1Al 1- x1O 3(ZnO) 2 ( x1 = 0.70)-In 1+ x2Al 1- x2O 3(ZnO) 2 ( x2 = 0.316-0.320), In 2O 3(ZnO) 3-In 1+ xAl 1- xO 3(ZnO) 3 ( x = 0.230), In 2O 3(ZnO) 4-In 1+ xAl 1- xO 3(ZnO) 4 ( x = 0.15-0.16), In 2O 3(ZnO) 5-In 1+ xAl 1- xO 3(ZnO) 5 ( x = 0.116-0.130), In 2O 3(ZnO) 6-In 1+ xAl 1- xO 3(ZnO) 6 ( x = 0.000-0.111), In 2O 3(ZnO) 7-In 1+ xAl 1- xO 3(ZnO) 7 ( x = 0.08), In 2O 3(ZnO) 8-In 1+ xAl 1- xO 3(ZnO) 8 ( x: undetermined), and In 2O 3(ZnO) m-InAlO 3(ZnO) m ( m = 9, 10, 11, 13, 15, 17, and 19). The space groups of these homologous phases belong to R3¯ m for m = odd or P6 3/ mmc for m = even. Their crystal structures, In 1+ xAl 1- xO 3(ZnO) m (0 < x < 1), consist of three kinds of layers: an InO 1.5 layer, an (In xAl 1- xZn)O 2.5 layer, and ZnO layers. A comparison of the phase relations in the In 2O 3- M2ZnO 4-ZnO systems ( M = Fe, Ga, or Al) is made and their characteristic features are discussed in terms of the ionic radii and site preferences of the M cations.
1976-02-01
N N N-~~ ~ - N N N X N N N N N 41 1 x N NNNWNNn Nxx xx 0 0 N N N N N N x N NX x N N z ~ ~ ~ ~ x x e x2d NNx CNNx xwNm N NNNNNNNNNNNNNNN - N x xNxx xN...to prevent grounding to the outer metal tube. These sections are then assembled into electro-tinned brass LUbes. The com :.-ession glass end seals are
Activity-based Calculation Models for the Brazilian Air Force Cellular Unit of Intendancy
2013-03-01
Braz (2004), the current battlefield is fluid and dynamic. The concentration of trained personnel and suitable material in the right place at the right...Identification of budget gaps; f) Elimination of superfluous activities; g) Selection of lower cost activities; h) Reduction of the time or the resources...x - x - 4 33% 8.4 Delivery mail - x x x x - - - x - x - 6 50% 9. Recreational facilities 9.1 Provide space and activities to entertainment x x
NASA Astrophysics Data System (ADS)
Akroune, A.; Casalot, A.
1987-05-01
V 1- xMn xO 2-2 xF 2 x samples (0 < x ≤ 0, 10) have been prepared by solid state reaction in sealed platinium tubes. The metal ⇄ insulator transition occurs at a quickly decreasing temperatures as MnF 2 increases. The crystallographic, magnetic, transport properties, and DTA have been determined and discussed.
1980-09-01
Waterlily .1! Kuphar variegatum x X x * : White Waterlily Numphaea tuberosa X X X X X Greater Duckweed Spirodela polrhiz x x Lesser Duckweed Lemna minor ...expected that this would be a minor portion of the project. A channel 6 feet deep and 30 feet wide is desired. 9. Johnson Slough (Clayton County, Iowa...76,276.74. The actual budget may be substantially less, however. MINORITY REPORT Unanimous vote. No minority opinion. ,p Michael Vanderfoy6 Chairman Side
The Application of Design to Cost and Life Cycle to Aircraft Engines.
1980-05-01
appearing in both columns include AGE (common and peculiar), transportation, management, and training. These cost elements are not usually large in...Proc. of install engine X CIP x Spare engine X Spare parts (base/depot) X Depot labor X Base labor X ECPs-mod/retro X X AGE (peculiar/common) X X...introduits de maniere aleatoire dans le cadre j’hypotheses. En outre les moteurs ou les sous-ensembles, compte tenu du suivi de leur age et de leur
Computational Homology for Software Validation
2015-03-01
convergence spaces is a continuous bijection whose inverse is continuous. Definition 3.4. Let x be a point of a convergence spaceX , and let U be a subset...reflector 9 Approved for Public Release; Distribution Unlimited. from an arbitrary topological spaceX to βX is an embedding if and only ifX is completely...a convergence spaceX will be written additively, whether or not T is Abelian. Furthermore, for all τ ∈ T and all x ∈ X , we will write τ(x) as x+ τ In
Investigation of Surface Preparations to Enhance Photon Doppler Velocimetry Measurements
2015-08-01
of Angle, Surface Profilometery, and Optical Photography at 10-, 20-, and 40-Times Magnifications 53 Appendix J. Kevlar Reflected Power... applicability to measure many velocities that the Army is interested in: floor accelerations due to an under- vehicle mine blast;4 material deformations from...x … x F HB-26 x … … … … x … x G Al2O3 x … … … … … … … H Polyethylene x … … … … x … … I Kevlar x … … … … … … x J Mild Steel … … … … … x
Finite-Difference Simulations of Rayleigh-Wave Scattering by Shallow Heterogeneity.
1987-11-01
in thiadocument are those of the. uthors and should not be interpreted as representing the.official policies , either expressed or- Implied, of the...be interpreted as necessarily representing the official policies , either expressed or implied, of the Defense Advanced Research Projects Agency or the...Ln o 3" X AID 4< >_x +<J ’--X ±4D£ 3,"-- Ln x +,3 D z N LJI X +© < CNCD C),_,* 0D x + u iIx + < 0 LJ x + X + 0d 10L LiX + <] O x + < 0 -d U-) L x -1
2011-04-01
L1u. Assume that geodesic lines, generated by the eikonal equation corresponding to the function c (x) are regular, i.e. any two points in R3 can be...source x0 is located far from Ω, then similarly with (107) ∆l (x, x0) ≈ 0 in Ω. The function l (x, x0) satisfies the eikonal equation [38] |∇xl (x, x0...called “inverse kinematic problem” which aims to recover the function c (x) from the eikonal equation assuming that the function l (x, x0) is known for
Zemkova, Hana; He, Mu-Lan; Koshimizu, Taka-aki; Stojilkovic, Stanko S
2004-08-04
The P2X receptors (P2XRs) are a family of ligand-gated channels activated by extracellular ATP through a sequence of conformational transitions between closed, open, and desensitized states. In this study, we examined the dependence of the activity of P2XRs on ectodomain structure and agonist potency. Experiments were done in human embryonic kidney 293 cells expressing rat P2X2aR, P2X2bR, and P2X3R, and chimeras having the V60-R180 or V60-F301 ectodomain sequences of P2X3R instead of the I66-H192 or I66-Y310 sequences of P2X2aR and P2X2bR. Chimeric P2X2a/V60-F301X3R and P2X2b/V60-F301X3R inherited the P2X3R ligand-selective profile, whereas the potency of agonists for P2X2a/V60-R180X3R was in between those observed at parental receptors. Furthermore, P2X2a/V60-F301X3R and P2X2a/V60-R180X3R desensitized in a P2X2aR-specific manner, and P2X2b/V60-F301X3R desensitized with rates comparable with those of P2X2bR. In striking contrast to parental receptors, the rates of decay in P2X2a/V60-F301X3R and P2X2b/V60-F301X3R currents after agonist withdrawal were 15- to 200-fold slower. For these chimeras, the decays in currents were not dependent on duration of stimuli and reflected both continuous desensitization and deactivation of receptors. Also, participation of deactivation in closure of channels inversely correlated with potency of agonists to activate receptors. The delay in deactivation was practically abolished in P2X2a/V60-R180X3R-expressing cells. However, the recovery from desensitization of P2X2a/V60-F301X3R and P2X2a/V60-R180X3R was similar and substantially delayed compared with that of parental receptors. These results indicate that both ectodomain halves participate in gating, but that the C and N halves influence the stability of open and desensitized conformation states, respectively, which in turn reflects on rates of receptor deactivation and resensitization.
X ray spectra of X Per. [oso-8 observations
NASA Technical Reports Server (NTRS)
Becker, R. H.; Boldt, E. A.; Holt, S. S.; Pravdo, S. H.; Robinson-Saba, J.; Serlemitsos, P. J.; Swank, J. H.
1978-01-01
The cosmic X-ray spectroscopy experiment on OSO-8 observed X Per for twenty days during two observations in Feb. 1976 and Feb. 1977. The spectrum of X Per varies in phase with its 13.9 min period, hardening significantly at X-ray minimum. Unlike other X-ray binary pulsar spectra, X Per's spectra do not exhibit iron line emission or strong absorption features. The data show no evidence for a 22 hour periodicity in the X-ray intensity of X Per. These results indicate that the X-ray emission from X Per may be originating from a neutron star in a low density region far from the optically identified Be star.
Ultra low thermal expansion, highly thermal shock resistant ceramic
Limaye, Santosh Y.
1996-01-01
Three families of ceramic compositions having the given formula: .phi..sub.1+X Zr.sub.4 P.sub.6-2X Si.sub.2X O.sub.24, .phi..sub.1+X Zr.sub.4-2X Y.sub.2X P.sub.6 O.sub.24 and .phi..sub.1+X Zr.sub.4-X Y.sub.X P.sub.6-2X Si.sub.X O.sub.24 wherein .phi. is either Strontium or Barium and X has a value from about 0.2 to about 0.8 have been disclosed. Ceramics formed from these compositions exhibit very low, generally near neutral, thermal expansion over a wide range of elevated temperatures.
Measurements of Local Strain Variation in Si(1-x)Ge(x)/Si Heterostructures
NASA Technical Reports Server (NTRS)
Bell, L. D.; Kaiser, W. J.; Manion, S. J.; Milliken, S. J.; Pike, W. T.; Fathauer, R. W.
1995-01-01
The energy splitting of the conduction-band minimum of Si(1-x), Ge(x), due to strain has been directly measured by the application of ballistic-electron-emission microscope (BEEM) spectroscopy to Ag/Si(1-x), Ge(x) structures. Experimental values for this conduction-band splitting agree well with calculations. For Au/Si(1-x), Ge(x), however, heterogeneity in the strain of the Si(1-x), Ge(x) layer is introduced by deposition of the Au. This variation is attributed to species interdiffusion, which produces a rough Si(1-x)Ge(x) surface. Preliminary modeling indicates that the observed roughness is consistent with the strain variation measured by BEEM.
Rare earth-iron magnetostrictive materials and devices using these materials
Savage, Howard T.; Clark, Arthur E.; McMasters, O. Dale
1981-12-29
Grain-oriented polycrystalline or single crystal magnetostrictive materials n the general formula Tb.sub.x Dy.sub.1-x Fe.sub.2-w, Tb.sub.x Ho.sub.1-x Fe.sub.2-w, Sm.sub.x Dy.sub.1-x Fe.sub.x-w, Sm.sub.x Ho.sub.1-x Fe.sub.2-w, Tb.sub.x Ho.sub.y Dy.sub.z Fe.sub.2-w, or Sm.sub.x Ho.sub.y Dy.sub.z Fe.sub.2-w, wherein O.ltoreq.w.ltoreq.0.20, and x+y+z=1. X, y, and z are selected to maximize the magnetostrictive effect and the magnetomechanical coupling coefficient K.sub.33. These material may be used in magnetostrictive transducers, delay lines, variable frequency resonators, and filters.
DOE Office of Scientific and Technical Information (OSTI.GOV)
Liu, Jingxiao; Luo, Jiayu; Shi, Fei, E-mail: shifei@dlpu.edu.cn
2015-01-15
F-doped Cs{sub 0.33}WO{sub 3−x}F{sub x} particles were successfully synthesized by the hydrothermal method with hydrofluoric acid as fluorine source, and a new kind of heat insulating films were prepared from dispersion of Cs{sub 0.33}WO{sub 3−x}F{sub x} nanoparticles in polyvinyl alcohol (PVA) aqueous solution. The effects of F doping on the crystal structure and morphology of Cs{sub 0.33}WO{sub 3−x}F{sub x} particles as well as the near-infrared (NIR) shielding ability and heat insulation properties of Cs{sub 0.33}WO{sub 3−x}F{sub x} films were investigated. The results indicated that HF acid addition could promote the formation of rod-like Cs{sub 0.33}WO{sub 3−x}F{sub x} particles during hydrothermalmore » synthesis and increase the yield of Cs{sub 0.33}WO{sub 3−x}F{sub x} powders. Moreover, the as-prepared films from dispersion solution of Cs{sub 0.33}WO{sub 3−x}F{sub x} particles exhibited higher near-infrared (NIR) shielding ability and heat insulating properties than that of the undoped Cs{sub 0.33}WO{sub 3} film. Particularly, the as-prepared Cs{sub 0.33}WO{sub 3−x}F{sub x} sample with F/W (molar ratio)=0.45 showed best NIR shielding ability and transparent heat insulating performance. The formation mechanism of nanorod-like particles and the effects of F doping on the properties of Cs{sub 0.33}WO{sub 3−x}F{sub x} products were discussed. - Graphical abstract: F-doped Cs{sub 0.33}WO{sub 3−x}F{sub x} particles were successfully synthesized by the hydrothermal method with hydrofluoric acid as fluorine source. HF acid addition in the precursor solution could increase the yield of Cs{sub 0.33}WO{sub 3−x}F{sub x} powders and promote the formation of rod-like Cs{sub 0.33}WO{sub 3−x}F{sub x} particles. Moreover, the as-prepared Cs{sub 0.33}WO{sub 3−x}F{sub x} films from dispersion solution of Cs{sub 0.33}WO{sub 3−x}F{sub x} particles exhibited higher near-infrared (NIR) shielding ability and heat insulating properties than that of the undoped Cs{sub x}WO{sub 3} film. Particularly, the as-prepared Cs{sub 0.33}WO{sub 3−x}F{sub x} sample with F/W (molar ratio)=0.45 showed best NIR shielding ability and transparent heat insulating performance. - Highlights: • F-doped Cs{sub 0.33}WO{sub 3−x}F{sub x} powders were successfully synthesized by the hydrothermal method. • HF acid addition could promote the formation of rod-like Cs{sub 0.33}WO{sub 3−x}F{sub x} particles. • The near infrared shielding ability of Cs{sub 0.33}WO{sub 3} was further improved by F doping. • The Cs{sub 0.33}WO{sub 3−x}F{sub x} films exhibited higher transparent heat insulation than Cs{sub 0.33}WO{sub 3}.« less
Relativized problems with abelian phase group in topological dynamics.
McMahon, D
1976-04-01
Let (X, T) be the equicontinuous minimal transformation group with X = pi(infinity)Z(2), the Cantor group, and S = [unk](infinity)Z(2) endowed with the discrete topology acting on X by right multiplication. For any countable group T we construct a function F:X x S --> T such that if (Y, T) is a minimal transformation group, then (X x Y, S) is a minimal transformation group with the action defined by (x, y)s = [xs, yF(x, s)]. If (W, T) is a minimal transformation group and varphi:(Y, T) --> (W, T) is a homomorphism, then identity x varphi:(X x Y, S) --> (X x W, S) is a homomorphism and has many of the same properties that varphi has. For this reason, one may assume that the phase group is abelian (or S) without loss of generality for many relativized problems in topological dynamics.
Maximum likelihood density modification by pattern recognition of structural motifs
Terwilliger, Thomas C.
2004-04-13
An electron density for a crystallographic structure having protein regions and solvent regions is improved by maximizing the log likelihood of a set of structures factors {F.sub.h } using a local log-likelihood function: (x)+p(.rho.(x).vertline.SOLV)p.sub.SOLV (x)+p(.rho.(x).vertline.H)p.sub.H (x)], where p.sub.PROT (x) is the probability that x is in the protein region, p(.rho.(x).vertline.PROT) is the conditional probability for .rho.(x) given that x is in the protein region, and p.sub.SOLV (x) and p(.rho.(x).vertline.SOLV) are the corresponding quantities for the solvent region, p.sub.H (x) refers to the probability that there is a structural motif at a known location, with a known orientation, in the vicinity of the point x; and p(.rho.(x).vertline.H) is the probability distribution for electron density at this point given that the structural motif actually is present. One appropriate structural motif is a helical structure within the crystallographic structure.
1994-04-01
sabinae Sabine shiner x Notropis texanus weed shiner x Notropis volucellus mimic shiner X Ogeocephalus radiatus polka-dot bat fish x Oligoplites saurus ...Elope saurus ladyfish x x Erimyzon oblongus creek chubsucker x Esox americanus vermiculatus grass pickerel x Etheostoma chiorosomum, bluntnose darter
Code of Federal Regulations, 2013 CFR
2013-07-01
..., 329-332 X Census tracts 13-75, 143, 158-161, 178-189, 295-297, 322, 324, 327 X Balance of city X (B... Allen Township X (C) Reading Air Basin X (D) Carbon County X (E) Remaining Portions of AQCR X III. South...) Remaining Pennsylvania Portion of the AQCR X Pennsylvania—Carbon Monoxide Designated Area Designation Date 1...
Code of Federal Regulations, 2011 CFR
2011-07-01
..., 329-332 X Census tracts 13-75, 143, 158-161, 178-189, 295-297, 322, 324, 327 X Balance of city X (B... Allen Township X (C) Reading Air Basin X (D) Carbon County X (E) Remaining Portions of AQCR X III. South...) Remaining Pennsylvania Portion of the AQCR X Pennsylvania—Carbon Monoxide Designated Area Designation Date 1...
Code of Federal Regulations, 2012 CFR
2012-07-01
..., 329-332 X Census tracts 13-75, 143, 158-161, 178-189, 295-297, 322, 324, 327 X Balance of city X (B... Allen Township X (C) Reading Air Basin X (D) Carbon County X (E) Remaining Portions of AQCR X III. South...) Remaining Pennsylvania Portion of the AQCR X Pennsylvania—Carbon Monoxide Designated Area Designation Date 1...
A sharp lower bound for the sum of a sine series with convex coefficients
NASA Astrophysics Data System (ADS)
Solodov, A. P.
2016-12-01
The sum of a sine series g(\\mathbf b,x)=\\sumk=1^∞ b_k\\sin kx with coefficients forming a convex sequence \\mathbf b is known to be positive on the interval (0,π). Its values near zero are conventionally evaluated using the Salem function v(\\mathbf b,x)=x\\sumk=1m(x) kb_k, m(x)=[π/x]. In this paper it is proved that 2π-2v(\\mathbf b,x) is not a minorant for g(\\mathbf b,x). The modified Salem function v_0(\\mathbf b,x)=x\\bigl(\\sumk=1m(x)-1 kb_k+(1/2)m(x)bm(x)\\bigr) is shown to satisfy the lower bound g(\\mathbf b,x)>2π-2v_0(\\mathbf b,x) in some right neighbourhood of zero. This estimate is shown to be sharp on the class of convex sequences \\mathbf b. Moreover, the upper bound for g(\\mathbf b,x) is refined on the class of monotone sequences \\mathbf b. Bibliography: 11 titles.
Wang, Zhenhai; Zhao, Mingwen; Wang, Xiaopeng; Xi, Yan; He, Xiujie; Liu, Xiangdong; Yan, Shishen
2012-12-05
The band alignment in ZnO-GaN and related heterostructures is crucial for uses in solar harvesting technology. Here, we report our density functional calculations of the band alignment and optical properties of ZnO-GaN and ZnO-(Ga(1-x)Zn(x))(N(1-x)O(x))-GaN heterostructures using a Heyd-Scuseria-Ernzerhof (HSE) hybrid functional. We found that the conventional GGA functionals underestimate not only the band gap but also the band offset of these heterostructures. Using the hybrid functional calculations, we show that the (Ga(1-x)Zn(x))(N(1-x)O(x)) solid solution has a direct band gap of about 2.608 eV, in good agreement with the experimental data. More importantly, this solid solution forms type-II band alignment with the host materials. A GaN-(Ga(1-x)Zn(x))(N(1-x)O(x))-ZnO core-shell solar cell model is presented to improve the visible light absorption ability and carrier collection efficiency.
Modelling the thermal conductivity of (U xTh 1-x)O 2 and (U xPu 1-x)O 2
Cooper, M. W. D.; Middleburgh, S. C.; Grimes, R. W.
2015-07-15
The degradation of thermal conductivity due to the non-uniform cation lattice of (U xTh 1-x)O 2 and (U xPu 1-x)O 2 solid solutions has been investigated by molecular dynamics, using the non-equilibrium method, from 300 to 2000 K. Degradation of thermal conductivity is predicted in (U xTh 1-x)O 2 and (U xPu 1-x)O 2 as compositions deviate from the pure end members: UO 2, PuO 2 and ThO 2. The reduction in thermal conductivity is most apparent at low temperatures where phonon-defect scattering dominates over phonon-phonon interactions. The effect is greater for (U xTh 1-x)O 2 than U xPu 1-x)Omore » 2 due to the greater mismatch in cation size. Parameters for an analytical expressions have been developed that describe the predicted thermal conductivities over the full temperature and compositional ranges. Finally, these expressions may be used in higher level fuel performance codes.« less
NASA Technical Reports Server (NTRS)
Hoover, Richard B. (Editor); Walker, Arthur B. C., Jr. (Editor)
1991-01-01
Topics discussed in this issue include the fabrication of multilayer X-ray/EUV coatings; the design, characterization, and test of multilayer X-ray/EUV coatings; multilayer X-ray/EUV monochromators and imaging microscopes; X-ray/EUV telescopes; the test and calibration performance of X-ray/EUV instruments; XUV/soft X-ray projection lithography; X-ray/EUV space observatories and missions; X-ray/EUV telescopes for solar research; X-ray/EUV polarimetry; X-ray/EUV spectrographs; and X-ray/EUV filters and gratings. Papers are presented on the deposition-controlled uniformity of multilayer mirrors, interfaces in Mo/Si multilayers, the design and analysis of an aspherical multilayer imaging X-ray microscope, recent developments in the production of thin X-ray reflecting foils, and the ultraprecise scanning technology. Consideration is also given to an active sun telescope array, the fabrication and performance at 1.33 nm of a 0.24-micron-period multilayer grating, a cylindrical proportional counter for X-ray polarimetry, and the design and analysis of the reflection grating arrays for the X-Ray Multi-Mirror Mission.
NASA Astrophysics Data System (ADS)
Blanchard, Peter E. R.; Grosvenor, Andrew P.
2018-05-01
The structural properties of (1-x)BaTiO3-xBiScO3 and (1-x)PbTiO3-xBiScO3 were investigated using powder X-ray diffraction and X-ray absorption spectroscopy. Diffraction measurements confirmed that substituting small amounts of BiScO3 into BaTiO3 initially stabilizes a cubic phase at x = 0.2 before impurity phases begin to form at x = 0.5. BiScO3 substitution also resulted in noticeable changes in the local coordination environment of Ti4+. X-ray absorption near-edge spectroscopy (XANES) analysis showed that replacing Ti4+ with Sc3+ results in an increase in the off-centre displacement of Ti4+ cations. Surprisingly, BiScO3 substitution has no effect on the displacement of the Ti4+ cation in the (1-x)PbTiO3-xBiScO3 solid solution.
Solvability of a fourth-order boundary value problem with periodic boundary conditions II
DOE Office of Scientific and Technical Information (OSTI.GOV)
Gupta, Chaitan P.
1991-01-01
Lemore » t f : [ 0 , 1 ] × R 4 → R be a function satisfying Caratheodory's conditions and e ( x ) ∈ L 1 [ 0 , 1 ] . This paper is concerned with the solvability of the fourth-order fully quasilinear boundary value problem d 4 u d x 4 + f ( x , u ( x ) , u ′ ( x ) , u ″ ( x ) , u ‴ ( x ) ) = e ( x ) , 0 < x < 1 , with u ( 0 ) − u ( 1 ) = u ′ ( 0 ) − u ′ ( 1 ) = u ″ ( 0 ) - u ″ ( 1 ) = u ‴ ( 0 ) - u ‴ ( 1 ) = 0 . This problem was studied earlier by the author in the special case when f was of the form f ( x , u ( x ) ) , i.e., independent of u ′ ( x ) , u ″ ( x ) , u ‴ ( x ) . It turns out that the earlier methods do not apply in this general case. The conditions need to be related to both of the linear eigenvalue problems d 4 u d x 4 = λ 4 u and d 4 u d x 4 = − λ 2 d 2 u d x 2 with periodic boundary conditions.« less
Computer Simulation of a 155-mm Projectile in a Scat Gun Assembly
2008-09-01
piston increases its kinetic energy as it is displaced a distance X. X X X MpsV2s /2 = f((P- vRT )/(Lpw -X))A - F)dx = (- vRT /(Lpw - X))AdY + f(PA -F...piston is displaced x, the critical displacement can be calculated using the Ideal Gas Law PV = vRT . YD = vRT /(A(Lp;v - x,i)) (ALpwv - x(,.ij
NASA Astrophysics Data System (ADS)
Kim, Youngmo; Park, Jiwoo; Sohn, Hyunchul
2018-01-01
Si1- x Ge x (:B) epitaxial layers were deposited by using reduced pressure chemical vapor deposition with SiH4, GeH4, and B2H6 source gases, and the dependences of the surface roughness of undoped Si1- x Ge x on the GeH4 flow rate and of Si1- x Ge x :B on the B2H6 flow rate were investigated. The root-mean-square (RMS) roughness value of the undoped Si1- x Ge x at constant thickness increased gradually with increasing Ge composition, resulting from an increase in the amplitude of the wavy surface before defect formation. At higher Ge compositions, the residual strain in Si1- x Ge x significantly decreased through the formation of defects along with an abrupt increase in the RMS roughness. The variation of the surface roughness of Si1- x Ge x :B depended on the boron (B) concentration. At low B concentrations, the RMS roughness of Si1- x Ge x remained constant regardless of Ge composition, which is similar to that of undoped Si1- x Ge x . However, at high B concentrations, the RMS roughness of Si1- x Ge x :B increased greatly due to B islanding. In addition, at very high B concentrations ( 9.9 at%), the RMS roughness of Si1- x Ge x :B decreased due to non-epitaxial growth.
Bulk and Thin Film Synthesis of Compositionally Variant Entropy-stabilized Oxides.
Sivakumar, Sai; Zwier, Elizabeth; Meisenheimer, Peter Benjamin; Heron, John T
2018-05-29
Here, we present a procedure for the synthesis of bulk and thin film multicomponent (Mg0.25(1-x)CoxNi0.25(1-x)Cu0.25(1-x)Zn0.25(1-x))O (Co variant) and (Mg0.25(1-x)Co0.25(1-x)Ni0.25(1-x)CuxZn0.25(1-x))O (Cu variant) entropy-stabilized oxides. Phase pure and chemically homogeneous (Mg0.25(1-x)CoxNi0.25(1-x)Cu0.25(1-x)Zn0.25(1-x))O (x = 0.20, 0.27, 0.33) and (Mg0.25(1-x)Co0.25(1-x)Ni0.25(1-x)CuxZn0.25(1-x))O (x = 0.11, 0.27) ceramic pellets are synthesized and used in the deposition of ultra-high quality, phase pure, single crystalline thin films of the target stoichiometry. A detailed methodology for the deposition of smooth, chemically homogeneous, entropy-stabilized oxide thin films by pulsed laser deposition on (001)-oriented MgO substrates is described. The phase and crystallinity of bulk and thin film materials are confirmed using X-ray diffraction. Composition and chemical homogeneity are confirmed by X-ray photoelectron spectroscopy and energy dispersive X-ray spectroscopy. The surface topography of thin films is measured with scanning probe microscopy. The synthesis of high quality, single crystalline, entropy-stabilized oxide thin films enables the study of interface, size, strain, and disorder effects on the properties in this new class of highly disordered oxide materials.
Reactive belite stabilization mechanisms by boron-bearing dopants
DOE Office of Scientific and Technical Information (OSTI.GOV)
Cuesta, Ana; Losilla, Enrique R.; Aranda, Miguel A.G.
2012-04-15
Belite-rich cements hold promise for reduced energy consumption and CO{sub 2} emissions, but their use is hindered by the slow hydration rates of ordinary belites. This drawback may be overcome by activation of belite by doping. Here, the doping mechanism of B and Na/B in belites is reported. For B-doping, three solid solutions have been tested: Ca{sub 2-x/2{open_square}x/2}(SiO{sub 4}){sub 1-x}(BO{sub 3}){sub x}, Ca{sub 2}(SiO{sub 4}){sub 1-x}(BO{sub 3}){sub x}O{sub x/2} and Ca{sub 2-x}B{sub x}(SiO{sub 4}){sub 1-x}(BO{sub 4}){sub x}. The experimental results support the substitution of silicate groups by tetrahedral borate groups with the concomitant substitution of calcium by boron for chargemore » compensation, Ca{sub 2-x}B{sub x}(SiO{sub 4}){sub 1-x}(BO{sub 4}){sub x}. Otherwise, the coupled Na/B-doping of belite has also been investigated and Ca{sub 2-x}Na{sub x}(SiO{sub 4}){sub 1-x}(BO{sub 3}){sub x} series is confirmed to exist for a large range of x values. Along this series, {alpha}'{sub H}-C{sub 2}S is the main phase (for x {>=} 0.10) and is single phase for x = 0.25. Finally, a new structural description for borax doping in belite has been developed for {alpha}'{sub H}-Ca{sub 1.85}Na{sub 0.15}(SiO{sub 4}){sub 0.85}(BO{sub 3}){sub 0.15}, which fits better borax activated belite cements in Rietveld mineralogical analysis.« less
DOE Office of Scientific and Technical Information (OSTI.GOV)
Nag, Abanti, E-mail: abanti@nal.res.in; Bose, Rapaka S.C.
Highlights: • The thermoelectric Ca{sub 1−x}Ln{sub x}Mn{sub 1−x}Nb{sub x}O{sub 3} (Ln = Yb, Lu) perovskite are prepared by solid state reaction. • The high temperature transport properties are explored. • The co-substituted Ca{sub 1−x}Ln{sub x}Mn{sub 1−x}Nb{sub x}O{sub 3} shows non-metal-like temperature dependence of resistivity. • The Seebeck coefficient of Ca{sub 1−x}Ln{sub x}Mn{sub 1−x}Nb{sub x}O{sub 3} exhibits metallic nature. • The puzzling transport phenomenon is originated from oxygen vacancy related defect centres. - Abstract: The co-substituted Ca{sub 1−x}Ln{sub x}Mn{sub 1−x}Nb{sub x}O{sub 3} (Ln = Yb, Lu; 0.02 ≤ x ≤ 0.08) are synthesized by solid-state reaction and the electronic transport propertiesmore » are investigated. Rietveld refinement confirms the formation of single phase orthorhombic structure with gradual increase of cell parameters with doping level. The electronic transport properties such as Seebeck coefficient and electrical resistivity decrease with increasing the dopant concentration for both the co-substituted compositions. All the compositions of Ca{sub 1−x}Ln{sub x}Mn{sub 1−x}Nb{sub x}O{sub 3} show nonmetal-like temperature dependence of resistivity; whereas metal-like temperature dependence of thermopower. This inconsistency is explained by the formation of oxygen vacancy associated defect centres that originates from partial reduction of Mn{sup 4+} to Mn{sup 3+} due to co-substitution. The defect centres act as extrinsic carriers and cause additional contribution to the entropy of the system, leading to increase of Seebeck coefficient as a function of temperature. The transport mechanism of charge carriers is explained in the framework of Mott’s small polaron hopping mechanism.« less
Phase relations in the pseudo ternary system In2O3-TiO2-BO (B: Zn, Co and Ni) at 1200 °C in air
NASA Astrophysics Data System (ADS)
Brown, Francisco; Jacobo-Herrera, Ivan Edmundo; Alvarez-Montaño, Victor Emmanuel; Kimizuka, Noboru; Hirano, Tomonosuke; Sekine, Ryotaro; Denholme, Saleem J.; Miyakawa, Nobuaki; Kudo, Akihiko; Iwase, Akihide; Michiue, Yuichi
2018-02-01
Phase relations in the pseudo ternary systems In2O3-TiO2-ZnO, In2O3-TiO2-CoO and In2O3-TiO2-NiO at 1200 °C in air were determined by means of a classic quenching method. In6Ti6BO22 (B: Zn, Co and Ni) which has the monoclinic In(Fe1/4Ti3/4)O27/8-type of structure with a 4-dimensional super space group exists in a stable form. There exist homologous phases In1+x(Ti1/2Zn1/2)1-xO3(ZnO)m (m: natural number, 0
DSTO Landmine Detection Test Targets
2005-06-01
cm diameter, 10 cm high. x x GS 32D50 Galvanised steel, pipe, hollow, 32 cm diameter, 50 cm long, ends capped x x GS 45D50 Galvanised Steel, pipe...hollow, 45 cm diameter, 50 cm long, ends capped x x GS 75D50 Galvanised Steel, pipe, hollow, 75 cm diameter, 50 cm long, ends capped x x
Evolution of Cygnus X-3 through its Radio and X-ray States
NASA Astrophysics Data System (ADS)
Szostek, A.; Zdziarski, A. A.; McCollough, M. L.
2009-05-01
Based on X-ray spectra and studies of the long-term correlated behavior between radio and soft X-ray, we present a detailed evolution of Cyg X-3 through its radio and X-ray states. We comment on the nature of the hard X-ray tail and possible Simbol X contribution in constraining the models.
17 CFR 229.601 - (Item 601) Exhibits.
Code of Federal Regulations, 2014 CFR
2014-04-01
... administered by the Commission. 2. In any case where two or more indentures, contracts, franchises, or other... computation of ratios X X X X X X X X (13) Annual report to security holders, Form 10-Q or quarterly report to... prospectus as permitted by the registration statement; or, in the case of the Form 10-K, where the annual...
17 CFR 229.601 - (Item 601) Exhibits.
Code of Federal Regulations, 2013 CFR
2013-04-01
... administered by the Commission. 2. In any case where two or more indentures, contracts, franchises, or other... computation of ratios X X X X X X X X (13) Annual report to security holders, Form 10-Q or quarterly report to... prospectus as permitted by the registration statement; or, in the case of the Form 10-K, where the annual...
17 CFR 229.601 - (Item 601) Exhibits.
Code of Federal Regulations, 2012 CFR
2012-04-01
... administered by the Commission. 2. In any case where two or more indentures, contracts, franchises, or other... computation of ratios X X X X X X X X (13) Annual report to security holders, Form 10-Q or quarterly report to... prospectus as permitted by the registration statement; or, in the case of the Form 10-K, where the annual...
Subtleties of Hidden Quantifiers in Implication
ERIC Educational Resources Information Center
Shipman, Barbara A.
2016-01-01
Mathematical conjectures and theorems are most often of the form P(x) ? Q(x), meaning ?x,P(x) ? Q(x). The hidden quantifier ?x is crucial in understanding the implication as a statement with a truth value. Here P(x) and Q(x) alone are only predicates, without truth values, since they contain unquantified variables. But standard textbook…
The Deployment Life Study. Appendixes
2014-01-01
dMdC SOFS x x immigration status Created for deployment Life Study x x Religious engagement or denomination FpnMAd (Trail and Karney, 2012) x x x x...Homefront Study (Chandra, Burns, et al., 2008; Chandra, Lara-Cinisomo, Jaycox, Tanielian, Han, et al., 2011) x (post) Health and well-being physical health...authorities. We will not be asking questions about sexual or physical | | | | | | | | | abuse of a child, but you should know that, if this information is
Practical To Tactical: Making the Case for a Shift in Ground Vehicle Robotics
2012-05-10
with Driver Warning I C R M x x x V x UNCLASSIFIED 21 Electronic Brake System ( ELB ) w/ Electronic Stability Control (ESC) Electric Power Assist...System ( ELB ) w/ Electronic Stability Control (ESC) Electric Power Assist Steering Steering Position Sensor Steering Torque Sensor Transmission...Computer I C R M x x x V x x Wheel Speed Sensors ESC Accelerometer/Rate Gyro UNCLASSIFIED 23 Electronic Brake System ( ELB ) w/ Electronic
Synchronizable Series Expressions. Part 2. Overview of the Theory and Implementation.
1987-11-01
more running time than shown in the table. because time is eventually required in order to collect the garbage it creates. Program Running ’rime Garbage...possible to simply put an enumerator where it is used.) (loop for x integer from I to 4 collect x) - (lotS* ((x (Eup I :to 4))) (declare (type integer x...below. (loop for x from 1 to 4 and for y = 0 then (1- x) collect (list x y)) - (lotS* ((x (Eup 1 :to 4)) (y (Tprevious (1- x) 0))) (Rlist (list x y
Geographic Resources Analysis Support System (GRASS) Version 4.0 User’s Reference Manual
1992-06-01
inpur-image need not be square; before processing, the X and Y dimensions of the input-image are padded with zeroes to the next highest power of two in...structures an input kowledge /control script with an appropriate combination of map layer category values (GRASS raster map layers that contain data on...F cos(x) cosine of x (x is in degrees) F exp(x) exponential function of x F exp(x,y) x to the power y F float(x) convert x to floating point F if
NASA Technical Reports Server (NTRS)
Curry, Donald M.; Lewis, Ronald K.; Hagen, Jeffrey D.
2002-01-01
An X-38 Crew Return Vehicle Seal Development is presented. The contents include: 1) X-38 Crew Return Vehicle; 2) X-38 TPS Configuration; 3) X-38 Seal Locations; 4) X-38 Rudder/Fin Seal Assembly; 5) Baseline X-38 Rudder/Fin Seal Design; 6) Rudder/Fin Seal to Bracket Assembly; 7) X-38 Rudder/Fin Vertical Rub Surface Inconel-0.10 inches; 8) X-38 Rudder/Fin Seal Analysis; 9) Seal Analysis Model; and 10) Governing Differential Equations for Equilibrium Thermal Assumption. The X-38 Rudder/Fin Seal temperature and pressure properties are also given.
Evaluation of Various Navigation System Concepts
1982-03-01
Naigatimon aar01 N DAutomatic x xx Parallel 0fn x x x x x’ "OLeg t dung. n Mrankuhld M ni raia x N x to~g TAN is I OmuI,2 2mN 0 x "to - - -x...and must permit design of indicators and controls which can be directly interpreted or operated by the pilot at his normal station aboard the...the responsibility of control. The organization that controls the system can theoretically limit access to the system. Because VOVO/DME, Loran-C, and
Post-Service Earnings of Vietnam-Era Veterans.
1987-12-01
vets, for ihany faictors that civilian waces . 1contribLitC to earnings. f5 S. Bolin. Hess & Little Reereosion analysis Use of military trainingiI! %1... Method to Learn Job On the Job lraining X X = of Employers X SES X Completed Civilian Training X Duncan X Change in Duncan X Rotter X I nion X ;IPR\\TE X...career 0 =No Method of entry ENTRY I = Drafted into military 2 = Enlisted 3 = OCS :ROTC*ACADEM Y 4 = Other Type of training TTYPE 0= None ini ilitary I
NASA Technical Reports Server (NTRS)
Gendreau, Keith (Inventor); Martins, Jose Vanderlei (Inventor); Arzoumanian, Zaven (Inventor)
2010-01-01
An X-ray diffraction and X-ray fluorescence instrument for analyzing samples having no sample preparation includes a X-ray source configured to output a collimated X-ray beam comprising a continuum spectrum of X-rays to a predetermined coordinate and a photon-counting X-ray imaging spectrometer disposed to receive X-rays output from an unprepared sample disposed at the predetermined coordinate upon exposure of the unprepared sample to the collimated X-ray beam. The X-ray source and the photon-counting X-ray imaging spectrometer are arranged in a reflection geometry relative to the predetermined coordinate.
Pipe Storage and Movement Study
1986-02-01
API 5L Points Higher Price Than API 5L Grades A or B Wall Range—X Grades X42 * X46* X52 * X60 X65 X70* * All Walls...thereof may be used at Mill Option for API 5L Grades X42, X46 and X52 unless specifically prohibited. * * DSAW only. NOTES: For Intermediate Grodes, apply...A53, BW, S 80, GALV 1-1/4", STL, A53, BW, S 80, GALV 2", STL, A53, BW, S 80, GALV 8", STL, API - 5L GR X-42, ERW, STD 3-1/2"OD, STL, API - 5L GR
Ultra low thermal expansion, highly thermal shock resistant ceramic
Limaye, S.Y.
1996-01-30
Three families of ceramic compositions having the given formula: {phi}{sub 1+X}Zr{sub 4}P{sub 6{minus}2X}Si{sub 2X}O{sub 24}, {phi}{sub 1+X}Zr{sub 4{minus}2X}Y{sub 2X}P{sub 6}O{sub 24} and {phi}{sub 1+X}Zr{sub 4{minus}X}Y{sub X}P{sub 6{minus}2X}Si{sub X}O{sub 24} wherein {phi} is either strontium or barium and X has a value from about 0.2 to about 0.8 have been disclosed. Ceramics formed from these compositions exhibit very low, generally near neutral, thermal expansion over a wide range of elevated temperatures. 7 figs.
X-Pinch And Its Applications In X-ray Radiograph
DOE Office of Scientific and Technical Information (OSTI.GOV)
Zou Xiaobing; Wang Xinxin; Liu Rui
2009-07-07
An X-pinch device and the related diagnostics of x-ray emission from X-pinch were briefly described. The time-resolved x-ray measurements with photoconducting diodes show that the x-ray pulse usually consists of two subnanosecond peaks with a time interval of about 0.5 ns. Being consistent with these two peaks of the x-ray pulse, two point x-ray sources of size ranging from 100 mum to 5 mum and depending on cut-off x-ray photon energy were usually observed on the pinhole pictures. The x-pinch was used as x-ray source for backlighting of the electrical explosion of single wire and the evolution of X-pinch, andmore » for phase-contrast imaging of soft biological objects such as a small shrimp and a mosquito.« less
Handbook for Sampling and Sample Preservation of Water and Wastewater
1992-05-01
integers from 1 to N. N E Xi = XI1 + X 2 + X 3 . ..... + XN i=l 1 In the above example (from Table 4.1), X1 = 35.8, X2 = 33.0, ... , XN = X52 32.4; N E...41e 0 b10) -4 r- -C) a) 5l %Dt C) ON qc -0 Cl qtr C -4 %D cvj qw a) C )L- L~~~J enC- ..4 m~a CV) .4 c P.. .4 cnm0 q5C) )n me .-4C) - (J 1 () e U m. 0-4...X(l) = X = 35.8, X(2) = X2 = 33.0,..., X(52) = X52 = 32.4. X(t) is the linear trend. X’(t) is the random component. In this case, the trend can be
Valence band offsets of Sc x Ga1-x N/AlN and Sc x Ga1-x N/GaN heterojunctions
NASA Astrophysics Data System (ADS)
Tsui, H. C. L.; Goff, L. E.; Palgrave, R. G.; Beere, H. E.; Farrer, I.; Ritchie, D. A.; Moram, M. A.
2016-07-01
The valence band offsets of Sc x Ga1-x N/AlN heterojunctions were measured by x-ray photoelectron spectroscopy (XPS) and were found to increase from 0.42 eV to 0.95 eV as the Sc content x increased from 0 to 0.15. The increase in valence band offset with increasing x is attributed to the corresponding increase in spontaneous polarization of the wurtzite structure. The Sc x Ga1-x N/AlN heterojunction is type I, similar to other III-nitride-based heterojunctions. The data also indicate that a type II staggered heterojunction, which can enhance spatial charge separation, could be formed if Sc x Ga1-x N is grown on GaN.
Soft X-ray variability over the present minimum of solar activity as observed by SphinX
NASA Astrophysics Data System (ADS)
Gburek, S.; Siarkowski, M.; Kepa, A.; Sylwester, J.; Kowalinski, M.; Bakala, J.; Podgorski, P.; Kordylewski, Z.; Plocieniak, S.; Sylwester, B.; Trzebinski, W.; Kuzin, S.
2011-04-01
Solar Photometer in X-rays (SphinX) is an instrument designed to observe the Sun in X-rays in the energy range 0.85-15.00 keV. SphinX is incorporated within the Russian TESIS X and EUV telescope complex aboard the CORONAS-Photon satellite which was launched on January 30, 2009 at 13:30 UT from the Plesetsk Cosmodrome, northern Russia. Since February, 2009 SphinX has been measuring solar X-ray radiation nearly continuously. The principle of SphinX operation and the content of the instrument data archives is studied. Issues related to dissemination of SphinX calibration, data, repository mirrors locations, types of data and metadata are discussed. Variability of soft X-ray solar flux is studied using data collected by SphinX over entire mission duration.
Thermal and electrochemical behavior of Cu{sub 4−x}Li{sub x}S{sub 2} (x=1, 2, 3) phases
DOE Office of Scientific and Technical Information (OSTI.GOV)
Chen, Erica M.; Poudeu, Pierre F.P., E-mail: ppoudeup@umich.edu
Several compositions of the Cu{sub 4−x}Li{sub x}S{sub 2} (x=1, 2, 3) series were synthesized via solid-state reaction of the elements. The structural stability at various temperatures and the effect of Li:Cu ratio on the thermal conductivity and the electrochemical performance of Cu{sub 4−x}Li{sub x}S{sub 2}/Li half-cells during charge–discharge process were investigated. Differential scanning calorimetry (DSC) measurements showed a sharp endothermic peak at 140 °C for Cu{sub 4−x}Li{sub x}S{sub 2} samples with x=1 and 2, which is ascribed to a structural phase transition. X-ray diffraction (XRD) measurements on various Cu{sub 4−x}Li{sub x}S{sub 2} samples at temperatures below and above 140 °Cmore » indicated a structural phase transition from the room temperature low-symmetry structure to the high temperature cubic structure of Cu{sub 2}S. The thermal conductivity of Cu{sub 4−x}Li{sub x}S{sub 2} samples decreases with decreasing Cu:Li ratio and with increasing temperature. The thermal conductivity of Cu{sub 4−x}Li{sub x}S{sub 2} samples at room temperature decreases from 1.2 W/m K for Cu:Li=3:1 to 0.7 W/m K for Cu:Li=1:3. Cyclic voltammetry of Cu{sub 4−x}Li{sub x}S{sub 2}/Li half-cells showed that high discharge capacity (165 mA h g{sup −1}) and stable reversible charge–discharge process is observed for Cu:Li=2:2, whereas other Cu:Li ratios lead to low discharge capacity and poor reversibility. The electrochemical behavior of Cu{sub 4−x}Li{sub x}S{sub 2}/Li half-cells is rationalized by taking into account the competing reactions of Li{sup +} ions with CuS and Cu{sub 2}S during discharge. - Graphical abstract: Tuning Li content in Cu{sub 4−x}Li{sub x}S{sub 2}/Li half-cells to maintain a Cu/Li ratio equal to unity affords maximum capacity and high stability of the charge–discharge process. - Highlights: • Cu:Li ratio strongly influenced crystal structure and properties of Cu{sub 4-x}Li{sub x}S{sub 2}. • Compositions with x = 1 and 2 undergo structural transformation at above 140 °C. • Thermal conductivity of Cu{sub 4-x}Li{sub x}S{sub 2} phases increases with decreasing Cu:Li ratio. • Stability of Cu{sub 4-x}Li{sub x}S{sub 2}/Li half-cells decreases with Cu:Li ratio. • Initial charge capacity of Cu{sub 4-x}Li{sub x}S{sub 2}/Li half-cells increases with Cu:Li ratio.« less
Introduction of meat sheep breeds in extensive systems of Patagonia: lamb growth and survival.
Alvarez, M; Rodríguez Iglesias, R M; García Vinent, J; Giorgetti, H; Baselga, M
2010-04-01
Genotype effects on lamb growth, survival, and commercial finishing were estimated in a 5-yr study aimed at assessing potential benefits from introducing meat breeds into extensive sheep systems of northeastern Patagonia. Five ram [Corriedale: CO; Border Leicester: BL; Ile de France: IF; Texel: TX; and synthetic CRIII (25% Merino, 37.5% IF, 37.5% TX)] and 5 dam (CO; synthetic CRIII; BLCO: BL x CO; IFCO: IF x CO; and TXCO: TX x CO) genotypes were represented in the study. Data were collected from 1,426 born and 1,258 weaned lambs of 9 resulting genotypes (CO x CO, BL x CO, IF x CO, TX x CO, CRIII x CO, CRIII x BLCO, CRIII x IFCO, CRIII x TXCO, and CRIII x CRIII). Birth weight was recorded on all lambs; subsequently, BW and BCS (scale 1 to 5) were recorded at regular intervals until weaning. Body weights were adjusted to 60 and 90 (weaning) d of age, and ADG were calculated from the adjusted BW for the periods 0 to 60 d and 60 to 90 d; BCS was adjusted to 90 d. Survival to weaning and percentage of lambs reaching commercial finishing (BW >or= 23 kg and BCS >or= 2.5 points) were also recorded. Significant (P < 0.05) genotype x litter size interactions were detected for birth weight and ADG 60 to 90 d. With the exception of CRIII x CO, crossbred and synthetic genotypes presented greater (P < 0.05) ADG 0 to 60 d and BW at 60 and 90 d than CO x CO lambs. Second cross lambs reared as singles presented greater ADG 60 to 90 d (P < 0.05) than BL x CO, TX x CO, and CRIII x CO, but less (P < 0.05) ADG 60 to 90 d, and no differences were observed for twins. The IF x CO, CRIII x BLCO, CRIII x IFCO, and CRIII x CRIII genotypes showed greater BCS at 90 d (P < 0.05) than CO x CO. The probability of greater commercial finishing for crossbred and synthetic genotypes relative to CO x CO was at least 79%. Probabilities of greater survival to weaning in CO x CO and CRIII x BLCO lambs relative to IF x CO, TX x CO, CRIII x CO, and CRIII x CRIII lambs were greater than 81%. Results indicate significant improvements in lamb BW and saleable lambs from the introduction of meat genotypes. Among the terminal sire breeds evaluated, BL and IF would produce the greatest impact. Differential nutritional management of pregnant ewes carrying twins and of twin lambs beyond 60 d should be implemented to mitigate litter size x genotype interactions constraining growth potential benefits, which may be critical for northeastern Patagonia conditions.
De Clercq, E; Stollar, B D; Hobbs, J; Fukui, T; Kakiuchi, N; Ikehara, M
1980-01-01
In addition to the 2'-azido analogue of (I)n x (C)n, (dIn3)n x (C)n, we have found two other (I)n x (C)n analogues, (dIfl)n x (C)n and (dIcl)n x (C)n, in which the 2'-hydroxyls of the (I)n strand are replaced by either fluorine or chlorine, to be highly effective in inducing interferon. This contrasted with the lack of interferon-inducing activity noted for various other 2'-halogeno analogues of (I)n x (C)n and (A)n x (U)n, i.e. (I)n x (dCcl)n, (dAfl)n x (U)n, (dAcl)n x (U)n, (A)n x (dUfl)n and (A)n x (dUcl)n. In most assay systems, viz. primary rabbit kidney cells, human diploid fibroblasts, HeLa cells, interferon-primed mouse L-929 cells, and intact rabbits, (dIfl)n x (C)n and (dIcl)n x (C)n induced interferon levels that were comparable to those induced by (I)n x (C)n. There was one particular system (L-929 cells treated with DEAE-dextran), however, in which (dIfl)n x (C)n and (dIcl)n x (C)n, unlike (I)n x (C)n, failed to stimulate interferon production. As monitored by both radiochemical and biological means, (dIfl)n x (C)n and, to a lesser extent, (dIcl)n x (C)n were more resistant to degradation by ribonuclease A, T1 and human serum nucleases than was (I)n x (C)n. In their reactivity towards antibodies to double-stranded RNA (dIfl)n x (C)n and (dIcl)n x (C)n conformed more closely to (I)n x (C)n than did other 2'-substituted (e.g. 2'-O-methyl or 2'-O-ethyl) analogues of (I)n x (C)n. The high interferon-inducing potency of (dIfl)n x (C)n and (dIcl)n x (C)n has both theoretical and practical implications. While our findings suggest that (dIfl)n x (C)n and (dIcl)n x (C)n should be further explored for their therapeutic potentials, they also strengthen the notion that the interferon-inducing capacity, and possibly other biological functions of double-stranded RNAs is dependent on the recognition of the overall conformation of the polynucleotide rather than on the binding of specific functional groups such as the 2'-hydroxyl group.
DOE Office of Scientific and Technical Information (OSTI.GOV)
Cao, Yong; Duan, Nanqi; Yan, Dong, E-mail: yand@hust.edu.cn
Ca{sub 0.01}La{sub 0.99−x}Sm{sub x}NbO{sub 4−δ} (x=0, 0.1, 0.2, 0.4, 0.6, 0.8, 0.99) is prepared by using a solid reaction route, and single phase is achieved. Structural and phase transformation of Ca{sub 0.01}La{sub 0.99−x}Sm{sub x}NbO{sub 4−δ} have been characterized by high temperature X-ray diffraction. The lattice parameters a, b, c decrease and γ increases with increasing x, at both room and high temperature. The phase transformation temperature increases linearly with increasing x for Ca{sub 0.01}La{sub 0.99−x}Sm{sub x}NbO{sub 4−δ}. The electrical conductivity of Ca{sub 0.01}La{sub 0.99−x}Sm{sub x}NbO{sub 4−δ} is measured in wet air. A clear relationship between the structural, phase transformation andmore » electrical conductivity of Ca{sub 0.01}La{sub 0.99−x}Sm{sub x}NbO{sub 4−δ} is built, which will provide a guideline to tailor the electrical conductivity. - Graphical abstract: Structural and phase transformation of Ca{sub 0.01}La{sub 0.99−x}Sm{sub x}NbO{sub 4−δ} have been characterized by high temperature X-ray diffraction, as well as the conductivity of Ca{sub 0.01}La{sub 0.99−x}Sm{sub x}NbO{sub 4−δ} in wet air. A clear relationship between the structural, phase transformation and electrical conductivity of Ca{sub 0.01}La{sub 0.99−x}Sm{sub x}NbO{sub 4−δ} is built. - Highlights: • Ca{sub 0.01}La{sub 0.99−x}Sm{sub x}NbO{sub 4−δ} with various Sm contents was prepared. • Structure, phase transformation and electrical conductivity of Ca{sub 0.01}La{sub 0.99−x}Sm{sub x}NbO{sub 4−δ} were characterized. • A relationship between the structure, phase transformation and electrical conductivity was well established.« less
Code of Federal Regulations, 2013 CFR
2013-10-01
...), telecommunications network management services (D316), automated news services, data services or other information... environmental laboratories * * X * * X (5) Research and development X X X X (6) Transportation services...
Code of Federal Regulations, 2014 CFR
2014-10-01
...), telecommunications network management services (D316), automated news services, data services or other information... environmental laboratories * * X * * X (5) Research and development X X X X (6) Transportation services...
DOE Office of Scientific and Technical Information (OSTI.GOV)
Auwal, I.A.; Güngüneş, H.; Güner, S.
Highlights: • SrBi{sub x}La{sub x}Y{sub x}Fe{sub 12−3x}O{sub 19} (0.0 ≤ x ≤ 0.33) hexaferrites have been prepared by sol-gel autocombustion. • XRD patterns show that SrBi{sub x}La{sub x}Y{sub x}Fe{sub 12−3x}O{sub 19} (0.0 ≤ x ≤ 0.33) hexaferrites exhibit hexagonal structure. • The intrinsic coercivity (H{sub ci}) above 15000 Oe reveals that all samples are magnetically hard materials. - Abstract: SrBi{sub x}La{sub x}Y{sub x}Fe{sub 12−3x}O{sub 19} (0.0 ≤ x ≤ 0.33) hexaferrites were produced via sol-gel auto combustion. XRD patterns show that all the samples are single-phase M-type strontium hexaferrite (SrM). The magnetic hysteresis (σ-H) loops revealed the ferromagnetic nature ofmore » nanoparticles (NPs). The coercive field decreases from 4740 Oe to 2720 Oe with increasing ion content. In particular, SrBi{sub x}La{sub x}Y{sub x}Fe{sub 12−3x}O{sub 19} NPs with x = 0.0, 0.1, 0.2 have suitable magnetic characteristics (σ{sub s} = 62.03–64.72 emu/g and H{sub c} = 3105–4740 Oe) for magnetic recording. The intrinsic coercivity (H{sub ci}) above 15000 Oe reveals that all samples are magnetically hard materials. Tauc plots were used to specify the direct optical energy band gap (E{sub g}) of NPs. The E{sub g} values are between 1.76 eV and 1.85 eV. {sup 57}Fe Mössbauer spectroscopy data, the variation in line width, isomer shift, quadrupole splitting, relative area and hyperfine magnetic field values on Bi{sup 3+} La{sup 3+} and Y{sup 3+} substitutions have been determined.« less
Pharmacological characterization of recombinant human and rat P2X receptor subtypes.
Bianchi, B R; Lynch, K J; Touma, E; Niforatos, W; Burgard, E C; Alexander, K M; Park, H S; Yu, H; Metzger, R; Kowaluk, E; Jarvis, M F; van Biesen, T
1999-07-02
ATP functions as a fast neurotransmitter through the specific activation of a family of ligand-gated ion channels termed P2X receptors. In this report, six distinct recombinant P2X receptor subtypes were pharmacologically characterized in a heterologous expression system devoid of endogenous P2 receptor activity. cDNAs encoding four human P2X receptor subtypes (hP2X1, hP2X3, hP2X4, and hP2X7), and two rat P2X receptor subtypes (rP2X2 and rP2X3), were stably expressed in 1321N1 human astrocytoma cells. Furthermore, the rP2X2 and rP2X3 receptor subtypes were co-expressed in these same cells to form heteromultimeric receptors. Pharmacological profiles were determined for each receptor subtype, based on the activity of putative P2 ligands to stimulate Ca2+ influx. The observed potency and kinetics of each response was receptor subtype-specific and correlated with their respective electrophysiological properties. Each receptor subtype exhibited a distinct pharmacological profile, based on its respective sensitivity to nucleotide analogs, diadenosine polyphosphates and putative P2 receptor antagonists. Alphabeta-methylene ATP (alphabeta-meATP), a putative P2X receptor-selective agonist, was found to exhibit potent agonist activity only at the hP2X1, hP2X3 and rP2X3 receptor subtypes. Benzoylbenzoic ATP (BzATP, 2' and 3' mixed isomers), which has been reported to act as a P2X7 receptor-selective agonist, was least active at the rat and human P2X7 receptors, but was a potent (nM) agonist at hP2X1, rP2X3 and hP2X3 receptors. These data comprise a systematic examination of the functional pharmacology of P2X receptor activation.
Anatomy of a Visible Light Activated Photocatalyst for Water Splitting
Phivilay, Somphonh Peter; Roberts, Charles; Gamalski, Andrew; ...
2018-06-08
The supported mixed oxide (Rh 2-yCr yO 3)/(Ga 1-xZn x)(N 1-xO x) photocatalyst, highly active for splitting of H 2O, was extensively characterized for its bulk and surface properties with the objective of developing fundamental structure-photoactivity relationships. Raman and UV-vis spectroscopy revealed that the molecular and electronic structures, respectively, of the oxynitride (Ga 1-xZn x)(N 1-xO x) support are not perturbed by the deposition of the (Rh 2-yCr yO 3) NPs. Photoluminescence (PL) spectroscopy, however, showed that the oxynitride (Ga 1-xZn x)(N 1-xO x) support is the source of excited electrons/holes and the (Rh 2-yCr yO 3) NPs greatly reducemore » the undesirable recombination of photoexcited electron/holes by acting as efficient electron traps as well as increase the lifetimes of the excitons. High Resolution-XPS and High Sensitivity-LEIS surface analyses reveal that the surfaces of the (Rh 2-yCr yO 3) NPs consist of Rh +3 and Cr +3 mixed oxide species. In Situ AP-XPS help to reveal that the Rh+3 and surface N atoms are involved in water splitting. Dispersed RhOx species on the (Ga 1-xZn x)(N 1-xO x) support and on CrO x NPs were found to be the photocatalytic active sites for H 2 generation and N and Zn sites from the (Ga 1-xZn x)(N 1-xO x) support are the photocatalytic active site for O 2 generation. The current investigation establishes the fundamental structure-photoactivity relationships of these visible light activated photocatalysts.« less
NASA Astrophysics Data System (ADS)
Trukhanov, S. V.; Lobanovski, L. S.; Bushinsky, M. V.; Khomchenko, V. A.; Pushkarev, N. V.; Troyanchuk, I. O.; Maignan, A.; Flahaut, D.; Szymczak, H.; Szymczak, R.
2004-11-01
The crystal structure, magnetization and electrical transport depending on the temperature and magnetic field for the doped stoichiometric La_{1-x}^{3 + } Sr_x^{2 + } Mn_{1-x}^{3 + } Mn_x^{4 + } O_3^{2-} as well as anion-deficient La_{1-x}^{3 + } Sr_x^{2 + } Mn^{3 + }O_{3-x/2}^{2-} (0le x le 0.30) ortomanganite systems have been experimentally studied. It is established that the stochiometric samples in the region of the 0 le x le 0.125 are an O'-orthorhombic perovskites whereas in the 0.175 le x le 0.30 - a rhombohedric. For the anion-deficient system the symmetry type of the unit cell is similar to the stoichiometric one. As a doping level increases the samples in the ground state undergo a number of the magnetic transitions. It is assumed that the samples with the large amount of oxygen vacancies are a cluster spin glasses (0.175 < x le 0.30) and temperature of the magnetic moment freezing is 40 K. All the anion-deficient samples are semiconductors and show considerable magnetoresistance over a wide temperature range with a peak for the x = 0.175 only. Concentration dependences of the spontaneous magnetization and magnetic ordering temperature for the anion-deficient La_{1-x}^{3 + } Sr_x^{2 + } Mn^{3 + }O_{3-x/2}^{2-} system have been established by the magnetic measurements and compared with those for the stoichiometric La_{1-x}^{3 + } Sr_x^{2 + } Mn_{1-x}^{3 + } Mn_x^{4 + } O_3^{2-} one. The magnetic propeprties of the anion-deficient samples may be interpreted on the base of the superexchange interaction and phase separation (chemical disorder) models.
DOE Office of Scientific and Technical Information (OSTI.GOV)
Lin, Yu-Chang; Lee, Hsin-Ying, E-mail: hylee@ee.ncku.edu.tw; Lee, Ching-Ting
2016-01-15
A plasma-enhanced atomic layer deposition (PE-ALD) system was used to deposit magnesium zinc oxide (Mg{sub x}Zn{sub 1−x}O) films with various Mg content (x). The Mg{sub x}Zn{sub 1-x}O films were applied to metal–semiconductor–metal ultraviolet (UV) photodetectors (MSM-UPDs) as an active layer. The Mg content in the Mg{sub x}Zn{sub 1-x}O films was modulated by adjusting the ZnO–MgO cycle ratios to 15:1, 12:1, and 9:1. Correspondingly, the Mg content in the Mg{sub x}Zn{sub 1-x}O films characterized using an energy dispersive spectrometer was 0.10, 0.13, and 0.16, respectively. The optical bandgap of the Mg{sub x}Zn{sub 1-x}O films increased from 3.56 to 3.66 eV withmore » an increase in Mg content from 0.10 to 0.16. The peak position of photoresponsivity for the Mg{sub x}Zn{sub 1-x}O MSM-UPDs was also shifted from 350 to 340 nm. The UV-visible rejection ratios of the Mg{sub x}Zn{sub 1-x}O MSM-UPDs were higher than 3 orders of magnitude. In addition, excellent detectivity and noise equivalent power for the Mg{sub x}Zn{sub 1-x}O MSM-UPDs were observed at a bias voltage of 5 V. The high performance of the Mg{sub x}Zn{sub 1-x}O MSM-UPDs was achieved by PE-ALD at a low temperature.« less
DOE Office of Scientific and Technical Information (OSTI.GOV)
Thirumal, M.; Jawahar, I.N.; Surendiran, K.P.
2002-11-20
Oxides belonging to the families Ba{sub 3}ZnTa{sub 2-x}Nb{sub x}O{sub 9} and Ba{sub 3}MgTa{sub 2-x}Nb{sub x}O{sub 9} were synthesized by the solid state reaction route. Sintering temperatures of 1300 deg. C led to oxides with disordered (cubic) perovskite structure. However, on sintering at 1425 deg. C hexagonally ordered structures were obtained for Ba{sub 3}MgTa{sub 2-x}Nb{sub x}O{sub 9} over the entire range (0{<=}x{<=}1) of composition, while for Ba{sub 3}ZnTa{sub 2-x}Nb{sub x}O{sub 9} the ordered structure exists in a limited range (0{<=}x{<=}0.5). The dielectric constant is close to 30 for the Ba{sub 3}ZnTa{sub 2-x}Nb{sub x}O{sub 9} family of oxides while the Mg analoguesmore » have lower dielectric constant of {approx}18 in the range 50 Hz to 500 kHz. At microwave frequencies (5-7 GHz) dielectric constant increases with increase in niobium concentration (22-26) for Ba{sub 3}ZnTa{sub 2-x}Nb{sub x}O{sub 9}; for Ba{sub 3}MgTa{sub 2-x}Nb{sub x}O{sub 9} it varies between 12 and 14. The 'Zn' compounds have much higher quality factors and lower temperature coefficient of resonant frequency compared to the 'Mg' analogues.« less
Anatomy of a Visible Light Activated Photocatalyst for Water Splitting
DOE Office of Scientific and Technical Information (OSTI.GOV)
Phivilay, Somphonh Peter; Roberts, Charles; Gamalski, Andrew
The supported mixed oxide (Rh 2-yCr yO 3)/(Ga 1-xZn x)(N 1-xO x) photocatalyst, highly active for splitting of H 2O, was extensively characterized for its bulk and surface properties with the objective of developing fundamental structure-photoactivity relationships. Raman and UV-vis spectroscopy revealed that the molecular and electronic structures, respectively, of the oxynitride (Ga 1-xZn x)(N 1-xO x) support are not perturbed by the deposition of the (Rh 2-yCr yO 3) NPs. Photoluminescence (PL) spectroscopy, however, showed that the oxynitride (Ga 1-xZn x)(N 1-xO x) support is the source of excited electrons/holes and the (Rh 2-yCr yO 3) NPs greatly reducemore » the undesirable recombination of photoexcited electron/holes by acting as efficient electron traps as well as increase the lifetimes of the excitons. High Resolution-XPS and High Sensitivity-LEIS surface analyses reveal that the surfaces of the (Rh 2-yCr yO 3) NPs consist of Rh +3 and Cr +3 mixed oxide species. In Situ AP-XPS help to reveal that the Rh+3 and surface N atoms are involved in water splitting. Dispersed RhOx species on the (Ga 1-xZn x)(N 1-xO x) support and on CrO x NPs were found to be the photocatalytic active sites for H 2 generation and N and Zn sites from the (Ga 1-xZn x)(N 1-xO x) support are the photocatalytic active site for O 2 generation. The current investigation establishes the fundamental structure-photoactivity relationships of these visible light activated photocatalysts.« less
Koshimizu, Taka-aki; Ueno, Susumu; Tanoue, Akito; Yanagihara, Nobuyuki; Stojilkovic, Stanko S; Tsujimoto, Gozoh
2002-12-06
P2X purinergic receptors (P2XRs) differ among themselves with respect to their ligand preferences and channel kinetics during activation, desensitization, and recovery. However, the contributions of distinct receptor subdomains to the subtype-specific behavior have been incompletely characterized. Here we show that homomeric receptors having the extracellular domain of the P2X(3) subunit in the P2X(2a)-based backbone (P2X(2a)/X(3)ex) mimicked two intrinsic functions of P2X(3)R, sensitivity to alphabeta-methylene ATP and ecto-ATPase-dependent recovery from endogenous desensitization; these two functions were localized to the N- and C-terminal halves of the P2X(3) extracellular loop, respectively. The chimeric P2X(2a)R/X(3)ex receptors also desensitized with accelerated rates compared with native P2X(2a)R, and the introduction of P2X(2) C-terminal splicing into the chimeric subunit (P2X(2b)/X(3)ex) further increased the rate of desensitization. Physical and functional heteromerization of native P2X(2a) and P2X(2b) subunits was also demonstrated. In heteromeric receptors, the ectodomain of P2X(3) was a structural determinant for ligand selectivity and recovery from desensitization, and the C terminus of P2X(2) was an important factor for the desensitization rate. Furthermore, [gamma-(32)P]8-azido ATP, a photoreactive agonist, was effectively cross-linked to P2X(3) subunit in homomeric receptors but not in heteromeric P2X(2) + P2X(3)Rs. These results indicate that heteromeric receptors formed by distinct P2XR subunits develop new functions resulting from integrative effects of the participating extracellular and C-terminal subdomains.
Growth of (Y1-x Ca x )Ba2Cu4O8 in ambient pressure and its tri-axial magnetic alignment
NASA Astrophysics Data System (ADS)
Horii, S.; Yamaki, M.; Shimoyama, J.; Kishio, K.; Doi, T.
2015-10-01
We report the growth of single crystals in ambient pressure and tri-axial orientation under modulated rotation magnetic fields (MRFs) for (Y1-x Ca x )Ba2Cu4O8 [(Y1-x Ca x )124] with x ≤ 0.1. Rectangular (Y1-x Ca x )124 crystals approximately 50 μm in size have been successfully grown for x ≤ 0.1 in a growth temperature region from 650 °C to 750 °C. Their critical temperatures increased with x and exhibited approximately 91 K for x = 0.1. By applying an MRF of 10 T, pulverised powders of (Y1-x Ca x )124 were tri-axially aligned in epoxy resin at room temperature in a whole x region below x = 0.1. The magnitude relationship of the magnetic susceptibilities (χ) along crystallographic directions for (Y1-x Ca x )124 was χ c > χ a > χ b at room temperature and was unchanged with a change in x. From changes in the degrees of the c-axis and the in-plane orientation (Δω) for the (Y1-x Ca x )124 powder samples aligned under three different MRF conditions, it was found that MRFs above at least 1 T were required to achieve almost complete tri-axial alignment with Δω < 5°. Irreversibility lines for H//c were successfully determined even from the powder samples by the introduction of magnetic alignment without using single crystalline samples. The present study indicates that magnetic alignment is a useful process for the fabrication of quasi-single-crystals from the perspective of solid-state physics and the production of cuprate superconducting materials.
[Ecological Trendofthe Incidence of Tuberculosis in Mianyang City During 2004-2013].
Zhang, Wen-Hao; Xiao, Chuan; Ren, Tao; Wang, Li-Ping; Wang, Lan; Yuan, Ping
2016-09-01
To determine the trend of the incidence of tuberculosis (TB) in Mianyang City during 2004-2013 and its ecological determinants. Linear correlations between TB incidence and ecological factors were analyzed using the data collected in Mianyang City from 2004 to 2013. A multivariate linear regression model was established to determine the ecological predictors of TB incidence. The incidence of TB in Mianyang City decreased over the period of 2004-2013. Economic development and increased health resources were negatively correlated with TB incidence. Population density was positively correlated with TB incidence. A multivariate linear regression equationon TB incidence ( y ) was established with the independent variables ( x₁ to x ₁₀) forming a component (using principal component analysis) to eliminate multicollinearity: y =117.692-1.467 x ₁-1.145 x ₂-1.961 x ₃-4.777 x ₄-2.690 x ₅-6.181 x ₆+82.234 x ₇-2.721 x ₈-0.351 x ₉-0.382 x ₁₀. The incidence of TB decreased with the increases of real GDP per capita ( x ₁), average wage of workers( x ₂), per capita disposable income of urban residents ( x ₃), rural per capita net income ( x ₄), per capita consumption expenditure of urban residents ( x ₅), per capita living consumption expenditure of rural residents ( x ₆), number of licensed (assistant) physicians per thousand population ( x ₈), urbanization rate ( x ₉),and per capita housing construction area of urban ( x ₁₀),while it increased with the increase of density of population ( x ₇). Socio-economic development, health resources and population density are predictors of TB incidence.
A Rutile Chevron Modulation in Delafossite-Like Ga 3–x In 3 Ti x O 9+x/2
DOE Office of Scientific and Technical Information (OSTI.GOV)
Rickert, Karl; Boullay, Philippe; Malo, Sylvie
2016-05-02
The structure solution of the modulated, delafossite-related, orthorhombic Ga 3–xIn 3Ti xO 9+x/2 for x = 1.5 is reported here in conjunction with a model describing the modulation as a function of x for the entire system. Previously reported structures in the related A 3–xIn 3Ti xO 9+x/2 (A = Al, Cr, or Fe) systems use X-ray diffraction to determine that the anion lattice is the source of modulation. Neutron diffraction, with its enhanced sensitivity to light atoms, offers a route to solving the modulation and is used here, in combination with precession electron diffraction tomography (PEDT), to solve themore » structure of Ga 1.5In 3Ti 1.5O 9.75. We construct a model that describes the anion modulation through the formation of rutile chevrons as a function of x. This model accommodates the orthorhombic phase (1.5 ≤ x ≤ 2.1) in the Ga 3-xIn 3Ti xO 9+x/2 system, which transitions to a biphasic mixture (2.2 ≤ x ≤ 2.3) with a monoclinic, delafossite-related phase (2.4 ≤ x ≤ 2.5). The optical band gaps of this system are determined, and are stable at ~3.4 eV before a ~0.4 eV decrease between x = 1.9 and 2.0. After this decrease, stability resumes at ~3.0 eV. Resistance to oxidation and reduction is also presented.« less
Luminescence in microcrystalline green emitting Li2Mg1-xZrO4:xTb3+ (0.1 ≤ x ≤ 2.0) phosphor
NASA Astrophysics Data System (ADS)
Panse, V. R.; Kokode, N. S.; Shinde, K. N.; Dhoble, S. J.
2018-03-01
Green emitting Li2Mg1-xZrO4:xTb3+ (0.1 ≤ x ≤ 2.0) phosphor powders were synthesized via the wet chemical synthesis and the luminescent proprieties were studied when excited at 380 nm and present a dominant and strong green luminescence peak at 543 nm, due to D-F transition. The preparation of Li2Mg1-xZrO4:xTb3+ (0.1 ≤ x ≤ 2.0) phosphor powders were confirmed by X-ray diffraction (XRD) results without any secondary or impurity phases. The size and morphology of the Li2Mg1-xZrO4:xTb3+ (0.1 ≤ x ≤ 2.0) phosphor powders were further examined by scanning electron microscopy (SEM). Photoluminescence (PL) results have shown strongest green emission at 543 nm, which is originated due to 5D4-7F5 transition of Tb3+ ion, for the Li2Mg1-xZrO4:xTb3+ (0.1 ≤ x ≤ 2.0) phosphor. The addition of concentration Tb3+ was greatly improved the photoluminescence properties of present phosphors. The present study suggests that the Li2Mg1-xZrO4:xTb3+ (0.1 ≤ x ≤ 2.0) phosphor is a strong candidate as a green component for phosphor-converted white light-emitting diodes (LEDs).
High resolution, multiple-energy linear sweep detector for x-ray imaging
Perez-Mendez, Victor; Goodman, Claude A.
1996-01-01
Apparatus for generating plural electrical signals in a single scan in response to incident X-rays received from an object. Each electrical signal represents an image of the object at a different range of energies of the incident X-rays. The apparatus comprises a first X-ray detector, a second X-ray detector stacked upstream of the first X-ray detector, and an X-ray absorber stacked upstream of the first X-ray detector. The X-ray absorber provides an energy-dependent absorption of the incident X-rays before they are incident at the first X-ray detector, but provides no absorption of the incident X-rays before they are incident at the second X-ray detector. The first X-ray detector includes a linear array of first pixels, each of which produces an electrical output in response to the incident X-rays in a first range of energies. The first X-ray detector also includes a circuit that generates a first electrical signal in response to the electrical output of each of the first pixels. The second X-ray detector includes a linear array of second pixels, each of which produces an electrical output in response to the incident X-rays in a second range of energies, broader than the first range of energies. The second X-ray detector also includes a circuit that generates a second electrical signal in response to the electrical output of each of the second pixels.
High resolution, multiple-energy linear sweep detector for x-ray imaging
Perez-Mendez, V.; Goodman, C.A.
1996-08-20
Apparatus is disclosed for generating plural electrical signals in a single scan in response to incident X-rays received from an object. Each electrical signal represents an image of the object at a different range of energies of the incident X-rays. The apparatus comprises a first X-ray detector, a second X-ray detector stacked upstream of the first X-ray detector, and an X-ray absorber stacked upstream of the first X-ray detector. The X-ray absorber provides an energy-dependent absorption of the incident X-rays before they are incident at the first X-ray detector, but provides no absorption of the incident X-rays before they are incident at the second X-ray detector. The first X-ray detector includes a linear array of first pixels, each of which produces an electrical output in response to the incident X-rays in a first range of energies. The first X-ray detector also includes a circuit that generates a first electrical signal in response to the electrical output of each of the first pixels. The second X-ray detector includes a linear array of second pixels, each of which produces an electrical output in response to the incident X-rays in a second range of energies, broader than the first range of energies. The second X-ray detector also includes a circuit that generates a second electrical signal in response to the electrical output of each of the second pixels. 12 figs.
NASA Astrophysics Data System (ADS)
Israyandi, Zahrina, Ida; Mulia, Kamarza
2017-03-01
One of many steps in palm oil refining process is deacidification which aims to separate free fatty acids and other compounds from the oil. The deacidification process was using a green solvent, known as NADES, that consisted of betaine monohydrate and propionic acid at molar ratio of 1:8. In this study, the process conditions were optimized using the response surface method (RSM) through central composite design in order to predict the maximum distribution coefficient of palmitic acid. The obtained regression equation of the basic model for optimization was: y = 0.717 + 0.003x1 + 0.043 x2 + 0.148x3 - 0.005 x1x1 - 0.030 x2x2 + 0.047 x3x3 - 0.008 x1x2 + 0.008 x1x3 + 0.033 x2x3. The independent variables are x1 ≡ temperature (40, 60, 80 °C), x2≡ amount of palmitic acid in the palm oil (2, 5, 8 %) and x3 ≡ mass ratios of oil to NADES (1:2, 1:1, 2:1). The optimum process condition found was temperature of 62.3°C, palmitic acid content of 8%, and NADES to palm oil mass ratio of 1:2, resulting in the maximum distribution coefficient of 0.96.
DOE Office of Scientific and Technical Information (OSTI.GOV)
Li, Tao; Du, Zehui; Tamura, Nobumichi
(1-x)Pb(Zn 1/3Nb 2/3)O 3-xPbTiO 3 ((1-x)PZN-xPT in short) is one of the most important piezoelectric materials. In this study, we extensively investigated (1-x)PZN-xPT (x = 0.07–0.11) ferroelectric single crystals using in-situ synchrotron μXRD, complemented by TEM and PFM, to correlate microstructures with phase transitions. The results reveal that (i) at 25°C, the equilibrium state of (1-x)PZN-xPT is a metastable orthorhombic phase for x = 0.07 and 0.08, while it shows coexistence of orthorhombic and tetragonal phases for x = 0.09 and x = 0.11, with all ferroelectric phases accompanied by ferroelastic domains; (ii) upon heating, the phase transformation in xmore » = 0.07 is Orthorhombic → Monoclinic → Tetragonal → Cubic. The coexistence of ferroelectric tetragonal and paraelectric cubic phases was in-situ observed in x = 0.08 above Curie temperature (T C), and (iii) phase transition can be explained by the evolution of the ferroelectric and ferroelastic domains. These results disclose that (1-x)PZN-xPT are in an unstable regime, which is possible factor for its anomalous dielectric response and high piezoelectric coefficient.« less
Li, Tao; Du, Zehui; Tamura, Nobumichi; ...
2017-11-10
(1-x)Pb(Zn 1/3Nb 2/3)O 3-xPbTiO 3 ((1-x)PZN-xPT in short) is one of the most important piezoelectric materials. In this study, we extensively investigated (1-x)PZN-xPT (x = 0.07–0.11) ferroelectric single crystals using in-situ synchrotron μXRD, complemented by TEM and PFM, to correlate microstructures with phase transitions. The results reveal that (i) at 25°C, the equilibrium state of (1-x)PZN-xPT is a metastable orthorhombic phase for x = 0.07 and 0.08, while it shows coexistence of orthorhombic and tetragonal phases for x = 0.09 and x = 0.11, with all ferroelectric phases accompanied by ferroelastic domains; (ii) upon heating, the phase transformation in xmore » = 0.07 is Orthorhombic → Monoclinic → Tetragonal → Cubic. The coexistence of ferroelectric tetragonal and paraelectric cubic phases was in-situ observed in x = 0.08 above Curie temperature (T C), and (iii) phase transition can be explained by the evolution of the ferroelectric and ferroelastic domains. These results disclose that (1-x)PZN-xPT are in an unstable regime, which is possible factor for its anomalous dielectric response and high piezoelectric coefficient.« less
NASA Technical Reports Server (NTRS)
Heyd, A. R.; Alterovitz, S. A.; Croke, E. T.
1995-01-01
Si(x)Ge(1-x)heterostructures on Si substrates have been widely studied due to the maturity of Si technology. However, work on Si(x)Ge)1-x) heterostructures on Ge substrates has not received much attention. A Si(x)Ge(1-x) layer on a Si substrate is under compressive strain while Si(x)Ge(1-x) on Ge is under tensile strain; thus the critical points will behave differently. In order to accurately characterize high Ge content Si(x)Ge(1-x) layers the energy shift algorithm used to calculate alloy compositions, has been modified. These results have been used along with variable angle spectroscopic ellipsometry (VASE) measurements to characterize Si(x)Ge(1-x)/Ge superlattices grown on Ge substrates. The results agree closely with high resolution x-ray diffraction measurements made on the same samples. The modified energy shift algorithm also allows the VASE analysis to be upgraded in order to characterize linearly graded layers. In this work VASE has been used to characterize graded Si(x)Ge(1-x) layers in terms of the total thickness, and the start and end alloy composition. Results are presented for a 1 micrometer Si(x)Ge(1-x) layer linearly graded in the range 0.5 less than or equal to x less than or equal to 1.0.
Karhunen Loève approximation of random fields by generalized fast multipole methods
NASA Astrophysics Data System (ADS)
Schwab, Christoph; Todor, Radu Alexandru
2006-09-01
KL approximation of a possibly instationary random field a( ω, x) ∈ L2( Ω, d P; L∞( D)) subject to prescribed meanfield Ea(x)=∫a(ω,x) dP(ω) and covariance Va(x,x')=∫(a(ω,x)-Ea(x))(a(ω,x')-Ea(x')) dP(ω) in a polyhedral domain D⊂Rd is analyzed. We show how for stationary covariances Va( x, x') = ga(| x - x'|) with ga( z) analytic outside of z = 0, an M-term approximate KL-expansion aM( ω, x) of a( ω, x) can be computed in log-linear complexity. The approach applies in arbitrary domains D and for nonseparable covariances Ca. It involves Galerkin approximation of the KL eigenvalue problem by discontinuous finite elements of degree p ⩾ 0 on a quasiuniform, possibly unstructured mesh of width h in D, plus a generalized fast multipole accelerated Krylov-Eigensolver. The approximate KL-expansion aM( x, ω) of a( x, ω) has accuracy O(exp(- bM1/ d)) if ga is analytic at z = 0 and accuracy O( M- k/ d) if ga is Ck at zero. It is obtained in O( MN(log N) b) operations where N = O( h- d).
Structure and dielectric properties of (Ba0.7Sr0.3)1- x Na x (Ti0.9Sn0.1)1- x Nb x O3 ceramics
NASA Astrophysics Data System (ADS)
Ghoudi, Hanen; Chkoundali, Souad; Aydi, Abdelhedi; Khirouni, Kamel
2017-11-01
(Ba0.7Sr0.3)1- x Na x (Ti0.9Sn0.1)1- x Nb x O3 ceramics with compositions x = 0.6, 0.7, 0.8 and 0.9 were synthesized using the solid-state reaction method. These ceramics were examined by X-ray diffraction and dielectric measurements over a broad temperature and frequency ranges. X-ray diffraction patterns revealed a single-perovskite phase crystallized in a cubic structure, for x < 0.8, and in tetragonal, for x ≥ 0.8, with Pm3m and P4mm spaces groups, respectively. Two types of behaviors, classical ferroelectric or relaxor, were observed depending on the x composition. It is noted that temperatures T C (the Curie temperature) or T m (the temperature of maximum permittivity) rise when x increases and the relaxor character grows more significantly when x composition decreases. To analyze the dielectric relaxation degree of relaxor, various models were considered. It was proven that an exponential function could well describe the temperature dependence of the static dielectric constant and relaxation time.
X inactivation in a mammal species with three sex chromosomes.
Veyrunes, Frédéric; Perez, Julie
2018-06-01
X inactivation is a fundamental mechanism in eutherian mammals to restore a balance of X-linked gene products between XY males and XX females. However, it has never been extensively studied in a eutherian species with a sex determination system that deviates from the ubiquitous XX/XY. In this study, we explore the X inactivation process in the African pygmy mouse Mus minutoides, that harbours a polygenic sex determination with three sex chromosomes: Y, X, and a feminizing mutant X, named X*; females can thus be XX, XX*, or X*Y, and all males are XY. Using immunofluorescence, we investigated histone modification patterns between the two X chromosome types. We found that the X and X* chromosomes are randomly inactivated in XX* females, while no histone modifications were detected in X*Y females. Furthermore, in M. minutoides, X and X* chromosomes are fused to different autosomes, and we were able to show that the X inactivation never spreads into the autosomal segments. Evaluation of X inactivation by immunofluorescence is an excellent quantitative procedure, but it is only applicable when there is a structural difference between the two chromosomes that allows them to be distinguished.
Compositional dependence of magnetic anisotropy in chemically synthesized Co3- x Fe x O4 (0 ≤ x ≤ 2)
NASA Astrophysics Data System (ADS)
Hayashi, Kensuke; Yamada, Keisuke; Shima, Mutsuhiro
2018-01-01
Magnetic anisotropy of Co3- x Fe x O4 (CFO, 0 ≤ x ≤ 2) thin-film and powder samples prepared by a sol-gel method has been investigated as a function of Fe composition x. Structural analyses by X-ray diffraction show that CFO powder samples exhibit diffraction peaks associated with the spinel structure when x < 2, while CFO thin-film samples with thickness of 130-510 nm yield the peaks when 0 ≤ x ≤ 2. CFO thin-film samples are highly (111)-oriented with the Lotgering factor greater than 0.9 when 0.6 ≤ x ≤ 1.3. The magnetic anisotropy constant K 1 of CFO powder samples estimated from their room-temperature hysteresis loops yields a minimum when x = 0.9. Relatively large in-plane magnetic anisotropy (K eff = 5.7 × 105 erg/cm3) is observed for the CFO thin-film sample when x = 1.3. With increasing x, the magnetic easy axis of the spinel CFO changes from 〈111〉 to 〈100〉 when x = 0.9.
Red Light-Emitting Diode Based on Blue InGaN Chip with CdTe x S(1 - x) Quantum Dots
NASA Astrophysics Data System (ADS)
Wang, Rongfang; Wei, Xingming; Qin, Liqin; Luo, Zhihui; Liang, Chunjie; Tan, Guohang
2017-01-01
Thioglycolic acid-capped CdTe x S(1 - x) quantum dots (QDs) were synthesized through a one-step approach in an aqueous medium. The CdTe x S(1 - x) QDs played the role of a color conversion center. The structural and luminescent properties of the obtained CdTe x S(1 - x) QDs were investigated. The fabricated red light-emitting hybrid device with the CdTe x S(1 - x) QDs as the phosphor and a blue InGaN chip as the excitation source showed a good luminance. The Commission Internationale de L'Eclairage coordinates of the light-emitting diode (LED) at (0.66, 0.29) demonstrated a red LED. Results showed that CdTe x S(1 - x) QDs can be excited by blue or near-UV regions. This feature presents CdTe x S(1 - x) QDs with an advantage over wavelength converters for LEDs.
NASA Technical Reports Server (NTRS)
Hoover, Richard B. (Editor)
1992-01-01
The present conference discusses the Advanced X-ray Astrophysics Facility (AXAF) calibration by means of synchrotron radiation and its X-ray reflectivity, X-ray scattering measurements from thin-foil X-ray mirrors, lobster-eye X-ray optics using microchannel plates, space-based interferometry at EUV and soft X-ray wavelengths, a water-window imaging X-ray telescope, a graded d-spacing multilayer telescope for high energy X-ray astronomy, photographic films for the multispectral solar telescope array, a soft X-ray ion chamber, and the development of hard X-ray optics. Also discussed are X-ray spectroscopy with multilayered optics, a slit aperture for monitoring X-ray experiments, an objective double-crystal spectrometer, a Ly-alpha coronagraph/polarimeter, tungsten/boron nitride multilayers for XUV optical applications, the evaluation of reflectors for soft X-ray optics, the manufacture of elastically bent crystals and multilayer mirrors, and selective photodevices for the VUV.
On Volterra quadratic stochastic operators with continual state space
DOE Office of Scientific and Technical Information (OSTI.GOV)
Ganikhodjaev, Nasir; Hamzah, Nur Zatul Akmar
2015-05-15
Let (X,F) be a measurable space, and S(X,F) be the set of all probability measures on (X,F) where X is a state space and F is σ - algebraon X. We consider a nonlinear transformation (quadratic stochastic operator) defined by (Vλ)(A) = ∫{sub X}∫{sub X}P(x,y,A)dλ(x)dλ(y), where P(x, y, A) is regarded as a function of two variables x and y with fixed A ∈ F . A quadratic stochastic operator V is called a regular, if for any initial measure the strong limit lim{sub n→∞} V{sup n }(λ) is exists. In this paper, we construct a family of quadratic stochastic operators defined on themore » segment X = [0,1] with Borel σ - algebra F on X , prove their regularity and show that the limit measure is a Dirac measure.« less
Suzaku Detection of Diffuse Hard X-Ray Emission Outside Vela X
NASA Technical Reports Server (NTRS)
Katsuda, Satoru; Mori, Koji; Petre, Robert; Yamaguchi, Hiroya; Tsunemi, Hiroshi; Bocchino, Fabrizio; Bamba, Aya; Miceli, Marco; Hewitt, John W.; Temim, Tea;
2011-01-01
Vela X is a large, 3 deg x 2 deg, radio-emitting pulsar wind nebula (PWN) powered by the Vela pulsar in the Vela supernova remnant. Using four Suzaku/XIS observations pointed just outside Vela X, we find hard X-ray emission extending throughout the fields of view. The hard X-ray spectra are well represented by a power-law. The photon index is measured to be constant at Gamma approximates 2.4, similar to that of the southern outer part of Vela X. The power-law flux decreases with increasing distance from the pulsar. These properties lead us to propose that the hard X-ray emission is associated with the Vela PWN. The larger X-ray extension found in this work strongly suggests that distinct populations relativistic electrons form the X-ray PWN and Vela X, as was recently inferred from multiwavelength spectral modeling of Vela X.
Software Process Modeling and Execution within Virtual Environments
1997-08-01
LhFEX@nOHX@nOe+L X@L X[Lhq³AKe.?HWLvJ&%HV,=>brP"sK\\QehJQFK\\QH�X@nOehJQuUJQehJQHWLe.=�RaHnX>V.VhJQHWY�=@seR³ qwe .?H"L.X>PH?³sP[X>ApX>SUHA...HWLhe.HWYðR³ qwe .?H"YKHWL.nOVhJQFehJQ=@Aº=>bX>VoehJcb X@nOeOLiX>RE=>u@H@IÛe.?H?KsP�X>AºX>S@HAKe+LJQAºe.?HFV.=nOHWL.LX>V.HV.HFV.H� LhH...EX@LiLhsReOX@LhGLCr�’?H ÊUÇ�ÅÄWÀEÕUÄ+Õ,Lhe+Xke.HYUJMY A=@e,nO=@V.V.HWLlFE=@AEY�e.=�XkA³ qwe +XULhGÙIX>AEY�Lh=JQe,giX@L’VoHP=>u@HWYC
Deconvolution by Homomorphic and Wiener Filtering
1988-09-01
XR?(e-j) =XR(e. 7w), XJ(e-jw) -Xei) and 4 ej) -Re’) ,ej)X~i) d+ ar g [X(e l a)[ ( Assumnption: both X(z) and X(z) are analytic in a region included the...consistent if 3k(wi+,) E IJ" g (X(ej"’+’)/wiJ - Arg[X(ej’")] + 2irk(wi+t ) < THLDI < r. The idea of the algorithm is to adapt the step size Aw imtil the phase...given by arg X(ejw) = S(eJw) dw, or, according to [141 ’ G " g [X(e-’÷.’)/T ,= argX(ejw) + LAW d argX(e(’+ )+ dargX(ei’) 1T2 where d-S(e’) = argX(e3d
Zefa, Edison; Redü, Darlan Rutz; Da Costa, Maria Kátia Matiotti; Fontanetti, Carmem S; Gottschalk, Marco Silva; Padilha, Giovanna Boff; Fernandes e Silva, Anelise; Martins, Luciano De P
2014-08-06
In this paper we describe a new species of Luzarinae cricket collected from the cave "Gruta de Ubajara, municipality of Ubajara, State of Ceará, Brazil, highlighting phallic sclerites morphology and chromosome complement as diagnostic characters. We presented meiotic and mitotic characterization in order to define the karyotype with 2n = 12 + X1X2♂/12 + X1X1X2X2♀. This represents the first record of X1X20 chromosomal sex system in Gryllidae.
UGent Participation in the Microblog Track 2012
2012-11-01
original one. A counter example is the query “ Steve Jobs ’ health” in topic 106. For this query, user wants to know about the health situation of Steve ...5x), “destroyer” (2x), “creator” (3x), “composed” (2x), and “products” (2x). These terms can be formed another query like: “ Steve Jobs is... Jobs ’. However, the returned title terms of top 30 tweets for this query are “steve” (7x), “jobs” (7x), “is” (2x), “of” (3x), “health” (1x), “apple
Archaeological Investigations at Sites 45-OK-250 and 45-OK-4, Chief Joseph Dam Project, Washington.
1984-01-01
level behind Chief Joseph Dam. Systematic random sampling using I x I x ’ - 0.1-m collection units in 1 x 1, 1 x 2, or 2 x 2 m cel Is disclosed...ft to the operating pool . level behind Chief Joseph Dam. Systematic random sampling using 1 x 1 x 0.1-i collection units In 1 x 1, 1 x 2, or 2 x 2 m...contingencies under which data were collected , describe data collection and analysis, and organize and summarize data In a torm useful to the widest
Compliance of 2012/13 Combat Ration Packs to the Recommended Nutritional Criteria
2014-08-01
mixes, instant noodle flavouring and processed cheese. Figure 26 Sodium content of 2012/13 CRP vs RNC. The red line indicates the UL and the black...various 1 x 50g Cereal Bar various 2 x 50g Cereal Bar various 1 x 50g Cereal Bar various 2 x 50g Muesli, Fruitful with Skim Milk 1 x 100g Noodles , Instant ...Candy 1 x 50g Noodles , Instant , Beef Flavour 1 x 40g Werther’s® Cream Candy 1 x 50g Lifesavers® Candy 1 x 34g Lifesavers® Candy 1 x 34g
Summary of Structural Evaluation and Design Support for the Underground Nuclear Test Program.
1979-07-01
consider using API -5LX pipe as this pipe has been shown to have high ductility (better than A36). This pipe comes in several grades (X42, X46, X52 , X56, X60...X65, X70) with the grade number representing the yield strength (ksi) of the steel. Grades X42 and X52 are readily available while the higher yield...strength steels are less readily available. I believe X52 has certainly a high enough yield strength (52,000 psi) for your application and that even
NASA Astrophysics Data System (ADS)
Li, Y. Q.; Hirosaki, N.; Xie, R. J.; Takeda, T.; Mitomo, M.
2008-12-01
The crystal structure, electronic structure, and photoluminescence properties of Eu xSi 6-zAl z-xO z+xN 8-z-x ( x=0-0.1, 0< z<1) and Eu xM ySi 6-zAl z-x-yO z+x+yN 8-z-x-y ( M=2Li, Mg, Ca, Sr, Ba) have been studied. Single-phase Eu xSi 6-zAl z-xO z+xN 8-z-x can be obtained in very narrow ranges of x⩽0.06 ( z=0.15) and z<0.5 ( x=0.3), indicating that limited Eu 2+ ions can be incorporated into nitrogen-rich Si 6-zAl zO zN 8-z. The Eu 2+ ion is found to occupy the 2 b site in a hexagonal unit cell ( P6 3/ m) and directly connected by six adjacent nitrogen/oxygen atoms ranging 2.4850-2.5089 Å. The calculated host band gaps by the relativistic DV-X α method are about 5.55 and 5.45 eV (without Eu 2+ 4 f5 d levels) for x=0 and 0.013 in Eu xSi 6-zAl z-xO z+xN 8-z-x ( z=0.15), in which the top of the 5 d orbitals overlap with the Si-3 s3 p and N-2 p orbitals within the bottom of the conduction band of the host. Eu xSi 6-zAl z-xO z+xN 8-z-x shows a strong green emission with a broad Eu 2+ band centered at about 530 nm under UV to near-UV excitation range. The excitation and emission spectra are hardly modified by Eu concentration and dual-doping ions of Li and other alkaline-earth ions with Eu. Higher Eu concentrations can significantly quench the luminescence of Eu 2+ and decrease the thermal quenching temperature. In addition, the emission spectrum can only be slightly tuned to the longer wavelengths (˜529-545 nm) by increasing z within the solid solution range of z<0.5. Furthermore, the luminescence intensity of Eu xSi 6-zAl z-xO z+xN 8-z-x can be improved by increasing z and the dual-doping of Li and Ba.
X-15 Hardware Design Challenges
NASA Technical Reports Server (NTRS)
Storms, Harrison A., Jr.
1991-01-01
Historical events in the development of the X-15 hardware design are presented. Some of the topics covered include: (1) drivers that led to the development of the X-15; (2) X-15 space research objectives; (3) original performance targets; (4) the X-15 typical mission; (5) X-15 dimensions and weight; (5) the propulsion system; (6) X-15 development milestones; (7) engineering and manufacturing challenges; (8) the X-15 structure; (9) ballistic flight control; (10) landing gear; (11) nose gear; and (12) an X-15 program recap.
2002-01-01
Oedogoniales Oedogoniaceae Bulbochaete sp. X Oedogonium sp. X X X Ulvophyceae Cladophorales Cladophoraceae Cladophora sp. X X X Cladophora glomerata X X...280,000 270,000 72,000 75,000 Oedogoniales Oedogoniaceae Oedogonium sp. 190,000 Ulvophyceae Cladophorales Cladophoraceae Cladophora sp. 20,000 Table 3...lubricum 600,000 850,000 660,000 Ulvophyceae Cladophorales Cladophoraceae Cladophora sp. 16,000 Charophyceae Zygnemateles Desmidiaceae Closterium
... News Physician Resources Professions Site Index A-Z X-ray (Radiography) - Abdomen Abdominal x-ray uses a ... of an abdominal x-ray? What is abdominal x-ray? An x-ray (radiograph) is a noninvasive ...
2010-09-30
abundant taxa (copepods and larvaceans), whereas the pump collected more rare taxa (cladocerans and siphonophores ). These differences could be due...4.2x 14848 6.8x Cladocerans 199 0.3x 195 0.88x Larvaceans 3016 1.3x 4102 3.5x Siphonophores 85 0.2x 215 0.14x
NASA Technical Reports Server (NTRS)
1976-01-01
Satellite X-ray experiments and ground-based programs aimed at observation of X-ray binaries are discussed. Experiments aboard OAO-3, OSO-8, Ariel 5, Uhuru, and Skylab are included along with rocket and ground-based observations. Major topics covered are: Her X-1, Cyg X-3, Cen X-3, Cyg X-1, the transient source A0620-00, other possible X-ray binaries, and plans and prospects for future observational programs.
Angus, Robert B.; Jeangirard, Constance; Stoianova, Desislava; Grozeva, Snejana; Kuznetsova, Valentina G.
2017-01-01
Abstract An account is given of the karyotypes and male meiosis of the Water Scorpion Nepa cinerea Linnaeus, 1758 and the Water Stick Insect Ranatra linearis (Linnaeus, 1758) (Heteroptera, Nepomorpha, Nepidae). A number of different approaches and techniques were tried: the employment of both male and female gonads and mid-guts as the sources of chromosomes, squash and air-drying methods for chromosome preparations, C-banding and fluorescence in situ hybridization (FISH) for chromosome study. We found that N. cinerea had a karyotype comprising 14 pairs of autosomes and a multiple sex chromosome system, which is X1X2X3X4Y (♂) / X1X1X2X2X3X3X4X4 (♀), whereas R. linearis had a karyotype comprising 19 pairs of autosomes and a multiple sex chromosome system X1X2X3X4Y (♂) / X1X1X2X2X3X3X4X4 (♀). In both N. cinerea and R. linearis, the autosomes formed chiasmate bivalents in spermatogenesis, and the sex chromosome univalents divided during the first meiotic division and segregated during the second one suggesting thus a post-reductional type of behaviour. These results confirm and amplify those of Steopoe (1925, 1927, 1931, 1932) but are inconsistent with those of other researchers. C-banding appeared helpful in pairing up the autosomes for karyotype assembly; however in R. linearis the chromosomes were much more uniform in size and general appearance than in N. cinerea. FISH for 18S ribosomal DNA (major rDNA) revealed hybridization signals on two of the five sex chromosomes in N. cinerea. In R. linearis, rDNA location was less obvious than in N. cinerea; however it is suggested to be similar. We have detected the presence of the canonical “insect” (TTAGG)n telomeric repeat in chromosomes of these species. This is the first application of C-banding and FISH in the family Nepidae. PMID:29114353
Dependence of purinergic P2X receptor activity on ectodomain structure.
He, Mu-Lan; Zemkova, Hana; Stojilkovic, Stanko S
2003-03-21
Purinergic receptors (P2XRs) activate and desensitize in response to the binding of extracellular nucleotides in a receptor- and ligand-specific manner, but the structural bases of their ligand preferences and channel kinetics have been incompletely characterized. Here we tested the hypothesis that affinity of agonists for binding domain accounts for a ligand-specific desensitization pattern. We generated chimeras using receptors with variable sensitivity to ATP in order: P2X(4)R > P2X(2a)R = P2X(2b)R P2X(7)R. Chimeras having the ectodomain Ile(66)-Tyr(310) sequence of P2X(2)R and Val(61)-Phe(313) sequence of P2X(7)R in the backbone of P2X(4)R were expressed but were non-functioning channels. P2X(2a) + X(4)R and P2X(2b) + X(4)R chimeras having the Val(66)-Tyr(315) ectodomain sequence of P2X(4)R in the backbones of P2X(2a)R and P2X(2b)R were functional and exhibited increased sensitivity to ligands as compared with both parental receptors. These chimeras also desensitized faster than parental receptors and in a ligand-nonspecific manner. However, like parental P2X(2b)R and P2X(2a)R, chimeric P2X(2b) + X(4)R desensitized more rapidly than P2X(2a) + X(4)R, and the rate of desensitization of P2X(2a)+X(4)R increased by substituting its Arg(371)-Pro(376) intracellular C-terminal sequence with the Glu(376)-Gly(381) sequence of P2X(4)R. These results indicate the relevance of interaction between the ectodomain and flanking regions around the transmembrane domains on ligand potency and receptor activation. Furthermore, the ligand potency positively correlates with the rate of receptor desensitization but does not affect the C-terminal-specific pattern of desensitization.
Analysis of Factors Affecting the Success of Onions Development Program in Kampar Regency
NASA Astrophysics Data System (ADS)
Amalia; Putri, Asgami
2017-12-01
The purpose of this study is to analyze the factors influencing the success of the onion plant development program in Kampar regency. The research method used was the applied survey method using interview technique and observation or direct supervision on the location of the object. The briefing of the interviews as well as the accuracy of collecting the required data was guided by the structured questionnaires. Determination technique of location / region sampling was done purposively based on the potency and capacity of commodity development. While the respondents were taken by cluster purvosive sampling method in order to classify the samples in accordance with the purpose of the study, determined by as many as 100 people taken from members of the farmer group. Analytical technique used is by using Logic Regression Analysis to determine the factors that influence the success of the program seen from the characteristics of farmers. From the results of this study it can be concluded that the factors influencing the success of onion development program in Kampar regency were a age (X1), education (X2), income (X3), ethnicity (X4), jobs (X5) And family responsibility (X6) could be made as follows: Log Y (P/1-p) = -1.778 +X10.021 + X20.028 - X30.213 + X41.986 + X52.930 - X60.455 From the above equation, it can be explained that the attributes that are positively related are X1 (age), X2 (education), X4 (ethnicity) and X5 (jobs) while the negative correlates are X3 (income) and X6 (family responsibility). From the logical regression result it can be seen that the significant value <0,05, then the independent variable influenced the dependent variable, so that when viewed from the table in the equation it was found that factors affecting the success rate of red onion development program in Kampar regency were X2 (education), X4 (ethnicity), X5 (jobs), and X6 (family responsibility).
46 CFR 13.121 - Courses for tankerman endorsements.
Code of Federal Regulations, 2013 CFR
2013-10-01
... (open and closed). (vii) Rules of the Coast Guard governing operations in general and prevention of..., carbon dioxide (CO2), foam... X Halogenated hydrocarbons X Pressure-water spray system in special..., spray, fog, and flooding) X Foam (high, medium and low expansion) X Carbon dioxide (CO2) X X Halon X...
46 CFR 13.121 - Courses for tankerman endorsements.
Code of Federal Regulations, 2011 CFR
2011-10-01
... (open and closed). (vii) Rules of the Coast Guard governing operations in general and prevention of..., carbon dioxide (CO2), foam... X Halogenated hydrocarbons X Pressure-water spray system in special..., spray, fog, and flooding) X Foam (high, medium and low expansion) X Carbon dioxide (CO2) X X Halon X...
46 CFR 13.121 - Courses for tankerman endorsements.
Code of Federal Regulations, 2012 CFR
2012-10-01
... (open and closed). (vii) Rules of the Coast Guard governing operations in general and prevention of..., carbon dioxide (CO2), foam... X Halogenated hydrocarbons X Pressure-water spray system in special..., spray, fog, and flooding) X Foam (high, medium and low expansion) X Carbon dioxide (CO2) X X Halon X...
Elliptic Curve Integral Points on y2 = x3 + 3x ‑ 14
NASA Astrophysics Data System (ADS)
Zhao, Jianhong
2018-03-01
The positive integer points and integral points of elliptic curves are very important in the theory of number and arithmetic algebra, it has a wide range of applications in cryptography and other fields. There are some results of positive integer points of elliptic curve y 2 = x 3 + ax + b, a, b ∈ Z In 1987, D. Zagier submit the question of the integer points on y 2 = x 3 ‑ 27x + 62, it count a great deal to the study of the arithmetic properties of elliptic curves. In 2009, Zhu H L and Chen J H solved the problem of the integer points on y 2 = x 3 ‑ 27x + 62 by using algebraic number theory and P-adic analysis method. In 2010, By using the elementary method, Wu H M obtain all the integral points of elliptic curves y 2 = x 3 ‑ 27x ‑ 62. In 2015, Li Y Z and Cui B J solved the problem of the integer points on y 2 = x 3 ‑ 21x ‑ 90 By using the elementary method. In 2016, Guo J solved the problem of the integer points on y 2 = x 3 + 27x + 62 by using the elementary method. In 2017, Guo J proved that y 2 = x 3 ‑ 21x + 90 has no integer points by using the elementary method. Up to now, there is no relevant conclusions on the integral points of elliptic curves y 2 = x 3 + 3x ‑ 14, which is the subject of this paper. By using congruence and Legendre Symbol, it can be proved that elliptic curve y 2 = x 3 + 3x ‑ 14 has only one integer point: (x, y) = (2, 0).
2010-01-01
Background X chromosome inactivation is a spectacular example of epigenetic silencing. In order to deduce how this complex system evolved, we examined X inactivation in a model marsupial, the tammar wallaby (Macropus eugenii). In marsupials, X inactivation is known to be paternal, incomplete and tissue-specific, and occurs in the absence of an XIST orthologue. Results We examined expression of X-borne genes using quantitative PCR, revealing a range of dosage compensation for different loci. To assess the frequency of 1X- or 2X-active fibroblasts, we investigated expression of 32 X-borne genes at the cellular level using RNA-FISH. In female fibroblasts, two-color RNA-FISH showed that genes were coordinately expressed from the same X (active X) in nuclei in which both loci were inactivated. However, loci on the other X escape inactivation independently, with each locus showing a characteristic frequency of 1X-active and 2X-active nuclei, equivalent to stochastic escape. We constructed an activity map of the tammar wallaby inactive X chromosome, which identified no relationship between gene location and extent of inactivation, nor any correlation with the presence or absence of a Y-borne paralog. Conclusions In the tammar wallaby, one X (presumed to be maternal) is expressed in all cells, but genes on the other (paternal) X escape inactivation independently and at characteristic frequencies. The paternal and incomplete X chromosome inactivation in marsupials, with stochastic escape, appears to be quite distinct from the X chromosome inactivation process in eutherians. We find no evidence for a polar spread of inactivation from an X inactivation center. PMID:21182760
Negative hyperconjugation and red-, blue- or zero-shift in X-Z∙∙∙Y complexes.
Joy, Jyothish; Jemmis, Eluvathingal D; Vidya, Kaipanchery
2015-01-01
A generalized explanation is provided for the existence of the red- and blue-shifting nature of X-Z bonds (Z=H, halogens, chalcogens, pnicogens, etc.) in X-Z∙∙∙Y complexes based on computational studies on a selected set of weakly bonded complexes and analysis of existing literature data. The additional electrons and orbitals available on Z in comparison to H make for dramatic differences between the H-bond and the rest of the Z-bonds. The nature of the X-group and its influence on the X-Z bond length in the parent X-Z molecule largely controls the change in the X-Z bond length on X-Z∙∙∙Y bond formation; the Y-group usually influences only the magnitude of the effects controlled by X. The major factors which control the X-Z bond length change are: (a) negative hyperconjugative donation of electron density from X-group to X-Z σ* antibonding molecular orbital (ABMO) in the parent X-Z, (b) induced negative hyperconjugation from the lone pair of electrons on Z to the antibonding orbitals of the X-group, and (c) charge transfer (CT) from the Y-group to the X-Z σ* orbital. The exchange repulsion from the Y-group that shifts partial electron density at the X-Z σ* ABMO back to X leads to blue-shifting and the CT from the Y-group to the σ* ABMO of X-Z leads to red-shifting. The balance between these two opposing forces decides red-, zero- or blue-shifting. A continuum of behaviour of X-Z bond length variation is inevitable in X-Z∙∙∙Y complexes.
Trunk extensor and flexor strength of long-distance race car drivers and physically active controls.
Baur, Heiner; Muller, Steffen; Pilz, Frederike; Mayer, Patrizia; Mayer, Frank
2010-09-01
Seventy percent of motor sports athletes report low back pain. Information on the physical capacity of race car drivers is limited. The purpose of this study was to compare the maximum trunk extensor and flexor strength of elite race car drivers and physically active controls. Thirteen elite race car drivers and 13 controls were measured in concentric mode for maximal trunk flexion and extension at 60° x s(-1) and 120° x s(-1). Peak torque (mean ± s) at 60° x s(-1) in trunk extension was 283 ± 80 N x m in the drivers and 260 ± 88 N x m in controls (P > 0.05). At 120° x s(-1), drivers produced peak torques of 248 ± 55 N x m compared with 237 ± 74 N x m for controls (P > 0.05). Peak torques in flexion were less than in extension for both groups (60° x s(-1): drivers 181 ± 56 N x m, controls 212 ± 54 N x m, P > 0.05; 120° x s(-1): drivers 191 ± 57 N x m, controls 207 ± 48 N x m, P > 0.05). Individual ratios of flexion to extension forces exhibited ratios of 0.88 (60° x s(-1)) and 0.93 (120° x s(-1)) for controls and 0.66 (60° x s(-1)) and 0.77 (120° x s(-1)) for drivers (60° x s(-1): P > 0.05; 120° x s(-1): P > 0.05). The maximum strength performance capacity of the trunk muscles of elite motor sport athletes competing in long-distance racing did not differ from that of anthropometrically matched and physically active controls.
NASA Astrophysics Data System (ADS)
Martinez-Miranda, Luz J.; Branch, Janelle; Thompson, Robert; Taylor, Jefferson W.; Salamanca-Riba, Lourdes
2012-02-01
We investigate the role order plays in the transfer of charges in ZnO nanoparticle - octylcyanobiphenyl (8CB) liquid crystal system for photovoltaic applications as well as the role the nominally 7x5x5nm^3 or 20x5x5nm^3 ZnO nanoparticles play in improving that order. Our results for the 5nm nanoparticles show an improvement in the alignment of the liquid crystal with increasing weight percentage of ZnO nanoparticles^1. Our results for the 7x5x5 nm^3 sample show that the current is larger than the current obtained for the 5 nm samples. We find that order is improved for concentrations close to 35% wt ZnO for both the 7x5x5 nm^3 and 20x5x5 nm^3. We have analyzed the X-ray scans for both the 7x5x5 and the 20x5x5 nm^3 samples. The signal corresponding to the liquid crystal aligned parallel to the substrate is much smaller than the peak corresponding to the liquid crystal aligned approximately at 70 with respect to the substrate for the 7x5x5 nm^3 sample whereas this same peak is comparable or more intense for the 20x5x5 nm^3 sample. 1. L. J. Mart'inez-Miranda, Kaitlin M. Traister, Iriselies Mel'endez-Rodr'iguez, and Lourdes Salamanca-Riba, Appl. Phys. Letts, 97, 223301 (2010).
Panescu, Dorin; Nerheim, Max; Kroll, Mark
2013-01-01
TASER(®) conducted electrical weapons (CEW) deliver electrical pulses that can inhibit a person's neuromuscular control or temporarily incapacitate. TASER X26, X26P, and X2 are among CEW models most frequently deployed by law enforcement agencies. The X2 CEW uses two cartridge bays while the X26 and X26P CEWs have only one. The TASER X26P CEW electronic output circuit design is equivalent to that of any one of the two TASER X2 outputs. The goal of this paper was to analyze the nominal electrical outputs of TASER X26, X26P, and X2 CEWs in reference to provisions of several international standards that specify safety requirements for electrical medical devices and electrical fences. Although these standards do not specifically mention CEWs, they are the closest electrical safety standards and hence give very relevant guidance. The outputs of two TASER X26 and two TASER X2 CEWs were measured and confirmed against manufacturer and other published specifications. The TASER X26, X26P, and X2 CEWs electrical output parameters were reviewed against relevant safety requirements of UL 69, IEC 60335-2-76 Ed 2.1, IEC 60479-1, IEC 60479-2, AS/NZS 60479.1, AS/NZS 60479.2 and IEC 60601-1. Prior reports on similar topics were reviewed as well. Our measurements and analyses confirmed that the nominal electrical outputs of TASER X26, X26P and X2 CEWs lie within safety bounds specified by relevant requirements of the above standards.
A Trial of Metformin in Individuals With Fragile X Syndrome
2018-06-05
Fragile X Syndrome; Fragile X Mental Retardation Syndrome; Mental Retardation, X Linked; Genetic Diseases, X-Linked; Trinucleotide Repeat Expansion; Fra(X) Syndrome; Intellectual Disability; FXS; Neurobehavioral Manifestations; Sex Chromosome Disorders
Time-Resolved Photoluminescence Studies of Si-doped AlGaN alloys
NASA Astrophysics Data System (ADS)
Nam, K. B.; Li, J.; Nakarmi, M. L.; Lin, J. Y.; Jiang, H. X.
2002-03-01
Si-doped n-type Al x Ga_1-x N alloys with x between 0.3 and 0.5 were grown by metal-organic chemical vapor deposition (MOCVD) on sapphire substrates. Time-resolved photoluminescence (PL) emission spectroscopy and variable temperature Hall-effect measurements were employed to study the optical and electrical properties of these epilayers. Our electrical data revealed that the conductivity of Si-doped Al x Ga_1-x N alloys (x > 0.4) increases with an increase of the Si doping concentration (N_Si) for a fixed x value and exhibits a sharp increase around N_Si= 1x10 ^18cm-3, suggesting the existence of a critical Si doping concentration needed to convert insulating Al x Ga_1-x N alloys (x > 0.4) to n-type conductivity. Time-resolved PL studies also showed that PL decay lifetime and activation energy decrease sharply when Si-doping concentration increases from N_Si= 0 to 1x10 ^18cm-3and then followed by gradual decreases as N_Si further increases. Our results thus suggest that Si-doping reduces the effect of carrier localization in Al x Ga_1-x N alloys and a sharp drop in carrier localization energy occurs at N_Si= 1x10 ^18cm-3, which is the critical Si-doping concentration needed to fill up the localized states in Al x Ga_1-x N alloys (x > 0.4). The implications of these results to UV optoelectronic devices are also discussed.
NASA Astrophysics Data System (ADS)
Arouca, R.; Silva Neto, M. B.; Chaves, C. M.; Nagao, M.; Watauchi, S.; Tanaka, I.; ElMassalami, M.
2017-09-01
Layered BiS 2 -based series, such as LaO 1-x F x BiS 2 and Sr 1-x La x FBiS 2 , offer ideal examples for studying normal and superconducting phase diagram of a solid solution that evolves from a nonmagnetic band-insulator parent. We constructed typical x-T phase diagrams of these systems based on events occurring in thermal evolution of their electrical resistivity, ρ(x, T) . Overall evolution of these diagrams can be rationalized in terms of (i) Mott-Efros-Shklovskii scenario which, within the semiconducting x regime (x_MIT = Mott metal-insulator transition), describes the doping influence on the thermally activated hopping conductivity. (ii) A granular metal (superconductor) scenario which, within x_MIT< x < x_solubility , describes the evolution of normal and superconducting properties in terms of conductance g, Coulomb charging energy E c and Josephson coupling J; their joint influence is usually captured within a g-\\frac{gE_c}{J}-T phase diagram. Based on analysis of the granular character of ρ(x, T) , we converted the x-T diagrams into projected g - T diagrams which, being fundamental, allow a better understanding of evolution of various granular-related properties (in particular the hallmarks of normal-state \\partialρ/\\partial T<0 feature and superconductor-insulator transition) and how such properties are influenced by x, pressure or heat treatment.
Xue, Dong; Myles, Charles W; Higgins, Craig
2016-08-11
Type II clathrates are interesting due to their potential thermoelectric applications. Powdered X-ray diffraction (XRD) data and density functional calculations for Na x Si 136 found a lattice contraction as x increases for 0 < x < 8 and an expansion as x increases for x > 8. This is explained by XRD data that shows that as x increases, the Si 28 cages are filled first for x < 8 and the Si 20 cages are then filled for x > 8. Motivated by this work, here we report the results of first-principles calculations of the structural and vibrational properties of the Type II clathrate compounds A x Si 136 , A x Ge 136 , and A x Sn 136 . We present results for the variation of the lattice constants, bulk moduli, and other structural parameters with x. These are contrasted for the Si, Ge, and Sn compounds and for guests A = Na, K, Rb, and Cs. We also present calculated results of phonon dispersion relations for Na₄Si 136 , Na₄Ge 136 , and Na₄Sn 136 and we compare these for the three materials. Finally, we present calculated results for the elastic constants in Na x Si 136 , Na x Ge 136 , and Na x Sn 136 for x = 4 and 8. These are compared for the three hosts, as well as for the two compositions.
X-ray Reciprocal Space Mapping of Graded Al x Ga1 - x N Films and Nanowires.
Stanchu, Hryhorii V; Kuchuk, Andrian V; Kladko, Vasyl P; Ware, Morgan E; Mazur, Yuriy I; Zytkiewicz, Zbigniew R; Belyaev, Alexander E; Salamo, Gregory J
2016-12-01
The depth distribution of strain and composition in graded Al x Ga1 - x N films and nanowires (NWs) are studied theoretically using the kinematical theory of X-ray diffraction. By calculating [Formula: see text] reciprocal space maps (RSMs), we demonstrate significant differences in the intensity distributions from graded Al x Ga1 - x N films and NWs. We attribute these differences to relaxation of the substrate-induced strain on the NWs free side walls. Finally, we demonstrate that the developed X-ray reciprocal space map model allows for reliable depth profiles of strain and Al composition determination in both Al x Ga1 - x N films and NWs.
Modular Multi-Sensor Display System Design Study. Volume 1. Requirements Analysis and Design Studies
1974-08-01
1 0.00001 0.00001 0.00003 Residual 1x2x3 1 0.01002 0.01002 0.0348 Total 11 0.28822 Gray Shade Quantization. The main effect of gray shade...Quantization 3 Tararets 1 x 2 1 x 3 Z x i 1x2x3 RppTiratjnns Totals Degrees Freedom 1 2 5 10 10 3j6 71 Sum Squares 0.6463 0.5985 1.2009...x 3 2x3 1x2x3 Replications Totals DF 1 2 5 2 5 10 10 36 71 5S 1708.8 1413.2 2355.5 39.6 1342.2 1563.9 1568.8 2583.8 12576.1
Recent observations with phase-contrast x-ray computed tomography
NASA Astrophysics Data System (ADS)
Momose, Atsushi; Takeda, Tohoru; Itai, Yuji; Tu, Jinhong; Hirano, Keiichi
1999-09-01
Recent development in phase-contrast X-ray computed tomography using an X-ray interferometer is reported. To observe larger samples than is possible with our previous X-ray interferometer, a large monolithic X-ray interferometer and a separated-type X-ray interferometer were studied. At the present time, 2.5 cm X 1.5 cm interference patterns have been generated with the X-ray interferometers using synchrotron X-rays. The large monolithic X-ray interferometer has produced interference fringes with 80% visibility, and has been used to measure various tissues. To produce images with higher spatial resolution, we fabricated another X-ray interferometer whose wafer was partially thinned by chemical etching. A preliminary test suggested that the spatial resolution has been improved.
Automated Continuous Commissioning of Commercial Buildings
2011-09-01
matched pair of supply and return chilled water temperature sensors, a pyranometer , and aspirated wet and dry bulb temperature sensors for the weather...temp X Aspirated weather station is required. Outside air wet bulb X Pyranometer X Wind speed & direction X Main power meter X Lighting load power X...Aspirated weather station is required. Outside air wet bulb X Pyranometer X Provides measurements on global horizontal solar radiation, beam radiation and
The energy gap in a-Si 1 - xC g: H alloys
NASA Astrophysics Data System (ADS)
Valladares, Ariel A.; Valladares, Alexander; Enrique Sansores, L.; Nelis, Mary Ann Me
1997-02-01
The electronic structure of amorphous tetrahedral clusters of the type a-Si 1 - xC g: H are studied using the pseudopotential SCF Hartree-Fock approximation. The reduced energy gap isgiven by Egr( x) - 1 + 0.84 x for x ⩽ 0.5, whereas experimentally Egr( x) = 1 + 0.96 x. For x ⩾ 0.5 the dip in the gap value reported experimentally is verified.
40 CFR Table 1 to Subpart X of... - General Provisions Applicability to Subpart X
Code of Federal Regulations, 2013 CFR
2013-07-01
... Subpart X 1 Table 1 to Subpart X of Part 63 Protection of Environment ENVIRONMENTAL PROTECTION AGENCY..., Subpt. X, Table 1 Table 1 to Subpart X of Part 63—General Provisions Applicability to Subpart X Reference Applies to subpart X Comment 63.1 Yes. 63.2 Yes. 63.3 Yes. 63.4 Yes. 63.5 Yes. 63.6(a), (b), (c...
Federal Register 2010, 2011, 2012, 2013, 2014
2011-03-25
... (NO X ) and Sulfur Oxides (SO X ) Secondary Review Panel (NO X -SO X Panel) and the CASAC Air..., including Oxides of Nitrogen and Oxides of Sulfur. As noticed in 76 FR 4109-4110, the NO X -SO X Panel held...). On May 12, 2011, CASAC will review the draft report of the NO X -SO X Panel that provides advice on...
40 CFR Table 1 to Subpart X of... - General Provisions Applicability to Subpart X
Code of Federal Regulations, 2014 CFR
2014-07-01
... Subpart X 1 Table 1 to Subpart X of Part 63 Protection of Environment ENVIRONMENTAL PROTECTION AGENCY..., Subpt. X, Table 1 Table 1 to Subpart X of Part 63—General Provisions Applicability to Subpart X Reference Applies to subpart X Comment 63.1 Yes. 63.2 Yes. 63.3 Yes. 63.4 Yes. 63.5 Yes. 63.6(a), (b), (c...
40 CFR Table 1 to Subpart X of... - General Provisions Applicability to Subpart X
Code of Federal Regulations, 2012 CFR
2012-07-01
... Subpart X 1 Table 1 to Subpart X of Part 63 Protection of Environment ENVIRONMENTAL PROTECTION AGENCY..., Subpt. X, Table 1 Table 1 to Subpart X of Part 63—General Provisions Applicability to Subpart X Reference Applies to subpart X Comment 63.1 Yes. 63.2 Yes. 63.3 Yes. 63.4 Yes. 63.5 Yes. 63.6(a), (b), (c...
NASA Astrophysics Data System (ADS)
Xie, Xi-Yang; Tian, Bo; Liu, Lei; Guan, Yue-Yang; Jiang, Yan
2017-06-01
In this paper, we investigate a generalized nonautonomous nonlinear equation, which describes the ultrashort optical pulse propagating in a nonlinear inhomogeneous fiber. Under certain integrable constraints, bilinear forms, bright one- and two-soliton solutions are obtained. Via certain transformation, we investigate the properties of the solitons with the first-order dispersion parameter σ1(x, t), second-order dispersion parameter σ2(x, t), third-order dispersion parameter σ3(x, t), phase modulation and gain (loss) v(x, t). Soliton propagation and collision are graphically presented and analyzed: One soliton is shown to maintain its amplitude and width during the propagation. When we choose σ1(x, t), σ2(x, t) and σ3(x, t) differently, travelling direction of the soliton is found to alter. v(x, t) is observed to affect the amplitude of the soliton. Head-on collision between the two solitons is presented with σ1(x, t), σ2(x, t), σ3(x, t) and v(x, t) as the constants, and solitons' amplitudes are the same before and after the collision. When σ1(x, t), σ2(x, t) and σ3(x, t) are chosen as certain functions, the solitons' traveling directions change during the collision. v(x, t) can influence the amplitudes of the two solitons.
Williams, Robert K.; Paranthaman, Mariappan; Chirayil, Thomas G.; Lee, Dominic F.; Goyal, Amit; Feenstra, Roeland
2002-01-01
A laminate article comprises a substrate and a biaxially textured (RE.sub.x A.sub.(1-x)).sub.2 O.sub.2-(x/2) buffer layer over the substrate, wherein 0
Rare earth zirconium oxide buffer layers on metal substrates
Williams, Robert K.; Paranthaman, Mariappan; Chirayil, Thomas G.; Lee, Dominic F.; Goyal, Amit; Feenstra, Roeland
2001-01-01
A laminate article comprises a substrate and a biaxially textured (RE.sub.x A.sub.(1-x)).sub.2 O.sub.2-(x/2) buffer layer over the substrate, wherein 0
Tan, Chaoliang; Zhao, Wei; Chaturvedi, Apoorva; ...
2016-02-24
The high-yield and scalable production of single-layer ternary transition metal dichalcogenide nanosheets with ≈66% of metallic 1T phase, including MoS 2xSe 2(1-x) and Mo xW 1-xS 2 is here achieved via electrochemical Li-intercalation and the exfoliation method. Thin film MoS 2xSe 2(1-x) nanosheets drop-cast on a fluorine-doped tin oxide substrate are used as an efficient electrocatalyst on the counter electrode for the tri-iodide reduction in a dye-sensitized solar cell.
Cone Quasi-Concave Multi-Objective Programming Theory and Dominance Cone Constructions.
1988-08-01
generalized cone concavity and nondominated solutions for later use in our development. We also derive some properties of generalized cone concavity. A set S...A-quasiconcave on S" if g(.x 1+(1-X)x 2)-Min{g(x0), g(x 2)) e IntA forallxl*x 2 E SandX e (0,1), where (in ( gi (x’), gi (x2)) Min [g (0i), g (x2 ) - 1...will lead to elimination of the points of J3 by using the dominance cone W3 . Associated with W3 , only the points of J1 and J2 are nondominated, and
1978-02-01
qw dt 6u 6V 6 d •Tf •Tf-rv + = -Brv - A’rw - C’ru - Mrq - Frr - F’rr - Hrp + H’rp 6 Tf q -1-= Cqw + A’qv + B’qu + Nqr + Fqq - F’qq + Gqp + G’qp...rr H 2 - Cqw - Aqv B’qu - Nqr - F2qq - 1lqP 1 -X L -X. F1 X F2 -G-X u rw qv p rr 2 qq B X B’ -X. =-X M = (Xq) G = -x G -- X.rv w qu.r 1 qp 2 r C=-X C
A mirror for lab-based quasi-monochromatic parallel x-rays
NASA Astrophysics Data System (ADS)
Nguyen, Thanhhai; Lu, Xun; Lee, Chang Jun; Jung, Jin-Ho; Jin, Gye-Hwan; Kim, Sung Youb; Jeon, Insu
2014-09-01
A multilayered parabolic mirror with six W/Al bilayers was designed and fabricated to generate monochromatic parallel x-rays using a lab-based x-ray source. Using this mirror, curved bright bands were obtained in x-ray images as reflected x-rays. The parallelism of the reflected x-rays was investigated using the shape of the bands. The intensity and monochromatic characteristics of the reflected x-rays were evaluated through measurements of the x-ray spectra in the band. High intensity, nearly monochromatic, and parallel x-rays, which can be used for high resolution x-ray microscopes and local radiation therapy systems, were obtained.
Hisatomi, Takashi; Maeda, Kazuhiko; Lu, Daling; Domen, Kazunari
2009-01-01
The influence of starting materials on the physicochemical and photocatalytic properties of (Ga(1-x)Zn(x))(N(1-x)O(x)) were investigated in an attempt to optimize the preparation conditions. The catalyst was successfully prepared by nitriding a starting mixture of ZnO and Ga2O3. A mixture of metallic zinc and GaN, however, did not afford the desired compound. The crystallinity, surface area, composition, and absorption characteristics of the resultant (Ga(1-x)Zn(x))(N(1-x)O(x)) solid solution are found to be dependent on the morphology of ZnO but largely insensitive to the choice of Ga2O3 polymorph. The use of coarser-grained ZnO results in a coarser-grained catalyst with elevated zinc and oxygen content and reduced uniformity in composition and crystallinity. The results demonstrate the importance of selecting appropriate ZnO and Ga2O3 starting materials for maximizing the photocatalytic activity of (Ga(1-x)Zn(x))(N(1-x)O(x)) for overall water splitting under visible light.
NASA Astrophysics Data System (ADS)
Li, Zhenhu; Ma, Yurong; Qi, Limin
2016-12-01
A strategy for the formation of magnetic Ni x Fe3-x O4 hollow nanospheres with very high specific surface areas was designed through a facile solvothermal method in mixed solvents of ethylene glycol and water in this work. The Ni/Fe ratios and the crystal phases of the Ni x Fe3-x O4 hollow nanocrystals can be readily tuned by changing the molar ratios of Ni to Fe in the precursors. An inside-out Ostwald ripening mechanism was proposed for the formation of uniform Ni x Fe3-x O4 hollow nanospheres. Moreover, the obtained Ni x Fe3-x O4 hollow nanospheres exhibited excellent adsorption capacity towards organic molecules such as Congo red in water. The maximum adsorption capacities of Ni x Fe3-x O4 hollow nanospheres for Congo red increase dramatically from 263 to 500 mg g-1 with the increase of the Ni contents (x) in Ni x Fe3-x O4 hollow nanospheres from 0.2 to 0.85. The synthesized Ni x Fe3-x O4 nanoparticles can be potentially applied for waste water treatment.
NASA Astrophysics Data System (ADS)
Xiaoge, Chen; Hongsong, Zhang; Sai, Su; Yongde, Zhao; An, Tang; Haoming, Zhang
2017-12-01
The (Yb1 - x La x )2AlTaO7 ( x = 0, 0.1, 0.3, 0.5) ceramics were prepared by solid-state reaction method. The phase composition, microstructure, thermophysical properties of (Yb1 - x La x )2AlTaO7 ceramics were investigated. Results reveal that (Yb1 - x La x )2AlTaO7 ( x = 0, 0.1, 0.3) ceramics exhibit a single pyrochlore-type structure, and the (Yb0.5La0.5)2AlTaO7 has an orthorhombic weberite structure. The thermal conductivities of (Yb1 - x La x )2AlTaO7 ( x = 0, 0.1, 0.3) ceramics decrease with increasing Yb2O3 contents. (Yb0.5La0.5)2AlTaO7 has the highest thermal conductivity among all the ceramics studied, within the range of 1.48-1.75 W/m K (20-1200 °C). The thermal expansion coefficients of (Yb1 - x La x )2AlTaO7 ceramics decrease gradually with increasing La2O3 fractions, and the thermal expansion coefficients are close to those of YSZ.
46 CFR 12.15-9 - Examination requirements.
Code of Federal Regulations, 2011 CFR
2011-10-01
... X X X 18. The procedure in preparing a turbine, reciprocating, or Diesel engine for standby; also... various types of generators and motors, both A.C. and D.C X X X 27. Operation, installation, and...
X-ray - lumbosacral spine; X-ray - lower spine ... The test is done in a hospital x-ray department or your health care provider's office by an x-ray technician. You will be asked to lie on the x-ray ...
Determination of Optimum Tropic Storage and Exposure Sites. Report 2. Empirical Data
1974-03-01
at the Fort Sherman site and the oldest at Gamboa. A taxonomic listing of trees, shrubs, vines and ground cover plants for each of these sites is...tibourbou X Avicennia nitida X Cordia alliodora X Cupania sylvatica X Hieronyma lax iflora X Laguncularia racemosa X Luehea seemanji X Ormosia
1980-12-22
fish in Nevada and Utah. COMMON NAME SCIENTIFIC NAME NEVADA UTAH SALMON, TROUT, GRAYLING & WHITEFISH Family SALMONIDAE King Salmon Oncorhynchus ...tsawytscha X Kokanee Red Salmon 0. nerka kennalyi I X X Lake Trout Salvelinus namayeush X Brook Trout S. fontinalis X Dolly Varden Trout S. malma X
Code of Federal Regulations, 2014 CFR
2014-07-01
..., 329-332 X Census tracts 13-75, 143, 158-161, 178-189, 295-297, 322, 324, 327 X Balance of city X (B... Allen Township X (C) Reading Air Basin X (D) Carbon County X (E) Remaining Portions of AQCR X III. South... Excludes Indian country located in each area, if any, unless otherwise specified. Pennsylvania—Carbon...
21 CFR Appendix B to Subpart B of... - Scope of Product Coverage
Code of Federal Regulations, 2010 CFR
2010-04-01
... Transducer ITX—Transducer, Ultrasonic, Diagnostic Diagnostic X-Ray Imaging Devices (except mammographic x-ray systems): RA 892.1600 Angiographic X-Ray System IZI—System, X-Ray, Angiographic RA 892.1650 Image-Intensified Fluoroscopic X-Ray System MQB—Solid State X-Ray Imager (Flat Panel/Digital Imager) JAA—System, X...
21 CFR Appendix B to Subpart B of... - Scope of Product Coverage
Code of Federal Regulations, 2011 CFR
2011-04-01
... Transducer ITX—Transducer, Ultrasonic, Diagnostic Diagnostic X-Ray Imaging Devices (except mammographic x-ray systems): RA 892.1600 Angiographic X-Ray System IZI—System, X-Ray, Angiographic RA 892.1650 Image-Intensified Fluoroscopic X-Ray System MQB—Solid State X-Ray Imager (Flat Panel/Digital Imager) JAA—System, X...
Material Development Study for a Hazardous Chemical Protective Clothing Outfit
1980-08-01
Analytical - X VCM Vinyl Chloride Unavailable - X ZEC Zectran Insoluble X X ZCN Zinc Cyanide Insoluble X X ZCT Zirconium Tetrachloride Water React. X 64...Environmental Rating of Plastics, Reprints of Design News, R. L. Peters , 6 December 1967, 20 December 1967, 22 November 1967, 8 November 1967. 13. Modern
NASA Astrophysics Data System (ADS)
Chen, Xiuli; Li, Xiaoxia; Yan, Xiao; Liu, Gaofeng; Zhou, Huanfu
2018-02-01
(Ba1-x Bi x )(Ti1-x Ni0.5x Sn0.5x )O3 (BBTNS, 0.02 ≤ x ≤ 0.1) samples have been synthesized by traditional solid-state reaction technique and their structural transformation and dielectric properties investigated. X-ray diffraction (XRD) analysis revealed that BBTNS could form a homogeneous solid solution, and the transformation from tetragonal to pseudocubic phase occurred at 0.04 ≤ &!nbsp;x ≤ 0.06. Optimized properties with stable ɛ r (˜ 1829 to 1838), small Δɛ/ɛ 25°C values (± 15%) over a broad temperature range from -60°C to 140°C, and low tan Δ (≤ 0.02) from 4°C to 194°C were obtained at x = 0.1. The relaxation and conduction process in the high-temperature region are attributed to thermal activation, and oxygen vacancies may be the ionic charge carriers in perovskite ferroelectrics.
Average and local crystal structures of (Ga 1–xZn x)(N 1–xO x) solid solution nanoparticles
Feygenson, Mikhail; Neuefeind, Joerg C.; Tyson, Trevor A.; ...
2015-11-06
We report the comprehensive study of the crystal structure of (Ga 1–xZn x)(N 1–xO x) solid solution nanoparticles by means of neutron and synchrotron x-ray scattering. In our study we used four different types of (Ga 1–xZn x)(N 1–xO x) nanoparticles, with diameters of 10–27 nm and x = 0.075–0.51, which show the narrow energy-band gaps from 2.21 to 2.61 eV. The Rietveld analysis of the neutron diffraction data revealed that the average crystal structure is the hexagonal wurtzite (space group P6 3mc), in agreement with previous reports on similar bulk materials. The pair-distribution function (PDF) analysis of the samemore » data found that the local structure is more disordered than the average one. It is best described by the model with a lower symmetry space group P1, where atoms are quasirandomly distorted from their nominal positions in the hexagonal wurtzite lattice.« less
Growth method for chalcongenide phase-change nanostructures
NASA Technical Reports Server (NTRS)
Yu, Bin (Inventor); Sun, Xuhui (Inventor); Meyyappan, Meyya (Inventor)
2010-01-01
A method for growth of an alloy for use in a nanostructure, to provide a resulting nanostructure compound including at least one of Ge.sub.xTe.sub.y, In.sub.xSb.sub.y, In.sub.xSe.sub.y, Sb.sub.xTe.sub.y, Ga.sub.xSb.sub.y, Ge.sub.xSb.sub.y,Te.sub.z, In.sub.xSb.sub.yTe.sub.z, Ga.sub.xSe.sub.yTe.sub.z, Sn.sub.xSb.sub.yTe.sub.z, In.sub.xSb.sub.yGe.sub.z, Ge.sub.wSn.sub.xSb.sub.yTe.sub.z, Ge.sub.wSb.sub.xSe.sub.yTe.sub.z, and Te.sub.wGe.sub.xSb.sub.yS.sub.z, where w, x, y and z are numbers consistent with oxidization states (2, 3, 4, 5, 6) of the corresponding elements. The melt temperatures for some of the resulting compounds are in a range 330-420.degree. C., or even lower with some compounds.
Oishi, Kohei; Yamayoshi, Seiya; Kawaoka, Yoshihiro
2018-03-01
The influenza A virus protein PA-X comprises an N-terminal PA region and a C-terminal PA-X-specific region. PA-X suppresses host gene expression, termed shutoff, via mRNA cleavage. Although the endonuclease active site in the N-terminal PA region of PA-X and basic amino acids in the C-terminal PA-X-specific region are known to be important for PA-X shutoff activity, other amino acids may also play a role. Here, we used yeast to identify novel amino acids of PA-X that are important for PA-X shutoff activity. Unlike wild-type PA-X, most PA-X mutants predominantly localized in the cytoplasm, indicating that these mutations decreased the shutoff activity of PA-X by affecting PA-X translocation to the nucleus. Mapping of the identified amino acids onto the N-terminal structure of PA revealed that some of them likely contribute to the formation of the endonuclease active site of PA. Copyright © 2018. Published by Elsevier Inc.
NASA Astrophysics Data System (ADS)
Chen, Wen; Wu, Wenwei; Zhou, Chong; Zhou, Shifang; Li, Miaoyu; Ning, Yu
2018-03-01
M-type hexagonal Sr1- x Co x Nd x Fe12- x O19 ( x = 0, 0.08, 0.16, and 0.24) has been synthesized by ball milling, followed by calcination in air. The calcined products have been characterized by x-ray powder diffraction (XRD), scanning electron microscopy (SEM), Fourier transform infrared spectra, and vibrating sample magnetometry. XRD and SEM analyses confirm the formation of M-type Sr hexaferrite with platelet-like morphology when Sr1- x Co x Nd x Fe12- x O19 ( x = 0, 0.08, 0.16, and 0.24) precursors are calcined at 950°C in air for 2.5 h. Lattice parameters " a" and " c" values of Sr1- x Co x Nd x Fe12- x O19 reflect a very small variation after doping of Nd3+ and Co2+ ions. Average crystallite size of Sr1- x Co x Nd x Fe12- x O19 sample, calcined at 1150°C, decreased obviously after doping of Co2+ and Nd3+ ions. This is because the bond energy of Nd3+-O2- is much larger than that of Sr2+-O2-. Magnetic characterization indicates that all the samples exhibit good magnetic properties. Substitution of Sr2+ and Fe3+ ions by Nd3+ and Co2+ ions can improve the specific saturation magnetizations and remanence of Sr1- x Co x Nd x Fe12- x O19. Sr0.84Co0.16Nd0.16Fe11.84O19, calcined at 1050°C, has the highest specific saturation magnetization value (74.75 ± 0.60 emu/g), remanence (45.15 ± 0.32 emu/g), and magnetic moment (14.34 ± 0.11 μ B); SrFe12O19, calcined at 1150°C, has the highest coercivity value (4037.01 ± 42.39 Oe). These magnetic parameters make this material a promising candidate for applications such as high-density magnetic recording and microwave absorbing materials.
Incorporation of economic values into the component traits of a ratio: feed efficiency.
Lin, C Y; Aggrey, S E
2013-04-01
Direct selection on a ratio (R) of 2 traits (x1/x2) does not have a mechanism to accommodate the relative economic values (a1 and a2) between x1 and x2 because selection criteria x1/x2 and a1x1/a2x2 rank animals in the same order. This study presented a procedure to incorporate the economic weights into ratio traits through linear transformation. The partial derivatives of a nonlinear profit function evaluated at the means were widely taken as economic weights in the literature. This study showed that the economic weights derived in this manner were erroneous because they actually contain a mixture of actual economic weights and transformation effects. The ratios 1/2 and 2/4 are considered equal by selection on R, but are treated differently by the linear index. In addition, this study presented a unified approach to compare 4 different selection strategies for genetic improvement of ratio traits: linear index (I), selection on the ratio (R), selection on difference between x1 and x2 (D), and selection on x1 alone. This study considered 3 levels of heritability each for variables x1 and x2 and 2 levels of genetic correlations (γG), 2 ratios of means (µ1/µ2), and 4 ratios of phenotypic variances giving a total of 96 scenarios. Linear index I was the most efficient of the 4 criteria compared in all 96 scenarios studied. The superiority of index I over R, D, and selection on x1 alone are particularly remarkable when x1 and x2 have a large difference in heritability and are highly correlated. Selection on x1 alone is an economically viable alternative to criterion I or R for the improvement of ratio traits particularly when x1 is more heritable than x2 and when x2 is costly to measure. Selection on D is more efficient than direct selection on R or selection on x1 alone when x1 is less heritable than x2 and the difference between µ1 and µ2 is small.
Xu, Hongwu; Chavez, Manuel E.; Mitchell, Jeremy N.; ...
2015-04-23
An analogue of the mineral pollucite (CsAlSi 2O 6), CsTiSi 2O 6.5 has a potential host phase for radioactive Cs. However, as 137Cs and 135Cs transmute to 137Ba and 135Ba, respectively, through the beta decay, it is essential to study the structure and stability of this phase upon Cs → Ba substitution. In this work, two series of Ba/Ti-substituted samples, Cs xBa (1-x)/2TiSi 2O 6.5 and Cs xBa 1-xTiSi 2O 7-0.5x, (x = 0.9 and 0.7), were synthesized by high-temperature crystallization from their respective precursors. Synchrotron X-ray diffraction and Rietveld analysis reveal that while Cs xBa (1-x)/2TiSi 2O 6.5 samplesmore » are phase-pure, Cs xBa 1-xTiSi 2O 7-0.5x samples contain Cs3x/(2+x)Ba (1-x)/(2+x)TiSi 2O 6.5 pollucites (i.e., also two-Cs-to-one-Ba substitution) and a secondary phase, fresnoite (Ba2TiSi2O8). Thus, the Cs xBa 1-xTiSi 2O 7-0.5x series is energetically less favorable than Cs xBa (1-x)/2TiSi 2O 6.5. To study the stability systematics of Cs xBa (1-x)/2TiSi 2O 6.5 pollucites, high-temperature calorimetric experiments were performed at 973 K with or without the lead borate solvent. Enthalpies of formation from the constituent oxides (and elements) have thus been derived. Our results show that with increasing Ba/(Cs + Ba) ratio, the thermodynamic stability of these phases decreases with respect to their component oxides. Hence, from the energetic viewpoint, continued Cs → Ba transmutation tends to destabilize the parent silicotitanate pollucite structure. However, the Ba-substituted pollucite co-forms with fresnoite (which incorporates the excess Ba), thereby providing viable ceramic waste forms for all the Ba decay products.« less
1988-04-01
commercially for conventional surface resistivity measure- ments. Lead or copper wire wrapped around an insulating cable is used for the downhole...3 x 106 -- Igneous rocks, basic Augite porphyry Kola Peninsula 9.5-12.6 105-107 Dry Basalt Berestovetskoe 15.6 5 x 10 5 Dry Basalt Kutai 10.3 5 x...acidic Granite Azerbaidjan 3.0 x 107 -- Granite Ubinskoe 0.36 x 109 3.2 x 1018 Granite Kola Peninsula 0.16 x 105 0.3 x 1016 Granite porphyry 4.5 x 10 5
Formal Modeling of Diffie-Hellman Derivability for Exploratory Automated Analysis
2013-06-01
monomials (displayed as a column vector for readability): (23) MA(x̄) = MA1(x̄) MA2 (x̄) ... MAr (x̄) = xα111 x α12 2 · · ·xα1nn xα211 x...ȳ β̄ ∈ F[y1, . . . , yr] and A ∈ Mr×n(Z) is such that P (MA1(x̄), MA2 (x̄), . . . ,MAr (x̄)) = 0 then for every γ̄, (28) ∑ β̄·A=γ̄ cβ̄ = 0. An...Corollary 8.3. Suppose (29) R(ȳ) = ∑ β̄ cβ̄Mβ̄(ȳ)∑ β̄ dβ̄Mβ̄(ȳ) ∈ F(y1, . . . , yr), A ∈Mr×n(Z) and γ̄ ∈M1×n(Z) are such that (30) R (MA1(x̄), MA2
Nb(x)Ti(1-x)N Superconducting-Nanowire Single-Photon Detectors
NASA Technical Reports Server (NTRS)
Stern, Jeffrey A.; Farr, William H.; Leduc, Henry G.; Bumble, Bruce
2008-01-01
Superconducting-nanowire single-photon detectors (SNSPDs) in which Nb(x)Ti(1-x)N (where x<1) films serve as the superconducting materials have shown promise as superior alternatives to previously developed SNSPDs in which NbN films serve as the superconducting materials. SNSPDs have potential utility in optical communications and quantum cryptography. Nb(x)Ti(1-x)N is a solid solution of NbN and TiN, and has many properties similar to those of NbN. It has been found to be generally easier to stabilize Nb(x)Ti(1-x)N in the high-superconducting-transition temperature phase than it is to so stabilize NbN. In addition, the resistivity and penetration depth of polycrystalline films of Nb(x)Ti(1-x)N have been found to be much smaller than those of films of NbN. These differences have been hypothesized to be attributable to better coupling at grain boundaries within Nb(x)Ti(1-x)N films.
The coupling of a disk corona and a jet for the radio/X-ray correlation in black hole X-ray binaries
NASA Astrophysics Data System (ADS)
Qiao, Erlin
2016-02-01
We interpret the radio/X-ray correlation of L R ~ L X ~1.4 for L X/L Edd >~ 10-3 with a detailed disk corona-jet model, in which the accretion flow and the jet are connected by a parameter, η, describing the fraction of the matter in the accretion flow ejected outward to form the jet. We calculate L R and L X at different Ṁ, adjusting η to fit the observed radio/X-ray correlation of the black hole X-ray transient H1743-322 for L X/L Edd > 10-3. It is found that the value of η for this radio/X-ray correlation for L X/L Edd > 10-3, is systematically less than that of the case for L X/L Edd < 10-3, which is consistent with the general idea that the jet is often relatively suppressed at the high luminosity phase in black hole X-ray binaries.
Magnetic properties of the layered III-VI diluted magnetic semiconductor Ga{sub 1−x}Fe{sub x}Te
DOE Office of Scientific and Technical Information (OSTI.GOV)
Pekarek, T. M.; Edwards, P. S.; Olejniczak, T. L.
2016-05-15
Magnetic properties of single crystalline Ga{sub 1−x}Fe{sub x}Te (x = 0.05) have been measured. GaTe and related layered III-VI semiconductors exhibit a rich collection of important properties for THz generation and detection. The magnetization versus field for an x = 0.05 sample deviates from the linear response seen previously in Ga{sub 1−x}Mn{sub x}Se and Ga{sub 1−x}Mn{sub x}S and reaches a maximum of 0.68 emu/g at 2 K in 7 T. The magnetization of Ga{sub 1−x}Fe{sub x}Te saturates rapidly even at room temperature where the magnetization reaches 50% of saturation in a field of only 0.2 T. In 0.1 T atmore » temperatures between 50 and 400 K, the magnetization drops to a roughly constant 0.22 emu/g. In 0 T, the magnetization drops to zero with no hysteresis present. The data is consistent with Van-Vleck paramagnetism combined with a pronounced crystalline anisotropy, which is similar to that observed for Ga{sub 1−x}Fe{sub x}Se. Neither the broad thermal hysteresis observed from 100-300 K in In{sub 1−x}Mn{sub x}Se nor the spin-glass behavior observed around 10.9 K in Ga{sub 1−x}Mn{sub x}S are observed in Ga{sub 1−x}Fe{sub x}Te. Single crystal x-ray diffraction data yield a rhombohedral space group bearing hexagonal axes, namely R3c. The unit cell dimensions were a = 5.01 Å, b = 5.01 Å, and c = 17.02 Å, with α = 90°, β = 90°, and γ = 120° giving a unit cell volume of 369 Å{sup 3}.« less
Endangered Species on U.S. Army Installations.
1982-08-01
OLOKELEANUM x VOTOTICHIUMr VIRIDE /MFSD. x PEUCEDANUM KAIJAIEJSEL x PTERALYXIA, KAUAI x RAUVOLFIA MFLLEPI x HAD x RAUVOLFIA SArJDWICENSIS VAR...HELLERI PLANTS UNnETERMIAED SCHOFIELD BARRACKS# RAUVOLFIA SANOWICENSIS VAR, SUBACUMINATA PLANTS UINDETERMINED SCHOFIELD BARRACKS, *EMYA KAUAIENSIS /HBD
Code of Federal Regulations, 2011 CFR
2011-07-01
... County X Buffalo County X Chippewa County X Clark County X Crawford County X Dunn County X Eau Claire... Unclassifiable/Attainment Chippewa County Unclassifiable/Attainment Clark County Unclassifiable/Attainment... Unclassifiable/Attainment Chippewa County Unclassifiable/Attainment Clark County Unclassifiable/Attainment...
Code of Federal Regulations, 2010 CFR
2010-07-01
... County X Buffalo County X Chippewa County X Clark County X Crawford County X Dunn County X Eau Claire... Unclassifiable/Attainment Chippewa County Unclassifiable/Attainment Clark County Unclassifiable/Attainment... Unclassifiable/Attainment Chippewa County Unclassifiable/Attainment Clark County Unclassifiable/Attainment...
46 CFR 12.15-9 - Examination requirements.
Code of Federal Regulations, 2013 CFR
2013-10-01
... X X X 18. The procedure in preparing a turbine, reciprocating, or Diesel engine for standby; also... supply of water to boilers, the dangers of high and low water and remedial action X X X 20. Operation...
46 CFR 12.15-9 - Examination requirements.
Code of Federal Regulations, 2012 CFR
2012-10-01
... X X X 18. The procedure in preparing a turbine, reciprocating, or Diesel engine for standby; also... supply of water to boilers, the dangers of high and low water and remedial action X X X 20. Operation...
Formation of Large-Amplitude Wave Groups in an Experimental Model Basin
2008-08-01
varying parameters, including amplitude, frequency, and signal duration. Superposition of thes finite regular waves produced repeatable wave groups at a...19 Regular Waves 20 Irregular Waves 21 Senix Wave Gages 21 GLRP 23 Instrumentation Calibration and Uncertainty 26 Senix Ultrasonic Wave Gages... signal output from sine wave superposition, two sine waves combined: x] + x2 (top) and x3 + x4 (middle), all four waves (x, + x2 + x, + xA
Federal Register 2010, 2011, 2012, 2013, 2014
2013-08-02
... 941, 941-PR, 941- SS, 941-X, 941-X(PR), Schedule B (Form 941), Schedule R (Form 941)and Schedule B... Islands), 941-X, Adjusted Employer's Quarterly Federal Tax Return or Claim for Refund, 941-X(PR), Schedule...: 941, 941-PR, 941-SS, 941-X, 941-X(PR), Schedule R (Form 941), Schedule B (Form 941), and Schedule B...
X-ray monitoring optical elements
Stoupin, Stanislav; Shvydko, Yury; Katsoudas, John; Blank, Vladimir D.; Terentyev, Sergey A.
2016-12-27
An X-ray article and method for analyzing hard X-rays which have interacted with a test system. The X-ray article is operative to diffract or otherwise process X-rays from an input X-ray beam which have interacted with the test system and at the same time provide an electrical circuit adapted to collect photoelectrons emitted from an X-ray optical element of the X-ray article to analyze features of the test system.
Thermoelectric properties of Ge 1-xSn xTe crystals grown by vertical Bridgman method
NASA Astrophysics Data System (ADS)
Wu, C. C.; Ferng, N. J.; Gau, H. J.
2007-06-01
Single crystals of Ge 1-xSn xTe compounds with x=0, 0.8, 0.9 and 1.0 were grown by vertical Bridgman method. The crystalline phase and stochiometry for these crystals were investigated by X-ray diffraction, metallographic microscope as well as electron-probe microanalysis (EPMA). Electrical property of the as-grown samples was characterized using room temperature resistivity and Hall measurements. The thermoelectric behaviors for the Ge 1-xSn xTe crystals were studied by means of thermal and carrier transport measurements. Temperature dependences of resistivity, Seebeck coefficient and thermal conductivity for the various compositions of Ge 1-xSn xTe were analyzed. A two-valence band model was proposed to describe the temperature dependence of thermoelectric property of the Ge 1-xSn xTe crystals. The dimensionless thermoelectric figure of merit ZT for the alloys was evaluated and discussed.
DOE Office of Scientific and Technical Information (OSTI.GOV)
Koike, Y.; Kakinuma, N.; Aoyama, M.
1999-12-01
Transport and {Tc} anomalies around x = 0.22 in La{sub 2{minus}x}Sr{sub x}CuO{sub 4} have been studied through the partial substitution of Zn, Ga and Ni for Cu. It has been found that the value of x where the anomalies occur shifts to lower x values through the Zn substitution, while it shifts to larger x values through the Ga substitution, and it disappears through the Ni substitution. There is a possibility that an order of holes and/or spins, such as the so-called stripe order, is formed or fluctuates around x = 0.22 in La{sub 2{minus}x}Sr{sub x}CuO{sub 4}.
On the geometry of a smooth model of a fibre product of families of K3 surfaces
DOE Office of Scientific and Technical Information (OSTI.GOV)
Nikol'skaya, O V
The Hodge conjecture on algebraic cycles is proved for a smooth projective model X of a fibre product X{sub 1}×{sub C}X{sub 2} of nonisotrivial 1-parameter families of K3 surfaces (possibly with degeneracies) X{sub k}→C (k=1,2) over a smooth projective curve C under the assumption that, for generic geometric fibres X{sub 1s} and X{sub 2s}, the ring End{sub Hg(X{sub 1{sub s)}}}NS{sub Q}(X{sub 1s}){sup ⊥} is an imaginary quadratic field, rankNS(X{sub 1s})≠18, and End{sub Hg(X{sub 2{sub s)}}}NS{sub Q}(X{sub 2s}){sup ⊥} is a totally real field or else rankNS(X{sub 1s})
IncX2 and IncX1-X2 Hybrid Plasmids Coexisting in a FosA6-Producing Escherichia coli Strain
Su, Jiachun; McElheny, Christi Lee; Wang, Minggui
2017-01-01
ABSTRACT IncX plasmids are receiving much attention as vehicles of carbapenem and colistin resistance genes, such as blaNDM, blaKPC, and mcr-1. Among them, IncX2 subgroup plasmids remain rare. Here, we characterized IncX2 and IncX1-X2 hybrid plasmids coexisting in a FosA6-producing Escherichia coli strain that were possibly generated as a consequence of recombination events between an R6K-like IncX2 plasmid and a pLN126_33-like IncX1 plasmid. Variable multidrug resistance mosaic regions were observed in these plasmids, indicating their potential to serve as flexible carriers of resistance genes. The diversity of IncX group plasmid backbones and accessory genes and the evolution of hybrid IncX plasmids pose a challenge in detecting and classifying them. PMID:28438937
DOE Office of Scientific and Technical Information (OSTI.GOV)
Watson, J.M.; Spencer, J.A.; Graves, J.A.M.
1990-09-01
Eight genes, located on the long arm of the human X chromosome and present on the marsupial X chromosome, were mapped by in situ hybridization to the chromosomes of the platypus Ornithorhynchus anatinus, one of the three species of monotreme mammals. All were located on the X chromosome. The authors conclude that the long arm of the human X chromosome represents a highly conserved region that formed part of the X chromosome in a mammalian ancestor at least 150 million years ago. Since three of these genes are located on the long arm of the platypus X chromosome, which ismore » G-band homologous to the Y chromosome and apparently exempt from X chromosome inactivation, the conservation of this region has evidently not depended on isolation by X-Y chromosome differentiation and X chromosome inactivation.« less
Chemistry of the Apollo 11 highland component
NASA Technical Reports Server (NTRS)
Laul, J. C.; Papike, J. J.; Simon, S. B.; Shearer, C. K.
1983-01-01
Thirty-eight Apollo 11 lunar highland fragments from coarse fines 10085 have been subjected to petrologic and chemical study. Six major chemical groups are identified: (a) high-K KREEP; (b) anorthosite with a 10X chondrite positive Eu anomaly and anorthosite with 30X positive Eu anomaly; (c) ANT; (d) LKFM; (e) anorthositic gabbro with no Eu anomaly, with a positive Eu anomaly, and with a negative Eu anomaly; and (f) dominant Highland component, 2X-10X chondrite with a positive 10X-14X Eu anomaly. Newly recognized groups are presented based on the REE patterns: (a) ANT group with 5X La and a 22X positive Eu anomaly; (b) 10X flat with 14X positive Eu anomaly; and (c) 2-3X flat with a 10X positive Eu anomaly. The highland suite is very low in K and REE, and is overall quite similar to the Apollo 16 suite.
Tuning of magnetism in DyMn1-xFexO3 (x<0.1) system by iron substitution
NASA Astrophysics Data System (ADS)
Mihalik, Matúš; Mihalik, Marián; Zentková, Mária; Uhlířová, Klára; Kratochvílová, Marie; Fitta, Magdalena; Quintero, Pedro A.; Meisel, Mark W.
2018-05-01
The effect of Fe doping on the magnetism of DyMn1-xFexO3 (x<0.1) single crystals is reported. Specifically, TN of the Mn sublattice decreases from 38 K (x = 0) to 33 K (x = 0.1), TS = 17.9 K (x = 0) connected with the transition of Mn-spins into the cycloidal magnetic phase decreases to 15.9 K (x = 0.01) and vanishes for higher x concentrations, while the ordering temperature of the Dy sublattice varies between 5.9 K (x = 0.01) and 4.1 K (x = 0.02). These results indicate the ground state magnetic structure of DyMnO3 can be destabilized, and the multiferroicity is completely suppressed by very low Fe doping. Similar effects were previously observed in the multiferroic TbMn1-xFexO3 system.
Zheng, Xingqun; Peng, Lishan; Yang, Na; Yang, Yanjun; Li, Jing; Wang, Jianchuan
2018-01-01
The transition-metal compounds (MX) have gained wide attention as hydrogen evolution reaction (HER) electrocatalysts; however, the interaction between the non-metallic atom (X) and the metal atom (M) in MX, and the role of X in the enhanced catalytic activity of MX, are still ambiguous. In this work, we constructed a simple model [X/Ni(100)] to decipher the contribution of X towards enhancing the catalytic activity of NiX, which allows us to accurately predict the trend in HER catalytic activity of NiX based on the easily accessible physico-chemical characteristics of X. Theoretical calculations showed that the electronegativity (χX) and the principle quantum number (nX) of X are two important descriptors for evaluating and predicting the HER catalytic activity of NiX catalysts effectively. X atoms in the VIA group can enhance the HER activity of X/Ni(100) more significantly than those in the second period due to the large χX or nX. At a relatively low X coverage, the S/Ni(100) possesses the best HER activity among all of the discussed X/Ni(100) models, and the optimum surface S : Ni atomic ratio is about 22–33%. Further experiments demonstrated that the Ni–Ni3S2 catalyst with a surface S : Ni atomic ratio of 28.9% exhibits the best catalytic activity and lowest charge transfer resistance. The trend in catalytic activity of NiX with differing X offers a new possible strategy to exploit MX materials and design new active catalysts rationally. PMID:29675227
P2X receptor ligands and pain.
Shieh, Char-Chang; Jarvis, Michael F; Lee, Chih-Hung; Perner, Richard J
2006-08-01
P2X receptors belong to a superfamily of ligand-gated ion channels that conduct the influx of Ca(2+), Na(+) and K(+) cations following activation by extracellular nucleotides such as ATP. Molecular cloning studies have identified seven subunits, namely P2X(1-7), that share approximately 40 - 50% identity in amino acid sequences within the subfamily. Using gene-silencing, pharmacological and electrophysiological approaches, recent studies have revealed roles for P2X(2), P2X(3), P2X(4) and P2X(7) receptors in nociceptive signalling. Homomeric P2X(3) and heteromeric P2X(2/3) receptors are highly localised in the peripheral sensory afferent neurons that conduct nociceptive sensory information to the spinal chord and brain. The discovery of A-317491, a selective and potent non-nucleotide P2X(3) antagonist, provided a pharmacological tool to determine the site and mode of action of P2X(3)-containing receptors in different pain behaviours, including neuropathic, inflammatory and visceral pain. Other P2X receptors (P2X(4) and P2X(7)) that are predominantly expressed in microglia, macrophages and cells of immune origin can trigger the release of cytokines, such as IL-1-beta and TNF-alpha. Genetic disruption of P2X(4) and P2X(7) signalling has been demonstrated to reduce inflammatory and neuropathic pain, suggesting that these two receptors might serve as integrators of neuroinflammation and pain. This article provides an overview of recent scientific literature and patents focusing on P2X(3), P2X(4) and P2X(7) receptors, and the identification of small molecule ligands for the potential treatment of neuropathic and inflammatory pain.
DOE Office of Scientific and Technical Information (OSTI.GOV)
Sumioka, Akio; Saito, Yuhki; Sakuma, Megumi
2008-03-10
The X11/MINT family proteins are adaptor scaffolding proteins involved in formation of multiprotein complexes, and trafficking and metabolism of membrane proteins such as the beta-amyloid precursor protein. We found that a significant portion of X11L and X11L2 are recovered in nuclear fraction of mouse brain homogenates. EGFP-X11s were not detected in the nucleus of N2a neuroblastoma cells; however, administration of leptomycin B (LMB) induced substantial nuclear accumulation of EGFP-X11L and EGFP-X11L2, while EGFP-X11 showed little accumulation. Fluorescence loss in photobleaching (FLIP) analysis indicated that EGFP-X11L2 and EGFP-X11L are shuttled between the cytoplasm and nucleus, the former more effectively than themore » latter. We identified a nuclear export signal (NES) in the N-terminus of X11L2, mutation of which induces nuclear accumulation of EGFP-X11L2 in the absence of LMB. X11L2 fused to the Gal4 DNA binding domain (DBD) showed transcriptional activity, suggesting that X11L2 could function as a transcriptional activator if tethered near a promoter. Interestingly, attenuation of the nucleo-cytoplasmic shuttling of GAL4-DBD-X11L2 by mutating the NES or attaching the SV40 nuclear localization signal significantly decreased the apparent transcriptional activity. Our observations suggest that X11L2 functions in the nucleus by a mechanism distinct from conventional transactivators.« less
Measuring the Dust Grains and Distance to X Persei Via Its X-ray Halo
NASA Astrophysics Data System (ADS)
Smith, Randall
2006-09-01
We propose to observe the X-ray halo of the high mass X-ray binary pulsar X Per to measure interstellar dust grains along the line of sight (LOS) and to determine the distance to X Per. The X-ray halo is formed by scattering from grains along the LOS, which for X Per appear to be concentrated in one molecular cloud. Unlike many other X-ray halo observations, this low-absorption high-latitude sightline is well-characterized from absorption spectroscopy done with HST, Copernicus, and FUSE. This halo observation will measure the distance to the cloud and the dust size distribution in it. We will also be able to determine the distance to X Per by measuring the time delayed pulses in the X-ray halo.
2014-06-01
Consider the BF defined as f : F22 → F2, with ANF given by 1⊕ x1⊕ x2. The truth table representation is given in Table 4.8. x2 x1 f 0 0 1 0 1 0 1 0 0 1 1...1 Table 4.8: Truth Table Representation for 1⊕ x1⊕ x2. WT F(w) =W ( f )(w) = ∑ x∈ F22 f (x) · (−1)<w·x> F(00) = 1(−1)0 +0+0+1(−1)0 = 2 F(01) = 1(−1)0...Fn2 [51, 68]. The function f (x) = x1x2 on F22 is bent since the Walsh-Hadamard spectrum is |F̂(u)| = 22/2 =(2,2,2,−2). Another version of Fourier
1991-01-01
LOCATIONS DRAWN BY J. WELL LOCATIONS DATE: 5-31. DATE -31-MGM= . ENCE CORNER (O’S. & O’W) ...........x xC.O.E. MONUIM:NT NO. 324 NORTH COOR. - 670.555.7 x...RUDWTREEVTO OTU M ~ HYRAULC GRDENTLIN A% A W0 78W.M. 3 B1 - ENCE CORNER tos & o’U) -x x -x .O. E. MIONUMENT NO. 324 x-x-NORTH COOR. -. 670;;55;.7 x...ROUNwATE ELEATIO CON4UR3 ~~~~W xRJJ t ZRQ N IN tW 9 . AILA~E 261~ W-03- 26.6W~~ 0 B’ ENCE CORNER (O’S. & O’W) -K XMx X - .O.E. MONUMENT NO. 324
Chen, Yi-Cun; Zhu, Wei; Zhong, Shu-Ping; Zheng, Fu-Chun; Gao, Fen-Fei; Zhang, Yan-Mei; Xu, Han; Zheng, Yan-Shan; Shi, Gang-Gang
2015-01-01
BACKGROUND AND PURPOSE Calcium antagonists play an important role in clinical practice. However, most of them have serious side effects. We have synthesized a series of novel calcium antagonists, quaternary ammonium salt derivatives of haloperidol with N-p-methoxybenzyl (X1), N-m-methoxybenzyl (X2) and N-o-methoxybenzyl (X3) groups. The objective of this study was to investigate the bioactivity of these novel calcium antagonists, especially the vasodilation activity and cardiac side-effects. The possible working mechanisms of these haloperidol derivatives were also explored. EXPERIMENTAL APPROACH Novel calcium antagonists were synthesized by amination. Compounds were screened for their activity of vasodilation on isolated thoracic aortic ring of rats. Their cardiac side effects were explored. The patch-clamp, confocal laser microscopy and the computer-fitting molecular docking experiments were employed to investigate the possible working mechanisms of these calcium antagonists. RESULTS The novel calcium antagonists, X1, X2 and X3 showed stronger vasodilation effect and less cardiac side effect than that of classical calcium antagonists. They blocked L-type calcium channels with an potent effect order of X1 > X2 > X3. Consistently, X1, X2 and X3 interacted with different regions of Ca2+-CaM-CaV1.2 with an affinity order of X1 > X2 > X3. CONCLUSIONS The new halopedidol derivatives X1, X2 and X3 are novel calcium antagonists with stronger vasodilation effect and less cardiac side effect. They could have wide clinical application. PMID:26544729
A Trainee Demand Analysis for the Expansion of the Marine Corps Embassy Security Group
2013-04-17
FY GIXid$ of serwite (GOS] 2010 3 lOll ~ ,2012 5 2013 X 2014 X ,2015 )t 2016 X 2017 X , 2018 X 2019 X ,1010 X L lntetfaee J oetachme;nt...Walkenbach, J. (2010). Microsoft Excel 2010 bible . Indianapolis, IN: Wiley. Wang, J., Egudo, R., & Galanis, G. (2007, August). Determining training demand
Test and Evaluation Report of the IMED Volumetric Infusion Pump Model 960A
1992-02-01
tested Ambient tempera- ture was out of test lim- its. Windshield anti-ice X Pitot heat X Vent blower X Windshield wiper X Heater X APU X Generator #1 X...Patterson John A. Dellinger, Air Force Base, OH 45433 Southwest Research Institute P. 0. Box 28510 Henry L. Taylor San Antonio, TX 78284 Director
Behavioral Influence Modeling and Simulation
2011-12-01
Distribution A: Approved for public release; distribution unlimited. 88ABW-2012-3864, 13 July 2012 Survey Monkey Pro: Survey Monkey Pro is an...long hair (X3), no tail (X14), and found in the zoo (X19). The brown bear has brown hair (X9), very large (X13), long hair (X3) and no tail (X14
Code of Federal Regulations, 2014 CFR
2014-07-01
... County X Pepin County X Pierce County X Polk County X St. Croix County X Trempealeau County X Vernon... Unclassifiable/Attainment Ozaukee County Unclassifiable/Attainment Pepin County Unclassifiable/Attainment Pierce... Unclassifiable/Attainment Pepin County Unclassifiable/Attainment Pierce County Unclassifiable/Attainment Polk...
Electrical conduction mechanism of LaNi{sub x}Me{sub 1−x}O{sub 3−δ} (Me = Fe, Mn)
DOE Office of Scientific and Technical Information (OSTI.GOV)
Niwa, Eiki, E-mail: e-niwa@phys.chs.nihon-u.ac.jp; Department of Integrated Sciences in Physics and Biology, College of Humanities and Sciences, Nihon University, Setagaya-ku, Tokyo 156-8550; Maeda, Hiroki
Graphical abstract: Compositional dependence of (a) electrical conductivity and (b) E{sub a} for hopping conduction of LaNi{sub x}Me{sub 1−x}O{sub 3} (Me = Fe, Mn). - Highlights: • Electrical conduction mechanism of LaNi{sub x}Me{sub 1−x}O{sub 3} (Me = Fe, Mn) was investigated. • Hopping conduction model could be applied for conductivity of both specimens. • The difference of E{sub a} due to that of energy level of Fe and Mn was observed. • Hole concentration estimated by iodimetry increases with increasing Ni content. - Abstract: Electrical conduction mechanism of LaNi{sub x}Fe{sub 1−x}O{sub 3−δ} and LaNi{sub x}Mn{sub 1−x}O{sub 3+δ} expected as Sr-freemore » new cathode material for solid oxide fuel cells was analyzed. Electrical conduction behaviors of both specimens could be well fitted by small polaron hopping conduction model. The electrical conductivity of LaNi{sub x}Fe{sub 1−x}O{sub 3−δ} increased with increasing Ni content, showing agreement with decrease of activation energy for hopping conduction. The decrease of electrical conductivity and increase of activation energy of LaNi{sub x}Mn{sub 1−x}O{sub 3+δ} were observed with increasing Ni content for 0.0 ≤ x ≤ 0.4. Further Ni substitution increased electrical conductivity and decreased activation energy for 0.4 ≤ x ≤ 0.6. It was revealed using iodometry that the difference of hole carrier density between LaNi{sub x}Fe{sub 1−x}O{sub 3−δ} and LaNi{sub x}Mn{sub 1−x}O{sub 3+δ} was small. It was suspected that the origin of the difference of electrical conduction behavior of LaNi{sub x}Fe{sub 1−x}O{sub 3−δ} and LaNi{sub x}Mn{sub 1-x}O{sub 3+δ} was difference of energy level of e{sub g} band composed of Fe 3d or Mn 3d orbitals and their overlapping quantity with O 2p and Ni 3d band.« less
Peristalsis is impaired in the small intestine of mice lacking the P2X3 subunit
Bian, Xiaochun; Ren, Jianhua; De Vries, Matthew; Schnegelsberg, Birthe; Cockayne, Debra A; Ford, Anthony P D W; Galligan, James J
2003-01-01
P2X receptors are ATP-gated cation channels composed of one or more of seven different subunits. P2X receptors participate in intestinal neurotransmission but the subunit composition of enteric P2X receptors is unknown. In this study, we used tissues from P2X3 wild-type (P2X3+/+) mice and mice in which the P2X3 subunit gene had been deleted (P2X3−/−) to investigate the role of this subunit in neurotransmission in the intestine. RT-PCR analysis of mRNA from intestinal tissues verified P2X3 gene deletion. Intracellular electrophysiological methods were used to record synaptic and drug-induced responses from myenteric neurons in vitro. Drug-induced longitudinal muscle contractions were studied in vitro. Intraluminal pressure-induced reflex contractions (peristalsis) of ileal segments were studied in vitro using a modified Trendelenburg preparation. Gastrointestinal transit was measured as the progression in 30 min of a liquid radioactive marker administered by gavage to fasted mice. Fast excitatory postsynaptic potentials recorded from S neurons (motoneurons and interneurons) were similar in tissues from P2X3+/+ and P2X3−/− mice. S neurons from P2X3+/+ and P2X3−/− mice were depolarized by application of ATP but not α,β-methylene ATP, an agonist of P2X3 subunit-containing receptors. ATP and α,β-methylene ATP induced depolarization of AH (sensory) neurons from P2X3+/+ mice. ATP, but not α,β-methylene ATP, caused depolarization of AH neurons from P2X3−/− mice. Peristalsis was inhibited in ileal segments from P2X3−/− mice but longitudinal muscle contractions caused by nicotine and bethanechol were similar in segments from P2X3+/+ and P2X3−/− mice. Gastrointestinal transit was similar in P2X3+/+ and P2X3−/− mice. It is concluded that P2X3 subunit-containing receptors participate in neural pathways underlying peristalsis in the mouse intestine in vitro. P2X3 subunits are localized to AH (sensory) but not S neurons. P2X3 receptors may contribute to detection of distention or intraluminal pressure increases and initiation of reflex contractions. PMID:12813150
Sealed-tube synthesis and phase diagram of Li{sub x}TiS{sub 2} (0 ≤ x ≤1)
DOE Office of Scientific and Technical Information (OSTI.GOV)
Zhang, Ziping; National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Science, Beijing 100190; Dong, Cheng, E-mail: chengdon@aphy.iphy.ac.cn
2015-01-15
Graphical abstract: We reported a new method to prepare Li{sub x}TiS{sub 2} (0 ≤ x ≤ 1) at 600 °C in sealed tube using Li{sub 2}S aslithium source. A schematic phase diagram of the Li{sub x}TiS{sub 2} system has been constructed based on the DTA and XRD data. - Abstract: We reported a new method to prepare Li{sub x}TiS{sub 2} (0 ≤ x ≤ 1) at 600 °C in sealed tube using Li{sub 2}S as lithium source. The Li{sub x}TiS{sub 2} samples were characterized by powder X-ray diffraction, scanning electron microscopy, energy dispersive X-ray spectroscopy, and differential thermal analysis. Themore » variations of the lattice parameters with lithium content x in Li{sub x}TiS{sub 2} were determined by X-ray powder diffraction analysis for both 1T and 3R phases. The phase transition between low-temperature 1T phase and high-temperature 3R phase was confirmed by the powder X-ray diffraction analysis. Based on the differential thermal analysis and X-ray diffraction results, a schematic phase diagram of the Li{sub x}TiS{sub 2} system has been constructed, providing a guideline to synthesize Li{sub x}TiS{sub 2} in 1T structure or 3R structure.« less
Differential Thermal Analysis of Hg(1-x)Mn(x)Te Alloys in the X=0 to 0.3 Range
NASA Technical Reports Server (NTRS)
Price, M. W.; Scripa, R. N.; Szofran, F. R.; Lehoczky, S. L.; Su, C-H
1998-01-01
Understanding the experimental conditions necessary for the development of radial and axial compositional homogeneity in directionally solidified Hg(0.89)Mn(0.11)Te(MMT) crystals has been difficult due to the lack of segregation coefficient data on the Hg(1-x)Mn(x)Te alloy system in the X = 0 to 0.3 composition range. Determining segregation coefficient data from the available Hg(1-x)Mn(x)Te alloy phase equilibria data is not practical due to discrepancies in the shape of the reported solidus and liquidus curves in the X = 0 to 0.3 range. To resolve these discrepancies and to obtain segregation coefficient data which can be used to understand homogeneity in directionally solidified MMT crystals, the solidus and liquidus temperatures of seven Hg(1-x)Mn(x)Te alloys in the X = 0 to 0.3 range were determined using differential thermal analysis (DTA). The Hg(1-x)Mn(x)Te phase diagram constructed for the X = 0 to 0.3 range of this alloy system from the DTA measurements clarifies the shape of the solidus and liquidus curves in this range. The segregation coefficient for the Hg(1-x)Mn(x)Te system was found to vary from 5 to 4.4 as the solidus composition increased from 0-30 atomic percent MnTe. This information will be useful in the analysis of axial and radial homogeneity of directionally solidified MMT crystals.
Menon, Debashish U; Coarfa, Cristian; Xiao, Weimin; Gunaratne, Preethi H; Meller, Victoria H
2014-11-18
Highly differentiated sex chromosomes create a lethal imbalance in gene expression in one sex. To accommodate hemizygosity of the X chromosome in male fruit flies, expression of X-linked genes increases twofold. This is achieved by the male- specific lethal (MSL) complex, which modifies chromatin to increase expression. Mutations that disrupt the X localization of this complex decrease the expression of X-linked genes and reduce male survival. The mechanism that restricts the MSL complex to X chromatin is not understood. We recently reported that the siRNA pathway contributes to localization of the MSL complex, raising questions about the source of the siRNAs involved. The X-linked 1.688 g/cm(3) satellite related repeats (1.688(X) repeats) are restricted to the X chromosome and produce small RNA, making them an attractive candidate. We tested RNA from these repeats for a role in dosage compensation and found that ectopic expression of single-stranded RNAs from 1.688(X) repeats enhanced the male lethality of mutants with defective X recognition. In contrast, expression of double-stranded hairpin RNA from a 1.688(X) repeat generated abundant siRNA and dramatically increased male survival. Consistent with improved survival, X localization of the MSL complex was largely restored in these males. The striking distribution of 1.688(X) repeats, which are nearly exclusive to the X chromosome, suggests that these are cis-acting elements contributing to identification of X chromatin.
Flexible Tagged Architecture for Trustworthy Multi-core Platforms
2015-06-01
well as two kernel benchmarks for SHA - 256 and GMAC, which are popular cryptographic standards. We compared the execution time of these benchmarks...UMC UMC on Flex fabric (FPGA) 266 90,384 10.8% 21 5.8% DIFT DIFT on Flex fabric (FPGA) 256 123,471 14.8% 23 6.3% BC BC on Flex fabric (FPGA) 229...0.25X) (1X) (0.5X) (0.25X) (1X) (0.5X) (0.25X) (1X) (0.5X) (0.25X) sha 1.01 1.01 1.01 1.01 1.06 1.16 1.03 1.07 1.15 1.00 1.33 1.50 gmac 1.01 1.01 1.09
Determining and Controlling the Magnesium Composition in CdTe/CdMgTe Heterostructures
LeBlanc, E. G.; Edirisooriya, M.; Ogedengbe, O. S.; ...
2017-06-05
The relationships between Mg composition, band gap, and lattice characteristics are investigated for Cd 1-xMg xTe barrier layers using a combination of cathodoluminescence, energy dispersive x-ray spectroscopy, variable angle spectral ellipsometry, and atom probe tomography. The use of a simplified, yet accurate, variable angle spectral ellipsometry analysis is shown to be appropriate for fast determination of composition in thin Cd 1-xMg xTe layers. The validity of using high-resolution x-ray diffraction for CdTe/Cd 1-xMg xTe double heterostructures is discussed. Furthermore, the stability of CdTe/Cd 1-xMg xTe heterostructures are investigated with respect to thermal processing.
DC-7B Aircraft Spray System for Large-Area Insect Control
1975-11-01
the ground. The two inert aerosol samnplers used were a 2.5-inch-diameter can wrapped with Printflex-card stock and a 2-mm-diameter pipe cleaner. The...mph (i to 6 m/sec). (2) One inert aerosol sampler (can wrapped with Printflex- card stock ) was positioned 20, 40, 60, and 80 meters above terrain on...4.040x105 2.174x105 9.195x104 2.950x105 1. 035x10 5 ETf 0.501 0.927 1.00 0.501 0.501 L (m) 1.408x104 7.376x103 7.488x103 1.028x104 8.662x103 H (i) 15
NASA Astrophysics Data System (ADS)
Li, Y. K.; Chen, Y. W.; Cheng, X. W.; Wu, C.; Cheng, B.
2018-05-01
In this paper, the valence electron structure parameters of Zr(x)Ti(x)Hf(x)Nb(x)Mo(x) alloys were calculated based on the empirical electron theory of solids and molecules (EET), and their performance through these parameters were predicted. Subsequently, the alloys with special valence electron structure parameters were prepared byarc melting. The hardness and high-temperature mechanical properties were analyzed to verify the prediction. Research shows that the influence of shared electron number nA on the strongest bond determines the strength of these alloys and the experiments are consistent with the theoretical prediction.
Determining and Controlling the Magnesium Composition in CdTe/CdMgTe Heterostructures
DOE Office of Scientific and Technical Information (OSTI.GOV)
LeBlanc, E. G.; Edirisooriya, M.; Ogedengbe, O. S.
The relationships between Mg composition, band gap, and lattice characteristics are investigated for Cd 1-xMg xTe barrier layers using a combination of cathodoluminescence, energy dispersive x-ray spectroscopy, variable angle spectral ellipsometry, and atom probe tomography. The use of a simplified, yet accurate, variable angle spectral ellipsometry analysis is shown to be appropriate for fast determination of composition in thin Cd 1-xMg xTe layers. The validity of using high-resolution x-ray diffraction for CdTe/Cd 1-xMg xTe double heterostructures is discussed. Furthermore, the stability of CdTe/Cd 1-xMg xTe heterostructures are investigated with respect to thermal processing.
DOE Office of Scientific and Technical Information (OSTI.GOV)
Roy, U. N.; Bolotnikov, A. E.; Camarda, G. S.
2015-02-01
We grew CdTe xSe 1-x crystals with nominal Se concentrations of 5%, 7%, and 10% by the vertical Bridgman technique, and evaluated their compositional homogeneity and structural quality at the NSLS’ X-ray fluorescence and white beam X-ray topography beam lines. Both X-ray fluorescence and photoluminescence mapping revealed very high compositional homogeneity of the CdTe xSe 1-x crystals. Here, we noted that those crystals with higher concentrations of Se were more prone to twinning than those with a lower content. The crystals were fairly free from strains and contained low concentrations of sub-grain boundaries and their networks.
LaCu 6-xAg x: A promising host of an elastic quantum critical point
DOE Office of Scientific and Technical Information (OSTI.GOV)
Poudel, Lekh; Dela Cruz, Clarina R.; Koehler, Michael R.
Structural properties of LaCu 6-xAg x have been investigated using neutron and x-ray diffraction, and resonant ultrasound spectroscopy (RUS) measurements. Diffraction measurements indicate a continuous structural transition from orthorhombic (Pnma) to monoclinic (P2₁/C) structure. RUS measurements show softening of natural frequencies at the structural transition, consistent with the elastic nature of the structural ground state. The structural transition temperatures in LaCu 6-xAg x decrease with Ag composition until the monoclinic phase is completely suppressed at x c=0.225. All of the evidence is consistent with the presence of an elastic quantum critical point in LaCu 6-xAg x.
1981-09-01
F6 .O...4X,F5.2,5X,F5 .2,SX,F6.3,4X,F8.6,2X,F8.6,2X,F7.3, Z5X,F5.1,4X,F5.2,3X,F7.2,4X, F6 .3, 4X , F6 .4) 340 FORMAT( F6 .O,F5.2,F5.2,F6.3,F8.6,F8.6,F7.3, ZF5. 1...New York NY 3 Data Courier Inc, Louisville Ky 40202 4 In Malaysia The Director, Defence Research Centre, Malaysia 5 In Australia Chief
Logistics and Maintenance Concepts for a Future Naval Force
2001-12-01
Co - opetition . Currency-Doubleday. Retrieved December 10, 2001 from...Navigation CND Can Not Duplicate CO Commanding Officer COMNAVAIRLANT Commander Naval Forces Atlantic COSAL Consolidated Ship Allowance List CPO...ra ul ic s C or ro si on , O pe ra tio na l f lig ht co nt ro ls de gr ad at io n W id es pr ea d W ir e D am ag e X X X X X X X X
NASA Astrophysics Data System (ADS)
Fokas, A. S.; Pogrebkov, A. K.
2003-03-01
We study the initial value problem of the Kadomtsev-Petviashvili I (KPI) equation with initial data u(x1,x2,0) = u1(x1)+u2(x1,x2), where u1(x1) is the one-soliton solution of the Korteweg-de Vries equation evaluated at zero time and u2(x1,x2) decays sufficiently rapidly on the (x1,x2)-plane. This involves the analysis of the nonstationary Schrödinger equation (with time replaced by x2) with potential u(x1,x2,0). We introduce an appropriate sectionally analytic eigenfunction in the complex k-plane where k is the spectral parameter. This eigenfunction has the novelty that in addition to the usual jump across the real k-axis, it also has a jump across a segment of the imaginary k-axis. We show that this eigenfunction can be reconstructed through a linear integral equation uniquely defined in terms of appropriate scattering data. In turn, these scattering data are uniquely constructed in terms of u1(x1) and u2(x1,x2). This result implies that the solution of the KPI equation can be obtained through the above linear integral equation where the scattering data have a simple t-dependence.
Compact x-ray source and panel
Sampayon, Stephen E [Manteca, CA
2008-02-12
A compact, self-contained x-ray source, and a compact x-ray source panel having a plurality of such x-ray sources arranged in a preferably broad-area pixelized array. Each x-ray source includes an electron source for producing an electron beam, an x-ray conversion target, and a multilayer insulator separating the electron source and the x-ray conversion target from each other. The multi-layer insulator preferably has a cylindrical configuration with a plurality of alternating insulator and conductor layers surrounding an acceleration channel leading from the electron source to the x-ray conversion target. A power source is connected to each x-ray source of the array to produce an accelerating gradient between the electron source and x-ray conversion target in any one or more of the x-ray sources independent of other x-ray sources in the array, so as to accelerate an electron beam towards the x-ray conversion target. The multilayer insulator enables relatively short separation distances between the electron source and the x-ray conversion target so that a thin panel is possible for compactness. This is due to the ability of the plurality of alternating insulator and conductor layers of the multilayer insulators to resist surface flashover when sufficiently high acceleration energies necessary for x-ray generation are supplied by the power source to the x-ray sources.
Wen, Shiya; Li, Miaozi; Yang, Junyu; Mei, Xianglin; Wu, Bin; Liu, Xiaolin; Heng, Jingxuan; Qin, Donghuan; Hou, Lintao; Xu, Wei; Wang, Dan
2017-11-08
CdSe x Te 1-x semiconductor nanocrystals (NCs), being rod-shaped/irregular dot-shaped in morphology, have been fabricated via a simple hot-injection method. The NCs composition is well controlled through varying molar ratios of Se to Te precursors. Through changing the composition of the CdSe x Te 1-x NCs, the spectral absorption of the NC thin film between 570-800 nm is proved to be tunable. It is shown that the bandgap of homogeneously alloyed CdSe x Te 1-x active thin film is nonlinearly correlated with the different compositions, which is perceived as optical bowing. The solar cell devices based on CdSe x Te 1-x NCs with the structure of ITO/ZnO/CdSe/CdSe x Te 1-x /MoO x /Au and the graded bandgap ITO/ZnO/CdSe( w / o )/CdSe x Te 1-x /CdTe/MoO x /Au are systematically evaluated. It was found that the performance of solar cells degrades almost linearly with the increase of alloy NC film thickness with respect to ITO/ZnO/CdSe/CdSe 0.2 Te 0.8 /MoO x /Au. From another perspective, in terms of the graded bandgap structure of ITO/ZnO/CdSe/CdSe x Te 1-x /CdTe/MoO x /Au, the performance is improved in contrast with its single-junction analogues. The graded bandgap structure is proved to be efficient when absorbing spectrum and the solar cells fabricated under the structure of ITO/ZnO/CdSe 0.8 Te 0.2 /CdSe 0.2 Te 0.8 /CdTe/MoO x /Au indicate power conversion efficiency (PCE) of 6.37%, a value among the highest for solution-processed inversely-structured CdSe x Te 1-x NC solar cells. As the NC solar cells are solution-processed under environmental conditions, they are promising for fabricating solar cells at low cost, roll by roll and in large area.
Precision, time, and cost: a comparison of three sampling designs in an emergency setting.
Deitchler, Megan; Deconinck, Hedwig; Bergeron, Gilles
2008-05-02
The conventional method to collect data on the health, nutrition, and food security status of a population affected by an emergency is a 30 x 30 cluster survey. This sampling method can be time and resource intensive and, accordingly, may not be the most appropriate one when data are needed rapidly for decision making. In this study, we compare the precision, time and cost of the 30 x 30 cluster survey with two alternative sampling designs: a 33 x 6 cluster design (33 clusters, 6 observations per cluster) and a 67 x 3 cluster design (67 clusters, 3 observations per cluster). Data for each sampling design were collected concurrently in West Darfur, Sudan in September-October 2005 in an emergency setting. Results of the study show the 30 x 30 design to provide more precise results (i.e. narrower 95% confidence intervals) than the 33 x 6 and 67 x 3 design for most child-level indicators. Exceptions are indicators of immunization and vitamin A capsule supplementation coverage which show a high intra-cluster correlation. Although the 33 x 6 and 67 x 3 designs provide wider confidence intervals than the 30 x 30 design for child anthropometric indicators, the 33 x 6 and 67 x 3 designs provide the opportunity to conduct a LQAS hypothesis test to detect whether or not a critical threshold of global acute malnutrition prevalence has been exceeded, whereas the 30 x 30 design does not. For the household-level indicators tested in this study, the 67 x 3 design provides the most precise results. However, our results show that neither the 33 x 6 nor the 67 x 3 design are appropriate for assessing indicators of mortality. In this field application, data collection for the 33 x 6 and 67 x 3 designs required substantially less time and cost than that required for the 30 x 30 design. The findings of this study suggest the 33 x 6 and 67 x 3 designs can provide useful time- and resource-saving alternatives to the 30 x 30 method of data collection in emergency settings.
1982-06-01
observation in our framework is the pair (y,x) with x considered given. The influence function for 52 at the Gaussian distribution with mean xB and variance...3/2 - (1+22)o2 2) 1+2x\\/2 x’) 2(3-9) (1+2X) This influence function is bounded in the residual y-xS, and redescends to an asymptote greater than...version of the influence function for B at the Gaussian distribution, given the x. and x, is defined as the normalized differenceJ (see Barnett and
2006-12-01
Undersea Warfare Commander VHF Very High Frequency VoIP Voice over Internet Protocol WCS Weapons...USN surface and undersea warfare, USN and USA communications and networking operations, and USAF acquisition and aircraft maintenance projects. In...kin g 1 x x BN -R EG T- BD E Co or di na tio n 1 x x x x Pr ov id in g Ba tte ry Ta sk in g, E ng ag e, C oo rd in at io n 1 1 x x x Pr ov id in
Diagnosability of Stochastic Chemical Kinetic Systems: A Discrete Event Systems Approach (PREPRINT)
2010-01-01
USA. E -mail: thorsley@u.washington.edu. This research is partially supported by the 2006 AFOSR MURI award “High Confidence Design for Distributed...occurrence of the finite sample path ω. These distributions are defined recursively to be π0(x) := π0(x), πωσ(x ′) := ∑ x∈X πω(x)r(x ′,σ | x) e −r(x ′,σ|x... e −rxτ . (2) This probability is this probability that the arrival time of the first event is greater than τ . For finite sample paths with strings
Electrical and structural properties of In-implanted Si 1–xGe x alloys
Feng, Ruixing; Kremer, F.; Sprouster, D. J.; ...
2016-01-14
Here, we report on the effects of dopant concentration and substrate stoichiometry on the electrical and structural properties of In-implanted Si 1–xGe x alloys. Correlating the fraction of electrically active In atoms from Hall Effect measurements with the In atomic environment determined by X-ray absorption spectroscopy, we observed the transition from electrically active, substitutional In at low In concentration to electrically inactive metallic In at high In concentration. The In solid-solubility limit has been quantified and was dependent on the Si 1–xGe x alloy stoichiometry; the solid-solubility limit increased as the Ge fraction increased. This result was consistent with densitymore » functional theory calculations of two In atoms in a Si 1–xGe x supercell that demonstrated that In–In pairing was energetically favorable for x ≲ 0.7 and energetically unfavorable for x ≳ 0.7. Transmission electron microscopy imaging further complemented the results described earlier with the In concentration and Si 1–xGe x alloy stoichiometry dependencies readily visible. We have demonstrated that low resistivity values can be achieved with In implantation in Si 1–xGe x alloys, and this combination of dopant and substrate represents an effective doping protocol.« less
Effect of cadmium incorporation on the properties of zinc oxide thin films
NASA Astrophysics Data System (ADS)
Bharath, S. P.; Bangera, Kasturi V.; Shivakumar, G. K.
2018-02-01
Cd x Zn1- x O (0 ≤ x ≤ 0.20) thin films are deposited on soda lime glass substrates using spray pyrolysis technique. To check the thermal stability, Cd x Zn1- x O thin films are subjected to annealing. Both the as-deposited and annealed Cd x Zn1- x O thin films are characterized using X-ray diffraction (XRD), scanning electron microscope (SEM) and energy-dispersive X-ray analysis (EDAX) to check the structural, surface morphological and compositional properties, respectively. XRD analysis reveals that the both as-deposited and annealed Cd x Zn1- x O thin films are (002) oriented with wurtzite structure. SEM studies confirm that as-deposited, as well as annealed Cd x Zn1- x O thin films are free from pinholes and cracks. Compositional analysis shows the deficiency in Cd content after annealing. Optical properties evaluated from UV-Vis spectroscopy shows red shift in the band gap for Cd x Zn1- x O thin films. Electrical property measured using two probe method shows a decrease in the resistance after Cd incorporation. The results indicate that cadmium can be successfully incorporated in zinc oxide thin films to achieve structural changes in the properties of films.
NASA Astrophysics Data System (ADS)
Selim, M. M.; Bezák, V.
2003-06-01
The one-dimensional version of the radiative transfer problem (i.e. the so-called rod model) is analysed with a Gaussian random extinction function (x). Then the optical length X = 0 Ldx(x) is a Gaussian random variable. The transmission and reflection coefficients, T(X) and R(X), are taken as infinite series. When these series (and also when the series representing T 2(X), T 2(X), R(X)T(X), etc.) are averaged, term by term, according to the Gaussian statistics, the series become divergent after averaging. As it was shown in a former paper by the authors (in Acta Physica Slovaca (2003)), a rectification can be managed when a `modified' Gaussian probability density function is used, equal to zero for X > 0 and proportional to the standard Gaussian probability density for X > 0. In the present paper, the authors put forward an alternative, showing that if the m.s.r. of X is sufficiently small in comparison with & $bar X$ ; , the standard Gaussian averaging is well functional provided that the summation in the series representing the variable T m-j (X)R j (X) (m = 1,2,..., j = 1,...,m) is truncated at a well-chosen finite term. The authors exemplify their analysis by some numerical calculations.
Enhanced Photocatalytic Activity in Bi1-x Ba x FeO3 Prepared by a PEG400 Assisted Sol-Gel Method
NASA Astrophysics Data System (ADS)
Zhang, Chenlan; Chen, Jianguo; Jin, Dengren; Cheng, Jinrong
2018-03-01
Ferroelectric Bi1-x Ba x FeO3 nanoparticles for x = 0, 0.01, 0.03, 0.05 and 0.10 were synthesized by a polyethylene glycol 400 (PEG400) assisted sol-gel method. X-ray diffraction reveals that Bi1-x Ba x FeO3 nanoparticles exhibit a distorted rhombohedral structure with the R3c space group, and the diffraction peaks shift upon incorporation of Ba. Transmission electron microscope analysis shows that the particle size of Bi1-x Ba x FeO3 nanoparticles is in the range of 30-60 nm, decreasing with an increase in Ba content. Bi1-x Ba x FeO3 nanoparticles have band gaps in the range of 1.68-2.0 eV, which are capable of responding to visible light irradiation. The rate of the photocatalytic degradation of Bi1-x Ba x FeO3 nanoparticles for x = 0.03 to methyl orange (MO) dye achieves about 81% under visible light irradiation for 3 h, which is higher than that of 66% for pure phase BiFeO3 (BFO). Moreover, the effects of Ba2+ modification on the band gap of BFO crystallites have been investigated and discussed.
Ho, Kristen K K; Deakin, Janine E; Wright, Megan L; Graves, Jennifer A Marshall; Grützner, Frank
2009-01-01
A common theme in the evolution of sex chromosomes is the massive loss of genes on the sex-specific chromosome (Y or W), leading to a gene imbalance between males (XY) and females (XX) in a male heterogametic species, or between ZZ and ZW in a female heterogametic species. Different mechanisms have evolved to compensate for this difference in dosage of X-borne genes between sexes. In therian mammals, one of the X chromosomes is inactivated, whereas bird dosage compensation is partial and gene-specific. In therian mammals, hallmarks of the inactive X are monoallelic gene expression, late DNA replication and chromatin condensation. Platypuses have five pairs of X chromosomes in females and five X and five Y chromosomes in males. Gene expression analysis suggests a more bird-like partial and gene-specific dosage compensation mechanism. We investigated replication timing and chromosome condensation of three of the five X chromosomes in female platypus. Our data suggest asynchronous replication of X-specific regions on X(1), X(3) and X(5) but show significantly different condensation between homologues for X(3) only, and not for X(1) or X(5). We discuss these results in relation to recent gene expression analysis of X-linked genes, which together give us insights into possible mechanisms of dosage compensation in platypus.
NASA Astrophysics Data System (ADS)
Yuan, Lei; Zhang, Hongpeng; Jia, Renxu; Guo, Lixin; Zhang, Yimen; Zhang, Yuming
2018-03-01
Energy band alignments between series band of Al-rich high-k materials (HfO2)x(Al2O3)1-x and β-Ga2O3 are investigated using X-Ray Photoelectron Spectroscopy (XPS). The results exhibit sufficient conduction band offsets (1.42-1.53 eV) in (HfO2)x(Al2O3)1-x/β-Ga2O3. In addition, it is also obtained that the value of Eg, △Ec, and △Ev for (HfO2)x(Al2O3)1-x/β-Ga2O3 change linearly with x, which can be expressed by 6.98-1.27x, 1.65-0.56x, and 0.48-0.70x, respectively. The higher dielectric constant and higher effective breakdown electric field of (HfO2)x(Al2O3)1-x compared with Al2O3, coupled with sufficient barrier height and lower gate leakage makes it a potential dielectric for high voltage β-Ga2O3 power MOSFET, and also provokes interest in further investigation of HfAlO/β-Ga2O3 interface properties.
Magnetic phase transitions and magnetic structures in RTxX2, RSn1+xGe1-x and RSn2 compounds
NASA Astrophysics Data System (ADS)
Gil, Alina
2018-02-01
The work presents the review of magnetic properties of the RTxX2, RSn1+xGe1-x and RSn2 compounds. The RTxX2 (where R - rare earth, T - 3d-metal, X - p-electron element: Si, Ge, Sn, and 1 ≥ x > 0) and RSn1+xGe1-x compounds (where x ≈ 0.1) crystallize in the orthorhombic crystal structure of CeNiSi2-type and RSn2 compounds crystallize in ZrSi2-type structure. Both structures are described by the space group Cmcm. The RSn1+xGe1-x compounds seem to be interesting due to the replacement of d-metal to p-electron element. The non-stoichiometric CeNiSi2-type of RTxX2 compounds may be regarded as partially filled ZrSi2-type compounds. The transitions from paramagnetic to antiferromagnetic or ferromagnetic states are observed at low temperatures and there are lots of variants of magnetic structures ranging from simple collinear to the sine-modulated structures with commensurate or incommensurate propagation vector. The comparison of magnetic properties of these compounds may help to find answers to questions concerning mechanisms of interaction between the magnetic moments.
BEaTriX, expanded x-ray beam facility for testing modular elements of telescope optics: an update
NASA Astrophysics Data System (ADS)
Pelliciari, C.; Spiga, D.; Bonnini, E.; Buffagni, E.; Ferrari, C.; Pareschi, G.; Tagliaferri, G.
2015-09-01
We present in this paper an update on the design of BEaTriX (Beam Expander Testing X-ray facility), an X-ray apparatus to be realized at INAF/OAB and that will generate an expanded, uniform and parallel beam of soft X-rays. BEaTriX will be used to perform the functional tests of X-ray focusing modules of large X-ray optics such as those for the ATHENA X-ray observatory, using the Silicon Pore Optics (SPO) as a baseline technology, and Slumped Glass Optics (SGO) as a possible alternative. Performing the tests in X-rays provides the advantage of an in-situ, at-wavelength quality control of the optical modules produced in series by the industry, performing a selection of the modules with the best angular resolution, and, in the case of SPOs, there is also the interesting possibility to align the parabolic and the hyperbolic stacks directly under X-rays, to minimize the aberrations. However, a parallel beam with divergence below 2 arcsec is necessary in order to measure mirror elements that are expected to reach an angular resolution of about 4 arcsec, since the ATHENA requirement for the entire telescope is 5 arcsec. Such a low divergence over the typical aperture of modular optics would require an X-ray source to be located in a several kilometers long vacuum tube. In contrast, BEaTriX will be compact enough (5 m x 14 m) to be housed in a small laboratory, will produce an expanded X-ray beam 60 mm x 200 mm broad, characterized by a very low divergence (1.5 arcsec HEW), strong polarization, high uniformity, and X-ray energy selectable between 1.5 keV and 4.5 keV. In this work we describe the BEaTriX layout and show a performance simulation for the X-ray energy of 4.5 keV.
Superconductivity in layered ZrP2-x Se x with PbFCl-type structure
NASA Astrophysics Data System (ADS)
Ishida, Shigeyuki; Fujihisa, Hiroshi; Hase, Izumi; Yanagi, Yousuke; Kawashima, Kenji; Oka, Kunihiko; Gotoh, Yoshito; Yoshida, Yoshiyuki; Iyo, Akira; Eisaki, Hiroshi; Kito, Hijiri
2016-05-01
We performed a systematic study of the crystal structure, physical properties, and electronic structure of PbFCl-type ZrP2-x Se x (0.3 ≤ x ≤ 0.9). We successfully synthesized single-phase polycrystalline samples for the Se substitution range of 0.4 ≤ x ≤ 0.8. The crystal structure of the compound is characterized by the alternate stacking of a two-dimensional P square net and a Zr-(P1-x Se x ) network. ZrP2-x Se x exhibits a dome-like superconductivity phase diagram and has a maximum superconducting transition temperature (T c) of 6.3 K for x ≈ 0.6. Resistivity and Hall measurements indicated that electron-phonon scattering plays a dominant role and that electron-type carriers dominate charge transport. Specific heat measurements confirmed that ZrP2-x Se x exhibits bulk superconductivity. Further, the value of the specific heat jump at T c (ΔC/γT c ≈ 1.35) is in keeping with the BCS weak-coupling model. These facts suggest a rather conventional pairing mechanism in ZrP2-x Se x . The x dependence of T c can be explained on the basis of the density of states (DOS) for x ≤ 0.7, whereas the decrease in T c with an increase in the DOS for x = 0.8 needs further investigation. One possible reason for the suppression of superconductivity is that the PbFCl-type structure becomes unstable for x ≥ 0.8. The results of electronic structure calculations agree reasonably well with those of the experimental observations, suggesting that the Zrd band plays a primary role in determining the physical properties. Further, the calculations predict a significant change in the Fermi-surface topology for x ≥ 0.8 this is a probable reason for the decrease in T c as well as the instability of the PbFCl-type structure.
DOE Office of Scientific and Technical Information (OSTI.GOV)
Nie, Xiaomeng; Guo, Yongquan
2016-01-15
The structures and optical and electric properties of europium doped CuIn{sub 1−x}Eu{sub x}Te{sub 2} have been studied systematically using powder X-ray diffraction (XRD), scanning electron microscopy (SEM) with energy dispersive spectrum (EDS), ultraviolet and visible spectrophotometer (UV–vis), and standard four-probe method. The studies reveal that the minor europium doping into CuIn{sub 1−x}Eu{sub x}Te{sub 2} could still stabilize the chalcopyrite structure in a solid solution of x=0.1. The lattice parameters are going up with increasing the content of europium in CuIn{sub 1−x}Eu{sub x}Te{sub 2} due to the size effect at In site. The structural refinement confirms that Eu partly substitutes formore » In and occupies the 4b crystal position. SEM morphologies show that the europium doping into CuIn{sub 1−x}Eu{sub x}Te{sub 2} can fine the grains from the largely agglomerated state to the uniformly separated state. The electrical resistivities of single phase CuIn{sub 1−x}Eu{sub x}Te{sub 2} follow a mixture model of hopping conductivity and variable range hopping conductivity. The absorption band-gaps of CuIn{sub 1−x}Eu{sub x}Te{sub 2} at room temperature tend to increase with increasing Eu content. CuIn{sub 1−x}Eu{sub x}Te{sub 2} might be a good candidate for photovoltaic cell. - Graphical abstract: CuIn{sub 0.9}Eu{sub 0.1}Te{sub 2} follows a mixture of hopping conductivity and variable range hopping conductivity mechanism. - Highlights: • Novel europium doped CuIn{sub 1−x}Eu{sub x}Te{sub 2}. • Potential application for devices and solar cells. • A mixture of hopping and variable range hopping conductivity mechanism.« less
Liu, Qing; Zhu, Hai-Yan; Liu, Fang; Ding, Zi-Yuan
2011-11-01
A laboratory test was conducted to study the effects of different temperature and salinity on the oxygen consumption rate and asphyxiation point of chaetognath Sagitta crassa. Both temperature and salinity had significant effects on the oxygen consumption rate (IO) and specific oxygen consumption rate (SO) of S. crassa. When the temperature raised from 5 degrees C to 25 degrees C, the IO and SO of S. crassa increased first, and then presented an obvious decreasing trend, with the regression function being y = 0.0058x3-0.2956x2 +4.415x-8.7816 (R2 = 0.99, P < 0.05) for IO and y = 0.0011x3-0.0546x2+0.8161x-1.6232 (R2 = 0.99, P < 0.05) for SO. The IO and SO at different temperature were in the ranges of 6.30-11.71 microg x ind(-1) x h(-1) and 1.22-2.16 microg x mg(-1) x h(-1), respectively, and the asphyxiation point was 4.18-6.87 mg x L(-1). When the salinity increased from 10 to 40, the IO and SO of S. crassa decreased gradually, with the regression function being y = -0.0068x2-0.1412x+21.702 (R2 = 0.89, P < 0.05) for IO and y = -0.0013x2 -0.0261x+ 4.0114 (R2 = 0.89, P < 0.05) for SO. The IO and SO at different salinity were in the ranges of 4.98-17.73 microg x ind(-1) x h(-1) and 0.92-3.56 microg x mg(-1) x h(-1), respectively, and the asphyxiation point was 4.02-6.24 mg x L(-1). Based on the differences in the oxygen consumption rate and asphyxiation point between S. crassa and other aquatic animals, it was concluded that S. crassa was a stenooxybiotic zooplankton species.
X-RAY DATA BOOKLET Center for X-ray Optics and Advanced Light Source Lawrence Berkeley National Laboratory Introduction X-Ray Properties of Elements Electron Binding Energies X-Ray Energy Emission Energies Table of X-Ray Properties Synchrotron Radiation Characteristics of Synchrotron Radiation History of X
Long Non-coding RNAs in the X-inactivation Center
Kalantry, Sundeep
2014-01-01
The X-inactivation center is a hotbed of functional long non-coding RNAs in eutherian mammals. These RNAs are thought to help orchestrate the epigenetic transcriptional states of the two X-chromosomes in females as well as of the single X-chromosome in males. To balance X-linked gene expression between the sexes, females undergo transcriptional silencing of most genes on one of the two X-chromosomes in a process termed X-chromosome inactivation. While one X-chromosome is inactivated, the other X-chromosome remains active. Moreover, with a few notable exceptions, the originally established epigenetic transcriptional profiles of the two is maintained as such through many rounds of cell division, essentially for the life of the organism. The stable divergent transcriptional fates of the two X-chromosomes, despite residing in a shared nucleoplasm, make X-inactivation a paradigm of epigenetic transcriptional regulation. Originally proposed in 1961 by Mary Lyon, the X-inactivation hypothesis has been validated through much experimentation over the last fifty years. In the last 25 years, the discovery and functional characterization has firmly established X-linked long non-coding RNAs as key players in choreographing X-chromosome inactivation. PMID:24297756
Crystal growth of magnetic dihydride GdxY1-xH2 for generation of spin current
NASA Astrophysics Data System (ADS)
Sakuraba, T.; Hirama, H.; Sakai, M.; Honda, Z.; Hayakawa, M.; Okoshi, T.; Kitajima, A.; Oshima, A.; Higuchi, K.; Hasegawa, S.
2013-09-01
Crystal growth of pure phases of GdxY1-xH2 (0≤x≤1) was successfully carried out by depositing GdxY1-x films and their hydrogenation, the growth results of which were investigated by X-ray diffraction measurements as well as temperature (T) dependence of magnetic susceptibility (χ). The fcc lattice constant in GdxY1-xH2 is found to be linearly increased with increasing x. Behavior characteristic to the para-to-antiferromagnetic transition are clearly observed in the χ-T curve for x=0.39, 0.47, 0.76, and 1.0 cases. The Néel temperature (TN) is found to be linearly decreased with decreasing x from x=1.0 (GdH2), and is predicted to show TN=0 K at x˜0.1 by extrapolating TN from large x region, implying the antiferromagnetic order disappears at x˜0.1. The quasi-zero Hall effect was observed for x=0, 0.19, 0.37, 0.39, and 0.47 cases, whereas a moderate Hall effect is observed for x=0.76 and 1.0 cases. The type of Hall effect is also discussed.
DOE Office of Scientific and Technical Information (OSTI.GOV)
Wang, Wei; Zhou, Qian; Dong, Yuan
We investigated the critical thickness (h{sub c}) for plastic relaxation of Ge{sub 1−x}Sn{sub x} grown by molecular beam epitaxy. Ge{sub 1−x}Sn{sub x} films with various Sn mole fraction x (x ≤ 0.17) and different thicknesses were grown on Ge(001). The strain relaxation of Ge{sub 1−x}Sn{sub x} films and the h{sub c} were investigated by high-resolution x-ray diffraction and reciprocal space mapping. It demonstrates that the measured h{sub c} values of Ge{sub 1−x}Sn{sub x} layers are as much as an order of magnitude larger than that predicted by the Matthews and Blakeslee (M-B) model. The People and Bean (P-B) model was also usedmore » to predict the h{sub c} values in Ge{sub 1−x}Sn{sub x}/Ge system. The measured h{sub c} values for various Sn content follow the trend, but slightly larger than that predicted by the P-B model.« less
NASA Technical Reports Server (NTRS)
Gangi, A. F.
1978-01-01
The data from the Apollo-14 and Apollo-16 Active Seismic Experiments were reanalyzed and show that a power-law velocity variation with depth is consistent with both the traveltimes and amplitudes of the first arrivals for source-to-geophone separations up to 32m. The data were improved by removing spurious glithches, flickering and stacking. While this improved the signal-to-noise ratios, it was not possible to measure the arrivals beyond 32m. The physical evidence that the shallow lunar regolith is made up of fine particles adds weight to the 1/6-power velocity model. The 1/6-power law predicts the traveltime t(x), varies with separation, x, as t(x) = t sub 0 (x/x sub 0) to the 5/6 power and, using a first-order theory, the amplitude, A(x), varies as A(x) = A sub 0 (x/x sub 0) to the (13-m)/12, M 1; the layer-velocity model predicts t(x) = t sub 0 (x/xsub 0) and A(x) = A sub 0 (x/x sub 0) to the 2nd power.
EXTREME ULTRAVIOLET EXPLORER OBSERVATIONS OF HERCULES X-1 OVER A 35 DAY CYCLE
DOE Office of Scientific and Technical Information (OSTI.GOV)
Leahy, D. A.; Dupuis, Jean, E-mail: leahy@ucalgary.c
2010-06-01
Observations of Hercules X-1 by the Extreme Ultraviolet Explorer covering most of the 35 day cycle are reported here. This is the only long extreme ultraviolet (EUV) observation of Her X-1. Simultaneous X-ray observations with the Rossi X-ray Timing Explorer All-Sky Monitor (RXTE/ASM) X-ray show that Her X-1 is in an X-ray anomalous low state. The first 4 days are also observed with the RXTE proportional counter array (PCA), which shows that the X-ray properties are nearly the same as for normal low states in Her X-1 with flux reduced by a factor of 2. In contrast, the EUV emissionmore » from Her X-1 is reduced by a factor of {approx}4 compared to normal low states. The twisted-tilted accretion disk responsible for the normal 35 day X-ray cycle can be modified to explain this behavior. An increased disk twist reduces the X-ray illumination of HZ Her by a factor of {approx}2 and of the disk surface by a somewhat larger factor, leading to a larger reduction in EUV flux compared to X-ray flux.« less
NASA Astrophysics Data System (ADS)
Sorokin, N. I.; Krivandina, E. A.; Zhmurova, Z. I.
2013-11-01
The density of single crystals of nonstoichiometric phases Ba1 - x La x F2 + x (0 ≤ x ≤ 0.5) and Sr0.8La0.2 - x Lu x F2.2 (0 ≤ x ≤ 0.2) with the fluorite (CaF2) structure type and R 1 - y Sr y F3 - y ( R = Pr, Nd; 0 ≤ y ≤ 0.15) with the tysonite (LaF3) structure type has been measured. Single crystals were grown from a melt by the Bridgman method. The measured concentration dependences of single crystal density are linear. The interstitial and vacancy models of defect formation in the fluorite and tysonite phases, respectively, are confirmed. To implement the composition control of single crystals of superionic conductors M 1 - x R x F2 + x and R 1 - y M y F3 - y in practice, calibration graphs of X-ray density in the MF2- RF3 systems ( M = Ca, Sr, Ba, Cd, Pb; R = La-Lu, Y) are plotted.
Khan, Mahmud; Mudryk, Ya.; Gschneidner, K. A.; ...
2011-12-27
HoAl₂ exhibits a first-order spin reorientation transition at 20 K, which is manifested as a sharp peak in the heat capacity. When Ho is partially replaced by only 5% of Tb, the sharp heat-capacity peak in Ho 1-xTb xAl₂ (x = 0.05) disappears, and then reappears again for x ≥ 0.07. For x = 0.05, the anomaly corresponding to the spin reorientation transition is barely seen in the heat capacity, but as x exceeds 0.07 the weak anomaly transforms to a sharp peak. The spin reorientation transition temperature increases to 29 K for x = 0.05, and as x increasesmore » further the transition shifts to lower temperature and returns to ~20 K for x = 0.25. The transition is no longer observed when x exceeds 0.60. Temperature-dependent x-ray powder-diffraction data confirm the first-order nature of the spin reorientation transition for the alloy with x = 0.40, and indicate that the compound retains the room-temperature cubic structure within the sensitivity of the technique. Experimental observations are discussed considering the easy magnetization directions of HoAl₂ and TbAl₂.« less
Zhao, Guijuan; Li, Huijie; Wang, Lianshan; Meng, Yulin; Ji, Zesheng; Li, Fangzheng; Wei, Hongyuan; Yang, Shaoyan; Wang, Zhanguo
2017-07-03
In this study, the indium composition x as well as the anisotropically biaxial strain in non-polar a-plane In x Ga 1-x N on GaN is studied by X-ray diffraction (XRD) analysis. In accordance with XRD reciprocal lattice space mapping, with increasing indium composition, the maximum of the In x Ga 1-x N reciprocal lattice points progressively shifts from a fully compressive strained to a fully relaxed position, then to reversed tensile strained. To fully understand the strain in the ternary alloy layers, it is helpful to grow high-quality device structures using a-plane nitrides. As the layer thickness increases, the strain of In x Ga 1-x N layer releases through surface roughening and the 3D growth-mode.
Hetero-site-specific X-ray pump-probe spectroscopy for femtosecond intramolecular dynamics
Picón, A.; Lehmann, C. S.; Bostedt, C.; Rudenko, A.; Marinelli, A.; Osipov, T.; Rolles, D.; Berrah, N.; Bomme, C.; Bucher, M.; Doumy, G.; Erk, B.; Ferguson, K. R.; Gorkhover, T.; Ho, P. J.; Kanter, E. P.; Krässig, B.; Krzywinski, J.; Lutman, A. A.; March, A. M.; Moonshiram, D.; Ray, D.; Young, L.; Pratt, S. T.; Southworth, S. H.
2016-01-01
New capabilities at X-ray free-electron laser facilities allow the generation of two-colour femtosecond X-ray pulses, opening the possibility of performing ultrafast studies of X-ray-induced phenomena. Particularly, the experimental realization of hetero-site-specific X-ray-pump/X-ray-probe spectroscopy is of special interest, in which an X-ray pump pulse is absorbed at one site within a molecule and an X-ray probe pulse follows the X-ray-induced dynamics at another site within the same molecule. Here we show experimental evidence of a hetero-site pump-probe signal. By using two-colour 10-fs X-ray pulses, we are able to observe the femtosecond time dependence for the formation of F ions during the fragmentation of XeF2 molecules following X-ray absorption at the Xe site. PMID:27212390
Hetero-site-specific X-ray pump-probe spectroscopy for femtosecond intramolecular dynamics.
Picón, A; Lehmann, C S; Bostedt, C; Rudenko, A; Marinelli, A; Osipov, T; Rolles, D; Berrah, N; Bomme, C; Bucher, M; Doumy, G; Erk, B; Ferguson, K R; Gorkhover, T; Ho, P J; Kanter, E P; Krässig, B; Krzywinski, J; Lutman, A A; March, A M; Moonshiram, D; Ray, D; Young, L; Pratt, S T; Southworth, S H
2016-05-23
New capabilities at X-ray free-electron laser facilities allow the generation of two-colour femtosecond X-ray pulses, opening the possibility of performing ultrafast studies of X-ray-induced phenomena. Particularly, the experimental realization of hetero-site-specific X-ray-pump/X-ray-probe spectroscopy is of special interest, in which an X-ray pump pulse is absorbed at one site within a molecule and an X-ray probe pulse follows the X-ray-induced dynamics at another site within the same molecule. Here we show experimental evidence of a hetero-site pump-probe signal. By using two-colour 10-fs X-ray pulses, we are able to observe the femtosecond time dependence for the formation of F ions during the fragmentation of XeF2 molecules following X-ray absorption at the Xe site.
NASA Astrophysics Data System (ADS)
Brown, Francisco; Jacobo-Herrera, Ivan; Alvarez-Montaño, Victor; Kimizuka, Noboru; Kurashina, Keiji; Michiue, Yuichi; Matsuo, Yoji; Mori, Shigeo; Ikeda, Naoshi; Medrano, Felipe
2017-07-01
Phase relations in the pseudo-binary systems RFeO3-R2Ti2O7 (R: Lu, Ho and Dy), RGaO3-R2Ti2O7 (R: Lu and Er), LuAlO3-Lu2Ti2O7 and RAO3-R2Ti2O7 (R: Lu and Yb. A: Cr and Mn) at elevated temperatures in air were determined by means of a classic quenching method. There exist Lu(Fe1-xTix)O3+x/2, R(Ga1-xTix)O3+x/2 (R: Lu and Er) and Lu(Al1-xTix)O3+x/2 (2/3≤ x≤3/4) having the Yb(Fe1-xTix)O3+x/2-type of crystal structure (x=0.72, space group: R3m, a(Å)=17.9773 and c(Å)=16.978 as a hexagonal setting) in these pseudo binary systems. Eighteen compounds R(A1-xTix)O3+x/2 (R: Lu-Sm and Y, A: Fe, Ga and Al) were newly synthesized and their lattice constants as a hexagonal setting were measured by means of the X-ray powder diffraction method. The R occupies the octahedral site and both A and Ti does the trigonalbipyramidal one in these compounds. Relation between lattice constants for the rhombic R(A1-xTix)O3+x/2 and the monoclinic In(A1-xTix)O3+x/2 are as follows, ah≈5 x bm, ch≈3 x cm x sin β and am=31/2 x bm, where ah and ch are the lattice constants as a hexagonal setting for R(A1-xTix)O3+x/2 and am, bm, cm and β are those of the monoclinic In(A1-xTix)O3+x/2. Crystal structural relationships among α-InGaO3 (hexagonal, high pressure form, space group: P63/mmc), InGaO3 (rhombic, hypothetical), (RAO3)n(BO)m and RAO3(ZnO)m (R: Lu-Ho, Y and In, A: Fe, Ga, and Al, B: divalent cation element, m, n: natural number), the orthorhombic-and monoclinic In(A1-xTix)O3+x/2 (A: Fe, Ga, Al, Cr and Mn) and the hexagonal-and rhombic R(A1-xTix)O3+x/2 (R: Lu-Sm and Y, A: Fe, Ga and Al) are schematically presented. We concluded that the crystal structures of both the α-InGaO3 (high pressure form, hexagonal, space group: P63/mmc) and the hypothetical InGaO3 (rhombic) are the key structures for constructing the crystal structures of these compounds having the cations with CN=5.
DOE Office of Scientific and Technical Information (OSTI.GOV)
Manigandan, D; Kumar, M; Mohandas, P
Purpose: To study the impact of different photon beam combination during VMAT planning and treatment delivery. Methods: Five prostate patients with no nodal involvement were chosen for the study and only prostate was considered as target (7920cGy/44fractions). In each case, three different VMAT plans were generated with two arcs (200°–160°&160°–200°). First plan used only 6MV in both arcs (6X-6X) and second utilized 6MV&15MV (6X-15X), whereas third one used 15MV&15MV (15X-15X). For consistency, all the plans were generated by the same planner using Monaco− treatment planning system (V5.1) for Elekta Synergy− linear accelerator with 1cm leaf-width. For plan comparison, target meanmore » dose, conformity index (CI)=Planning target volume (PTV) covered by 95% of prescription dose/PTV were analyzed. Mean doses of bladder, rectum, left femur and right femur were analyzed. Integral dose (liter-Gray) to normal tissue (patient volume minus PTV), total monitor unit (MU) required to deliver a plan and gamma pass rate for each plan was analyzed. Results: The CI for PTV was 0.9937±0.0037, 0.9917±0.0033, and 0.9897±0.0048 for 6X-6X, 6X-15X and 15X-15X, respectively. Mean dose to target slightly increases with the decrease of energy. Mean doses to bladder were 3546.23±692.13cGy, 3487.43±715.53cGy and 3504.40±683.1cGy for 6X-6X, 6X-15X and 15X-15X, respectively. Mean doses to rectum were 4294.60±309.5cGy, 4277.07±279.93cGy and 4290.77±379.07cGy. Mean doses to left femur were 2737.13±545.93cGy, 2668.67±407.12cGy and 2416.77±300.73cGy and mean doses to the right femur were 2682.70±460.81cGy, 2722.58±541.92cGy and 2598.57±481.83cGy. Higher Integral doses to normal tissue observed for 6X-6X (163.06±24.6 Litre-Gray) followed by 6X-15X (154.35±24.74 Litre-Gray) and 15X-15X (145.84±26.03 Litre-Gray). Average MU required to deliver one fraction was 680.75±72.09, 634.81±95.07 and 605.06±114.65. Gamma pass rates were 99.83±0.21, 99.53±0.27 and 99.2±0.20. Conclusion: 6X-15X VMAT plan offer dosimetric advantage compared to 6X-6X in terms of lesser MU and integral dose without significant compromise in plan quality, where as in 15X-15X, neutron contamination risk is relatively higher.« less
Fernández-Anca, Damián; García-Seijo, M Inés; García-Fernández, M Esther
2013-07-28
The reactivity of the unusual d(8) trigonal-bipyramidal systems [MX(PP3)]X (X = Cl: M = Pd(1a), Pt(2a); X = Br: M = Pd(3a), Pt(4a); X = I: M = Pd(5a), Pt(6a); PP3 = tris[2-(diphenylphosphino)ethyl]phosphine) in CHCl3-CH3OH, the square-pyramidal compounds [MCl(NP3)]Cl (M = Pd(7a); Pt(8a); NP3 = tris[2-(diphenylphosphino)ethyl]amine) in CD3OD-DMF and the distorted square-planar mononuclear [MX(PNP)]X (M = Pd: X = Cl(10a); M = Pt: X = I(10b); PNP = bis[2-(diphenylphosphino)ethyl]amine) and the heteronuclear [PdAu2X4(PP3)] [X = I(9a), Cl(14a), Br(15a)] and [MAuX2(PP3)]X [M = Pd: X = Cl(16a); M = Pt: X = Cl(17a), Br(18a)] species in CDCl3 with PPh3 + SnX2 has been explored to establish the factors that influence the nature of the products. With the mononuclear precursors the course of the reaction is strongly dependent on the tripodal or linear arrangement of the polydentate ligand and in the former case on the halogen. Thus, while for chlorides (1a-2a, 7a-8a) and bromides (3a-4a) the reaction led to the trigonal-bipyramidal compounds [M(SnCl3)(AP3)][SnCl3] [A = P: M = Pd(1), Pt(2); A = N: M = Pd(7), Pt(8)], [MBr(PP3)][SnBr3] [M = Pd(4), Pt(6)] containing M-Sn and M-Br bonds, respectively, for iodides (5a-6a) resulted in the unknown neutral square-planar compounds [MI2(PP(PO)2)(SnI2)2] [M = Pd(9) and Pt(10)] bearing two dangling P=O-SnI2 units and P2MI2 environments. However, complexes of the type [PtCl(PP2PO)X]X' [X = SnCl2, X' = [SnCl3](-)(11)] and [M(PP(PO)2)2X4]X'2 [X = SnCl2, X' = [SnCl3](-): M = Pd(12), Pt(13)] showing P=O-SnCl2 arms were obtained by direct reaction of [PtCl(PP2PO)]Cl (11a) and [M(PP(PO)2)2]Cl2 [M = Pd(12a), Pt(13a)] with SnCl2 in CH3OH. Although complex 9 was also prepared by interaction of the heteronuclear iodide 9a with PPh3 + SnI2 in CDCl3, the use of the neutral and ionic heteronuclear chlorides and bromides (14a-18a) as starting materials afforded the distorted square-planar ionic systems [MAuX'(PP3)(PPh3)][SnX3]2 [M = Pd: X = Cl, X' = SnCl3(-)(14); X = Br, X' = SnBr3(-)(15); M = Pt: X = Cl, X' = SnCl3(-)(17); X = Br, X' = SnBr3(-)(18)] containing M-SnX3 and P-Au-PPh3 functionalities. It was found that these reactions where the heteronuclear species are the precursors proceed via the trigonal-bipyramidal halides not only with X = Cl and Br(1a-4a) but also I(5a). When the precursors were 10a and 10b the reaction occurred with formation of [Pd(PNP)(PPh3)][SnCl3]2 (23) and [Pt(PNP)(PPh3)][SnCl2I]2 (24) showing M-PPh3 units and trihalostannato counter anions.
Vertebral radiography; X-ray - spine; Thoracic x-ray; Spine x-ray; Thoracic spine films; Back films ... The test is done in a hospital radiology department or in the health care provider's office. You will lie on the x-ray table in different positions. If the x-ray ...
USAF 1990 Research Initiation Program. Volume 3
1992-06-25
the reinforcement outward, both on the entrance and exit sides. The reinforcement was bent outward like a membrane under internal prressure. This led...potential of a neuron. C: cell capacitance. R: membrane resistance. w: synaptic weight. h(x): sigmoidal function describing the firing rate. y: external...Proof: The uncertain closed loop plant may be written as x(t)=(A+AA)x(t)+(Ao+ AAo )x(t-T) (B+AB)F(C AC)x(t) =(A+BFC)x(t)+(AA+ABFC+BFAC+ABFAC)x(t)+(Ao+Ao)X(t
Frederick Green; Rachel A. Arango; Stan T. Lebow
2010-01-01
Field trials were designed to evaluate the ability of the experimental wood preservative NâN-naphthaloylhydroxylamine (NHA) to inhibit fungal decay and termite damage at the USDA Harrison Experimental Forest (HEF) in Saucier, MS. Twenty replicate 19 x 19 x 457 mm (0.75 x 0.75 x 18 in.) southern yellow pine stakes and 10 replicate 19 x 19 x 76 mm (0.75 x 0.75 x 3 in.)...
Observations of Near-Bottom Flow in a Wave-Dominated Nearshore Environment.
1994-02-01
E 0 0 0 ~- X : (- 1.. pI m~ ffm ~o .pcr onf> ..... X • -- E X/• x,. "£ "*.. . .. . 0o 0 0 a c c ,(s0wO) (S/PH w) (SlUwo) . 7109 I 3 I Mean of LDV...1 I 8250 ASM X,ANDA #&HBF :REM 0000 OXXX ACCA 8260 ASM X,ANDB #&HBF :REM 0000 1XXX ACCB 8270 ASM X,STAB &H17 :REM /CS=0 3 8280 ASM X,STAA &H17 :REM
User’s Manual for Strategic Satellite System Terminal Segment Life Cycle Cost Model. Volume 2
1981-03-01
BASE TO/38X,15HDEPOT IN MONTHS,35X,F15.3/28X,55H + OSTC - ORDER AND SHIPPING TIME FROM A SATELLITE BASE/38X,26HT0 I +TS CIMP BASE IN MONTHS,24X,F15.3...COST OF PACKING AND SHIP +PING FROM A SATELLITE/38X,47HBASE TO ITS CIMP BASE IN $ PER NET WE +IGHT POUND,3X,F15.3/28X,54HCPPDC1) -COST OF PACKING AND
Direct Studies of Fracture Mechanisms in Metals at Highest Magnification.
1982-05-01
high speed optical cinema - tography. This technique records the spreading of a crack as seen on the surface of a metal with a resolution of a few...In WA MA a. E-4 ->-O zLi .1 x x fnH 0. w Vr ’=4 >_ _4__ ____ 0.tox x 0 a0 ’U(A.~ ~ ~ XX of 4. 1cn ti _ _ _ _ H toEW X) r4 x U 41 $4 > 4J 0 4 x x x
SphinX: The Solar Photometer in X-Rays
NASA Astrophysics Data System (ADS)
Gburek, Szymon; Sylwester, Janusz; Kowalinski, Miroslaw; Bakala, Jaroslaw; Kordylewski, Zbigniew; Podgorski, Piotr; Plocieniak, Stefan; Siarkowski, Marek; Sylwester, Barbara; Trzebinski, Witold; Kuzin, Sergey V.; Pertsov, Andrey A.; Kotov, Yurij D.; Farnik, Frantisek; Reale, Fabio; Phillips, Kenneth J. H.
2013-04-01
Solar Photometer in X-rays (SphinX) was a spectrophotometer developed to observe the Sun in soft X-rays. The instrument observed in the energy range ≈ 1 - 15 keV with resolution ≈ 0.4 keV. SphinX was flown on the Russian CORONAS-PHOTON satellite placed inside the TESIS EUV and X telescope assembly. The spacecraft launch took place on 30 January 2009 at 13:30 UT at the Plesetsk Cosmodrome in Russia. The SphinX experiment mission began a couple of weeks later on 20 February 2009 when the first telemetry dumps were received. The mission ended nine months later on 29 November 2009 when data transmission was terminated. SphinX provided an excellent set of observations during very low solar activity. This was indeed the period in which solar activity dropped to the lowest level observed in X-rays ever. The SphinX instrument design, construction, and operation principle are described. Information on SphinX data repositories, dissemination methods, format, and calibration is given together with general recommendations for data users. Scientific research areas in which SphinX data find application are reviewed.
NASA Astrophysics Data System (ADS)
Tang, Rui; Wei, Xuedong; Liu, Yongning; Zhu, Changchun; Zhu, Jiewu; Yu, Guang
La 1.3 - xSm xCaMg 0.7Ni 9 (x = 0-0.3) hydrogen storage alloys were prepared by inductive melting and the effect of the Sm content on the structure and electrochemical properties was investigated in the paper. The Sm substitution for La in La 1.3 - xSm xCaMg 0.7Ni 9 (x = 0-0.3) alloys does not change the main phase structure (the rhombohedral PuNi 3-type structure), but leads to a shrinkage of unit cell and a decrease of hydrogen storage capacity. With the increase of the Sm content in the alloys, the maximum discharge capacity of electrode decreases from 400.2 (x = 0) to 346.6 mAh g -1 (x = 0.3), but the high-rate dischargeability and cycling stability is improved. After 100 cycles, the capacity retention rate increases from 75 (x = 0) to 85% (x = 0.3).
Classification of X-ray sources in the direction of M31
NASA Astrophysics Data System (ADS)
Vasilopoulos, G.; Hatzidimitriou, D.; Pietsch, W.
2012-01-01
M31 is our nearest spiral galaxy, at a distance of 780 kpc. Identification of X-ray sources in nearby galaxies is important for interpreting the properties of more distant ones, mainly because we can classify nearby sources using both X-ray and optical data, while more distant ones via X-rays alone. The XMM-Newton Large Project for M31 has produced an abundant sample of about 1900 X-ray sources in the direction of M31. Most of them remain elusive, giving us little signs of their origin. Our goal is to classify these sources using criteria based on properties of already identified ones. In particular we construct candidate lists of high mass X-ray binaries, low mass X-ray binaries, X-ray binaries correlated with globular clusters and AGN based on their X-ray emission and the properties of their optical counterparts, if any. Our main methodology consists of identifying particular loci of X-ray sources on X-ray hardness ratio diagrams and the color magnitude diagrams of their optical counterparts. Finally, we examined the X-ray luminosity function of the X-ray binaries populations.
NASA Technical Reports Server (NTRS)
Fan, W. C.; Zborowski, J. T.; Golding, T. D.; Shih, H. D.
1992-01-01
Reflection high-energy electron diffraction (RHEED) during molecular beam epitaxy is used to study the growth and interface formation of the Ga(1-x)In(x)Sb/InAs (x is not greater than 0.4) strained-layer superlattices (SLSs) on GaSb(100) substrates. A number of surface atomic structures were observed in the growth of the SLS: a (1 x 3) phase from the InAs epilayer surface, a (2 x 3) phase, a (2 x 4) phase, and diffuse (1 x 1)-like phases from the InAs epilayer surface. It is suggested that the long-range order quality of the interface of Ga(1-x)In(x)Sb on InAs may be better than that of the interface of InAs on Ga(1-x)In(x)Sb, but the abruptness of the interfaces would still be compatible. The RHEED intensity variations in the formation of the interfaces are discussed in terms of interface chemical reactions.
Dual energy scanning beam laminographic x-radiography
Majewski, Stanislaw; Wojcik, Randolph F.
1998-01-01
A multiple x-ray energy level imaging system includes a scanning x-ray beam and two detector design having a first low x-ray energy sensitive detector and a second high x-ray energy sensitive detector. The low x-ray energy detector is placed next to or in front of the high x-ray energy detector. The low energy sensitive detector has small stopping power for x-rays. The lower energy x-rays are absorbed and converted into electrical signals while the majority of the higher energy x-rays pass through undetected. The high energy sensitive detector has a large stopping power for x-rays as well as it having a filter placed between it and the object to absorb the lower energy x-rays. In a second embodiment; a single energy sensitive detector is provided which provides an output signal proportional to the amount of energy in each individual x-ray it absorbed. It can then have an electronic threshold or thresholds set to select two or more energy ranges for the images. By having multiple detectors located at different positions, a dual energy laminography system is possible.
Dual energy scanning beam laminographic x-radiography
Majewski, S.; Wojcik, R.F.
1998-04-21
A multiple x-ray energy level imaging system includes a scanning x-ray beam and two detector design having a first low x-ray energy sensitive detector and a second high x-ray energy sensitive detector. The low x-ray energy detector is placed next to or in front of the high x-ray energy detector. The low energy sensitive detector has small stopping power for x-rays. The lower energy x-rays are absorbed and converted into electrical signals while the majority of the higher energy x-rays pass through undetected. The high energy sensitive detector has a large stopping power for x-rays as well as it having a filter placed between it and the object to absorb the lower energy x-rays. In a second embodiment; a single energy sensitive detector is provided which provides an output signal proportional to the amount of energy in each individual x-ray it absorbed. It can then have an electronic threshold or thresholds set to select two or more energy ranges for the images. By having multiple detectors located at different positions, a dual energy laminography system is possible. 6 figs.
X-ray lithography using holographic images
Howells, Malcolm R.; Jacobsen, Chris
1995-01-01
A non-contact X-ray projection lithography method for producing a desired X-ray image on a selected surface of an X-ray-sensitive material, such as photoresist material on a wafer, the desired X-ray image having image minimum linewidths as small as 0.063 .mu.m, or even smaller. A hologram and its position are determined that will produce the desired image on the selected surface when the hologram is irradiated with X-rays from a suitably monochromatic X-ray source of a selected wavelength .lambda.. On-axis X-ray transmission through, or off-axis X-ray reflection from, a hologram may be used here, with very different requirements for monochromaticity, flux and brightness of the X-ray source. For reasonable penetration of photoresist materials by X-rays produced by the X-ray source, the wavelength X, is preferably chosen to be no more than 13.5 nm in one embodiment and more preferably is chosen in the range 1-5 nm in the other embodiment. A lower limit on linewidth is set by the linewidth of available microstructure writing devices, such as an electron beam.
Girkontaite, I; Frischholz, S; Lammi, P; Wagner, K; Swoboda, B; Aigner, T; Von der Mark, K
1996-09-01
For studies on processing and tissue distribution of type X collagen, monoclonal antibodies were prepared against human recombinant collagen type X (hrCol X) and tested by ELISA, immunoblotting and immunohistology. Forty-two clones were obtained which were grouped into four different subsets based on their reactivity against native and denatured hrCol X, pepsin-treated hrCol X, and the C-terminal NC-1 domain. Here we present results obtained with four monoclonal antibodies: Clone X 53, a representative of group I, binds with high affinity to both native and pepsin-digested hrCol X but with low affinity to the NC-1 dimer; monoclonal antibodies of group II and III recognized native and denatured hrCol X but not NC-1; antibodies of group II, but not III, reacted to some extent with pepsin treated hrCol X; one antibody (X 34) was obtained that reacted strongly with the isolated NC-1 dimer and native hrCol X but not with the NC-1 monomer or pepsin-digested hrCol X (group IV). Antibodies of all groups stained specifically the hypertrophic zone of fetal human epiphyseal cartilage. Mab X 53 stained the peri- and extracellular matrix of hypertrophic chondrocytes in the lower hypertrophic zone and in the calcified cartilage core in endochondral bone trabecules, while clone X 34 stained intracellularly and the pericellular matrix. All other tissues or cells of the epiphysis were negative. Antibody X 53 reacted also with canine, murine and guinea pig hypertrophic cartilage in tissue sections, but not with bovine or porcine type X collagen. In sections of osteoarthritic cartilage, clusters of hypertrophic chondrocytes in the deep zone were stained, confirming previous observations on enhanced chondrocyte hypertrophy and type X collagen expression in osteoarthritic articular cartilage.
An Icosahedral Quasicrystal and Its 1/0 Crystalline Approximant in the Ca–Au–Al System
DOE Office of Scientific and Technical Information (OSTI.GOV)
Pham, Joyce; Kreyssig, Andreas; Goldman, Alan I.
2016-10-17
A new icosahedral quasicrystalline phase, CaAu4.5–xAl1.5+x [0.11 ≤ x ≤ 0.40(6); CaAu4.4Al1.6, aQC = 5.383(4) Å, and Pm35], and its lowest-order 1/0 cubic crystalline approximant phase, CaAu3+xAl1–x [0 ≤ x ≤ 0.31(1); a = 9.0766(5)–9.1261(8) Å, Pa3(No. 205), and Pearson symbol cP40], have been discovered in the Ca-poor region of the Ca–Au–Al system. In the crystalline approximant, eight [Au3–xAl1+x] tetrahedra fill the unit cell, and each tetrahedron is surrounded by four Ca atoms, thus forming a three-dimensional network of {Ca4/4[Au3–xAl1+x]} tetrahedral stars. A computational study of Au and Al site preferences concurs with the experimental results, which indicate a preferencemore » for near-neighbor Au–Al interactions over Au–Au and Al–Al interactions. Analysis of the electronic density of states and the associated crystal orbital Hamilton population curves was used to rationalize the descriptions of CaAu4.5–xAl1.5+x [0.11 ≤ x ≤ 0.46(6)] and CaAu3+xAl1–x [0 ≤ x ≤ 0.31(1)] as polar intermetallic species, whereby Ca atoms engage in polar covalent bonding with the electronegative, electron-deficient [Au3–xAl1+x] tetrahedral clusters and the observed phase width of the crystalline approximant.« less
Using mini-rockwool blocks as growing media for limited-cluster tomato production
NASA Technical Reports Server (NTRS)
Logendra, L. S.; Gianfagna, T. J.; Janes, H. W.
2001-01-01
Rockwool is an excellent growing medium for the hydroponic production of tomato; however, the standard size rockwool blocks [4 x 4 x 2.5 inches (10 x 10 x 6.3 cm) or 3 x 3 x 2.5 inches (7.5 x 7.5 x 6.3 cm)] are expensive. The following experiments were conducted with less expensive minirock wool blocks (MRBs), on rayon polyester material (RPM) as a bench top liner, to reduce the production cost of tomatoes (Lycopersicon esculentum) grown in a limited-cluster, ebb and flood hydroponic cultivation system. Fruit yield for single-cluster plants growing in MRBs [2 x 2 x 1.6 inches (5 x 5 x 4 cm) and 1.6 x 1.6 x 1.6 inches (4 x 4 x 4 cm)] was not significantly different from plants grown in larger sized blocks (3 x 3 x 2.5 inches). When the bench top was lined with RPM, roots penetrated the RPM, and an extensive root mat developed between the RPM and the bench top. The fruit yield from plants on RPM was significantly increased compared to plants without RPM due to increases in fruit size and fruit number. RPM also significantly reduced the incidence of blossom-end rot. In a second experiment, single- and double-cluster plants were grown on RPM. Fruit yield for double-cluster plants was 40% greater than for single-cluster plants due to an increase in fruit number, although the fruit were smaller in size. As in the first experiment, fruit yield for all plants grown in MRBs was not significantly different from plants grown in the larger sized blocks. MRBs and a RPM bench liner are an effective combination in the production of limited-cluster hydroponic tomatoes.
Hassinger, Elena; Gredat, G.; Valade, F.; ...
2016-04-01
In the temperature-concentration phase diagram of most iron-based superconductors, antiferromagnetic order is gradually suppressed to zero at a critical point, and a dome of superconductivity forms around that point. The nature of the magnetic phase and its fluctuations is of fundamental importance for elucidating the pairing mechanism. In Ba 1–xK xFe 2As 2 and Ba 1–xNa xFe 2As 2, it has recently become clear that the usual stripelike magnetic phase, of orthorhombic symmetry, gives way to a second magnetic phase, of tetragonal symmetry, near the critical point, in the range from x = 0.24 to x = 0.28 for Bamore » 1–xK xFe 2As 2. In a prior study, an unidentified phase was discovered for x < 0.24 but under applied pressure, whose onset was detected as a sharp anomaly in the resistivity. Here we report measurements of the electrical resistivity of Ba 1–xK xFe 2As 2 under applied hydrostatic pressures up to 2.75 GPa, for x = 0.22, 0.24, and 0.28. The critical pressure above which the unidentified phase appears is seen to decrease with increasing x and vanish at x = 0.24, thereby linking the pressure-induced phase to the tetragonal magnetic phase observed at ambient pressure. In the temperature-concentration phase diagram of Ba 1–xK xFe 2As 2, we find that pressure greatly expands the tetragonal magnetic phase, while the stripelike phase shrinks. As a result, this reveals that pressure may be a powerful tuning parameter with which to explore the interplay between magnetism and superconductivity in this material.« less
Unusual Black Hole Binary LMC X-3: A Transient High-Mass X-Ray Binary That Is Almost Always On?
NASA Technical Reports Server (NTRS)
Torpin, Trevor J.; Boyd, Patricia T.; Smale, Alan P.; Valencic, Lynne A.
2017-01-01
We have analyzed a rich, multimission, multiwavelength data set from the black hole X-ray binary (BHXB) LMC X-3, covering a new anomalous low state (ALS), during which the source flux falls to an unprecedentedly low and barely detectable level, and a more normal low state. Simultaneous X-ray and UV/optical monitoring data from Swift are combined with pointed observations from the Rossi X-ray Timing Explorer (RXTE) and X-ray Multi- Mirror Mission (XMM-Newton) and light curves from the Monitor of All-Sky X-ray Image (MAXI) instrument to compare the source characteristics during the ALS with those seen during the normal low state. An XMM-Newton spectrum obtained during the ALS can be modeled using an absorbed power law with Gamma = 1.41‚+/- 0.65 and a luminosity of 7.97 x 10(exp 33) erg/s (0.6-5 keV). The Swift X-ray and UV light curves indicate an X-ray lag of approx. 8 days as LMC X-3 abruptly exits the ALS, suggesting that changes in the mass accretion rate from the donor drive the X-ray lag. The normal low state displays an asymmetric profile in which the exit occurs more quickly than the entry, with minimum X-ray flux a factor of approx. 4300 brighter than during the ALS. The UV brightness of LMC X-3 in the ALS is also fainter and less variable than during normal low states. The existence of repeated ALSs in LMC X-3, as well as a comparison with other BHXBs, implies that it is very close to the transient/persistent X-ray source dividing line. We conclude that LMC X-3 is a transient source that is almost always "on."
Sex-specific silencing of X-linked genes by Xist RNA
Gayen, Srimonta; Maclary, Emily; Hinten, Michael; Kalantry, Sundeep
2016-01-01
X-inactive specific transcript (Xist) long noncoding RNA (lncRNA) is thought to catalyze silencing of X-linked genes in cis during X-chromosome inactivation, which equalizes X-linked gene dosage between male and female mammals. To test the impact of Xist RNA on X-linked gene silencing, we ectopically induced endogenous Xist by ablating the antisense repressor Tsix in mice. We find that ectopic Xist RNA induction and subsequent X-linked gene silencing is sex specific in embryos and in differentiating embryonic stem cells (ESCs) and epiblast stem cells (EpiSCs). A higher frequency of XΔTsixY male cells displayed ectopic Xist RNA coating compared with XΔTsixX female cells. This increase reflected the inability of XΔTsixY cells to efficiently silence X-linked genes compared with XΔTsixX cells, despite equivalent Xist RNA induction and coating. Silencing of genes on both Xs resulted in significantly reduced proliferation and increased cell death in XΔTsixX female cells relative to XΔTsixY male cells. Thus, whereas Xist RNA can inactivate the X chromosome in females it may not do so in males. We further found comparable silencing in differentiating XΔTsixY and 39,XΔTsix (XΔTsixO) ESCs, excluding the Y chromosome and instead implicating the X-chromosome dose as the source of the sex-specific differences. Because XΔTsixX female embryonic epiblast cells and EpiSCs harbor an inactivated X chromosome prior to ectopic inactivation of the active XΔTsix X chromosome, we propose that the increased expression of one or more X-inactivation escapees activates Xist and, separately, helps trigger X-linked gene silencing. PMID:26739568
Put, Brecht; Vereecken, Philippe M; Mees, Maarten J; Rosciano, Fabio; Radu, Iuliana P; Stesmans, Andre
2015-11-21
RF-sputtered thin films of spinel Li(x)Mg(1-2x)Al(2+x)O4 were investigated for use as solid electrolyte. The usage of this material can enable the fabrication of a lattice matched battery stack, which is predicted to lead to superior battery performance. Spinel Li(x)Mg(1-2x)Al(2+x)O4 thin films, with stoichiometry (x) ranging between 0 and 0.25, were formed after a crystallization anneal as shown by X-ray diffraction and transmission electron microscopy. The stoichiometry of the films was evaluated by elastic recoil detection and Rutherford backscattering and found to be slightly aluminum rich. The excellent electronic insulation properties were confirmed by both current-voltage measurements as well as by copper plating tests. The electrochemical stability window of the material was probed using cyclic voltammetry. Lithium plating and stripping was observed together with the formation of a Li-Pt alloy, indicating that Li-ions passed through the film. This observation contradicted with impedance measurements at open circuit potential, which showed no apparent Li-ion conductivity of the film. Impedance spectroscopy as a function of potential showed the occurrence of Li-ion intercalation into the Li(x)Mg(1-2x)Al(2+x)O4 layers. When incorporating Li-ions in the material the ionic conductivity can be increased by 3 orders of magnitude. Therefore it is anticipated that the response of Li(x)Mg(1-2x)Al(2+x)O4 is more adequate for a buffer layer than as the solid electrolyte.
Schneider, Katherine Bacon; Palmer, Tanya M.; Grossman, Alan D.
2002-01-01
Many microbes use secreted peptide-signaling molecules to stimulate changes in gene expression in response to high population density, a process called quorum sensing. ComX pheromone is a modified 10-amino-acid peptide used by Bacillus subtilis to modulate changes in gene expression in response to crowding. comQ and comX are required for production of ComX pheromone. We found that accumulation of ComX pheromone in culture supernatant paralleled cell growth, indicating that there was no autoinduction of production of ComX pheromone. We overexpressed comQ and comX separately and together and found that overexpression of comX alone was sufficient to cause an increase in production of ComX pheromone and early induction of a quorum-responsive promoter. These results indicate that the extracellular concentration of ComX pheromone plays a major role in determining the timing of the quorum response and that expression of comX is limiting for production of ComX pheromone. We made alanine substitutions in the residues that comprise the peptide backbone of ComX pheromone. Analysis of these mutants highlighted the importance of the modification for ComX pheromone function and identified three residues (T50, G54, and D55) that are unlikely to interact with proteins involved in production of or response to ComX pheromone. We have also identified and mutated a putative isoprenoid binding domain of ComQ. Mutations in this domain eliminated production of ComX pheromone, consistent with the hypothesis that ComQ is involved in modifying ComX pheromone and that the modification is likely to be an isoprenoid. PMID:11751817
NASA Astrophysics Data System (ADS)
Zhong, Yuhan; Wang, Peida; Mei, Huayue; Jia, Zhenyuan; Cheng, Nanpu
2018-06-01
CuInTe2 chalcopyrite compound is widely used in the fields of optoelectronics and pyroelectricity, and doping atoms can further improve the physical properties of the CuInTe2 compound. For all we know, this is the first time that the elastic behaviors and lattice dynamical properties of Ag-doped CuInTe2 compounds with the tetragonal system are determined theoretically. The elastic, lattice dynamical and thermal properties of Cu1‑x Ag x InTe2 (x = 0, 0.25, 0.5, 0.75 and 1) compounds have been investigated by using density functional theory. The obtained elastic constants of Cu1‑x Ag x InTe2 compounds indicate that these compounds are mechanically stable and elastic anisotropic. The anisotropy of the {001} plane is more obvious than those of the {100} and {010} planes. Additionally, with increasing Ag doping concentrations, the bulk and shear moduli of Cu1‑x Ag x InTe2 compounds decrease and their toughness improves. The phonon spectra and density of states reveal that Cu (or Ag) atoms in Cu1‑x Ag x InTe2 compounds form chemical bonds with Te atoms, and Cu-Te bonds are gradually replaced by Ag-Te bonds with increasing Ag doping concentration. Vibration modes of Cu1‑x Ag x InTe2 compounds at the {{Γ }} point in the Brillouin zone show that each Cu1‑x Ag x InTe2 (x = 0 and 1) crystal includes five irreducible representations (A1, A2, B1, B2 and E). As for Cu1‑x Ag x InTe2 (x = 0.25, 0.5 and 0.75) compounds, each crystal has three irreducible representations (A, B and E). The atomic displacements of several typical phonon modes in CuInTe2 crystals have been analyzed to deepen the understanding of lattice vibrations in Cu1‑x AgxInTe2 compounds. With increasing Ag doping concentration, the Debye temperatures of Cu1‑x Ag x InTe2 compounds decrease, while their heat capacities increase.
Chase, C C; Olson, T A; Hammond, A C; Menchaca, M A; West, R L; Johnson, D D; Butts, W T
1998-12-01
We conducted a multiyear study in two phases to determine preweaning performance traits of Senepol (S x S), Hereford (H x H), and reciprocal (S x H and H x S) F1 crossbred calves and feedlot performance and carcass characteristics of steers. In Phase I, from 1985 to 1989, data from S x S (n = 194), H x H (n = 383), and S x H (n = 120) calves were used. Numbers of S x S cows were increased during Phase I so that data from H x S (n = 74) calves could be included in Phase II (1990 to 1992) in addition to S x S (n = 118), H x H (n = 130), and S x H (n = 56) calves. Also during Phase II, feedlot performance and carcass characteristics were determined for S x S (n = 30), H x H (n = 26), H x S (n = 36), and S x H (n = 26) steers. In Phase I, S x S calves had heavier (P < .01) birth weights and heavier (P < .01) 205-d adjusted weaning weights than H x H calves. Birth weights of S x H calves were heavier (P < .01) than the mean of the purebred calves, but 205-d adjusted weaning weights did not differ (P > .10). In phase II, direct heterosis was 3.5% for birth weight (P < .05) and 5.1% for 205-d adjusted weaning weight (P < .01). Senepol maternal breed effects were 1.9 kg for birth weight (P < .10) and 37.9 kg for 205-d adjusted weaning weight (P < .01). Levels of direct heterosis, Senepol maternal breed effects, and Hereford direct breed effects were significant for most feedlot performance traits of steer calves that were fed to a common end point. Breeds did not differ (P > .10) for USDA yield and quality grades, and direct heterosis was not significant for Warner-Bratzler shear force. These results demonstrate significant levels of heterosis in preweaning performance between S x S and H x H calves and in feedlot performance of steers. Levels of heterosis were smaller and nonsignificant for most carcass traits including meat tenderness, which did not differ between S x S and H x H steers in this study.
Investigation of Modularly Configured Attached Processors with Intelligent Memories
1994-09-30
sequence of computations becomes cl = c11 + C[i, i] := Cli, j] + A[i, k) * Blk, j]; al x bti, c12 - c12 + k X bkX2, C13 = C1 3 + alk X b 3 , ... , c =n...Cin + alk X bkn, C2 1 = Cat + a2k x bkl , The sequence of computations becomes cii = a I x bli, C22 = cU2 + a2k x b2, ... Cj a2 1x bij, ca3j = aa x...1 to 1/2 Least significant 1/2 address bits Fig. 1. Block diagram of a memory module PREGVJKE is v I pis P16 16 ItO16 = 4-81T OECD - = AMKSS A s-Byrf
5f delocalization-induced suppression of quadrupolar order in U(Pd 1-xPt x)₃
Walker, H. C.; Le, M. D.; McEwen, K. A.; ...
2011-12-27
We present bulk magnetic and transport measurements and x-ray resonant scattering measurements on U(Pd 1-xPt x)₃ for x=0.005 and 0.01, which demonstrate the high sensitivity of the quadrupolar order in the canonical antiferroquadrupolar ordered system UPd₃ to doping with platinum. Bulk measurements for x=0.005 reveal behavior similar to that seen in UPd₃, albeit at a lower temperature, and x-ray resonant scattering provides evidence of quadrupolar order described by the Q xy order parameter. In contrast, bulk measurements reveal only an indistinct transition in x=0.01, consistent with the observation of short-range quadrupolar order in our x-ray resonant scattering results.
NASA Technical Reports Server (NTRS)
Rossj, B.
1981-01-01
The evolution of X-ray astronomy up to the launching of the Einstein observatory is presented. The evaluation proceeded through the following major steps: (1) discovery of an extrasolar X-ray source, Sco X-1, orders of magnitude stronger than astronomers believed might exist; (2) identification of a strong X-ray source with the Crab Nebula; (3) identification of Sco X-1 with a faint, peculiar optical object; (4) demonstration that X-ray stars are binary systems, each consisting of a collapsed object accreting matter from an ordinary star; (5) discovery of X-ray bursts; (6) discovery of exceedingly strong X-ray emission from active galaxies, quasars and clusters of galaxies; (7) demonstration that the principal X-ray source is a hot gas filling the space between galaxies.
History of the "Detector Materials Engineering" Crystal Growth Process for Bulk Hg1- x Cd x Te
NASA Astrophysics Data System (ADS)
Higgins, W. M.; Nelson, D. A.; Roy, R. G.; Murosako, R. P.; Lancaster, R. A.; Tower, J.; Norton, P.
2013-11-01
This paper reviews the history and technology of a bulk Hg1- x Cd x Te crystal growth process that was developed in the early 1980s at Honeywell Electro-Optics Division (presently BAE Systems, Electronic Solutions). The crystal growth process name, DME, was an acronym for the department name: Detector Materials Engineering. This was an accelerated crucible rotation technique (ACRT) vertical traveling heater method growth process. Crystal growth occurred in the pseudobinary Hg1- x Cd x Te system. ACRT mixing allowed the lower-density, higher- x-value Hg1- x Cd x Te growth nutrient in the upper region of the ampoule to replenish the depleted melt and allowed the growth of constant- x-value, higher-density Hg1- x Cd x Te. The material grown by this research and production growth process yielded single crystals that had improved purity, compositional uniformity, precipitate density, and reproducibility in comparison with solid-state recrystallization and other bulk Hg1- x Cd x Te growth techniques. Radial and longitudinal nonuniformities in x-value for Hg1- x Cd x Te were reduced to <0.0008/cm. The net electrically active background impurities did not exceed 1 × 1014 cm-3. Electron mobilities in excess of 1.5 × 106 cm2/V-s were observed at 77 K. Structural defects of less than 104 cm-2 were measured. Te precipitates were not observed. As a result of these material improvements, long-wavelength infrared (LWIR) photoconductive devices fabricated from DME material had highly desired performance characteristics.
Barz, W P; Francia, F; Venturoli, G; Melandri, B A; Verméglio, A; Oesterhelt, D
1995-11-21
The pufX gene is essential for photoheterotrophic growth of the purple bacterium Rhodobacter sphaeroides. In order to analyze the molecular function of the PufX membrane protein, we constructed a chromosomal pufX deletion mutant and phenotypically compared it to a pufX+ control strain and to two suppressor mutants which are able to grow photosynthetically in the absence of pufX. Using this genetic background, we confirmed that PufX is required for photoheterotrophic growth under anaerobic conditions, although all components of the photosynthetic apparatus were present in similar amounts in all strains investigated. We show that the deletion of PufX is not lethal for illuminated pufX- cells, suggesting that PufX is required for photosynthetic cell division. Since chromatophores isolated from the pufX- mutant were found to be unsealed vesicles, the role of PufX in photosynthetic energy transduction was studied in vivo. We show that PufX is essential for light-induced ATP synthesis (photophosphorylation) in anaerobically incubated cells. Measurements of absorption changes induced by a single turnover flash demonstrated that PufX is not required for electron flow through the reaction center and the cytochrome bc1 complex under anaerobic conditions. During prolonged illumination, however, PufX is essential for the generation of a sufficiently large membrane potential to allow photosynthetic growth. These in vivo results demonstrate that under anaerobic conditions PufX plays an essential role in facilitating effective interaction of the components of the photosynthetic apparatus.
Rangel-Yescas, Gisela E; Vazquez-Cuevas, Francisco G; Garay, Edith; Arellano, Rogelio O
2012-01-01
P2X receptors are trimeric, ATP-gated cation channels. In mammals seven P2X subtypes have been reported (P2X1-P2X7), as well as several variants generated by alternative splicing. Variants confer to the homomeric or heteromeric channels distinct functional and/or pharmacological properties. Molecular biology, biochemical, and functional analysis by electrophysiological methods were used to identify and study a new variant of the P2X1 receptor named P2X1b. This new variant, identified in rat optic nerve, was also expressed in other tissues. P2X1b receptors lack amino acids 182 to 208 of native P2X1, a region that includes residues that are highly conserved among distinct P2X receptors. When expressed in Xenopus oocytes, P2X1b was not functional as a homomer; however, when co-expressed with P2X1, it downregulated the electrical response generated by ATP compared with that of oocytes expressing P2X1 alone, and it seemed to form heteromeric channels with a modestly enhanced ATP potency. A decrease in responses to ATP in oocytes co-expressing different ratios of P2X1b to P2X1 was completely eliminated by overnight pretreatment with apyrase. Thus, it is suggested that P2X1b regulates, through a use-dependent mechanism, the availability, in the plasma membrane, of receptor channels that can be operated by ATP.
A Comparison of Selective Pressures in Plant X-Linked and Autosomal Genes
Krasovec, Marc; Filatov, Dmitry A.
2018-01-01
Selection is expected to work differently in autosomal and X-linked genes because of their ploidy difference and the exposure of recessive X-linked mutations to haploid selection in males. However, it is not clear whether these expectations apply to recently evolved sex chromosomes, where many genes retain functional X- and Y-linked gametologs. We took advantage of the recently evolved sex chromosomes in the plant Silene latifolia and its closely related species to compare the selective pressures between hemizygous and non-hemizygous X-linked genes as well as between X-linked genes and autosomal genes. Our analysis, based on over 1000 genes, demonstrated that, similar to animals, X-linked genes in Silene evolve significantly faster than autosomal genes—the so-called faster-X effect. Contrary to expectations, faster-X divergence was detectable only for non-hemizygous X-linked genes. Our phylogeny-based analyses of selection revealed no evidence for faster adaptation in X-linked genes compared to autosomal genes. On the other hand, partial relaxation of purifying selection was apparent on the X-chromosome compared to the autosomes, consistent with a smaller genetic diversity in S. latifolia X-linked genes (πx = 0.016; πaut = 0.023). Thus, the faster-X divergence in S. latifolia appears to be a consequence of the smaller effective population size rather than of a faster adaptive evolution on the X-chromosome. We argue that this may be a general feature of “young” sex chromosomes, where the majority of X-linked genes are not hemizygous, preventing haploid selection in heterogametic sex. PMID:29751495
NASA Astrophysics Data System (ADS)
Hornschemeier, A. E.; Heckman, T. M.; Ptak, A. F.; Tremonti, C. A.; Colbert, E. J. M.
2005-01-01
We have cross-correlated X-ray catalogs derived from archival Chandra X-Ray Observatory ACIS observations with a Sloan Digital Sky Survey Data Release 2 (DR2) galaxy catalog to form a sample of 42 serendipitously X-ray-detected galaxies over the redshift interval 0.03
Ternary lanthanum sulfide selenides {alpha}-LaS{sub 2-x}Se{sub x} (0
DOE Office of Scientific and Technical Information (OSTI.GOV)
Bartsch, Christian; Doert, Thomas, E-mail: thomas.doert@chemie.tu-dresden.de
2012-01-15
Mixed lanthanum sulfide selenides LaS{sub 2-x}Se{sub x} (0
NASA Astrophysics Data System (ADS)
Han, I.; Demir, L.
2009-11-01
Kβ -to- Kα x-ray intensity ratios of Fe, Cr, and Ni have been measured in pure metals and in alloys of FexNi1-x ( x=0.8 , 0.7, 0.6, 0.5, 0.4, 0.3, and 0.2), NixCr1-x ( x=0.8 , 0.6, 0.5, 0.4, and 0.2), FexCr1-x ( x=0.9 , 0.7, and 0.5), and FexCryNi1-(x+y) ( x=0.7-y=0.1 , x=0.5-y=0.2 , x=0.4-y=0.3 , x=0.3-y=0.3 , x=0.2-y=0.2 , and x=0.1-y=0.2 ) following excitation by 22.69 keV x rays from a 10 mCi C109d radioactive point source. The valence-electron configurations of these metals were determined by corporation of measured Kβ -to- Kα x-ray intensity ratios with the results of multiconfiguration Dirac-Fock calculation for various valence-electron configurations. Valence-electron configurations of 3d transition metals in alloys indicate significant differences with respect to the pure metals. Our analysis indicates that these differences arise from delocalization and/or charge transfer phenomena in alloys. Namely, the observed change of the valence-electron configurations of metals in alloys can be explained with the transfer of 3d electrons from one element to the other element and/or the rearrangement of electrons between 3d and 4s,4p states of individual metal atoms.