Sample records for gamma energy release

  1. Energy spectra of cosmic gamma-ray bursts

    NASA Technical Reports Server (NTRS)

    Cline, T. L.; Desai, U. D.; Klebesadel, R. W.; Strong, I. B.

    1973-01-01

    Spectral measurements of six cosmic gamma-ray bursts in the energy region of 0.1 to 1.2 MeV, made using a semi-omnidirectional X-ray detector on IMP-6 are reported. These measurements confirm the hard X-ray or gamma-ray nature of the bursts, as inferred from the original observations by Klebesadel et al., (1973), and show that their maximum energy release is in this several hundred keV region. Each burst consists of several 1 or 2-second pulses each with the characteristic spectrum of approximately 150-keV exponential, followed by a softer decay. There is no evidence of line structure in this energy region, or for a marked change in the energy spectrum within a given pulse. Event size spectra are estimated for galactic and extragalactic models; the total emission is consistent with present measurements of the diffuse background, and unlikely to account for any spectral feature in the few-MeV region.

  2. Fermi Observations of High-Energy Gamma-Ray Emission from GRB 080916C

    DOE PAGES

    Abdo, A. A.; Ackermann, M.; Arimoto, M.; ...

    2009-02-19

    Gamma-ray bursts (GRBs) are highly energetic explosions signaling the death of massive stars in distant galaxies. The Gamma-ray Burst Monitor and Large Area Telescope onboard the Fermi Observatory together record GRBs over a broad energy range spanning about 7 decades of gammaray energy. In September 2008, Fermi observed the exceptionally luminous GRB 080916C, with the largest apparent energy release yet measured. The high-energy gamma rays are observed to start later and persist longer than the lower energy photons. A simple spectral form fits the entire GRB spectrum, providing strong constraints on emission models. Finally, the known distance of the burstmore » enables placing lower limits on the bulk Lorentz factor of the outflow and on the quantum gravity mass.« less

  3. Fermi observations of high-energy gamma-ray emission from GRB 080916C.

    PubMed

    Abdo, A A; Ackermann, M; Arimoto, M; Asano, K; Atwood, W B; Axelsson, M; Baldini, L; Ballet, J; Band, D L; Barbiellini, G; Baring, M G; Bastieri, D; Battelino, M; Baughman, B M; Bechtol, K; Bellardi, F; Bellazzini, R; Berenji, B; Bhat, P N; Bissaldi, E; Blandford, R D; Bloom, E D; Bogaert, G; Bogart, J R; Bonamente, E; Bonnell, J; Borgland, A W; Bouvier, A; Bregeon, J; Brez, A; Briggs, M S; Brigida, M; Bruel, P; Burnett, T H; Burrows, D; Busetto, G; Caliandro, G A; Cameron, R A; Caraveo, P A; Casandjian, J M; Ceccanti, M; Cecchi, C; Celotti, A; Charles, E; Chekhtman, A; Cheung, C C; Chiang, J; Ciprini, S; Claus, R; Cohen-Tanugi, J; Cominsky, L R; Connaughton, V; Conrad, J; Costamante, L; Cutini, S; Deklotz, M; Dermer, C D; de Angelis, A; de Palma, F; Digel, S W; Dingus, B L; do Couto E Silva, E; Drell, P S; Dubois, R; Dumora, D; Edmonds, Y; Evans, P A; Fabiani, D; Farnier, C; Favuzzi, C; Finke, J; Fishman, G; Focke, W B; Frailis, M; Fukazawa, Y; Funk, S; Fusco, P; Gargano, F; Gasparrini, D; Gehrels, N; Germani, S; Giebels, B; Giglietto, N; Giommi, P; Giordano, F; Glanzman, T; Godfrey, G; Goldstein, A; Granot, J; Greiner, J; Grenier, I A; Grondin, M-H; Grove, J E; Guillemot, L; Guiriec, S; Haller, G; Hanabata, Y; Harding, A K; Hayashida, M; Hays, E; Hernando Morat, J A; Hoover, A; Hughes, R E; Jóhannesson, G; Johnson, A S; Johnson, R P; Johnson, T J; Johnson, W N; Kamae, T; Katagiri, H; Kataoka, J; Kavelaars, A; Kawai, N; Kelly, H; Kennea, J; Kerr, M; Kippen, R M; Knödlseder, J; Kocevski, D; Kocian, M L; Komin, N; Kouveliotou, C; Kuehn, F; Kuss, M; Lande, J; Landriu, D; Larsson, S; Latronico, L; Lavalley, C; Lee, B; Lee, S-H; Lemoine-Goumard, M; Lichti, G G; Longo, F; Loparco, F; Lott, B; Lovellette, M N; Lubrano, P; Madejski, G M; Makeev, A; Marangelli, B; Mazziotta, M N; McBreen, S; McEnery, J E; McGlynn, S; Meegan, C; Mészáros, P; Meurer, C; Michelson, P F; Minuti, M; Mirizzi, N; Mitthumsiri, W; Mizuno, T; Moiseev, A A; Monte, C; Monzani, M E; Moretti, E; Morselli, A; Moskalenko, I V; Murgia, S; Nakamori, T; Nelson, D; Nolan, P L; Norris, J P; Nuss, E; Ohno, M; Ohsugi, T; Okumura, A; Omodei, N; Orlando, E; Ormes, J F; Ozaki, M; Paciesas, W S; Paneque, D; Panetta, J H; Parent, D; Pelassa, V; Pepe, M; Perri, M; Pesce-Rollins, M; Petrosian, V; Pinchera, M; Piron, F; Porter, T A; Preece, R; Rainò, S; Ramirez-Ruiz, E; Rando, R; Rapposelli, E; Razzano, M; Razzaque, S; Rea, N; Reimer, A; Reimer, O; Reposeur, T; Reyes, L C; Ritz, S; Rochester, L S; Rodriguez, A Y; Roth, M; Ryde, F; Sadrozinski, H F-W; Sanchez, D; Sander, A; Saz Parkinson, P M; Scargle, J D; Schalk, T L; Segal, K N; Sgrò, C; Shimokawabe, T; Siskind, E J; Smith, D A; Smith, P D; Spandre, G; Spinelli, P; Stamatikos, M; Starck, J-L; Stecker, F W; Steinle, H; Stephens, T E; Strickman, M S; Suson, D J; Tagliaferri, G; Tajima, H; Takahashi, H; Takahashi, T; Tanaka, T; Tenze, A; Thayer, J B; Thayer, J G; Thompson, D J; Tibaldo, L; Torres, D F; Tosti, G; Tramacere, A; Turri, M; Tuvi, S; Usher, T L; van der Horst, A J; Vigiani, L; Vilchez, N; Vitale, V; von Kienlin, A; Waite, A P; Williams, D A; Wilson-Hodge, C; Winer, B L; Wood, K S; Wu, X F; Yamazaki, R; Ylinen, T; Ziegler, M

    2009-03-27

    Gamma-ray bursts (GRBs) are highly energetic explosions signaling the death of massive stars in distant galaxies. The Gamma-ray Burst Monitor and Large Area Telescope onboard the Fermi Observatory together record GRBs over a broad energy range spanning about 7 decades of gammaray energy. In September 2008, Fermi observed the exceptionally luminous GRB 080916C, with the largest apparent energy release yet measured. The high-energy gamma rays are observed to start later and persist longer than the lower energy photons. A simple spectral form fits the entire GRB spectrum, providing strong constraints on emission models. The known distance of the burst enables placing lower limits on the bulk Lorentz factor of the outflow and on the quantum gravity mass.

  4. Interferon-gamma (INF-gamma) release test can detect cutaneous adverse effects to statins.

    PubMed

    Goldberg, Ilan; Isman, Gila; Shirazi, Idit; Brenner, Sarah

    2009-12-01

    An increasing number of cutaneous adverse effects are being reported as use of statins becomes more widespread. A study was undertaken to establish the relationship between statin and a cutaneous reaction by the in vitro interferon-gamma (INF-gamma) release test. The lymphocytes of 20 patients with suspected drug-induced skin reaction were incubated with and without the drug. The level of INF-gamma from the supernatant was measured by enzyme-linked immunosorbent assay (ELISA), and the increase calculated. Response was positive in 27 (21.43%) of the 126 drugs. Statin was the only drug with a positive response in 80% of those cases. Nine of 20 patients (45.0%) had complete resolution after discontinuation of the drug; 6 (30.0%) who replaced one drug by another statin had partial or no resolution; and 5 (20.0%) had no resolution despite cessation of statins of all kinds. A positive INF-gamma release test was found in patients who developed skin reactions while taking statins; the test's reliability was strengthened by prompt improvement following elimination of the suspected drug in the majority of patients.

  5. Very high-energy gamma rays from gamma-ray bursts.

    PubMed

    Chadwick, Paula M

    2007-05-15

    Very high-energy (VHE) gamma-ray astronomy has undergone a transformation in the last few years, with telescopes of unprecedented sensitivity having greatly expanded the source catalogue. Such progress makes the detection of a gamma-ray burst at the highest energies much more likely than previously. This paper describes the facilities currently operating and their chances for detecting gamma-ray bursts, and reviews predictions for VHE gamma-ray emission from gamma-ray bursts. Results to date are summarized.

  6. Acetylcholine Release in Prefrontal Cortex Promotes Gamma Oscillations and Theta-Gamma Coupling during Cue Detection.

    PubMed

    Howe, William M; Gritton, Howard J; Lusk, Nicholas A; Roberts, Erik A; Hetrick, Vaughn L; Berke, Joshua D; Sarter, Martin

    2017-03-22

    The capacity for using external cues to guide behavior ("cue detection") constitutes an essential aspect of attention and goal-directed behavior. The cortical cholinergic input system, via phasic increases in prefrontal acetylcholine release, plays an essential role in attention by mediating such cue detection. However, the relationship between cholinergic signaling during cue detection and neural activity dynamics in prefrontal networks remains unclear. Here we combined subsecond measures of cholinergic signaling, neurophysiological recordings, and cholinergic receptor blockade to delineate the cholinergic contributions to prefrontal oscillations during cue detection in rats. We first confirmed that detected cues evoke phasic acetylcholine release. These cholinergic signals were coincident with increased neuronal synchrony across several frequency bands and the emergence of theta-gamma coupling. Muscarinic and nicotinic cholinergic receptors both contributed specifically to gamma synchrony evoked by detected cues, but the effects of blocking the two receptor subtypes were dissociable. Blocking nicotinic receptors primarily attenuated high-gamma oscillations occurring during the earliest phases of the cue detection process, while muscarinic (M1) receptor activity was preferentially involved in the transition from high to low gamma power that followed and corresponded to the mobilization of networks involved in cue-guided decision making. Detected cues also promoted coupling between gamma and theta oscillations, and both nicotinic and muscarinic receptor activity contributed to this process. These results indicate that acetylcholine release coordinates neural oscillations during the process of cue detection. SIGNIFICANCE STATEMENT The capacity of learned cues to direct attention and guide responding ("cue detection") is a key component of goal-directed behavior. Rhythmic neural activity and increases in acetylcholine release in the prefrontal cortex contribute to

  7. Acetylcholine Release in Prefrontal Cortex Promotes Gamma Oscillations and Theta–Gamma Coupling during Cue Detection

    PubMed Central

    Hetrick, Vaughn L.; Berke, Joshua D.

    2017-01-01

    The capacity for using external cues to guide behavior (“cue detection”) constitutes an essential aspect of attention and goal-directed behavior. The cortical cholinergic input system, via phasic increases in prefrontal acetylcholine release, plays an essential role in attention by mediating such cue detection. However, the relationship between cholinergic signaling during cue detection and neural activity dynamics in prefrontal networks remains unclear. Here we combined subsecond measures of cholinergic signaling, neurophysiological recordings, and cholinergic receptor blockade to delineate the cholinergic contributions to prefrontal oscillations during cue detection in rats. We first confirmed that detected cues evoke phasic acetylcholine release. These cholinergic signals were coincident with increased neuronal synchrony across several frequency bands and the emergence of theta–gamma coupling. Muscarinic and nicotinic cholinergic receptors both contributed specifically to gamma synchrony evoked by detected cues, but the effects of blocking the two receptor subtypes were dissociable. Blocking nicotinic receptors primarily attenuated high-gamma oscillations occurring during the earliest phases of the cue detection process, while muscarinic (M1) receptor activity was preferentially involved in the transition from high to low gamma power that followed and corresponded to the mobilization of networks involved in cue-guided decision making. Detected cues also promoted coupling between gamma and theta oscillations, and both nicotinic and muscarinic receptor activity contributed to this process. These results indicate that acetylcholine release coordinates neural oscillations during the process of cue detection. SIGNIFICANCE STATEMENT The capacity of learned cues to direct attention and guide responding (“cue detection”) is a key component of goal-directed behavior. Rhythmic neural activity and increases in acetylcholine release in the prefrontal cortex

  8. High energy gamma ray astronomy

    NASA Technical Reports Server (NTRS)

    Fichtel, Carl E.

    1987-01-01

    High energy gamma ray astronomy has evolved with the space age. Nonexistent twenty-five years ago, there is now a general sketch of the gamma ray sky which should develop into a detailed picture with the results expected to be forthcoming over the next decade. The galactic plane is the dominant feature of the gamma ray sky, the longitude and latitude distribution being generally correlated with galactic structural features including the spiral arms. Two molecular clouds were already seen. Two of the three strongest gamma ray sources are pulsars. The highly variable X-ray source Cygnus X-3 was seen at one time, but not another in the 100 MeV region, and it was also observed at very high energies. Beyond the Milky Way Galaxy, there is seen a diffuse radiation, whose origin remains uncertain, as well as at least one quasar, 3C 273. Looking to the future, the satellite opportunities for high energy gamma ray astronomy in the near term are the GAMMA-I planned to be launched in late 1987 and the Gamma Ray Observatory, scheduled for launch in 1990. The Gamma Ray Observatory will carry a total of four instruments covering the entire energy range from 30,000 eV to 3 x 10 to the 10th eV with over an order of magnitude increase in sensitivity relative to previous satellite instruments.

  9. Very High-Energy Gamma-Ray Sources.

    ERIC Educational Resources Information Center

    Weekes, Trevor C.

    1986-01-01

    Discusses topics related to high-energy, gamma-ray astronomy (including cosmic radiation, gamma-ray detectors, high-energy gamma-ray sources, and others). Also considers motivation for the development of this field, the principal results to date, and future prospects. (JN)

  10. Alternative mechanism by which IFN-gamma enhances tumor recognition: active release of heat shock protein 72.

    PubMed

    Bausero, Maria A; Gastpar, Robert; Multhoff, Gabriele; Asea, Alexzander

    2005-09-01

    IFN-gamma exhibits differential effects depending on the target and can induce cellular activation and enhance survival or mediate cell death via activation of apoptotic pathways. In this study, we demonstrate an alternative mechanism by which IFN-gamma enhances tumor recognition, mediated by the active release of Hsp72. We demonstrate that stimulation of 4T1 breast adenocarcinoma cells and K562 erythroleukemic cells with IFN-gamma triggers the cellular stress response, which results in the enhanced expression of total Hsp72 expression without a significant increase in cell death. Intracellular expression of Hsp72 was abrogated in cells stably transfected with a mutant hsf-1 gene. IFN-gamma-induced Hsp72 expression correlated with enhanced surface expression and consequent release of Hsp72 into the culture medium. Pretreatment of tumors with compounds known to the block the classical protein transport pathway, including monensin, brefeldin A, tunicamycin, and thapsigargin, did not significantly block Hsp72 release. However, pretreatment with intracellular calcium chelator BAPTA-AM or disruption of lipid rafts using methyl beta-cyclodextrin completely abrogated IFN-gamma-induced Hsp72 release. Biochemical characterization revealed that Hsp72 is released within exosomes and has the ability to up-regulate CD83 expression and stimulate IL-12 release by naive dendritic cells. Pretreatment with neutralizing mAb or depletion of Hsp72 completely abrogated its chaperokine function. Taken together, these findings are indicative of an additional previously unknown mechanism by which IFN-gamma promotes tumor surveillance and furthers our understanding of the central role of extracellular Hsp72 as an endogenous adjuvant and danger signal.

  11. Pulsed high-energy gamma rays from PSR 1055-52

    NASA Technical Reports Server (NTRS)

    Fierro, J. M.; Bertsch, D. L.; Brazier, K. T.; Chiang, J.; D'Amico, N.; Fichtel, C. E.; Hartman, R. C.; Hunter, S. D.; Johnston, S.; Kanbach, G.

    1993-01-01

    The Energetic Gamma Ray Experiment Telescope (EGRET) aboard the Compton Gamma Ray Observatory has detected a high-energy gamma-ray source at a position coincident with that of the radio pulsar PSR 1055-52. Analysis of the EGRET data at the radio pulsar period of 197 ms has revealed pulsed gamma-radiation at energies above 300 MeV, making PSR 1055-52 the fifth detected high-energy gamma-ray pulsar. The pulsed radiation from PSR 1055-52 has a very hard photon spectral index of -1.18 +/- 0.16 and a high efficiency for converting its rotational energy into gamma-rays. No unpulsed emission was observed.

  12. Gamma-ray transfer and energy deposition in supernovae

    NASA Technical Reports Server (NTRS)

    Swartz, Douglas A.; Sutherland, Peter G.; Harkness, Robert P.

    1995-01-01

    Solutions to the energy-independent (gray) radiative transfer equations are compared to results of Monte Carlo simulations of the Ni-56 and Co-56 decay gamma-ray energy deposition in supernovae. The comparison shows that an effective, purely absorptive, gray opacity, kappa(sub gamma) approximately (0. 06 +/- 0.01)Y(sub e) sq cm/g, where Y is the total number of electrons per baryon, accurately describes the interaction of gamma-rays with the cool supernova gas and the local gamma-ray energy deposition within the gas. The nature of the gamma-ray interaction process (dominated by Compton scattering in the relativistic regime) creates a weak dependence of kappa(sub gamma) on the optical thickness of the (spherically symmetric) supernova atmosphere: The maximum value of kappa(sub gamma) applies during optically thick conditions when individual gamma-rays undergo multiple scattering encounters and the lower bound is reached at the phase characterized by a total Thomson optical depth to the center of the atmosphere tau(sub e) approximately less than 1. Gamma-ray deposition for Type Ia supernova models to within 10% for the epoch from maximum light to t = 1200 days. Our results quantitatively confirm that the quick and efficient solution to the gray transfer problem provides an accurate representation of gamma-ray energy deposition for a broad range of supernova conditions.

  13. Gamma Rays at Very High Energies

    NASA Astrophysics Data System (ADS)

    Aharonian, Felix

    This chapter presents the elaborated lecture notes on Gamma Rays at Very High Energies given by Felix Aharonian at the 40th Saas-Fee Advanced Course on "Astrophysics at Very High Energies". Any coherent description and interpretation of phenomena related to gammarays requires deep knowledge of many disciplines of physics like nuclear and particle physics, quantum and classical electrodynamics, special and general relativity, plasma physics, magnetohydrodynamics, etc. After giving an introduction to gamma-ray astronomy the author discusses the astrophysical potential of ground-based detectors, radiation mechanisms, supernova remnants and origin of the galactic cosmic rays, TeV emission of young supernova remnants, gamma-emission from the Galactic center, pulsars, pulsar winds, pulsar wind nebulae, and gamma-ray loud binaries.

  14. Very high energy gamma-ray binary stars.

    PubMed

    Lamb, R C; Weekes, T C

    1987-12-11

    One of the major astronomical discoveries of the last two decades was the detection of luminous x-ray binary star systems in which gravitational energy from accretion is released by the emission of x-ray photons, which have energies in the range of 0.1 to 10 kiloelectron volts. Recent observations have shown that some of these binary sources also emit photons in the energy range of 10(12) electron volts and above. Such sources contain a rotating neutron star that is accreting matter from a companion. Techniques to detect such radiation are ground-based, simple, and inexpensive. Four binary sources (Hercules X-1, 4U0115+63, Vela X-1, and Cygnus X-3) have been observed by at least two independent groups. Although the discovery of such very high energy "gamma-ray binaries" was not theoretically anticipated, models have now been proposed that attempt to explain the behavior of one or more of the sources. The implications of these observations is that a significant portion of the more energetic cosmic rays observed on Earth may arise from the action of similar sources within the galaxy during the past few million years.

  15. The EGRET high energy gamma ray telescope

    NASA Technical Reports Server (NTRS)

    Hartman, R. C.; Bertsch, D. L.; Fichtel, C. E.; Hunter, S. D.; Kanbach, G.; Kniffen, D. A.; Kwok, P. W.; Lin, Y. C.; Mattox, J. R.; Mayer-Hasselwander, H. A.

    1992-01-01

    The Energetic Gamma Ray Experiment Telescope (EGRET) on the Compton Gamma Ray Observatory (GRO) is sensitive in the energy range from about 20 MeV to about 30,000 MeV. Electron-positron pair production by incident gamma photons is utilized as the detection mechanism. The pair production occurs in tantalum foils interleaved with the layers of a digital spark chamber system; the spark chamber records the tracks of the electron and positron, allowing the reconstruction of the arrival direction of the gamma ray. If there is no signal from the charged particle anticoincidence detector which surrounds the upper part of the detector, the spark chamber array is triggered by two hodoscopes of plastic scintillators. A time of flight requirement is included to reject events moving backward through the telescope. The energy of the gamma ray is primarily determined by absorption of the energies of the electron and positron in a 20 cm deep NaI(Tl) scintillator.

  16. The EGRET high energy gamma ray telescope

    NASA Astrophysics Data System (ADS)

    Hartman, R. C.; Bertsch, D. L.; Fichtel, C. E.; Hunter, S. D.; Kanbach, G.; Kniffen, D. A.; Kwok, P. W.; Lin, Y. C.; Mattox, J. R.; Mayer-Hasselwander, H. A.; Michelson, P. F.; von Montigny, C.; Nolan, P. L.; Pinkau, K.; Rothermel, H.; Schneid, E.; Sommer, M.; Sreekumar, P.; Thompson, D. J.

    1992-02-01

    The Energetic Gamma Ray Experiment Telescope (EGRET) on the Compton Gamma Ray Observatory (GRO) is sensitive in the energy range from about 20 MeV to about 30,000 MeV. Electron-positron pair production by incident gamma photons is utilized as the detection mechanism. The pair production occurs in tantalum foils interleaved with the layers of a digital spark chamber system; the spark chamber records the tracks of the electron and positron, allowing the reconstruction of the arrival direction of the gamma ray. If there is no signal from the charged particle anticoincidence detector which surrounds the upper part of the detector, the spark chamber array is triggered by two hodoscopes of plastic scintillators. A time of flight requirement is included to reject events moving backward through the telescope. The energy of the gamma ray is primarily determined by absorption of the energies of the electron and positron in a 20 cm deep NaI(Tl) scintillator.

  17. A tandem-based compact dual-energy gamma generator.

    PubMed

    Persaud, A; Kwan, J W; Leitner, M; Leung, K-N; Ludewigt, B; Tanaka, N; Waldron, W; Wilde, S; Antolak, A J; Morse, D H; Raber, T

    2010-02-01

    A dual-energy tandem-type gamma generator has been developed at E. O. Lawrence Berkeley National Laboratory and Sandia National Laboratories. The tandem accelerator geometry allows higher energy nuclear reactions to be reached, thereby allowing more flexible generation of MeV-energy gammas for active interrogation applications. Both positively charged ions and atoms of hydrogen are created from negative ions via a gas stripper. In this paper, we show first results of the working tandem-based gamma generator and that a gas stripper can be utilized in a compact source design. Preliminary results of monoenergetic gamma production are shown.

  18. Further characterization of [3H]gamma-aminobutyric acid release from isolated neuronal growth cones: role of intracellular Ca2+ stores.

    PubMed

    Lockerbie, R O; Gordon-Weeks, P R

    1986-04-01

    We have recently shown that growth cones isolated from neonatal rat forebrain possess uptake and release mechanisms for the neurotransmitter gamma-aminobutyric acid. About half of the K+-induced release of [3H]gamma-aminobutyric acid from isolated growth cones is dependent on extracellular Ca2+. The remaining component of the [3H]gamma-aminobutyric acid release is unaffected by removal of extracellular Ca2+ and is resistant to blockade by the voltage-sensitive Ca2+-channel blocker methoxyverapamil. In the present series of experiments we have used caffeine to assess the possible role of intracellular stores of Ca2+ in supporting that component of the K+-induced release of [3H]gamma-aminobutyric acid from isolated growth cones that is independent of extracellular Ca2+. We have chosen caffeine because of its well established effect of releasing Ca2+ from smooth endoplasmic reticulum in muscle. We found that caffeine can release [3H]gamma-aminobutyric acid from isolated growth cones. This effect persists in Ca2+-free medium, in the presence of methoxyverapamil and in the absence of Na+. Furthermore, isobutylmethylxanthine could not substitute for caffeine suggesting that the caffeine effect is not due to phosphodiesterase inhibition and the subsequent rise in intracellular cyclic nucleotides. A combination of the mitochondrial poisons, Antimycin A and sodium azide had no effect on the release of [3H]gamma-aminobutyric acid induced either by caffeine or by high K+. We conclude that caffeine causes the release of Ca2+ from a non-mitochondrial store within the growth cone and that this Ca2+ store supports that component of the K+-induced release of [3H]gamma-aminobutyric acid that is independent of extracellular Ca2+.

  19. Systematic search for very-high-energy gamma-ray emission from bow shocks of runaway stars

    NASA Astrophysics Data System (ADS)

    H.E.S.S. Collaboration; Abdalla, H.; Abramowski, A.; Aharonian, F.; Ait Benkhali, F.; Akhperjanian, A. G.; Andersson, T.; Angüner, E. O.; Arakawa, M.; Arrieta, M.; Aubert, P.; Backes, M.; Balzer, A.; Barnard, M.; Becherini, Y.; Becker Tjus, J.; Berge, D.; Bernhard, S.; Bernlöhr, K.; Blackwell, R.; Böttcher, M.; Boisson, C.; Bolmont, J.; Bordas, P.; Bregeon, J.; Brun, F.; Brun, P.; Bryan, M.; Büchele, M.; Bulik, T.; Capasso, M.; Carr, J.; Casanova, S.; Cerruti, M.; Chakraborty, N.; Chalme-Calvet, R.; Chaves, R. C. G.; Chen, A.; Chevalier, J.; Chrétien, M.; Coffaro, M.; Colafrancesco, S.; Cologna, G.; Condon, B.; Conrad, J.; Cui, Y.; Davids, I. D.; Decock, J.; Degrange, B.; Deil, C.; Devin, J.; deWilt, P.; Dirson, L.; Djannati-Ataï, A.; Domainko, W.; Donath, A.; Drury, L. O.'C.; Dutson, K.; Dyks, J.; Edwards, T.; Egberts, K.; Eger, P.; Ernenwein, J.-P.; Eschbach, S.; Farnier, C.; Fegan, S.; Fernandes, M. V.; Fiasson, A.; Fontaine, G.; Förster, A.; Funk, S.; Füßling, M.; Gabici, S.; Gajdus, M.; Gallant, Y. A.; Garrigoux, T.; Giavitto, G.; Giebels, B.; Glicenstein, J. F.; Gottschall, D.; Goyal, A.; Grondin, M.-H.; Hahn, J.; Haupt, M.; Hawkes, J.; Heinzelmann, G.; Henri, G.; Hermann, G.; Hervet, O.; Hinton, J. A.; Hofmann, W.; Hoischen, C.; Holler, M.; Horns, D.; Ivascenko, A.; Iwasaki, H.; Jacholkowska, A.; Jamrozy, M.; Janiak, M.; Jankowsky, D.; Jankowsky, F.; Jingo, M.; Jogler, T.; Jouvin, L.; Jung-Richardt, I.; Kastendieck, M. A.; Katarzyński, K.; Katsuragawa, M.; Katz, U.; Kerszberg, D.; Khangulyan, D.; Khélifi, B.; Kieffer, M.; King, J.; Klepser, S.; Klochkov, D.; Kluźniak, W.; Kolitzus, D.; Komin, Nu.; Kosack, K.; Krakau, S.; Kraus, M.; Krüger, P. P.; Laffon, H.; Lamanna, G.; Lau, J.; Lees, J.-P.; Lefaucheur, J.; Lefranc, V.; Lemière, A.; Lemoine-Goumard, M.; Lenain, J.-P.; Leser, E.; Lohse, T.; Lorentz, M.; Liu, R.; López-Coto, R.; Lypova, I.; Marandon, V.; Marcowith, A.; Mariaud, C.; Marx, R.; Maurin, G.; Maxted, N.; Mayer, M.; Meintjes, P. J.; Meyer, M.; Mitchell, A. M. W.; Moderski, R.; Mohamed, M.; Mohrmann, L.; Morå, K.; Moulin, E.; Murach, T.; Nakashima, S.; de Naurois, M.; Niederwanger, F.; Niemiec, J.; Oakes, L.; O'Brien, P.; Odaka, H.; Öttl, S.; Ohm, S.; Ostrowski, M.; Oya, I.; Padovani, M.; Panter, M.; Parsons, R. D.; Pekeur, N. W.; Pelletier, G.; Perennes, C.; Petrucci, P.-O.; Peyaud, B.; Piel, Q.; Pita, S.; Poon, H.; Prokhorov, D.; Prokoph, H.; Pühlhofer, G.; Punch, M.; Quirrenbach, A.; Raab, S.; Reimer, A.; Reimer, O.; Renaud, M.; de los Reyes, R.; Richter, S.; Rieger, F.; Romoli, C.; Rowell, G.; Rudak, B.; Rulten, C. B.; Sahakian, V.; Saito, S.; Salek, D.; Sanchez, D. A.; Santangelo, A.; Sasaki, M.; Schlickeiser, R.; Schüssler, F.; Schulz, A.; Schwanke, U.; Schwemmer, S.; Seglar-Arroyo, M.; Settimo, M.; Seyffert, A. S.; Shafi, N.; Shilon, I.; Simoni, R.; Sol, H.; Spanier, F.; Spengler, G.; Spies, F.; Stawarz, Ł.; Steenkamp, R.; Stegmann, C.; Stycz, K.; Sushch, I.; Takahashi, T.; Tavernet, J.-P.; Tavernier, T.; Taylor, A. M.; Terrier, R.; Tibaldo, L.; Tiziani, D.; Tluczykont, M.; Trichard, C.; Tsuji, N.; Tuffs, R.; Uchiyama, Y.; van der Walt, D. J.; van Eldik, C.; van Rensburg, C.; van Soelen, B.; Vasileiadis, G.; Veh, J.; Venter, C.; Viana, A.; Vincent, P.; Vink, J.; Voisin, F.; Völk, H. J.; Vuillaume, T.; Wadiasingh, Z.; Wagner, S. J.; Wagner, P.; Wagner, R. M.; White, R.; Wierzcholska, A.; Willmann, P.; Wörnlein, A.; Wouters, D.; Yang, R.; Zabalza, V.; Zaborov, D.; Zacharias, M.; Zanin, R.; Zdziarski, A. A.; Zech, A.; Zefi, F.; Ziegler, A.; Żywucka, N.

    2018-04-01

    Context. Runaway stars form bow shocks by ploughing through the interstellar medium at supersonic speeds and are promising sources of non-thermal emission of photons. One of these objects has been found to emit non-thermal radiation in the radio band. This triggered the development of theoretical models predicting non-thermal photons from radio up to very-high-energy (VHE, E ≥ 0.1 TeV) gamma rays. Subsequently, one bow shock was also detected in X-ray observations. However, the data did not allow discrimination between a hot thermal and a non-thermal origin. Further observations of different candidates at X-ray energies showed no evidence for emission at the position of the bow shocks either. A systematic search in the Fermi-LAT energy regime resulted in flux upper limits for 27 candidates listed in the E-BOSS catalogue. Aim. Here we perform the first systematic search for VHE gamma-ray emission from bow shocks of runaway stars. Methods: Using all available archival H.E.S.S. data we search for very-high-energy gamma-ray emission at the positions of bow shock candidates listed in the second E-BOSS catalogue release. Out of the 73 bow shock candidates in this catalogue, 32 have been observed with H.E.S.S. Results: None of the observed 32 bow shock candidates in this population study show significant emission in the H.E.S.S. energy range. Therefore, flux upper limits are calculated in five energy bins and the fraction of the kinetic wind power that is converted into VHE gamma rays is constrained. Conclusions: Emission from stellar bow shocks is not detected in the energy range between 0.14 and 18 TeV.The resulting upper limits constrain the level of VHE gamma-ray emission from these objects down to 0.1-1% of the kinetic wind energy.

  20. Method of incident low-energy gamma-ray direction reconstruction in the GAMMA-400 gamma-ray space telescope

    NASA Astrophysics Data System (ADS)

    Kheymits, M. D.; Leonov, A. A.; Zverev, V. G.; Galper, A. M.; Arkhangelskaya, I. V.; Arkhangelskiy, A. I.; Suchkov, S. I.; Topchiev, N. P.; Yurkin, Yu T.; Bakaldin, A. V.; Dalkarov, O. D.

    2016-02-01

    The GAMMA-400 gamma-ray space-based telescope has as its main goals to measure cosmic γ-ray fluxes and the electron-positron cosmic-ray component produced, theoretically, in dark-matter-particles decay or annihilation processes, to search for discrete γ-ray sources and study them in detail, to examine the energy spectra of diffuse γ-rays — both galactic and extragalactic — and to study gamma-ray bursts (GRBs) and γ-rays from the active Sun. Scientific goals of GAMMA-400 telescope require fine angular resolution. The telescope is of a pair-production type. In the converter-tracker, the incident gamma-ray photon converts into electron-positron pair in the tungsten layer and then the tracks are detected by silicon- strip position-sensitive detectors. Multiple scattering processes become a significant obstacle in the incident-gamma direction reconstruction for energies below several gigaelectronvolts. The method of utilising this process to improve the resolution is proposed in the presented work.

  1. Accurate Wavelength Measurement of High-Energy Gamma Rays from the 35Cl(n,{gamma}) Reactions

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

    Belgya, T.; Molnar, G.L.; Mutti, P.

    2005-05-24

    The energies of eight gamma rays in the 36Cl level scheme have been measured with high precision using the 35Cl(n,{gamma}) reaction and the GAMS4 spectrometer. From these energies, a skeleton decay scheme for 36Cl was constructed, and the binding energy of 36Cl was determined to higher precision than previously. It is shown that using this new information, binding energy determination from Ge detector experiments for other nuclei can also be made with higher precision than now available. The measurement of additional weaker 36Cl gamma rays is continuing.

  2. Gamma-ray, neutron, and hard X-ray studies and requirements for a high-energy solar physics facility

    NASA Technical Reports Server (NTRS)

    Ramaty, R.; Dennis, B. R.; Emslie, A. G.

    1988-01-01

    The requirements for future high-resolution spatial, spectral, and temporal observation of hard X-rays, gamma rays and neutrons from solar flares are discussed in the context of current high-energy flare observations. There is much promise from these observations for achieving a deep understanding of processes of energy release, particle acceleration and particle transport in a complicated environment such as the turbulent and highly magnetized atmosphere of the active sun.

  3. Estimation of neutron energy distributions from prompt gamma emissions

    NASA Astrophysics Data System (ADS)

    Panikkath, Priyada; Udupi, Ashwini; Sarkar, P. K.

    2017-11-01

    A technique of estimating the incident neutron energy distribution from emitted prompt gamma intensities from a system exposed to neutrons is presented. The emitted prompt gamma intensities or the measured photo peaks in a gamma detector are related to the incident neutron energy distribution through a convolution of the response of the system generating the prompt gammas to mono-energetic neutrons. Presently, the system studied is a cylinder of high density polyethylene (HDPE) placed inside another cylinder of borated HDPE (BHDPE) having an outer Pb-cover and exposed to neutrons. The emitted five prompt gamma peaks from hydrogen, boron, carbon and lead can be utilized to unfold the incident neutron energy distribution as an under-determined deconvolution problem. Such an under-determined set of equations are solved using the genetic algorithm based Monte Carlo de-convolution code GAMCD. Feasibility of the proposed technique is demonstrated theoretically using the Monte Carlo calculated response matrix and intensities of emitted prompt gammas from the Pb-covered BHDPE-HDPE system in the case of several incident neutron spectra spanning different energy ranges.

  4. A novel system to diagnose cutaneous adverse drug reactions employing the cellscan--comparison with histamine releasing test and Inf-gamma Releasing Test.

    PubMed

    Goldberg, Ilan; Gilburd, Boris; Kravitz, Martine Szyper; Kivity, Shmuel; Chaim, Berta Ben; Klein, Tirza; Schiffenbauer, Yael; Trubniykovr, Ela; Brenner, Sarah; Shoenfeld, Yehuda

    2005-03-01

    There are several mechanisms to describe allergic drug reactions yet the methods to diagnose them are limited. To compare several conventional clinical and laboratory methods to diagnose skin reactions to drugs to a new method of diagnosing drug reactions by the CellScan system. The study entailed 21 patients who were diagnosed as suffering from drug eruptions, and 105 healthy controls with no history of drug allergy. The drugs were classified into two groups according to suspicion of causing drug allergy: high and low. Most of the patients were on more than one drug, leading to 41 patient-drug interactions (assays). Histamine releasing test (HRT), interferon (INF)-gamma releasing test and CellScan examination were performed on lymphocytes of the patients and controls. The HRTwas interpreted as positive in 9 out of 18 (50%) patients and in 13 out of 35 (37%) assays. Based on the INF-gamma releasing test, positive results were observed in 16 out of 21 (76%) patients and in 24 out of 41 (59%) assays. In the CellScan test (CST), positive results were observed in 17 out of 21 (81%) patients and in 29 out of 41 (71%) assays. The rate of identifying the drug for eruption in the high suspicion level drugs was 9 out of 22 (41%) assays in the HRT, 20 out of 24 (83%) assays in the INF-gamma releasing test, and 21 out of 24 (87%) studies with the CellScan method. The rate of determining of the drug that caused the eruption in the low suspicion level drugs was 4 out of 13 (31 %) in the HRT, 4 out of 17 (24%) assays in the INF-gamma releasing test, and 8 out of 17 (47%) analyses in the CST. When examined in the CellScan, 99 out of 105 (94%) controls were interpreted as negative. This preliminary study indicates that the CellScan seems to be an easy and promising method for the detection of drugs responsible for adverse skin reactions. In contrast to the HRT and to the Interferon-gamma secretion test, the CellScan method is characterized by its ability to track and monitor the

  5. Gamma ray energy tracking in GRETINA

    NASA Astrophysics Data System (ADS)

    Lee, I. Y.

    2011-10-01

    The next generation of stable and exotic beam accelerators will provide physics opportunities to study nuclei farther away from the line of stability. However, these experiments will be more demanding on instrumentation performance. These come from the lower production rate for more exotic beams, worse beam impurities, and large beam velocity from the fragmentation and inverse reactions. Gamma-ray spectroscopy will be one of the most effective tools to study exotic nuclei. However, to fully exploit the physics reach provided by these new facilities, better gamma-ray detector will be needed. In the last 10 years, a new concept, gamma-ray energy tracking array, was developed. Tracking arrays will increase the detection sensitivity by factors of several hundred compared to current arrays used in nuclear physics research. Particularly, the capability of reconstructing the position of the interaction with millimeters resolution is needed to correct the Doppler broadening of gamma rays emitted from high velocity nuclei. GRETINA is a gamma-ray tracking array which uses 28 Ge crystals, each with 36 segments, to cover ¼ of the 4 π of the 4 π solid angle. The gamma ray tracking technique requires detailed pulse shape information from each of the segments. These pulses are digitized using 14-bit 100 MHz flash ADCs, and digital signal analysis algorithms implemented in the on-board FPGAs provides energy, time and selection of pulse traces. A digital trigger system, provided flexible trigger functions including a fast trigger output, and also allows complicated trigger decisions to be made up to 20 microseconds. Further analyzed, carried out in a computer cluster, determine the energy, time, and three-dimensional positions of all gamma-ray interactions in the array. This information is then utilized, together with the characteristics of Compton scattering and pair-production processes, to track the scattering sequences of the gamma rays. GRETINA construction is completed in

  6. The Extragalactic Background Light and the Gamma-ray Opacity of the Universe

    NASA Technical Reports Server (NTRS)

    Dwek, Eli; Krennrich, Frank

    2012-01-01

    The extragalactic background light (EBL) is one of the fundamental observational quantities in cosmology. All energy releases from resolved and unresolved extragalactic sources, and the light from any truly diffuse background, excluding the cosmic microwave background (CMB), contribute to its intensity and spectral energy distribution. It therefore plays a crucial role in cosmological tests for the formation and evolution of stellar objects and galaxies, and for setting limits on exotic energy releases in the universe. The EBL also plays an important role in the propagation of very high energy gamma-rays which are attenuated en route to Earth by pair producing gamma-gamma interactions with the EBL and CMB. The EBL affects the spectrum of the sources, predominantly blazars, in the approx 10 GeV to 10 TeV energy regime. Knowledge of the EBL intensity and spectrum will allow the determination of the intrinsic blazar spectrum in a crucial energy regime that can be used to test particle acceleration mechanisms and VHE gamma-ray production models. Conversely, knowledge of the intrinsic gamma-ray spectrum and the detection of blazars at increasingly higher redshifts will set strong limits on the EBL and its evolution. This paper reviews the latest developments in the determination of the EBL and its impact on the current understanding of the origin and production mechanisms of gamma-rays in blazars, and on energy releases in the universe. The review concludes with a summary and future directions in Cherenkov Telescope Array techniques and in infrared ground-based and space observatories that will greatly improve our knowledge of the EBL and the origin and production of very high energy gamma-rays.

  7. The relationship between Q gamma and Ca release from the sarcoplasmic reticulum in skeletal muscle

    PubMed Central

    1991-01-01

    Asymmetric membrane currents and fluxes of Ca2+ release were determined in skeletal muscle fibers voltage clamped in a Vaseline-gap chamber. The conditioning pulse protocol 1 for suppressing Ca2+ release and the "hump" component of charge movement current (I gamma), described in the first paper of this series, was applied at different test pulse voltages. The amplitude of the current suppressed during the ON transient reached a maximum at slightly suprathreshold test voltages (- 50 to -40 mV) and decayed at higher voltages. The component of charge movement current suppressed by 20 microM tetracaine also went through a maximum at low pulse voltages. This anomalous voltage dependence is thus a property of I gamma, defined by either the conditioning protocol or the tetracaine effect. A negative (inward-going) phase was often observed in the asymmetric current during the ON of depolarizing pulses. This inward phase was shown to be an intramembranous charge movement based on (a) its presence in the records of total membrane current, (b) its voltage dependence, with a maximum at slightly suprathreshold voltages, (c) its association with a "hump" in the asymmetric current, (d) its inhibition by interventions that reduce the "hump", (e) equality of ON and OFF areas in the records of asymmetric current presenting this inward phase, and (f) its kinetic relationship with the time derivative of Ca release flux. The nonmonotonic voltage dependence of the amplitude of the hump and the possibility of an inward phase of intramembranous charge movement are used as the main criteria in the quantitative testing of a specific model. According to this model, released Ca2+ binds to negatively charged sites on the myoplasmic face of the voltage sensor and increases the local transmembrane potential, thus driving additional charge movement (the hump). This model successfully predicts the anomalous voltage dependence and all the kinetic properties of I gamma described in the previous

  8. Observational clues to the energy release process in impulsive solar bursts

    NASA Technical Reports Server (NTRS)

    Batchelor, David

    1990-01-01

    The nature of the energy release process that produces impulsive bursts of hard X-rays and microwaves during solar flares is discussed, based on new evidence obtained using the method of Crannell et al. (1978). It is shown that the hard X-ray spectral index gamma is negatively correlated with the microwave peak frequency, suggesting a common source for the microwaves and X-rays. The thermal and nonthermal models are compared. It is found that the most straightforward explanations for burst time behavior are shock-wave particle acceleration in the nonthermal model and thermal conduction fronts in the thermal model.

  9. Energy release in solar flares

    NASA Technical Reports Server (NTRS)

    Brown, John C.; Correia, Emilia; Farnik, Frantisek; Garcia, Howard; Henoux, Jean-Claude; La Rosa, Ted N.; Machado, Marcos E. (Compiler); Nakajima, Hiroshi; Priest, Eric R.

    1994-01-01

    Team 2 of the Ottawa Flares 22 Workshop dealt with observational and theoretical aspects of the characteristics and processes of energy release in flares. Main results summarized in this article stress the global character of the flaring phenomenon in active regions, the importance of discontinuities in magnetic connectivity, the role of field-aligned currents in free energy storage, and the fragmentation of energy release in time and space.

  10. Studies of the Low-energy Gamma Background

    NASA Astrophysics Data System (ADS)

    Bikit, K.; Mrđa, D.; Bikit, I.; Slivka, J.; Veskovic, M.; Knezevic, D.

    The investigations of contribution to the low-energy part of background gamma spectrum (below 100 keV) and knowing detection efficiency for this region are important for both, a fundamental, as well as for applied research. In this work, the components contributing to the low-energy region of background gamma spectrum for shielded detector are analyzed, including the production and spectral distribution of muon-induced continuous low-energy radiation in the vicinity of high-purity germanium detector.In addition, the detection efficiency for low energy gamma region is determined using the GEANT 4 simulation package. This technique offers excellent opportunity to predict the detection response in mentioned region. Unfortunately, the frequently weakly known dead layer thickness on the surface of the extended-range detector, as well as some processes which are not incorporated in simulation (e.g. charge collection from detector active volume) may limit the reliability of simulation technique. Thus, the 14, 17, 21, 26, 33, 59.5 keV transitions in the calibrated 241Am point source were used to check the simulated efficiencies.

  11. Peroxisome-proliferator-activated receptor-{gamma} agonists inhibit the release of proinflammatory cytokines from RSV-infected epithelial cells

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

    Arnold, Ralf; Koenig, Wolfgang

    2006-03-15

    The epithelial cells of the airways are the target cells for respiratory syncytial virus (RSV) infection and the site of the majority of the inflammation associated with the disease. Recently, peroxisome-proliferator-activated receptor {gamma} (PPAR{gamma}), a member of the nuclear hormone receptor superfamily, has been shown to possess anti-inflammatory properties. Therefore, we investigated the role of PPAR{gamma} agonists (15d-PGJ{sub 2}, ciglitazone and troglitazone) on the synthesis of RSV-induced cytokine release from RSV-infected human lung epithelial cells (A549). We observed that all PPAR{gamma} ligands inhibited dose-dependently the release of TNF-{alpha}, GM-CSF, IL-1{alpha}, IL-6 and the chemokines CXCL8 (IL-8) and CCL5 (RANTES) frommore » RSV-infected A549 cells. Concomitantly, the PPAR{gamma} ligands diminished the cellular amount of mRNA encoding for IL-6, CXCL8 and CCL5 and the RSV-induced binding activity of the transcription factors NF-{kappa}B (p65/p50) and AP-1 (c-fos), respectively. Our data presented herein suggest a potential application of PPAR{gamma} ligands in the anti-inflammatory treatment of RSV infection.« less

  12. Understanding the connection between the energy released during solar flares and their emission in the lower atmosphere

    NASA Astrophysics Data System (ADS)

    da Costa, F. Rubio

    2017-10-01

    While progress has been made on understanding how energy is released and deposited along the solar atmosphere during explosive events such as solar flares, the chromospheric and coronal heating through the sudden release of magnetic energy remain an open problem in solar physics. Recent hydrodynamic models allow to investigate the energy deposition along a flare loop and to study the response of the chromosphere. These results have been improved with the consideration of transport and acceleration of particles along the loop. RHESSI and Fermi/GBM X-ray and gamma-ray observations help to constrain the spectral properties of the injected electrons. The excellent spatial, spectral and temporal resolution of IRIS will also help us to constrain properties of explosive events, such as the continuum emission during flares or their emission in the chromosphere.

  13. A gamma-ray burst with a high-energy spectral component inconsistent with the synchrotron shock model.

    PubMed

    González, M M; Dingus, B L; Kaneko, Y; Preece, R D; Dermer, C D; Briggs, M S

    2003-08-14

    Gamma-ray bursts are among the most powerful events in nature. These events release most of their energy as photons with energies in the range from 30 keV to a few MeV, with a smaller fraction of the energy radiated in radio, optical, and soft X-ray afterglows. The data are in general agreement with a relativistic shock model, where the prompt and afterglow emissions correspond to synchrotron radiation from shock-accelerated electrons. Here we report an observation of a high-energy (multi-MeV) spectral component in the burst of 17 October 1994 that is distinct from the previously observed lower-energy gamma-ray component. The flux of the high-energy component decays more slowly and its fluence is greater than the lower-energy component; it is described by a power law of differential photon number index approximately -1 up to about 200 MeV. This observation is difficult to explain with the standard synchrotron shock model, suggesting the presence of new phenomena such as a different non-thermal electron process, or the interaction of relativistic protons with photons at the source.

  14. Neutron Capture Energies for Flux Normalization and Approximate Model for Gamma-Smeared Power

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

    Kim, Kang Seog; Clarno, Kevin T.; Liu, Yuxuan

    The Consortium for Advanced Simulation of Light Water Reactors (CASL) Virtual Environment for Reactor Applications (VERA) neutronics simulator MPACT has used a single recoverable fission energy for each fissionable nuclide assuming that all recoverable energies come only from fission reaction, for which capture energy is merged with fission energy. This approach includes approximations and requires improvement by separating capture energy from the merged effective recoverable energy. This report documents the procedure to generate recoverable neutron capture energies and the development of a program called CapKappa to generate capture energies. Recoverable neutron capture energies have been generated by using CapKappa withmore » the evaluated nuclear data file (ENDF)/B-7.0 and 7.1 cross section and decay libraries. The new capture kappas were compared to the current SCALE-6.2 and the CASMO-5 capture kappas. These new capture kappas have been incorporated into the Simplified AMPX 51- and 252-group libraries, and they can be used for the AMPX multigroup (MG) libraries and the SCALE code package. The CASL VERA neutronics simulator MPACT does not include a gamma transport capability, which limits it to explicitly estimating local energy deposition from fission, neutron, and gamma slowing down and capture. Since the mean free path of gamma rays is typically much longer than that for the neutron, and the total gamma energy is about 10% to the total energy, the gamma-smeared power distribution is different from the fission power distribution. Explicit local energy deposition through neutron and gamma transport calculation is significantly important in multi-physics whole core simulation with thermal-hydraulic feedback. Therefore, the gamma transport capability should be incorporated into the CASL neutronics simulator MPACT. However, this task will be timeconsuming in developing the neutron induced gamma production and gamma cross section libraries. This study is to

  15. Search of the energetic gamma-ray experiment telescope (EGRET) data for high-energy gamma-ray microsecond bursts

    NASA Technical Reports Server (NTRS)

    Fichtel, C. E.; Bertsch, D. L.; Dingus, B. L.; Esposito, J. A.; Hartman, R. C.; Hunter, S. D.; Kanbach, G.; Kniffen, D. A.; Lin, Y. C.; Mattox, J. R.

    1994-01-01

    Hawking (1974) and Page & Hawking (1976) investigated theoretically the possibility of detecting high-energy gamma rays produced by the quantum-mechanical decay of a small black hole created in the early universe. They concluded that, at the very end of the life of the small black hole, it would radiate a burst of gamma rays peaked near 250 MeV with a total energy of about 10(exp 34) ergs in the order of a microsecond or less. The characteristics of a black hole are determined by laws of physics beyond the range of current particle accelerators; hence, the search for these short bursts of high-energy gamma rays provides at least the possibility of being the first test of this region of physics. The Compton Observatory Energetic Gamma-Ray Experiment Telescope (EGRET) has the capability of detecting directly the gamma rays from such bursts at a much fainter level than SAS 2, and a search of the EGRET data has led to an upper limit of 5 x 10(exp -2) black hole decays per cu pc per yr, placing constraints on this and other theories predicting microsecond high-energy gamma-ray bursts.

  16. OV-104's RMS releases Gamma Ray Observatory (GRO) during STS-37 deployment

    NASA Image and Video Library

    1991-04-07

    Atlantis', Orbiter Vehicle (OV) 104's, remote manipulator system (RMS) releases Gamma Ray Observatory (GRO) during STS-37 deployment. Visible on the GRO as it drifts away from the RMS end effector are the four complement instruments: the Energetic Gamma Ray Experiment (bottom); Imaging Compton Telescope (COMPTEL) (center); Oriented Scintillation Spectrometer Experiment (OSSE) (top); and Burst and Transient Source Experiment (BATSE) (at four corners). GRO's solar array (SA) panels are extended and are in orbit configuration. View was taken through aft flight deck window which reflects some of the crew compartment interior.

  17. Forecasting of future earthquakes in the northeast region of India considering energy released concept

    NASA Astrophysics Data System (ADS)

    Zarola, Amit; Sil, Arjun

    2018-04-01

    This study presents the forecasting of time and magnitude size of the next earthquake in the northeast India, using four probability distribution models (Gamma, Lognormal, Weibull and Log-logistic) considering updated earthquake catalog of magnitude Mw ≥ 6.0 that occurred from year 1737-2015 in the study area. On the basis of past seismicity of the region, two types of conditional probabilities have been estimated using their best fit model and respective model parameters. The first conditional probability is the probability of seismic energy (e × 1020 ergs), which is expected to release in the future earthquake, exceeding a certain level of seismic energy (E × 1020 ergs). And the second conditional probability is the probability of seismic energy (a × 1020 ergs/year), which is expected to release per year, exceeding a certain level of seismic energy per year (A × 1020 ergs/year). The logarithm likelihood functions (ln L) were also estimated for all four probability distribution models. A higher value of ln L suggests a better model and a lower value shows a worse model. The time of the future earthquake is forecasted by dividing the total seismic energy expected to release in the future earthquake with the total seismic energy expected to release per year. The epicentre of recently occurred 4 January 2016 Manipur earthquake (M 6.7), 13 April 2016 Myanmar earthquake (M 6.9) and the 24 August 2016 Myanmar earthquake (M 6.8) are located in zone Z.12, zone Z.16 and zone Z.15, respectively and that are the identified seismic source zones in the study area which show that the proposed techniques and models yield good forecasting accuracy.

  18. Albedo gamma-rays observation at energies above 30 MeV

    NASA Astrophysics Data System (ADS)

    Galper, A. M.; Grachev, V. M.; Dmitrenko, V. V.; Kirillov-Ugriumov, V. G.; Liakhov, V. A.; Prokhorova, L. A.; Riumin, V. V.; Ulin, S. E.

    Albedo gamma-ray observations are presented, which were carried out with the small gamma-ray telescope Elena-F on Salyut-6 at the 30-410 MeV and 50-420 MeV energy ranges. For the equatorial region from 15.0-17.5 GV, the albedo gamma-ray fluxes are 40 plus or minus 20 ph/sq m-s-sr, and the measured power law index of the differential energy spectrum is 1.6 plus or minus 0.5. The orbital station data are compared with simultaneous observations performed on a balloon, and the power law index of the differential energy spectrum of albedo gamma-rays measured by the balloon amounts to 2.1 plus or minus 0.4.

  19. Building an Efficient Model for Afterburn Energy Release

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

    Alves, S; Kuhl, A; Najjar, F

    2012-02-03

    Many explosives will release additional energy after detonation as the detonation products mix with the ambient environment. This additional energy release, referred to as afterburn, is due to combustion of undetonated fuel with ambient oxygen. While the detonation energy release occurs on a time scale of microseconds, the afterburn energy release occurs on a time scale of milliseconds with a potentially varying energy release rate depending upon the local temperature and pressure. This afterburn energy release is not accounted for in typical equations of state, such as the Jones-Wilkins-Lee (JWL) model, used for modeling the detonation of explosives. Here wemore » construct a straightforward and efficient approach, based on experiments and theory, to account for this additional energy release in a way that is tractable for large finite element fluid-structure problems. Barometric calorimeter experiments have been executed in both nitrogen and air environments to investigate the characteristics of afterburn for C-4 and other materials. These tests, which provide pressure time histories, along with theoretical and analytical solutions provide an engineering basis for modeling afterburn with numerical hydrocodes. It is toward this end that we have constructed a modified JWL equation of state to account for afterburn effects on the response of structures to blast. The modified equation of state includes a two phase afterburn energy release to represent variations in the energy release rate and an afterburn energy cutoff to account for partial reaction of the undetonated fuel.« less

  20. New Fermi-LAT event reconstruction reveals more high-energy gamma rays from gamma-ray bursts

    DOE PAGES

    Atwood, W. B.; Baldini, L.; Bregeon, J.; ...

    2013-08-19

    Here, based on the experience gained during the four and a half years of the mission, the Fermi-LAT Collaboration has undertaken a comprehensive revision of the event-level analysis going under the name of Pass 8. Although it is not yet finalized, we can test the improvements in the new event reconstruction with the special case of the prompt phase of bright gamma-ray bursts (GRBs), where the signal-to-noise ratio is large enough that loose selection cuts are sufficient to identify gamma rays associated with the source. Using the new event reconstruction, we have re-analyzed 10 GRBs previously detected by the Largemore » Area Telescope (LAT) for which an X-ray/optical follow-up was possible and found four new gamma rays with energies greater than 10 GeV in addition to the seven previously known. Among these four is a 27.4 GeV gamma ray from GRB 080916C, which has a redshift of 4.35, thus making it the gamma ray with the highest intrinsic energy (~147 GeV) detected from a GRB. We present here the salient aspects of the new event reconstruction and discuss the scientific implications of these new high-energy gamma rays, such as constraining extragalactic background light models, Lorentz invariance violation tests, the prompt emission mechanism, and the bulk Lorentz factor of the emitting region.« less

  1. High-energy emission in gamma-ray bursts

    NASA Technical Reports Server (NTRS)

    Matz, S. M.; Forrest, D. J.; Vestrand, W. T.; Chupp, E. L.; Share, G. H.; Rieger, E.

    1985-01-01

    Between February 1980 and August 1983 the Gamma-Ray Spectrometer on the Solar Maximum Mission Satellite (SMM) detected 72 events identified as being of cosmic origin. These events are an essentially unbiased subset of all gamma-ray bursts. The measured spectra of these events show that high energy (greater than 1 MeV) emission is a common and energetically important feature. There is no evidence for a general high-energy cut-off or a distribution of cut-offs below about 6 MeV. These observations imply a limit on the preferential beaming of high energy emission. This constraint, combined with the assumption of isotropic low energy emission, implies that the typical magnetic field strength at burst radiation sites is less than 1 x 10 to the 12th gauss.

  2. Gamma-ray astronomy: From Fermi up to the HAWC high-energy {gamma}-ray observatory in Sierra Negra

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

    Carraminana, Alberto; Collaboration: HAWC Collaboration

    Gamma-rays represent the most energetic electromagnetic window for the study of the Universe. They are studied both from space at MeV and GeV energies, with instruments like the Fermi{gamma}-ray Space Telescope, and at TeV energies with ground based instruments profiting of particle cascades in the atmosphere and of the Cerenkov radiation of charged particles in the air or in water. The Milagro gamma-ray observatory represented the first instrument to successfully implement the water Cerenkov technique for {gamma}-ray astronomy, opening the ground for the more sensitive HAWC {gamma}-ray observatory, currently under development in the Sierra Negra site and already providing earlymore » science results.« less

  3. Hard X-ray and low-energy gamma-ray spectrometers

    NASA Technical Reports Server (NTRS)

    Gehrels, N.; Crannell, C. J.; Orwig, L. E.; Forrest, D. J.; Lin, R. P.; Starr, R.

    1988-01-01

    Basic principles of operation and characteristics of scintillation and semi-conductor detectors used for solar hard X-ray and gamma-ray spectrometers are presented. Scintillation materials such as NaI offer high stopping power for incident gamma rays, modest energy resolution, and relatively simple operation. They are, to date, the most often used detector in solar gamma-ray spectroscopy. The scintillator BGO has higher stopping power than NaI, but poorer energy resolution. The primary advantage of semi-conductor materials such as Ge is their high-energy resolution. Monte-Carlo simulations of the response of NaI and Ge detectors to model solar flare inputs show the benefit of high resoluton for studying spectral lines. No semi-conductor material besides Ge is currently available with adequate combined size and purity to make general-use hard X-ray and gamma-ray detectors for solar studies.

  4. Quantification of Energy Release in Composite Structures

    NASA Technical Reports Server (NTRS)

    Minnetyan, Levon

    2003-01-01

    Energy release rate is usually suggested as a quantifier for assessing structural damage tolerance. Computational prediction of energy release rate is based on composite mechanics with micro-stress level damage assessment, finite element structural analysis and damage progression tracking modules. This report examines several issues associated with energy release rates in composite structures as follows: Chapter I demonstrates computational simulation of an adhesively bonded composite joint and validates the computed energy release rates by comparison with acoustic emission signals in the overall sense. Chapter II investigates the effect of crack plane orientation with respect to fiber direction on the energy release rates. Chapter III quantifies the effects of contiguous constraint plies on the residual stiffness of a 90 ply subjected to transverse tensile fractures. Chapter IV compares ICAN and ICAN/JAVA solutions of composites. Chapter V examines the effects of composite structural geometry and boundary conditions on damage progression characteristics.

  5. Quantification of Energy Release in Composite Structures

    NASA Technical Reports Server (NTRS)

    Minnetyan, Levon; Chamis, Christos C. (Technical Monitor)

    2003-01-01

    Energy release rate is usually suggested as a quantifier for assessing structural damage tolerance. Computational prediction of energy release rate is based on composite mechanics with micro-stress level damage assessment, finite element structural analysis and damage progression tracking modules. This report examines several issues associated with energy release rates in composite structures as follows: Chapter I demonstrates computational simulation of an adhesively bonded composite joint and validates the computed energy release rates by comparison with acoustic emission signals in the overall sense. Chapter II investigates the effect of crack plane orientation with respect to fiber direction on the energy release rates. Chapter III quantifies the effects of contiguous constraint plies on the residual stiffness of a 90 deg ply subjected to transverse tensile fractures. Chapter IV compares ICAN and ICAN/JAVA solutions of composites. Chapter V examines the effects of composite structural geometry and boundary conditions on damage progression characteristics.

  6. Very High Energy Gamma Ray Extension of GRO Observations

    NASA Technical Reports Server (NTRS)

    Weekes, Trevor C.

    1994-01-01

    The membership, progress, and invited talks, publications, and proceedings made by the Whipple Gamma Ray Collaboration is reported for june 1990 through May 1994. Progress was made in the following areas: the May 1994 Markarian Flare at Whipple and EGRET (Energetic Gamma Ray Experiment Telescope) energies; AGN's (Active Galactic Nuclei); bursts; supernova remnants; and simulations and energy spectra.

  7. Significance of medium energy gamma ray astronomy in the study of cosmic rays

    NASA Technical Reports Server (NTRS)

    Fichtel, C. E.; Kniffen, D. A.; Thompson, D. J.; Bignami, G. F.; Cheung, C. Y.

    1975-01-01

    Medium energy (about 10 to 30 MeV) gamma ray astronomy provides information on the product of the galactic electron cosmic ray intensity and the galactic matter to which the electrons are dynamically coupled by the magnetic field. Because high energy (greater than 100 MeV) gamma ray astronomy provides analogous information for the nucleonic cosmic rays and the relevant matter, a comparison between high energy and medium energy gamma ray intensities provides a direct ratio of the cosmic ray electrons and nucleons throughout the galaxy. A calculation of gamma ray production by electron bremsstrahlung shows that: bremsstrahlung energy loss is probably not negligible over the lifetime of the electrons in the galaxy; and the approximate bremsstrahlung calculation often used previously overestimates the gamma ray intensity by about a factor of two. As a specific example, expected medium energy gamma ray intensities are calculated for the speral arm model.

  8. Inverse modelling of radionuclide release rates using gamma dose rate observations

    NASA Astrophysics Data System (ADS)

    Hamburger, Thomas; Stohl, Andreas; von Haustein, Christoph; Thummerer, Severin; Wallner, Christian

    2014-05-01

    relatively sparse grid and the temporal resolution of available data may be low within the order of hours or a day. Gamma dose rates on the other hand are observed routinely on a much denser grid and higher temporal resolution. Gamma dose rate measurements contain no explicit information on the observed spectrum of radionuclides and have to be interpreted carefully. Nevertheless, they provide valuable information for the inverse evaluation of the source term due to their availability (Saunier et al., 2013). We present a new inversion approach combining an atmospheric dispersion model and observations of radionuclide activity concentrations and gamma dose rates to obtain the source term of radionuclides. We use the Lagrangian particle dispersion model FLEXPART (Stohl et al., 1998; Stohl et al., 2005) to model the atmospheric transport of the released radionuclides. The gamma dose rates are calculated from the modelled activity concentrations. The inversion method uses a Bayesian formulation considering uncertainties for the a priori source term and the observations (Eckhardt et al., 2008). The a priori information on the source term is a first guess. The gamma dose rate observations will be used with inverse modelling to improve this first guess and to retrieve a reliable source term. The details of this method will be presented at the conference. This work is funded by the Bundesamt für Strahlenschutz BfS, Forschungsvorhaben 3612S60026. References Davoine, X. and Bocquet, M., Atmos. Chem. Phys., 7, 1549-1564, 2007. Devell, L., et al., OCDE/GD(96)12, 1995. Eckhardt, S., et al., Atmos. Chem. Phys., 8, 3881-3897, 2008. Saunier, O., et al., Atmos. Chem. Phys., 13, 11403-11421, 2013. Stohl, A., et al., Atmos. Environ., 32, 4245-4264, 1998. Stohl, A., et al., Atmos. Chem. Phys., 5, 2461-2474, 2005. Stohl, A., et al., Atmos. Chem. Phys., 12, 2313-2343, 2012.

  9. Search for medium-energy gamma-ray pulsars

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

    Sweeney, W.E. Jr.

    1987-01-01

    Results are presented from a search for pulsed gamma rays from four radio pulsars, chosen for their interest to gamma-ray astronomers in previous studies. The data set used for the search consists of gamma-ray events at energies of 1-30 MeV, detected during a 40-hour balloon flight of the UCR double Compton scatter telescope launched at the National Scientific Balloon Facility in Palestine, Texas, USA on September 30, 1978. No statistically significant signals were detected from any of the pulsars. Three sigma upper limits to pulsed 1-30 MeV gamma ray flux from PSR 0950+08, PSR 1822+09, PSR 1929+10, and PSR 1953+29more » are presented. Two complete exposures to PSR 0950+08 were obtained. The reported tentative detection of 1-20 MeV gamma rays from PSR 0950+08 is not confirmed.« less

  10. Energy input and response from prompt and early optical afterglow emission in gamma-ray bursts.

    PubMed

    Vestrand, W T; Wren, J A; Wozniak, P R; Aptekar, R; Golentskii, S; Pal'shin, V; Sakamoto, T; White, R R; Evans, S; Casperson, D; Fenimore, E

    2006-07-13

    The taxonomy of optical emission detected during the critical first few minutes after the onset of a gamma-ray burst (GRB) defines two broad classes: prompt optical emission correlated with prompt gamma-ray emission, and early optical afterglow emission uncorrelated with the gamma-ray emission. The standard theoretical interpretation attributes prompt emission to internal shocks in the ultra-relativistic outflow generated by the internal engine; early afterglow emission is attributed to shocks generated by interaction with the surrounding medium. Here we report on observations of a bright GRB that, for the first time, clearly show the temporal relationship and relative strength of the two optical components. The observations indicate that early afterglow emission can be understood as reverberation of the energy input measured by prompt emission. Measurements of the early afterglow reverberations therefore probe the structure of the environment around the burst, whereas the subsequent response to late-time impulsive energy releases reveals how earlier flaring episodes have altered the jet and environment parameters. Many GRBs are generated by the death of massive stars that were born and died before the Universe was ten per cent of its current age, so GRB afterglow reverberations provide clues about the environments around some of the first stars.

  11. Ground-based very high energy gamma ray astronomy: Observational highlights

    NASA Technical Reports Server (NTRS)

    Turver, K. E.

    1986-01-01

    It is now more than 20 years since the first ground based gamma ray experiments involving atmospheric Cerenkov radiation were undertaken. The present highlights in observational ground-based very high energy (VHE) gamma ray astronomy and the optimism about an interesting future for the field follow progress in these areas: (1) the detection at increased levels of confidence of an enlarged number of sources so that at present claims were made for the detection, at the 4 to 5 sd level of significance, of 8 point sources; (2) the replication of the claimed detections with, for the first time, confirmation of the nature and detail of the emission; and (3) the extension of gamma ray astronomy to the ultra high energy (UHE) domain. The pattern, if any, to emerge from the list of sources claimed so far is that X-ray binary sources appear to be copious emitters of gamma rays over at least 4 decades of energy. These X-ray sources which behave as VHE and UHE gamma ray emitters are examined.

  12. Prospects for future very high-energy gamma-ray sky survey: Impact of secondary gamma rays

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

    Inoue, Yoshiyuki; Kalashev, Oleg E.; Kusenko, Alexander

    2014-02-01

    Very high-energy gamma-ray measurements of distant blazars can be well explained by secondary gamma rays emitted by cascades induced by ultra-high-energy cosmic rays. The secondary gamma rays will enable one to detect a large number of blazars with future ground based gamma-ray telescopes such as Cherenkov Telescope Array (CTA). We show that the secondary emission process will allow CTA to detect 100, 130, 150, 87, and 8 blazars above 30 GeV, 100 GeV, 300 GeV, 1 TeV, and 10 TeV, respectively, up to z~8 assuming the intergalactic magnetic field (IGMF) strength B=10-17 G and an unbiased all sky survey withmore » 0.5 h exposure at each field of view, where total observing time is ~540 h. These numbers will be 79, 96, 110, 63, and 6 up to z~5 in the case of B=10-15 G. This large statistics of sources will be a clear evidence of the secondary gamma-ray scenarios and a new key to studying the IGMF statistically. We also find that a wider and shallower survey is favored to detect more and higher redshift sources even if we take into account secondary gamma rays.« less

  13. High energy gamma ray results from the second small astronomy satellite

    NASA Technical Reports Server (NTRS)

    Fichtel, C. E.; Hartman, R. C.; Kniffen, D. A.; Thompson, D. J.; Bignami, G. F.; Oegelman, H.; Oezel, M. F.; Tuemer, T.

    1974-01-01

    A high energy (35 MeV) gamma ray telescope employing a thirty-two level magnetic core spark chamber system was flown on SAS 2. The high energy galactic gamma radiation is observed to dominate over the general diffuse radiation along the entire galactic plane, and when examined in detail, the longitudinal and latitudinal distribution seem generally correlated with galactic structural features, particularly with arm segments. The general high energy gamma radiation from the galactic plane, explained on the basis of its angular distribution and magnitude, probably results primarily from cosmic ray interactions with interstellar matter.

  14. Energy dependence of polarization across broad deexcitation gamma-ray line profiles

    NASA Astrophysics Data System (ADS)

    Werntz, Carl; Lang, F. L.

    1998-04-01

    The energy profiles of deexcitation gamma-ray lines from recoiling inelastically scattered nuclei exhibit detailed structure. MeV-wide gamma-ray lines from the direction of the Orion nebula have been detected (H. Bloemen, et al., Astr. and Astrophys. L5, 281 (1994).) by COMPTEL whose source is postulated to be cosmic ray carbon and oxygen nuclei shock accelerated near supernova remnants colliding with ambient hydrogen and helium. Even when the heavy ion velocity distributions are isotropic, structure characteristic of the multipolarity of the gamma transition remains (A. M. Bykov et al, Astr. and Astrophys. 607, L37 (1996); B. Kozlovsky et al, Astrophys. J. 484, (1997).). In experiments in which the energy dependent structure of the deexcitation gamma-ray profiles is not resolved, the gammas display a high degree of linear polarization that rapidly changes with gamma-beam angle. We calculate the polarization, both linear and circular, as a function of gamma-ray energy across the laboratory line profiles of C12*(4.44) and O16*(6.13) inelastically excited by protons and alphas. We then investigate the polarization in the surviving structures for isotropic energetic ions colliding with ^1H and ^4He.

  15. High energy gamma-ray observations of SN 1987A

    NASA Technical Reports Server (NTRS)

    Sood, R. K.; Thomas, J. A.; Waldron, L.; Manchanda, R. K.; Rochester, G. K.

    1988-01-01

    Results are presented from observations of SN 1987A made with a combined high energy gamma ray and hard X-ray payload carried on a balloon flight over Alice Springs, Australia on April 5, 1988. The payload instrumentation is described, emphasizing the characteristics of the gamma-ray detector. The gamma-ray emission profile is illustrated and the preliminary results of the observations are summarized.

  16. Nuclear energy release from fragmentation

    NASA Astrophysics Data System (ADS)

    Li, Cheng; Souza, S. R.; Tsang, M. B.; Zhang, Feng-Shou

    2016-08-01

    It is well known that binary fission occurs with positive energy gain. In this article we examine the energetics of splitting uranium and thorium isotopes into various numbers of fragments (from two to eight) with nearly equal size. We find that the energy released by splitting 230,232Th and 235,238U into three equal size fragments is largest. The statistical multifragmentation model (SMM) is applied to calculate the probability of different breakup channels for excited nuclei. By weighing the probability distributions of fragment multiplicity at different excitation energies, we find the peaks of energy release for 230,232Th and 235,238U are around 0.7-0.75 MeV/u at excitation energy between 1.2 and 2 MeV/u in the primary breakup process. Taking into account the secondary de-excitation processes of primary fragments with the GEMINI code, these energy peaks fall to about 0.45 MeV/u.

  17. System to quantify gamma-ray radial energy deposition in semiconductor detectors

    DOEpatents

    Kammeraad, Judith E.; Blair, Jerome J.

    2001-01-01

    A system for measuring gamma-ray radial energy deposition is provided for use in conjunction with a semiconductor detector. The detector comprises two electrodes and a detector material, and defines a plurality of zones within the detecting material in parallel with the two electrodes. The detector produces a charge signal E(t) when a gamma-ray interacts with the detector. Digitizing means are provided for converting the charge signal E(t) into a digitized signal. A computational means receives the digitized signal and calculates in which of the plurality of zones the gamma-ray deposited energy when interacting with the detector. The computational means produces an output indicating the amount of energy deposited by the gamma-ray in each of the plurality of zones.

  18. Testing the Gamma-Ray Burst Energy Relationships

    NASA Technical Reports Server (NTRS)

    Band, David L.; Preece, Robert D.

    2005-01-01

    Building on Nakar & Piran's analysis of the Amati relation relating gamma-ray burst peak energies E(sub p) and isotropic energies E(sub iso ) we test the consistency of a large sample of BATSE bursts with the Amati and Ghirlanda (which relates peak energies and actual gamma-ray energies E(sub gamma)) relations. Each of these relations can be exp ressed as a ratio of the different energies that is a function of red shift (for both the Amati and Ghirlanda relations) and beaming fraction f(sub B) (for the Ghirlanda relation). The most rigorous test, whic h allows bursts to be at any redshift, corroborates Nakar & Piran's r esult - 88% of the BATSE bursts are inconsistent with the Amati relat ion - while only l.6% of the bursts are inconsistent with the Ghirlan da relation if f(sub B) = 1. Modelling the redshift distribution resu lts in an energy ratio distribution for the Amati relation that is sh ifted by an order of magnitude relative to the observed distributions; any sub-population satisfying the Amati relation can comprise at mos t approx. 18% of our burst sample. A similar analysis of the Ghirland a relation depends sensitively on the beaming fraction distribution f or small values of f(sub B); for reasonable estimates of this distrib ution about a third of the burst sample is inconsistent with the Ghir landa relation. Our results indicate that these relations are an artifact of the selection effects of the burst sample in which they were f ound; these selection effects may favor sub-populations for which the se relations are valid.

  19. Fermi-LAT Observations of the Gamma-Ray Burst GRB 130427A

    NASA Technical Reports Server (NTRS)

    Ackermann, M.; Ajello, M.; Asano, K.; Atwood, W. B.; Axelsson, M.; Baldini, L.; Ballet, J.; Barbiellini, G.; Baring, M. G.; Bastieri, D.; hide

    2013-01-01

    The observations of the exceptionally bright gamma-ray burst (GRB) 130427A by the Large Area Telescope aboard the Fermi Gamma-ray Space Telescope provide constraints on the nature of these unique astrophysical sources. GRB 130427A had the largest fluence, highest-energy photon (95 GeV), longest gamma-ray duration (20 hours), and one of the largest isotropic energy releases ever observed from a GRB. Temporal and spectral analyses of GRB 130427A challenge the widely accepted model that the nonthermal high-energy emission in the afterglow phase of GRBs is synchrotron emission radiated by electrons accelerated at an external shock.

  20. Gamma ray bursts of black hole universe

    NASA Astrophysics Data System (ADS)

    Zhang, T. X.

    2015-07-01

    Slightly modifying the standard big bang theory, Zhang recently developed a new cosmological model called black hole universe, which has only a single postulate but is consistent with Mach's principle, governed by Einstein's general theory of relativity, and able to explain existing observations of the universe. In the previous studies, we have explained the origin, structure, evolution, expansion, cosmic microwave background radiation, quasar, and acceleration of black hole universe, which grew from a star-like black hole with several solar masses through a supermassive black hole with billions of solar masses to the present state with hundred billion-trillions of solar masses by accreting ambient matter and merging with other black holes. This study investigates gamma ray bursts of black hole universe and provides an alternative explanation for the energy and spectrum measurements of gamma ray bursts according to the black hole universe model. The results indicate that gamma ray bursts can be understood as emissions of dynamic star-like black holes. A black hole, when it accretes its star or merges with another black hole, becomes dynamic. A dynamic black hole has a broken event horizon and thus cannot hold the inside hot (or high-frequency) blackbody radiation, which flows or leaks out and produces a GRB. A star when it collapses into its core black hole produces a long GRB and releases the gravitational potential energy of the star as gamma rays. A black hole that merges with another black hole produces a short GRB and releases a part of their blackbody radiation as gamma rays. The amount of energy obtained from the emissions of dynamic star-like black holes are consistent with the measurements of energy from GRBs. The GRB energy spectra derived from this new emission mechanism are also consistent with the measurements.

  1. Polarization of the prompt gamma-ray emission from the gamma-ray burst of 6 December 2002.

    PubMed

    Coburn, Wayne; Boggs, Steven E

    2003-05-22

    Observations of the afterglows of gamma-ray bursts (GRBs) have revealed that they lie at cosmological distances, and so correspond to the release of an enormous amount of energy. The nature of the central engine that powers these events and the prompt gamma-ray emission mechanism itself remain enigmatic because, once a relativistic fireball is created, the physics of the afterglow is insensitive to the nature of the progenitor. Here we report the discovery of linear polarization in the prompt gamma-ray emission from GRB021206, which indicates that it is synchrotron emission from relativistic electrons in a strong magnetic field. The polarization is at the theoretical maximum, which requires a uniform, large-scale magnetic field over the gamma-ray emission region. A large-scale magnetic field constrains possible progenitors to those either having or producing organized fields. We suggest that the large magnetic energy densities in the progenitor environment (comparable to the kinetic energy densities of the fireball), combined with the large-scale structure of the field, indicate that magnetic fields drive the GRB explosion.

  2. Cen A Optical Gamma Composite

    NASA Image and Video Library

    2017-12-08

    NASA release April 1, 2010 The gamma-ray output from Cen A's lobes exceeds their radio output by more than ten times. High-energy gamma rays detected by Fermi's Large Area Telescope are depicted as purple in this gamma ray/optical composite of the galaxy. Credit: NASA/DOE/Fermi LAT Collaboration, Capella Observatory To learn more about these images go to: www.nasa.gov/mission_pages/GLAST/news/smokestack-plumes.html NASA Goddard Space Flight Center is home to the nation's largest organization of combined scientists, engineers and technologists that build spacecraft, instruments and new technology to study the Earth, the sun, our solar system, and the universe.

  3. Low energy prompt gamma-ray tests of a large volume BGO detector.

    PubMed

    Naqvi, A A; Kalakada, Zameer; Al-Anezi, M S; Raashid, M; Khateeb-ur-Rehman; Maslehuddin, M; Garwan, M A

    2012-01-01

    Tests of a large volume Bismuth Germinate (BGO) detector were carried out to detect low energy prompt gamma-rays from boron and cadmium-contaminated water samples using a portable neutron generator-based Prompt Gamma Neutron Activation Analysis (PGNAA) setup. Inspite of strong interference between the sample- and the detector-associated prompt gamma-rays, an excellent agreement has been observed between the experimental and calculated yields of the prompt gamma-rays, indicating successful application of the large volume BGO detector in the PGNAA analysis of bulk samples using low energy prompt gamma-rays. Copyright © 2011 Elsevier Ltd. All rights reserved.

  4. High probability neurotransmitter release sites represent an energy efficient design

    PubMed Central

    Lu, Zhongmin; Chouhan, Amit K.; Borycz, Jolanta A.; Lu, Zhiyuan; Rossano, Adam J; Brain, Keith L.; Zhou, You; Meinertzhagen, Ian A.; Macleod, Gregory T.

    2016-01-01

    Nerve terminals contain multiple sites specialized for the release of neurotransmitters. Release usually occurs with low probability, a design thought to confer many advantages. High probability release sites are not uncommon but their advantages are not well understood. Here we test the hypothesis that high probability release sites represent an energy efficient design. We examined release site probabilities and energy efficiency at the terminals of two glutamatergic motor neurons synapsing on the same muscle fiber in Drosophila larvae. Through electrophysiological and ultrastructural measurements we calculated release site probabilities to differ considerably between terminals (0.33 vs. 0.11). We estimated the energy required to release and recycle glutamate from the same measurements. The energy required to remove calcium and sodium ions subsequent to nerve excitation was estimated through microfluorimetric and morphological measurements. We calculated energy efficiency as the number of glutamate molecules released per ATP molecule hydrolyzed, and high probability release site terminals were found to be more efficient (0.13 vs. 0.06). Our analytical model indicates that energy efficiency is optimal (~0.15) at high release site probabilities (~0.76). As limitations in energy supply constrain neural function, high probability release sites might ameliorate such constraints by demanding less energy. Energy efficiency can be viewed as one aspect of nerve terminal function, in balance with others, because high efficiency terminals depress significantly during episodic bursts of activity. PMID:27593375

  5. High energy neutrinos from gamma-ray bursts with precursor supernovae.

    PubMed

    Razzaque, Soebur; Mészáros, Peter; Waxman, Eli

    2003-06-20

    The high energy neutrino signature from proton-proton and photo-meson interactions in a supernova remnant shell ejected prior to a gamma-ray burst provides a test for the precursor supernova, or supranova, model of gamma-ray bursts. Protons in the supernova remnant shell and photons entrapped from a supernova explosion or a pulsar wind from a fast-rotating neutron star remnant provide ample targets for protons escaping the internal shocks of the gamma-ray burst to interact and produce high energy neutrinos. We calculate the expected neutrino fluxes, which can be detected by current and future experiments.

  6. Interferon-gamma promotes the survival and Fc epsilon RI-mediated histamine release in cultured human mast cells.

    PubMed Central

    Yanagida, M; Fukamachi, H; Takei, M; Hagiwara, T; Uzumaki, H; Tokiwa, T; Saito, H; Iikura, Y; Nakahata, T

    1996-01-01

    We examined the effects of interferon-gamma (IFN-gamma) on 100% pure human mast cells generated in suspension cultures of umbilical cord blood mononuclear cells in the presence of stem cell factor (SCF) and interleukin-6 (IL-6). When mast cells were suspended in serum-free medium without any cytokine after the withdrawal of SCF and IL-6, they died over a period of 5 days because of apoptosis. IFN-gamma in the cultures suppressed apoptosis and prolonged their survival in a dose-dependent manner. This survival-promoting effect of IFN-gamma was blocked by neutralizing antibodies to IFN-gamma or to IFN-gamma receptor (IFN-gamma R). When mast cells were incubated with IFN-gamma in serum-free medium for more than 4 hr during sensitization, immunoglobulin E (IgE)/anti-IgE antibody-induced histamine release was effectively enhanced. Polymerase chain reaction (PCR) amplification of the alpha-chain of IFN-gamma R (IFN-gamma R alpha) yielded products of the correct size predicted from the sequence of the receptor. In addition, flow cytometry using anti-IFN-gamma R monoclonal antibodies (mAbs) indicated that these mast cells bear IFN-gamma R on their surface. These findings suggested that IFN-gamma activates human mast cells via specific receptors in certain aspects of inflammatory reactions. Images Figure 2 Figure 4 PMID:9014819

  7. Inverse modelling of radionuclide release rates using gamma dose rate observations

    NASA Astrophysics Data System (ADS)

    Hamburger, Thomas; Evangeliou, Nikolaos; Stohl, Andreas; von Haustein, Christoph; Thummerer, Severin; Wallner, Christian

    2015-04-01

    Severe accidents in nuclear power plants such as the historical accident in Chernobyl 1986 or the more recent disaster in the Fukushima Dai-ichi nuclear power plant in 2011 have drastic impacts on the population and environment. Observations and dispersion modelling of the released radionuclides help to assess the regional impact of such nuclear accidents. Modelling the increase of regional radionuclide activity concentrations, which results from nuclear accidents, underlies a multiplicity of uncertainties. One of the most significant uncertainties is the estimation of the source term. That is, the time dependent quantification of the released spectrum of radionuclides during the course of the nuclear accident. The quantification of the source term may either remain uncertain (e.g. Chernobyl, Devell et al., 1995) or rely on estimates given by the operators of the nuclear power plant. Precise measurements are mostly missing due to practical limitations during the accident. The release rates of radionuclides at the accident site can be estimated using inverse modelling (Davoine and Bocquet, 2007). The accuracy of the method depends amongst others on the availability, reliability and the resolution in time and space of the used observations. Radionuclide activity concentrations are observed on a relatively sparse grid and the temporal resolution of available data may be low within the order of hours or a day. Gamma dose rates, on the other hand, are observed routinely on a much denser grid and higher temporal resolution and provide therefore a wider basis for inverse modelling (Saunier et al., 2013). We present a new inversion approach, which combines an atmospheric dispersion model and observations of radionuclide activity concentrations and gamma dose rates to obtain the source term of radionuclides. We use the Lagrangian particle dispersion model FLEXPART (Stohl et al., 1998; Stohl et al., 2005) to model the atmospheric transport of the released radionuclides. The

  8. Very-high-energy gamma rays from a distant quasar: how transparent is the universe?

    PubMed

    Albert, J; Aliu, E; Anderhub, H; Antonelli, L A; Antoranz, P; Backes, M; Baixeras, C; Barrio, J A; Bartko, H; Bastieri, D; Becker, J K; Bednarek, W; Berger, K; Bernardini, E; Bigongiari, C; Biland, A; Bock, R K; Bonnoli, G; Bordas, P; Bosch-Ramon, V; Bretz, T; Britvitch, I; Camara, M; Carmona, E; Chilingarian, A; Commichau, S; Contreras, J L; Cortina, J; Costado, M T; Covino, S; Curtef, V; Dazzi, F; De Angelis, A; De Cea Del Pozo, E; de Los Reyes, R; De Lotto, B; De Maria, M; De Sabata, F; Mendez, C Delgado; Dominguez, A; Dorner, D; Doro, M; Errando, M; Fagiolini, M; Ferenc, D; Fernández, E; Firpo, R; Fonseca, M V; Font, L; Galante, N; López, R J García; Garczarczyk, M; Gaug, M; Goebel, F; Hayashida, M; Herrero, A; Höhne, D; Hose, J; Hsu, C C; Huber, S; Jogler, T; Kneiske, T M; Kranich, D; La Barbera, A; Laille, A; Leonardo, E; Lindfors, E; Lombardi, S; Longo, F; López, M; Lorenz, E; Majumdar, P; Maneva, G; Mankuzhiyil, N; Mannheim, K; Maraschi, L; Mariotti, M; Martínez, M; Mazin, D; Meucci, M; Meyer, M; Miranda, J M; Mirzoyan, R; Mizobuchi, S; Moles, M; Moralejo, A; Nieto, D; Nilsson, K; Ninkovic, J; Otte, N; Oya, I; Panniello, M; Paoletti, R; Paredes, J M; Pasanen, M; Pascoli, D; Pauss, F; Pegna, R G; Perez-Torres, M A; Persic, M; Peruzzo, L; Piccioli, A; Prada, F; Prandini, E; Puchades, N; Raymers, A; Rhode, W; Ribó, M; Rico, J; Rissi, M; Robert, A; Rügamer, S; Saggion, A; Saito, T Y; Salvati, M; Sanchez-Conde, M; Sartori, P; Satalecka, K; Scalzotto, V; Scapin, V; Schmitt, R; Schweizer, T; Shayduk, M; Shinozaki, K; Shore, S N; Sidro, N; Sierpowska-Bartosik, A; Sillanpää, A; Sobczynska, D; Spanier, F; Stamerra, A; Stark, L S; Takalo, L; Tavecchio, F; Temnikov, P; Tescaro, D; Teshima, M; Tluczykont, M; Torres, D F; Turini, N; Vankov, H; Venturini, A; Vitale, V; Wagner, R M; Wittek, W; Zabalza, V; Zandanel, F; Zanin, R; Zapatero, J

    2008-06-27

    The atmospheric Cherenkov gamma-ray telescope MAGIC, designed for a low-energy threshold, has detected very-high-energy gamma rays from a giant flare of the distant Quasi-Stellar Radio Source (in short: radio quasar) 3C 279, at a distance of more than 5 billion light-years (a redshift of 0.536). No quasar has been observed previously in very-high-energy gamma radiation, and this is also the most distant object detected emitting gamma rays above 50 gigaelectron volts. Because high-energy gamma rays may be stopped by interacting with the diffuse background light in the universe, the observations by MAGIC imply a low amount for such light, consistent with that known from galaxy counts.

  9. Dosimetry of high-energy electron linac produced photoneutrons and the bremsstrahlung gamma-rays using TLD-500 and TLD-700 dosimeter pairs

    NASA Astrophysics Data System (ADS)

    Mukherjee, Bhaskar; Makowski, Dariusz; Simrock, Stefan

    2005-06-01

    The neutron and gamma doses are crucial to interpreting the radiation effects in microelectronic devices operating in a high-energy accelerator environment. This report highlights a method for an accurate estimation of photoneutron and the accompanying bremsstrahlung (gamma) doses produced by a 450 MeV electron linear accelerator (linac) operating in pulsed mode. The principle is based on the analysis of thermoluminescence glow-curves of TLD-500 (Aluminium Oxide) and TLD-700 (Lithium Fluoride) dosimeter pairs. The gamma and fast neutron response of the TLD-500 and TLD-700 dosimeter pairs were calibrated with a 60Co (gamma) and a 241Am-Be (α, n) neutron standard-source, respectively. The Kinetic Energy Released in Materials (kerma) conversion factor for photoneutrons was evaluated by folding the neutron kerma (dose) distribution in 7LiF (the main component of the TLD-700 dosimeter) with the energy spectra of the 241Am-Be (α, n) neutrons and electron accelerator produced photoneutrons. The neutron kerma conversion factors for 241Am-Be neutrons and photoneutrons were calculated to be 2.52×10 -3 and 1.37×10 -3 μGy/a.u. respectively. The bremsstrahlung (gamma) dose conversion factor was evaluated to be 7.32×10 -4 μGy/a.u. The above method has been successfully utilised to assess the photoneutron and bremsstrahlung doses from a 450 MeV electron linac operating at DESY Research Centre in Hamburg, Germany.

  10. Development of a Telescope for Medium-Energy Gamma-Ray Astronomy

    NASA Technical Reports Server (NTRS)

    Hunter, Stanley D.

    2010-01-01

    Since the launch of AGILE and FERMI, the scientific progress in high-energy (E(sub gamma) greater than approximately 200 MeV) gamma-ray science has been, and will continue to be dramatic. Both of these telescopes cover a broad energy range from approximately 20 MeV to greater than 10 GeV. However, neither instrument is optimized for observations below approximately 200 MeV where many astrophysical objects exhibit unique, transitory behavior, such as spectral breaks, bursts, and flares. Hence, while significant progress from current observations is expected, there will nonetheless remain a significant sensitivity gap in the medium-energy (approximately 0.1-200 MeV) regime; the lower end of this range remains largely unexplored whereas the upper end will allow comparison with FERMI data. Tapping into this unexplored regime requires significant improvements in sensitivity. A major emphasis of modern detector development, with the goal of providing significant improvements in sensitivity in the medium-energy regime, focuses on high-resolution electron tracking. The Three-Dimensional Track Imager (3-DTI) technology being developed at GSFC provides high resolution tracking of the electron-positron pair from gamma-ray interactions from 5 to 200 MeV. The 3-DTI consists of a time projection chamber (TPC) and 2-D cross-strip microwell detector (MWD). The low-density and homogeneous design of the 3-DTI, offers unprecedented sensitivity by providing angular resolution near the kinematic limit. Electron tracking also enables measurement of gamma-ray polarization, a new tool to study astrophysical phenomenon. We describe the design, fabrication, and performance of a 30x30x30 cubic centimeters 3-DTI detector prototype of a medium-energy gamma-ray telescope.

  11. Very high energy gamma ray extension of GRO observations

    NASA Technical Reports Server (NTRS)

    Weekes, Trevor C.

    1992-01-01

    This has been an exiciting year for high energy gamma-ray astronomy, both from space and from ground-based observatories. It has been a particularly active period for the Whipple Observatory gamma-ray group. In phase 1 of the Compton Gamma Ray Observatory (GRO), there has not been too much opportunity for overlapping observations with the Energetic Gamma Ray Experiment Telescope (EGRET) and the other GRO telescopes; however, significant progress was made in the development of data analysis techniques and in improving the sensitivity of the technique which will have direct application in correlative observations in phase 2. Progress made during the period 1 Jul. 1991 - 31 Dec. 1991 is presented.

  12. Superconducting High Energy Resolution Gamma-ray Spectrometers

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

    Chow, D T

    2002-02-22

    We have demonstrated that a bulk absorber coupled to a TES can serve as a good gamma-ray spectrometer. Our measured energy resolution of 70 eV at 60 keV is among the best measurements in this field. We have also shown excellent agreement between the noise predictions and measured noise. Despite this good result, we noted that our detector design has shortcomings with a low count rate and vulnerabilities with the linearity of energy response. We addressed these issues by implementation of an active negative feedback bias. We demonstrated the effects of active bias such as additional pulse shortening, reduction ofmore » TES change in temperature during a pulse, and linearization of energy response at low energy. Linearization at higher energy is possible with optimized heat capacities and thermal conductivities of the microcalorimeter. However, the current fabrication process has low control and repeatability over the thermal properties. Thus, optimization of the detector performance is difficult until the fabrication process is improved. Currently, several efforts are underway to better control the fabrication of our gamma-ray spectrometers. We are developing a full-wafer process to produce TES films. We are investigating the thermal conductivity and surface roughness of thicker SiN membranes. We are exploring alternative methods to couple the absorber to the TES film for reproducibility. We are also optimizing the thermal conductivities within the detector to minimize two-element phonon noise. We are experimenting with different absorber materials to optimize absorption efficiency and heat capacity. We are also working on minimizing Johnson noise from the E S shunt and SQUID amplifier noise. We have shown that our performance, noise, and active bias models agree very well with measured data from several microcalorimeters. Once the fabrication improvements have been implemented, we have no doubt that our gamma-ray spectrometer will achieve even more spectacular

  13. Utility of an interferon-gamma release assay for latent tuberculosis diagnosis in a case of bullous pemphigoid.

    PubMed

    Goodfellow, Alfred; Keeling, Douglas N; Hayes, Robert C; Webster, Duncan

    2009-01-01

    With increasing use of immunosuppressive therapy, including tumor necrosis factor alpha inhibitors, there is concern about infectious complications, including reactivation of latent Mycobacterium tuberculosis infection. Routine testing prior to administration of systemic immunosuppression includes the tuberculin skin test, which lacks sensitivity and specificity and may be difficult to interpret in the presence of extensive cutaneous disease. Treatment of individuals with latent tuberculosis infection is recommended when immunosuppressive medications are to be employed. We report a case in which a diagnosis of latent tuberculosis infection in a patient with extensive bullous pemphigoid was clarified by the use of an interferon-gamma release assay after equivocal tuberculin skin test results. Interferon-gamma release assays are useful adjuncts to the tuberculin skin test in the diagnosis of latent tuberculosis infection in the setting of extensive cutaneous disease.

  14. Studying the High Energy Gamma Ray Sky with Gamma Ray Large Area Space Telescope (GLAST)

    NASA Technical Reports Server (NTRS)

    Kamae, T.; Ohsugi, T.; Thompson, D. J.; Watanabe, K.

    1998-01-01

    Building on the success of the Energetic Gamma Ray Experiment Telescope (EGRET) on the Compton Gamma Ray Observatory, the Gamma Ray Large Area Space Telescope (GLAST) will make a major step in the study of such subjects as blazars, gamma Ray bursts, the search for dark matter, supernova remnants, pulsars, diffuse radiation, and unidentified high energy sources. The instrument will be built on new and mature detector technologies such as silicon strip detectors, low-power low-noise LSI, and a multilevel data acquisition system. GLAST is in the research and development phase, and one full tower (of 25 total) is now being built in collaborating institutes. The prototype tower will be tested thoroughly at Stanford Linear Accelerator Center (SLAC) in the fall of 1999.

  15. A Search for Ultra--High-Energy Gamma-Ray Emission from Five Supernova Remnants

    NASA Astrophysics Data System (ADS)

    Allen, G. E.; Berley, D.; Biller, S.; Burman, R. L.; Cavalli-Sforza, M.; Chang, C. Y.; Chen, M. L.; Chumney, P.; Coyne, D.; Dion, C. L.; Dorfan, D.; Ellsworth, R. W.; Goodman, J. A.; Haines, T. J.; Hoffman, C. M.; Kelley, L.; Klein, S.; Schmidt, D. M.; Schnee, R.; Shoup, A.; Sinnis, C.; Stark, M. J.; Williams, D. A.; Wu, J.-P.; Yang, T.; Yodh, G. B.

    1995-07-01

    The majority of the cosmic rays in our Galaxy with energies in the range of ~1010--1014 eV are thought to be accelerated in supernova remnants (SNRs). Measurements of SNR gamma-ray spectra in this energy region could support or contradict this concept. The Energetic Gamma-Ray Experiment Telescope (EGRET) collaboration has reported six sources of gamma rays above 108 eV whose coordinates are coincident with SNRs. Five of these sources are within the field of view of the CYGNUS extensive air shower detector. A search of the CYGNUS data set reveals no evidence of gamma-ray emission at energies ~1014 eV for these five SNRs. The flux upper limits from the CYGNUS data are compared to the lower energy fluxes measured with the EGRET detector using Drury, Aharonian, & Volk's recent model of gamma-ray production in the shocks of SNRs. The results suggest one or more of the following: (1) the gamma-ray spectra for these five SNRs soften by about 1014 eV, (2) the integral gamma-ray spectra of the SNRs are steeper than about E-1.3, or (3) most of the gamma rays detected with the EGRET instrument for each SNR are not produced in the SNR's shock but are produced at some other site (such as a pulsar).

  16. Gamma-oryzanol-loaded calcium pectinate microparticles reinforced with chitosan: optimization and release characteristics.

    PubMed

    Lee, Ji-Soo; Kim, Jong Soo; Lee, Hyeon Gyu

    2009-05-01

    Response surface methodology was used to optimize microparticle preparation conditions, including the ratio of pectin:gamma-oryzanol (OZ) (X(1)), agitation speed (X(2)), and the concentration of emulsifier (X(3)), for maximal entrapment efficiency (EE) of OZ-loaded Ca pectinate microparticles. The optimized values of X(1), X(2), and X(3) were found to be 2.72:5.28, 1143.5 rpm, and 2.61%, respectively. Experimental results obtained for the optimum formulation agreed favorably with the predicted results, indicating the usefulness of predicting models for EE. In order to evaluate the effect of chitosan-coating and blending on the release pattern of the entrapped OZ from microparticles, chitosan-coated and blended Ca pectinate microparticles were prepared. Release studies revealed that the chitosan treatments, especially the chitosan-coating, were effective in suppressing the release in both simulated gastric fluid (SGF) and intestinal fluid (SIF).

  17. Energy spectrum of extragalactic gamma-ray sources

    NASA Technical Reports Server (NTRS)

    Protheroe, R. J.

    1985-01-01

    The result of Monte Carlo electron photon cascade calculations for propagation of gamma rays through regions of extragalactic space containing no magnetic field are given. These calculations then provide upper limits to the expected flux from extragalactic sources. Since gamma rays in the 10 to the 14th power eV to 10 to the 17th power eV energy range are of interest, interactions of electrons and photons with the 3 K microwave background radiation are considered. To obtain an upper limit to the expected gamma ray flux from sources, the intergalactic field is assumed to be so low that it can be ignored. Interactions with photons of the near-infrared background radiation are not considered here although these will have important implications for gamma rays below 10 to the 14th power eV if the near infrared background radiation is universal. Interaction lengths of electrons and photons in the microwave background radiation at a temperature of 2.96 K were calculated and are given.

  18. Energy- and time-resolved detection of prompt gamma-rays for proton range verification.

    PubMed

    Verburg, Joost M; Riley, Kent; Bortfeld, Thomas; Seco, Joao

    2013-10-21

    In this work, we present experimental results of a novel prompt gamma-ray detector for proton beam range verification. The detection system features an actively shielded cerium-doped lanthanum(III) bromide scintillator, coupled to a digital data acquisition system. The acquisition was synchronized to the cyclotron radio frequency to separate the prompt gamma-ray signals from the later-arriving neutron-induced background. We designed the detector to provide a high energy resolution and an effective reduction of background events, enabling discrete proton-induced prompt gamma lines to be resolved. Measuring discrete prompt gamma lines has several benefits for range verification. As the discrete energies correspond to specific nuclear transitions, the magnitudes of the different gamma lines have unique correlations with the proton energy and can be directly related to nuclear reaction cross sections. The quantification of discrete gamma lines also enables elemental analysis of tissue in the beam path, providing a better prediction of prompt gamma-ray yields. We present the results of experiments in which a water phantom was irradiated with proton pencil-beams in a clinical proton therapy gantry. A slit collimator was used to collimate the prompt gamma-rays, and measurements were performed at 27 positions along the path of proton beams with ranges of 9, 16 and 23 g cm(-2) in water. The magnitudes of discrete gamma lines at 4.44, 5.2 and 6.13 MeV were quantified. The prompt gamma lines were found to be clearly resolved in dimensions of energy and time, and had a reproducible correlation with the proton depth-dose curve. We conclude that the measurement of discrete prompt gamma-rays for in vivo range verification of clinical proton beams is feasible, and plan to further study methods and detector designs for clinical use.

  19. Gamma-ray astronomy in the medium energy (10-50 MeV) range

    NASA Technical Reports Server (NTRS)

    Kniffen, D. A.; Bertsch, D. L.; Morris, D. J.; Palmeira, R. A. R.; Rao, K. R.

    1977-01-01

    To observe the medium energy component of the intense galactic center gamma-ray emission, two balloon flights of a medium energy gamma-ray spark chamber telescope were flown in Brazil in 1975. The results indicate the emission is higher than previously thought and above the predictions of a theoretical model proposed.

  20. DISCOVERY OF HIGH-ENERGY AND VERY HIGH ENERGY {gamma}-RAY EMISSION FROM THE BLAZAR RBS 0413

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

    Aliu, E.; Archambault, S.; Arlen, T.

    2012-05-10

    We report on the discovery of high-energy (HE; E > 0.1 GeV) and very high energy (VHE; E > 100 GeV) {gamma}-ray emission from the high-frequency-peaked BL Lac object RBS 0413. VERITAS, a ground-based {gamma}-ray observatory, detected VHE {gamma} rays from RBS 0413 with a statistical significance of 5.5 standard deviations ({sigma}) and a {gamma}-ray flux of (1.5 {+-} 0.6{sub stat} {+-} 0.7{sub syst}) Multiplication-Sign 10{sup -8} photons m{sup -2} s{sup -1} ({approx}1% of the Crab Nebula flux) above 250 GeV. The observed spectrum can be described by a power law with a photon index of 3.18 {+-} 0.68{sub stat}more » {+-} 0.30{sub syst}. Contemporaneous observations with the Large Area Telescope (LAT) on the Fermi Gamma-ray Space Telescope detected HE {gamma} rays from RBS 0413 with a statistical significance of more than 9{sigma}, a power-law photon index of 1.57 {+-} 0.12{sub stat}+{sup 0.11}{sub -0.12sys}, and a {gamma}-ray flux between 300 MeV and 300 GeV of (1.64 {+-} 0.43{sub stat}{sup +0.31}{sub -0.22sys}) Multiplication-Sign 10{sup -5} photons m{sup -2} s{sup -1}. We present the results from Fermi-LAT and VERITAS, including a spectral energy distribution modeling of the {gamma}-ray, quasi-simultaneous X-ray (Swift-XRT), ultraviolet (Swift-UVOT), and R-band optical (MDM) data. We find that, if conditions close to equipartition are required, both the combined synchrotron self-Compton/external-Compton and the lepto-hadronic models are preferred over a pure synchrotron self-Compton model.« less

  1. Radio galaxies dominate the high-energy diffuse gamma-ray background

    DOE PAGES

    Hooper, Dan; Linden, Tim; Lopez, Alejandro

    2016-08-09

    It has been suggested that unresolved radio galaxies and radio quasars (sometimes referred to as misaligned active galactic nuclei) could be responsible for a significant fraction of the observed diffuse gamma-ray background. In this study, we use the latest data from the Fermi Gamma-Ray Space Telescope to characterize the gamma-ray emission from a sample of 51 radio galaxies. In addition to those sources that had previously been detected using Fermi data, we report here the first statistically significant detection of gamma-ray emission from the radio galaxies 3C 212, 3C 411, and B3 0309+411B. Combining this information with the radio fluxes,more » radio luminosity function, and redshift distribution of this source class, we find that radio galaxies dominate the diffuse gamma-ray background, generating 77.2(+25.4)(-9.4)% of this emission at energies above ~1 GeV . We discuss the implications of this result and point out that it provides support for scenarios in which IceCube's high-energy astrophysical neutrinos also originate from the same population of radio galaxies.« less

  2. Discovery of very-high-energy gamma-rays from the Galactic Centre ridge.

    PubMed

    Aharonian, F; Akhperjanian, A G; Bazer-Bachi, A R; Beilicke, M; Benbow, W; Berge, D; Bernlöhr, K; Boisson, C; Bolz, O; Borrel, V; Braun, I; Breitling, F; Brown, A M; Chadwick, P M; Chounet, L-M; Cornils, R; Costamante, L; Degrange, B; Dickinson, H J; Djannati-Ataï, A; Drury, L O'C; Dubus, G; Emmanoulopoulos, D; Espigat, P; Feinstein, F; Fontaine, G; Fuchs, Y; Funk, S; Gallant, Y A; Giebels, B; Gillessen, S; Glicenstein, J F; Goret, P; Hadjichristidis, C; Hauser, D; Hauser, M; Heinzelmann, G; Henri, G; Hermann, G; Hinton, J A; Hofmann, W; Holleran, M; Horns, D; Jacholkowska, A; de Jager, O C; Khélifi, B; Klages, S; Komin, Nu; Konopelko, A; Latham, I J; Le Gallou, R; Lemière, A; Lemoine-Goumard, M; Leroy, N; Lohse, T; Marcowith, A; Martin, J M; Martineau-Huynh, O; Masterson, C; McComb, T J L; de Naurois, M; Nolan, S J; Noutsos, A; Orford, K J; Osborne, J L; Ouchrif, M; Panter, M; Pelletier, G; Pita, S; Pühlhofer, G; Punch, M; Raubenheimer, B C; Raue, M; Raux, J; Rayner, S M; Reimer, A; Reimer, O; Ripken, J; Rob, L; Rolland, L; Rowell, G; Sahakian, V; Saugé, L; Schlenker, S; Schlickeiser, R; Schuster, C; Schwanke, U; Siewert, M; Sol, H; Spangler, D; Steenkamp, R; Stegmann, C; Tavernet, J-P; Terrier, R; Théoret, C G; Tluczykont, M; van Eldik, C; Vasileiadis, G; Venter, C; Vincent, P; Völk, H J; Wagner, S J

    2006-02-09

    The source of Galactic cosmic rays (with energies up to 10(15) eV) remains unclear, although it is widely believed that they originate in the shock waves of expanding supernova remnants. At present the best way to investigate their acceleration and propagation is by observing the gamma-rays produced when cosmic rays interact with interstellar gas. Here we report observations of an extended region of very-high-energy (> 10(11) eV) gamma-ray emission correlated spatially with a complex of giant molecular clouds in the central 200 parsecs of the Milky Way. The hardness of the gamma-ray spectrum and the conditions in those molecular clouds indicate that the cosmic rays giving rise to the gamma-rays are likely to be protons and nuclei rather than electrons. The energy associated with the cosmic rays could have come from a single supernova explosion around 10(4) years ago.

  3. Energy spectrum of medium energy gamma-rays from the galactic center region. [experimental design

    NASA Technical Reports Server (NTRS)

    Palmeira, R. A. R.; Ramanujarao, K.; Dutra, S. L. G.; Bertsch, D. L.; Kniffen, D. A.; Morris, D. J.

    1978-01-01

    A balloon-borne magnetic core digitized spark chamber with two assemblies of spark-chambers above and below the scintillation counters was used to measure the medium energy gamma ray flux from the galactic center region. Gamma ray calculations are based on the multiple scattering of the pair electrons in 15 aluminum plates interleaved in the spark chamber modules. Counting rates determined during ascent and at ceiling indicate the presence of diffuse component in this energy range. Preliminary results give an integral flux between 15 and 70 MeV compared to the differential points in other results.

  4. A New View of the High Energy Gamma-Ray Sky with the Ferrni Gamma-Ray Space Telescope

    NASA Technical Reports Server (NTRS)

    McEnery, Julie

    2009-01-01

    Following its launch in June 2008, high energy gamma-ray observations by the Fermi Gamma-ray Space Telescope have opened a new and important window on a wide variety of phenomena, including pulsars, black holes and active galactic nuclei, gamma-ray bursts, supernova remnants and the origin of cosmic rays, and searches for hypothetical new phenomena such as super symmetric dark matter annihilations. In this talk I will describe the current status of the Fermi observatory and review the science highlights from the first year of observations.

  5. GammaLib and ctools. A software framework for the analysis of astronomical gamma-ray data

    NASA Astrophysics Data System (ADS)

    Knödlseder, J.; Mayer, M.; Deil, C.; Cayrou, J.-B.; Owen, E.; Kelley-Hoskins, N.; Lu, C.-C.; Buehler, R.; Forest, F.; Louge, T.; Siejkowski, H.; Kosack, K.; Gerard, L.; Schulz, A.; Martin, P.; Sanchez, D.; Ohm, S.; Hassan, T.; Brau-Nogué, S.

    2016-08-01

    The field of gamma-ray astronomy has seen important progress during the last decade, yet to date no common software framework has been developed for the scientific analysis of gamma-ray telescope data. We propose to fill this gap by means of the GammaLib software, a generic library that we have developed to support the analysis of gamma-ray event data. GammaLib was written in C++ and all functionality is available in Python through an extension module. Based on this framework we have developed the ctools software package, a suite of software tools that enables flexible workflows to be built for the analysis of Imaging Air Cherenkov Telescope event data. The ctools are inspired by science analysis software available for existing high-energy astronomy instruments, and they follow the modular ftools model developed by the High Energy Astrophysics Science Archive Research Center. The ctools were written in Python and C++, and can be either used from the command line via shell scripts or directly from Python. In this paper we present the GammaLib and ctools software versions 1.0 that were released at the end of 2015. GammaLib and ctools are ready for the science analysis of Imaging Air Cherenkov Telescope event data, and also support the analysis of Fermi-LAT data and the exploitation of the COMPTEL legacy data archive. We propose using ctools as the science tools software for the Cherenkov Telescope Array Observatory.

  6. AGATE: A High Energy Gamma-Ray Telescope Using Drift Chambers

    NASA Astrophysics Data System (ADS)

    Mukherjee, R.; Dingus, B. L.; Esposito, J. A.; Bertsch, D. L.; Cuddapah, R.; Fichtel, C. E.; Hartman, R. C.; Hunter, S. D.; Thompson, D. J.

    1996-01-01

    The exciting results from the highly successful Energetic Gamma-Ray Experiment Telescope (EGRET) instrument on the Compton Gamma-Ray Observatory (CGRO) has contributed significantly to increasing our understanding of high energy gamma-ray astronomy. A follow-on mission to EGRET is needed to continue these scientific advances as well as to address the several new scientific questions raised by EGRET. Here we describe the work being done on the development of the Advanced Gamma-Ray Astronomy Telescope Experiment (AGATE), visualized as the successor to EGRET. In order to achieve the scientific goals, AGATE will have higher sensitivity than EGRET in the energy range 30 MeV to 30 GeV, larger effective area, better angular resolution, and an extended low and high energy range. In its design, AGATE will follow the tradition of the earlier gamma-ray telescopes, SAS-2, COS B, and EGRET, and will have the same four basic components of an anticoincidence system, directional coincidence system, track imaging, and energy measurement systems. However, due to its much larger size, AGATE will use drift chambers as its track imaging system rather than the spark chambers used by EGRET. Drift chambers are an obvious choice as they have less deadtime per event, better spatial resolution, and are relatively easy and inexpensive to build. Drift chambers have low power requirements, so that many layers of drift chambers can be included. To test the feasibility of using drift chambers, we have constructed a prototype instrument consisting of a stack of sixteen 1/2m × 1/2m drift chambers and have measured the spatial resolution using atmospheric muons. The results on the drift chamber performance in the laboratory are presented here.

  7. Superconducting gamma and fast-neutron spectrometers with high energy resolution

    DOEpatents

    Friedrich, Stephan; , Niedermayr, Thomas R.; Labov, Simon E.

    2008-11-04

    Superconducting Gamma-ray and fast-neutron spectrometers with very high energy resolution operated at very low temperatures are provided. The sensor consists of a bulk absorber and a superconducting thermometer weakly coupled to a cold reservoir, and determines the energy of the incident particle from the rise in temperature upon absorption. A superconducting film operated at the transition between its superconducting and its normal state is used as the thermometer, and sensor operation at reservoir temperatures around 0.1 K reduces thermal fluctuations and thus enables very high energy resolution. Depending on the choice of absorber material, the spectrometer can be configured either as a Gamma-spectrometer or as a fast-neutron spectrometer.

  8. Development of a Telescope for Medium-Energy Gamma-ray Astronomy

    NASA Technical Reports Server (NTRS)

    Sunter, Stan

    2012-01-01

    Since the launch of AGILE and FERMI, the scientific progress in high-energy (Eg greater than approximately 200 MeV) gamma-ray science has been, and will continue to be dramatic. Both of these telescopes cover a broad energy range from approximately 20 MeV to greater than 10 GeV. However, neither instrument is optimized for observations below approximately 200 MeV where many astrophysical objects exhibit unique, transitory behavior, such as spectral breaks, bursts, and flares. Hence, while significant progress from current observations is expected, there will nonetheless remain a significant sensitivity gap in the medium-energy (approximately 0.1-200 MeV) regime; the lower end of this range remains largely unexplored whereas the upper end will allow comparison with FERMI data. Tapping into this unexplored regime requires significant improvements in sensitivity. A major emphasis of modern detector development, with the goal of providing significant improvements in sensitivity in the medium-energy regime, focuses on high-resolution electron tracking. The Three-Dimensional Track Imager (3-DTI) technology being developed at GSFC provides high resolution tracking of the electron-positron pair from gamma-ray interactions from 5 to 200 MeV. The 3-DTI consists of a time projection chamber (TPC) and 2-D cross-strip microwell detector (MWD). The low-density and homogeneous design of the 3-DTI, offers unprecedented sensitivity by providing angular resolution near the kinematic limit. Electron tracking also enables measurement of gamma-ray polarization, a new tool to study astrophysical phenomenon. We describe the design, fabrication, and performance of a 30x30x30 cm3 3-DTI detector prototype of a medium-energy gamma-ray telescope.

  9. Fermi-LAT observations of the gamma-ray burst GRB 130427A.

    PubMed

    Ackermann, M; Ajello, M; Asano, K; Atwood, W B; Axelsson, M; Baldini, L; Ballet, J; Barbiellini, G; Baring, M G; Bastieri, D; Bechtol, K; Bellazzini, R; Bissaldi, E; Bonamente, E; Bregeon, J; Brigida, M; Bruel, P; Buehler, R; Burgess, J Michael; Buson, S; Caliandro, G A; Cameron, R A; Caraveo, P A; Cecchi, C; Chaplin, V; Charles, E; Chekhtman, A; Cheung, C C; Chiang, J; Chiaro, G; Ciprini, S; Claus, R; Cleveland, W; Cohen-Tanugi, J; Collazzi, A; Cominsky, L R; Connaughton, V; Conrad, J; Cutini, S; D'Ammando, F; de Angelis, A; DeKlotz, M; de Palma, F; Dermer, C D; Desiante, R; Diekmann, A; Di Venere, L; Drell, P S; Drlica-Wagner, A; Favuzzi, C; Fegan, S J; Ferrara, E C; Finke, J; Fitzpatrick, G; Focke, W B; Franckowiak, A; Fukazawa, Y; Funk, S; Fusco, P; Gargano, F; Gehrels, N; Germani, S; Gibby, M; Giglietto, N; Giles, M; Giordano, F; Giroletti, M; Godfrey, G; Granot, J; Grenier, I A; Grove, J E; Gruber, D; Guiriec, S; Hadasch, D; Hanabata, Y; Harding, A K; Hayashida, M; Hays, E; Horan, D; Hughes, R E; Inoue, Y; Jogler, T; Jóhannesson, G; Johnson, W N; Kawano, T; Knödlseder, J; Kocevski, D; Kuss, M; Lande, J; Larsson, S; Latronico, L; Longo, F; Loparco, F; Lovellette, M N; Lubrano, P; Mayer, M; Mazziotta, M N; McEnery, J E; Michelson, P F; Mizuno, T; Moiseev, A A; Monzani, M E; Moretti, E; Morselli, A; Moskalenko, I V; Murgia, S; Nemmen, R; Nuss, E; Ohno, M; Ohsugi, T; Okumura, A; Omodei, N; Orienti, M; Paneque, D; Pelassa, V; Perkins, J S; Pesce-Rollins, M; Petrosian, V; Piron, F; Pivato, G; Porter, T A; Racusin, J L; Rainò, S; Rando, R; Razzano, M; Razzaque, S; Reimer, A; Reimer, O; Ritz, S; Roth, M; Ryde, F; Sartori, A; Parkinson, P M Saz; Scargle, J D; Schulz, A; Sgrò, C; Siskind, E J; Sonbas, E; Spandre, G; Spinelli, P; Tajima, H; Takahashi, H; Thayer, J G; Thayer, J B; Thompson, D J; Tibaldo, L; Tinivella, M; Torres, D F; Tosti, G; Troja, E; Usher, T L; Vandenbroucke, J; Vasileiou, V; Vianello, G; Vitale, V; Winer, B L; Wood, K S; Yamazaki, R; Younes, G; Yu, H-F; Zhu, S J; Bhat, P N; Briggs, M S; Byrne, D; Foley, S; Goldstein, A; Jenke, P; Kippen, R M; Kouveliotou, C; McBreen, S; Meegan, C; Paciesas, W S; Preece, R; Rau, A; Tierney, D; van der Horst, A J; von Kienlin, A; Wilson-Hodge, C; Xiong, S; Cusumano, G; La Parola, V; Cummings, J R

    2014-01-03

    The observations of the exceptionally bright gamma-ray burst (GRB) 130427A by the Large Area Telescope aboard the Fermi Gamma-ray Space Telescope provide constraints on the nature of these unique astrophysical sources. GRB 130427A had the largest fluence, highest-energy photon (95 GeV), longest γ-ray duration (20 hours), and one of the largest isotropic energy releases ever observed from a GRB. Temporal and spectral analyses of GRB 130427A challenge the widely accepted model that the nonthermal high-energy emission in the afterglow phase of GRBs is synchrotron emission radiated by electrons accelerated at an external shock.

  10. Neutron and gamma-ray energy reconstruction for characterization of special nuclear material

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

    Clarke, Shaun D.; Hamel, Michael C.; Di fulvio, Angela

    Characterization of special nuclear material may be performed using energy spectroscopy of either the neutron or gamma-ray emissions from the sample. Gamma-ray spectroscopy can be performed relatively easily using high-resolution semiconductors such as high-purity germanium. Neutron spectroscopy, by contrast, is a complex inverse problem. Here, results are presented for 252Cf and PuBe energy spectra unfolded using a single EJ309 organic scintillator; excellent agreement is observed with the reference spectra. Neutron energy spectroscopy is also possible using a two-plane detector array, whereby time-offlight kinematics can be used. With this system, energy spectra can also be obtained as a function of position.more » Finally, spatial-dependent energy spectra are presented for neutron and gamma-ray sources that are in excellent agreement with expectations.« less

  11. Neutron and gamma-ray energy reconstruction for characterization of special nuclear material

    DOE PAGES

    Clarke, Shaun D.; Hamel, Michael C.; Di fulvio, Angela; ...

    2017-06-30

    Characterization of special nuclear material may be performed using energy spectroscopy of either the neutron or gamma-ray emissions from the sample. Gamma-ray spectroscopy can be performed relatively easily using high-resolution semiconductors such as high-purity germanium. Neutron spectroscopy, by contrast, is a complex inverse problem. Here, results are presented for 252Cf and PuBe energy spectra unfolded using a single EJ309 organic scintillator; excellent agreement is observed with the reference spectra. Neutron energy spectroscopy is also possible using a two-plane detector array, whereby time-offlight kinematics can be used. With this system, energy spectra can also be obtained as a function of position.more » Finally, spatial-dependent energy spectra are presented for neutron and gamma-ray sources that are in excellent agreement with expectations.« less

  12. High-Energy Aspects of Small-Scale Energy Release at the Sun

    NASA Astrophysics Data System (ADS)

    Glesener, L.; Vievering, J. T.; Wright, P. J.; Hannah, I. G.; Panchapakesan, S. A.; Ryan, D.; Krucker, S.; Hudson, H. S.; Grefenstette, B.; White, S. M.; Smith, D. M.; Marsh, A.; Kuhar, M.; Christe, S.; Buitrago-Casas, J. C.; Musset, S.; Inglis, A. R.

    2017-12-01

    Large, powerful solar flares have been investigated in detail for decades, but it is only recently that high-energy aspects of small flares could be measured. These small-scale energy releases offer the opportunity to examine how particle acceleration characteristics scale down, which is critical for constraining energy transfer theories such as magnetic reconnection. Probing to minuscule flare sizes also brings us closer to envisioning the characteristics of the small "nanoflares" that may be responsible for heating the corona. A new window on small-scale flaring activity is now opening with the use of focusing hard X-ray instruments to observe the Sun. Hard X-rays are emitted by flare-accelerated electrons and strongly heated plasma, providing a relatively direct method of measuring energy release and particle acceleration properties. This work will show the first observations of sub-A class microflares using the FOXSI sounding rocket and the NuSTAR astrophysics spacecraft, both of which directly focus hard X-rays but have limited observing time on the Sun. These instruments serve as precursors to a spacecraft version of FOXSI, which will explore energy release across the entire range of flaring activity.

  13. Production of gamma rays with energies greater than 30 MeV in the atmosphere

    NASA Technical Reports Server (NTRS)

    Thompson, D.; Fichtel, C.; Kniffen, D.

    1974-01-01

    A three-dimensional study of atmospheric gamma rays with energy greater than 30 MeV has been carried out. Experimental results were obtained from four balloon flights from Palestine, Texas, with a 15 cm by 15 cm digitized wire grid spark chamber. The energy spectrum for downward-moving gamma rays steepens with increasing atmospheric depth. Near the top of the atmosphere, the spectrum steepens with increasing zenith angle. Experimental results compare reasonably well with a three-dimensional Monte Carlo calculation of atmospheric gamma ray production. Inclusion of upward-moving gamma rays makes possible the use of atmospheric secondaries for in-flight calibration of satellite gamma ray detectors.

  14. An Experiment to Demonstrate the Energy Broadening of Annihilation Gamma Rays

    ERIC Educational Resources Information Center

    Ouseph, P. J.; DuBard, James L.

    1978-01-01

    Shows that when positions annihilate in solid materials the energy distribution of the annihilation gamma rays is much broader than that of a 0.511-Mev gamma peak. This broadening is caused by the momentum distribution of the electrons in the material. (Author/GA)

  15. PHEV Energy Use Estimation: Validating the Gamma Distribution for Representing the Random Daily Driving Distance

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

    Lin, Zhenhong; Dong, Jing; Liu, Changzheng

    2012-01-01

    The petroleum and electricity consumptions of plug-in hybrid electric vehicles (PHEVs) are sensitive to the variation of daily vehicle miles traveled (DVMT). Some studies assume DVMT to follow a Gamma distribution, but such a Gamma assumption is yet to be validated. This study finds the Gamma assumption valid in the context of PHEV energy analysis, based on continuous GPS travel data of 382 vehicles, each tracked for at least 183 days. The validity conclusion is based on the found small prediction errors, resulting from the Gamma assumption, in PHEV petroleum use, electricity use, and energy cost. The finding that themore » Gamma distribution is valid and reliable is important. It paves the way for the Gamma distribution to be assumed for analyzing energy uses of PHEVs in the real world. The Gamma distribution can be easily specified with very few pieces of driver information and is relatively easy for mathematical manipulation. Given the validation in this study, the Gamma distribution can now be used with better confidence in a variety of applications, such as improving vehicle consumer choice models, quantifying range anxiety for battery electric vehicles, investigating roles of charging infrastructure, and constructing online calculators that provide personal estimates of PHEV energy use.« less

  16. CALCULATION OF GAMMA SPECTRA IN A PLASTIC SCINTILLATOR FOR ENERGY CALIBRATIONAND DOSE COMPUTATION.

    PubMed

    Kim, Chankyu; Yoo, Hyunjun; Kim, Yewon; Moon, Myungkook; Kim, Jong Yul; Kang, Dong Uk; Lee, Daehee; Kim, Myung Soo; Cho, Minsik; Lee, Eunjoong; Cho, Gyuseong

    2016-09-01

    Plastic scintillation detectors have practical advantages in the field of dosimetry. Energy calibration of measured gamma spectra is important for dose computation, but it is not simple in the plastic scintillators because of their different characteristics and a finite resolution. In this study, the gamma spectra in a polystyrene scintillator were calculated for the energy calibration and dose computation. Based on the relationship between the energy resolution and estimated energy broadening effect in the calculated spectra, the gamma spectra were simply calculated without many iterations. The calculated spectra were in agreement with the calculation by an existing method and measurements. © The Author 2016. Published by Oxford University Press. All rights reserved. For Permissions, please email: journals.permissions@oup.com.

  17. The future of high energy gamma ray astronomy and its potential astrophysical implications

    NASA Technical Reports Server (NTRS)

    Fichtel, C. E.

    1982-01-01

    Future satellites should carry instruments having over an order of magnitude greater sensitivity than those flown thus far as well as improved energy and angular resolution. The information to be obtained from these experiments should greatly enhance knowledge of: the very energetic and nuclear processes associated with compact objects; the structure of our galaxy; the origin and dynamic pressure effects of the cosmic rays; the high energy particles and energetic processes in other galaxies; and the degree of matter-antimatter symmetry of the universe. The relevant aspects of extragalactic gamma ray phenomena are emphasized along with the instruments planned. The high energy gamma ray results of forthcoming programs such as GAMMA-1 and the Gamma Ray Observatory should justify even more sophisticated telescopes. These advanced instruments might be placed on the space station currently being considered by NASA.

  18. Decreased release of histamine and sulfidoleukotrienes by human peripheral blood leukocytes after wasp venom immunotherapy is partially due to induction of IL-10 and IFN-gamma production of T cells.

    PubMed

    Pierkes, M; Bellinghausen, I; Hultsch, T; Metz, G; Knop, J; Saloga, J

    1999-02-01

    Recent studies provide evidence that venom immunotherapy (VIT) alters the pattern of cytokine production by inducing an allergen-specific T-cell shift in cytokine expression from TH2 (IL-4, IL-5) to TH1 (IFN-gamma) cytokines and also inducing the production of IL-10. This study was carried out to analyze whether these changes in cytokine production of T cells already observed 1 week after the initiation of VIT in subjects with wasp venom allergy also influence the reactivity of effector cells, such as mast cells and basophils. All subjects included in this study had a history of severe systemic allergic reactions to wasp stings and positive skin test responses with venom and venom-specific IgE in the sera. Peripheral blood leukocytes were isolated before and after the initiation of VIT (rush therapy reaching a maintenance dose of 100 microg venom injected subcutaneously within 1 week) and preincubated with or without addition of IL-10, IFN-gamma, IL-10 + IFN-gamma, anti-IL-10, or anti-IFN-gamma. After stimulation with wasp venom, histamine and sulfidoleukotriene release were assessed by ELISA and compared with spontaneous release and total histamine content. After the induction of VIT, venom-induced absolute and relative histamine and sulfidoleukotriene release were reduced. This was at least partially due to the induction of IFN-gamma and IL-10 production, because (1) neutralization of IL-10 and IFN-gamma by mAbs partially restored the release after the initiation of VIT and (2) the addition of exogenous IFN-gamma and IL-10 caused a statistically significant diminution of the venom-induced histamine and sulfidoleukotriene release before VIT. Depletion of CD2(+) T cells also restored the releasability after VIT. These data indicate that T cells (producing IL-10 and IFN-gamma after VIT) play a key role for the inhibition of histamine and sulfidoleukotriene release of effector cells.

  19. Some aspects of the scientific significance of high energy gamma ray astrophysics

    NASA Technical Reports Server (NTRS)

    Fichtel, Carl E.

    1991-01-01

    The attraction of high energy gamma-ray astronomy lies in this radiation relating directly to those processes in astrophysical situations which deviate most from thermo-dynamic equilibrium. Some examples of these phenomena which are known to or expected to emit gamma rays are cosmic rays as they interact in intergalactic space, the high energy particles in the magnetic fields of neutron stars, the death of a black hole, the explosion and residual of a supernova, lumps of Weakly Interacting Massive Particles, energetic solar particles interacting near the sun, and very high energy particles in the extreme conditions associated with active galaxies. Although the intensities are known to be low as seen near the earth, a partially compensating characteristic is that the very penetrating nature of high energy gamma rays increases the probability that they can escape from their origin and reach the solar system.

  20. Effect of thiopental sodium on the release of glutamate and gamma-aminobutyric acid from rats prefrontal cortical synaptosomes.

    PubMed

    Liu, Hongliang; Yao, Shanglong

    2004-01-01

    To investigate the effect of thiopental sodium on the release of glutamate and gamma-aminobutyric acid (GABA) from synaptosomes in the prefrontal cortex, synaptosomes were made, the spontaneous release and the evoked release by 30 mmol/L KCl or 20 micromol/L veratridine of glutamate and GABA were performed under various concentrations of thiopental sodium (10-300 micromol/L), glutamate and GABA concentrations were determined by reversed-phase high-performance liquid chromatography. Our results showed that spontaneous release and evoked release of glutamate were significantly inhibited by 30 micromol/L, 100 micromol/L and 300 micromol/L thiopental sodium, IC50 of thiopental sodium was 25.8 +/- 2.3 micromol/L for the spontaneous release, 23.4 +/- 2.4 micromol/L for KCl-evoked release, and 24.3 +/- 1.8 micromol/L for veratridine-evoked release. But GABA spontaneous release and evoked release were unaffected. The study showed that thiopental sodium with clinically related concentrations could inhibit the release of glutamate, but had no effect on the release of GABA from rats prefrontal cortical synaptosomes.

  1. Highlights of the study of energy release in flares

    NASA Technical Reports Server (NTRS)

    Rust, D. M.; Batchelor, D. A.

    1987-01-01

    From February 26 to March 1, 1979, 32 solar flare investigators attended a workshop at Cambridge, MA to define objectives and devise a scientific program for the study of energy release in flares (SERF) during the coming solar maximum. Herein, some major results of the ensuing five-year effort to observe and understand the flare energy release process and its effects (energetic particle production, coronal and chromospheric heating, electromagnetic radiations, and mass motions and ejections) are reviewed. The central issue - what processes store and release the energy liberated in flares - remains unresolved except in the most general terms (e.g., it is generally agreed that the energy is stored in sheared or stressed magnetic fields and released by field annihilation during some MHD instability). Resolving that issue is still one of the most important goals in solar physics, but the advances during the SERF program have brought it closer.

  2. Microelectromechanical high-density energy storage/rapid release system

    NASA Astrophysics Data System (ADS)

    Rodgers, M. Steven; Allen, James J.; Meeks, Kent D.; Jensen, Brian D.; Miller, Samuel L.

    1999-08-01

    One highly desirable characteristic of electrostatically driven microelectromechanical systems (MEMS) is that they consume very little power. The corresponding drawback is that the force they produce may be inadequate for many applications. It has previously been demonstrated that gear reduction units or microtransmissions can substantially increase the torque generated by microengines. Operating speed, however, is also reduced by the transmission gear ratio. Some applications require both high speed and high force. If this output is only required for a limited period of time, then energy could be stored in a mechanical system and rapidly released upon demand. We have designed, fabricated, and demonstrated a high-density energy storage/rapid release system that accomplishes this task. Built using a 5-level surface micromachining technology, the assembly closely resembles a medieval crossbow. Energy releases on the order of tens of nanojoules have already been demonstrated, and significantly higher energy systems are under development.

  3. The Highest-Energy Photons Seen by the Energetic Gamma-Ray Experiment Telescope (EGRET) on the Compton Gamma Ray Observatory

    NASA Technical Reports Server (NTRS)

    Thompson, D. J.; Bertsch, D. L.; ONeal, R. H., Jr.

    2005-01-01

    During its nine-year lifetime, the Energetic Gamma Ray Experiment Telescope (EGBET) on the Compton Gamma Ray Observatory (CGRO) detected 1506 cosmic photons with measured energy E>10 GeV. Of this number, 187 are found within a 1 deg of sources that are listed in the Third EGRET Catalog and were included in determining the detection likelihood, flux, and spectra of those sources. In particular, five detected EGRET pulsars are found to have events above 10 GeV, and together they account for 37 events. A pulsar not included in the Third EGRET Catalog has 2 events, both with the same phase and in one peak of the lower-energy gamma-ray light-curve. Most of the remaining 1319 events appear to be diffuse Galactic and extragalactic radiation based on the similarity of the their spatial and energy distributions with the diffuse model and in the E>100, MeV emission. No significant time clustering which would suggest a burst was detected.

  4. Gamma-ray bursts from cusps on superconducting cosmic strings at large redshifts

    NASA Technical Reports Server (NTRS)

    Paczynski, Bohdan

    1988-01-01

    Babul et al. (1987) proposed that some gamma-ray bursts may be caused by energy released at the cusps of oscillating loops made of superconducting cosmic strings. It is claimed that there were some errors and omissions in that work, which are claimed to be corrected in the present paper. Arguments are presented, that given certain assumptions, the cusps on oscillating superconducting cosmic strings produce highly collimated and energetic electromagnetic bursts and that a fair fraction of electromagnetic energy is likely to come out as gamma rays.

  5. Gamma-ray bursts at high and very high energies

    NASA Astrophysics Data System (ADS)

    Piron, Frédéric

    2016-06-01

    Gamma-Ray Bursts (GRBs) are extra-galactic and extremely energetic transient emissions of gamma rays, which are thought to be associated with the death of massive stars or the merger of compact objects in binary systems. Their huge luminosities involve the presence of a newborn stellar-mass black hole emitting a relativistic collimated outflow, which accelerates particles and produces non-thermal emissions from the radio domain to the highest energies. In this article, I review recent progresses in the understanding of GRB jet physics above 100 MeV, based on Fermi observations of bright GRBs. I discuss the physical implications of these observations and their impact on GRB modeling, and I present some prospects for GRB observation at very high energies in the near future.

  6. Characterization of the Gamma Response of a Cadmium Capture-gated Neutron Spectrometer

    NASA Astrophysics Data System (ADS)

    Hogan, Nathaniel; Rees, Lawrence; Czirr, Bart; Bastola, Suraj

    2010-10-01

    We have studied the gamma response of a newly developed capture-gated neutron spectrometer. Such spectrometers detect a dual signal from incoming neutrons, allowing for differentiation between other particles, such as gamma rays. The neutron provides a primary light pulse in either plastic or liquid scintillator through neutron-proton collisions. A capture material then delivers a second pulse as the moderated neutron captures in the intended material, which then de-excites with the release of gamma energy. The presented spectrometer alternates one centimeter thick plastic scintillators with sheets of cadmium inserted in between for neutron capture. The neutron capture in cadmium offers a release of gamma energy ˜ 9 MeV. To verify that the interaction was caused by a neutron, the response functions of both events must be well known. Due to the prior existence of many capture-gated neutron spectrometers, the proton recoil pulse has already been studied, but the capture pulse is unique to each spectrometer and must be measured. Experimental results agree with theoretical Monte-Carlo code, both suggesting that the optics and geometry of the spectrometer play a large role in its efficiency. Results prove promising for the efficiency of the spectrometer.

  7. Energy Release in Solar Flares,

    DTIC Science & Technology

    1982-10-01

    Plasma Research, Stanford University P. Kaufmanu CRAA/CNPq -Conseiho lacional de Desenvolvimento Cientifico e Tecnologico, Slo Paulo, SP, Brasil D.F...three phases of energy release in solar flares (Sturrock, 1980). However, a recent article by Feldman e a.. (1982) points to a significant

  8. Can gamma irradiation during radiotherapy influence the metal release process for biomedical CoCrMo and 316L alloys?

    PubMed

    Wei, Zheng; Edin, Jonathan; Karlsson, Anna Emelie; Petrovic, Katarina; Soroka, Inna L; Odnevall Wallinder, Inger; Hedberg, Yolanda

    2018-02-09

    The extent of metal release from implant materials that are irradiated during radiotherapy may be influenced by irradiation-formed radicals. The influence of gamma irradiation, with a total dose of relevance for radiotherapy (e.g., for cancer treatments) on the extent of metal release from biomedical stainless steel AISI 316L and a cobalt-chromium alloy (CoCrMo) was investigated in physiological relevant solutions (phosphate buffered saline with and without 10 g/L bovine serum albumin) at pH 7.3. Directly after irradiation, the released amounts of metals were significantly higher for irradiated CoCrMo as compared to nonirradiated CoCrMo, resulting in an increased surface passivation (enhanced passive conditions) that hindered further release. A similar effect was observed for 316L showing lower nickel release after 1 h of initially irradiated samples as compared to nonirradiated samples. However, the effect of irradiation (total dose of 16.5 Gy) on metal release and surface oxide composition and thickness was generally small. Most metals were released initially (within seconds) upon immersion from CoCrMo but not from 316L. Albumin induced an increased amount of released metals from AISI 316L but not from CoCrMo. Albumin was not found to aggregate to any greater extent either upon gamma irradiation or in the presence of trace metal ions, as determined using different light scattering techniques. Further studies should elucidate the effect of repeated friction and fractionated low irradiation doses on the short- and long term metal release process of biomedical materials. © 2018 Wiley Periodicals, Inc. J Biomed Mater Res Part B: Appl Biomater, 2018. © 2018 The Authors Journal of Biomedical Materials Research Part B: Applied Biomaterials Published by Wiley Periodicals, Inc.

  9. How Soft Gamma Repeaters Might Make Fast Radio Bursts

    NASA Astrophysics Data System (ADS)

    Katz, J. I.

    2016-08-01

    There are several phenomenological similarities between soft gamma repeaters (SGRs) and fast radio bursts (FRBs), including duty factors, timescales, and repetition. The sudden release of magnetic energy in a neutron star magnetosphere, as in popular models of SGRs, can meet the energy requirements of FRBs, but requires both the presence of magnetospheric plasma, in order for dissipation to occur in a transparent region, and a mechanism for releasing much of that energy quickly. FRB sources and SGRs are distinguished by long-lived (up to thousands of years) current-carrying coronal arches remaining from the formation of the young neutron star, and their decay ends the phase of SGR/AXP/FRB activity even though “magnetar” fields may persist. Runaway increases in resistance when the current density exceeds a threshold, releases magnetostatic energy in a sudden burst, and produces high brightness GHz emission of FRB by a coherent process. SGRs are produced when released energy thermalizes as an equlibrium pair plasma. The failures of some alternative FRB models and the non-detection of SGR 1806-20 at radio frequencies are discussed in the appendices.

  10. Search for Very-high-energy Emission from Gamma-Ray Bursts Using the First 18 Months of Data from the HAWC Gamma-Ray Observatory

    NASA Astrophysics Data System (ADS)

    Alfaro, R.; Alvarez, C.; Álvarez, J. D.; Arceo, R.; Arteaga-Velázquez, J. C.; Avila Rojas, D.; Ayala Solares, H. A.; Barber, A. S.; Bautista-Elivar, N.; Becerril, A.; Belmont-Moreno, E.; BenZvi, S. Y.; Bernal, A.; Braun, J.; Brisbois, C.; Caballero-Mora, K. S.; Capistrán, T.; Carramiñana, A.; Casanova, S.; Castillo, M.; Cotti, U.; Cotzomi, J.; Coutiño deLeón, S.; De la Fuente, E.; De León, C.; DeYoung, T.; Diaz Hernandez, R.; Dingus, B. L.; DuVernois, M. A.; Díaz-Vélez, J. C.; Ellsworth, R. W.; Engel, K.; Fiorino, D. W.; Fraija, N.; García-González, J. A.; Garfias, F.; Gerhardt, M.; González Muñoz, A.; González, M. M.; Goodman, J. A.; Hampel-Arias, Z.; Harding, J. P.; Hernandez-Almada, A.; Hernandez, S.; Hona, B.; Hui, C. M.; Hüntemeyer, P.; Iriarte, A.; Jardin-Blicq, A.; Joshi, V.; Kaufmann, S.; Kieda, D.; Lauer, R. J.; Lee, W. H.; Lennarz, D.; León Vargas, H.; Linnemann, J. T.; Longinotti, A. L.; Raya, G. Luis; Luna-García, R.; López-Coto, R.; Malone, K.; Marinelli, S. S.; Martinez, O.; Martinez-Castellanos, I.; Martínez-Castro, J.; Martínez-Huerta, H.; Matthews, J. A.; Miranda-Romagnoli, P.; Moreno, E.; Mostafá, M.; Nellen, L.; Newbold, M.; Noriega-Papaqui, R.; Pelayo, R.; Pérez-Pérez, E. G.; Pretz, J.; Ren, Z.; Rho, C. D.; Rivière, C.; Rosa-González, D.; Rosenberg, M.; Ruiz-Velasco, E.; Salazar, H.; Salesa Greus, F.; Sandoval, A.; Schneider, M.; Schoorlemmer, H.; Sinnis, G.; Smith, A. J.; Springer, R. W.; Surajbali, P.; Taboada, I.; Tibolla, O.; Tollefson, K.; Torres, I.; Ukwatta, T. N.; Vianello, G.; Weisgarber, T.; Westerhoff, S.; Wood, J.; Yapici, T.; Younk, P. W.; Zepeda, A.; Zhou, H.; HAWC Collaboration

    2017-07-01

    The High Altitude Water Cherenkov (HAWC) Gamma-ray Observatory is an extensive air shower detector operating in central Mexico that has recently completed its first two years of full operations. If for a burst like GRB 130427A at a redshift of 0.34 and a high-energy component following a power law with index 1.66, the high-energy component is extended to higher energies with no cutoff other than that from extragalactic background light attenuation, HAWC would observe gamma-rays with a peak energy of ˜300 GeV. This paper reports the results of HAWC observations of 64 gamma-ray bursts (GRBs) detected by Swift and Fermi, including 3 GRBs that were also detected by the Large Area Telescope (Fermi-LAT). An ON/OFF analysis method is employed, searching on the timescale given by the observed light curve at keV-MeV energies and also on extended timescales. For all GRBs and timescales, no statistically significant excess of counts is found and upper limits on the number of gamma-rays and the gamma-ray flux are calculated. GRB 170206A, the third brightest short GRB detected by the Gamma-ray Burst Monitor on board the Fermi satellite (Fermi-GBM) and also detected by the LAT, occurred very close to zenith. The LAT measurements can neither exclude the presence of a synchrotron self-Compton component nor constrain its spectrum. Instead, the HAWC upper limits constrain the expected cutoff in an additional high-energy component to be less than 100 {GeV} for reasonable assumptions about the energetics and redshift of the burst.

  11. Fermi-LAT Observations of the Gamma-Ray Burst GRB 130427A

    DOE PAGES

    Ackermann, M.; Ajello, M.; Asano, K.; ...

    2013-11-21

    The Large Area Telescope aboard the Fermi Gamma-ray Space Telescope provide constraints on the nature of these unique astrophysical sources using the observations of the exceptionally bright gamma-ray burst (GRB) 130427A. We found that GRB 130427A had the largest fluence, highest-energy photon (95 GeV), longest γ-ray duration (20 hours), and one of the largest isotropic energy releases ever observed from a GRB. Temporal and spectral analyses of GRB 130427A challenge the widely accepted model that the nonthermal high-energy emission in the afterglow phase of GRBs is synchrotron emission radiated by electrons accelerated at an external shock.

  12. Very-high energy gamma-ray astronomy. A 23-year success story in high-energy astroparticle physics

    NASA Astrophysics Data System (ADS)

    Lorenz, E.; Wagner, R.

    2012-08-01

    Very-high energy (VHE) gamma quanta contribute only a minuscule fraction - below one per million - to the flux of cosmic rays. Nevertheless, being neutral particles they are currently the best "messengers" of processes from the relativistic/ultra-relativistic Universe because they can be extrapolated back to their origin. The window of VHE gamma rays was opened only in 1989 by the Whipple collaboration, reporting the observation of TeV gamma rays from the Crab nebula. After a slow start, this new field of research is now rapidly expanding with the discovery of more than 150 VHE gamma-ray emitting sources. Progress is intimately related with the steady improvement of detectors and rapidly increasing computing power. We give an overview of the early attempts before and around 1989 and the progress after the pioneering work of the Whipple collaboration. The main focus of this article is on the development of experimental techniques for Earth-bound gamma-ray detectors; consequently, more emphasis is given to those experiments that made an initial breakthrough rather than to the successors which often had and have a similar (sometimes even higher) scientific output as the pioneering experiments. The considered energy threshold is about 30 GeV. At lower energies, observations can presently only be performed with balloon or satellite-borne detectors. Irrespective of the stormy experimental progress, the success story could not have been called a success story without a broad scientific output. Therefore we conclude this article with a summary of the scientific rationales and main results achieved over the last two decades.

  13. Primary gamma-rays with E gamma or = to 10(15) eV: Evidence for ultrahigh energy particle acceleration in galactic sources

    NASA Technical Reports Server (NTRS)

    Aharonian, F. A.; Mamidjanian, E. A.; Nikolsky, S. I.; Tukish, E. I.

    1985-01-01

    The recently observed primary ultra high energy gamma-rays (UHEGR) testify to the cosmic ray (CR) acceleration in the Galaxy. The available data may be interpreted as gamma-ray production due to photomeson production in CR sources.

  14. Modulated high-energy gamma-ray emission from the microquasar Cygnus X-3.

    PubMed

    Abdo, A A; Ackermann, M; Ajello, M; Axelsson, M; Baldini, L; Ballet, J; Barbiellini, G; Bastieri, D; Baughman, B M; Bechtol, K; Bellazzini, R; Berenji, B; Blandford, R D; Bloom, E D; Bonamente, E; Borgland, A W; Brez, A; Brigida, M; Bruel, P; Burnett, T H; Buson, S; Caliandro, G A; Cameron, R A; Caraveo, P A; Casandjian, J M; Cecchi, C; Celik, O; Chaty, S; Cheung, C C; Chiang, J; Ciprini, S; Claus, R; Cohen-Tanugi, J; Cominsky, L R; Conrad, J; Corbel, S; Corbet, R; Dermer, C D; de Palma, F; Digel, S W; do Couto e Silva, E; Drell, P S; Dubois, R; Dubus, G; Dumora, D; Farnier, C; Favuzzi, C; Fegan, S J; Focke, W B; Fortin, P; Frailis, M; Fusco, P; Gargano, F; Gehrels, N; Germani, S; Giavitto, G; Giebels, B; Giglietto, N; Giordano, F; Glanzman, T; Godfrey, G; Grenier, I A; Grondin, M-H; Grove, J E; Guillemot, L; Guiriec, S; Hanabata, Y; Harding, A K; Hayashida, M; Hays, E; Hill, A B; Hjalmarsdotter, L; Horan, D; Hughes, R E; Jackson, M S; Jóhannesson, G; Johnson, A S; Johnson, T J; Johnson, W N; Kamae, T; Katagiri, H; Kawai, N; Kerr, M; Knödlseder, J; Kocian, M L; Koerding, E; Kuss, M; Lande, J; Latronico, L; Lemoine-Goumard, M; Longo, F; Loparco, F; Lott, B; Lovellette, M N; Lubrano, P; Madejski, G M; Makeev, A; Marchand, L; Marelli, M; Max-Moerbeck, W; Mazziotta, M N; McColl, N; McEnery, J E; Meurer, C; Michelson, P F; Migliari, S; Mitthumsiri, W; Mizuno, T; Monte, C; Monzani, M E; Morselli, A; Moskalenko, I V; Murgia, S; Nolan, P L; Norris, J P; Nuss, E; Ohsugi, T; Omodei, N; Ong, R A; Ormes, J F; Paneque, D; Parent, D; Pelassa, V; Pepe, M; Pesce-Rollins, M; Piron, F; Pooley, G; Porter, T A; Pottschmidt, K; Rainò, S; Rando, R; Ray, P S; Razzano, M; Rea, N; Readhead, A; Reimer, A; Reimer, O; Richards, J L; Rochester, L S; Rodriguez, J; Rodriguez, A Y; Romani, R W; Ryde, F; Sadrozinski, H F-W; Sander, A; Saz Parkinson, P M; Sgrò, C; Siskind, E J; Smith, D A; Smith, P D; Spinelli, P; Starck, J-L; Stevenson, M; Strickman, M S; Suson, D J; Takahashi, H; Tanaka, T; Thayer, J B; Thompson, D J; Tibaldo, L; Tomsick, J A; Torres, D F; Tosti, G; Tramacere, A; Uchiyama, Y; Usher, T L; Vasileiou, V; Vilchez, N; Vitale, V; Waite, A P; Wang, P; Wilms, J; Winer, B L; Wood, K S; Ylinen, T; Ziegler, M

    2009-12-11

    Microquasars are accreting black holes or neutron stars in binary systems with associated relativistic jets. Despite their frequent outburst activity, they have never been unambiguously detected emitting high-energy gamma rays. The Fermi Large Area Telescope (LAT) has detected a variable high-energy source coinciding with the position of the x-ray binary and microquasar Cygnus X-3. Its identification with Cygnus X-3 is secured by the detection of its orbital period in gamma rays, as well as the correlation of the LAT flux with radio emission from the relativistic jets of Cygnus X-3. The gamma-ray emission probably originates from within the binary system, opening new areas in which to study the formation of relativistic jets.

  15. Peculiarities of gamma-quanta distribution at 20 TeV energy

    NASA Technical Reports Server (NTRS)

    Ermakov, P. M.; Loktionov, A. A.; Lukin, Y. T.; Sadykov, T. K.

    1985-01-01

    The angular distribution of protons from the fragmentational region is analyzed. The gamma-quanta families are generated in a dense target by cosmic ray particles at 20 Tev energy. Families were found which had dense groups (spikes) of gamma-quanta where the rapidity/density is 3 times more than the average value determined for all registered families. The experimental data is compared with the results of artificial families simulation.

  16. Coded-aperture imaging of the Galactic center region at gamma-ray energies

    NASA Technical Reports Server (NTRS)

    Cook, Walter R.; Grunsfeld, John M.; Heindl, William A.; Palmer, David M.; Prince, Thomas A.

    1991-01-01

    The first coded-aperture images of the Galactic center region at energies above 30 keV have revealed two strong gamma-ray sources. One source has been identified with the X-ray source IE 1740.7 - 2942, located 0.8 deg away from the nucleus. If this source is at the distance of the Galactic center, it is one of the most luminous objects in the galaxy at energies from 35 to 200 keV. The second source is consistent in location with the X-ray source GX 354 + 0 (MXB 1728-34). In addition, gamma-ray flux from the location of GX 1 + 4 was marginally detected at a level consistent with other post-1980 measurements. No significant hard X-ray or gamma-ray flux was detected from the direction of the Galactic nucleus or from the direction of the recently discovered gamma-ray source GRS 1758-258.

  17. Universal statistics of soft gamma-ray repeating (SGR) bursts

    NASA Astrophysics Data System (ADS)

    Kondratyev, V. N.; Korovina, Yu. V.

    2018-01-01

    Soft gamma repeater (SGR) bursts are considered as a release of magnetic energy stored in the baryon degrees of freedom of the magnetar crust. It is shown that this interpretation allows all observations of these bursts to be systematized and universal statistical properties to be revealed and explained.

  18. High energy gamma-ray astronomy; Proceedings of the International Conference, ANN Arbor, MI, Oct. 2-5, 1990

    NASA Astrophysics Data System (ADS)

    Matthews, James

    The present volume on high energy gamma-ray astronomy discusses the composition and properties of heavy cosmic rays greater than 10 exp 12 eV, implications of the IRAS Survey for galactic gamma-ray astronomy, gamma-ray emission from young neutron stars, and high-energy diffuse gamma rays. Attention is given to observations of TeV photons at the Whipple Observatory, TeV gamma rays from millisecond pulsars, recent data from the CYGNUS experiment, and recent results from the Woomera Telescope. Topics addressed include bounds on a possible He/VHE gamma-ray line signal of Galactic dark matter, albedo gamma rays from cosmic ray interactions on the solar surface, source studies, and the CANGAROO project. Also discussed are neural nets and other methods for maximizing the sensitivity of a low-threshold VHE gamma-ray telescope, a prototype water-Cerenkov air-shower detector, detection of point sources with spark chamber gamma-ray telescopes, and real-time image parameterization in high energy gamma-ray astronomy using transputers. (For individual items see A93-25002 to A93-25039)

  19. Spectrometer of high energy gamma quantums

    NASA Technical Reports Server (NTRS)

    Blokhintsev, I. D.; Melioranskiy, A. S.; Kalinkin, L. F.; Nagornykh, Y. I.; Pryakhin, Y. A.

    1979-01-01

    A detailed description of the apparatus GG-2M is given. The spectrometer contains a Cerenkov and scintillation (including anticoincidence) counter. The energies of the gamma quantums are measured by a shower calorimeter, in which scintillation counters are used in the capacity of detectors. Results are given for tuning the device on mu-mesons of cosmic rays. The data of physical tuning allow more reliable interpretation of the results of measurements which are received on the satellites.

  20. GLAST: Exploring Nature's Highest Energy Processes with the Gamma-ray Large Area Space Telescope

    NASA Technical Reports Server (NTRS)

    Digel, Seth; Myers, J. D.; White, Nicholas E. (Technical Monitor)

    2001-01-01

    The Gamma-ray Large Area Space Telescope (GLAST) is an international and multi-agency space mission that will study the cosmos in the energy range 10 keV-300 GeV. Several successful exploratory missions in gamma-ray astronomy led to the Energetic Gamma Ray Experiment Telescope (EGRET) instrument on the Compton Gamma Ray Observatory (CGRO). Launched in 1991, EGRET made the first complete survey of the sky in the 30 MeV-10 GeV range. EGRET showed the high-energy gamma-ray sky to be surprisingly dynamic and diverse, with sources ranging from the sun and moon to massive black holes at large redshifts. Most of the gamma-ray sources detected by EGRET remain unidentified. In light of the discoveries with EGRET, the great potential of the next generation gamma-ray telescope can be appreciated. GLAST will have an imaging gamma-ray telescope vastly more capable than instruments flown previously, as well as a secondary instrument to augment the study of gamma-ray bursts. The main instrument, the Large Area Telescope (LAT), will have superior area, angular resolution, field of view, and deadtime that together will provide a factor of 30 or more advance in sensitivity, as well as provide capability for study of transient phenomena. The GLAST Burst Monitor (GBM) will have a field of view several times larger than the LAT and will provide spectral coverage of gamma-ray bursts that extends from the lower limit of the LAT down to 10 keV. The basic parameters of the GBM are compared to those of the Burst and Transient Source Experiment (BATSE) instrument on CGRO in Table 1-2. With the LAT and GBM, GLAST will be a flexible observatory for investigating the great range of astrophysical phenomena best studied in high-energy gamma rays. NASA plans to launch GLAST in late 2005.

  1. Activation measurement of the 3He(alpha,gamma)7Be cross section at low energy.

    PubMed

    Bemmerer, D; Confortola, F; Costantini, H; Formicola, A; Gyürky, Gy; Bonetti, R; Broggini, C; Corvisiero, P; Elekes, Z; Fülöp, Zs; Gervino, G; Guglielmetti, A; Gustavino, C; Imbriani, G; Junker, M; Laubenstein, M; Lemut, A; Limata, B; Lozza, V; Marta, M; Menegazzo, R; Prati, P; Roca, V; Rolfs, C; Alvarez, C Rossi; Somorjai, E; Straniero, O; Strieder, F; Terrasi, F; Trautvetter, H P

    2006-09-22

    The nuclear physics input from the 3He(alpha,gamma)7Be cross section is a major uncertainty in the fluxes of 7Be and 8B neutrinos from the Sun predicted by solar models and in the 7Li abundance obtained in big-bang nucleosynthesis calculations. The present work reports on a new precision experiment using the activation technique at energies directly relevant to big-bang nucleosynthesis. Previously such low energies had been reached experimentally only by the prompt-gamma technique and with inferior precision. Using a windowless gas target, high beam intensity, and low background gamma-counting facilities, the 3He(alpha,gamma)7Be cross section has been determined at 127, 148, and 169 keV center-of-mass energy with a total uncertainty of 4%. The sources of systematic uncertainty are discussed in detail. The present data can be used in big-bang nucleosynthesis calculations and to constrain the extrapolation of the 3He(alpha,gamma)7Be astrophysical S factor to solar energies.

  2. Statistical Measurement of the Gamma-Ray Source-count Distribution as a Function of Energy

    NASA Astrophysics Data System (ADS)

    Zechlin, Hannes-S.; Cuoco, Alessandro; Donato, Fiorenza; Fornengo, Nicolao; Regis, Marco

    2016-08-01

    Statistical properties of photon count maps have recently been proven as a new tool to study the composition of the gamma-ray sky with high precision. We employ the 1-point probability distribution function of six years of Fermi-LAT data to measure the source-count distribution dN/dS and the diffuse components of the high-latitude gamma-ray sky as a function of energy. To that aim, we analyze the gamma-ray emission in five adjacent energy bands between 1 and 171 GeV. It is demonstrated that the source-count distribution as a function of flux is compatible with a broken power law up to energies of ˜50 GeV. The index below the break is between 1.95 and 2.0. For higher energies, a simple power-law fits the data, with an index of {2.2}-0.3+0.7 in the energy band between 50 and 171 GeV. Upper limits on further possible breaks as well as the angular power of unresolved sources are derived. We find that point-source populations probed by this method can explain {83}-13+7% ({81}-19+52%) of the extragalactic gamma-ray background between 1.04 and 1.99 GeV (50 and 171 GeV). The method has excellent capabilities for constraining the gamma-ray luminosity function and the spectra of unresolved blazars.

  3. Observation of fluctuation of gamma-ray count rate accompanying thunderstorm activity and energy spectrum of gamma rays in the atmosphere up to several kilometers altitude from the ground

    NASA Astrophysics Data System (ADS)

    Torii, T.; Sanada, Y.; Watanabe, A.

    2017-12-01

    In the vicinity of the tops of high mountains and in the coastal areas of the Sea of Japan in winter, the generation of high energy photons that lasts more than 100 seconds at the occurrence of thunderclouds has been reported. At the same time, 511 keV gamma rays are also detected. On the other hand, we irradiated a radiosonde equipped with gamma-ray detectors at the time of thunderstorm and observed fluctuation in gamma-ray count-rate. As a result, we found that the gamma-ray count-rate increases significantly near the top of the thundercloud. Therefore, in order to investigate the fluctuation of the energy of the gamma rays, we developed a radiation detector for radiosonde to observe the fluctuation of the low energy gamma-ray spectrum and observed the fluctuation of the gamma-ray spectrum. We will describe the counting rate and spectral fluctuation of gamma-ray detectors for radiosonde observed in the sky in Fukushima prefecture, Japan.

  4. An improved time of flight gamma-ray telescope to monitor diffuse gamma-ray in the energy range 5 MeV - 50 MeV

    NASA Technical Reports Server (NTRS)

    Dacostafereiraneri, A.; Bui-Van, A.; Lavigne, J. M.; Sabaud, C.; Vedrenne, G.; Agrinier, B.; Gouiffes, C.

    1985-01-01

    A time of flight measuring device is the basic triggering system of most of medium and high energy gamma-ray telescopes. A simple gamma-ray telescope has been built in order to check in flight conditions the functioning of an advanced time of flight system. The technical ratings of the system are described. This telescope has been flown twice with stratospheric balloons, its axis being oriented at various Zenital directions. Flight results are presented for diffuse gamma-rays, atmospheric secondaries, and various causes of noise in the 5 MeV-50 MeV energy range.

  5. Influence of poly (lactide-co-glycolide) type and gamma irradiation on the betamethasone acetate release from the in situ forming systems.

    PubMed

    Rafienia, Mohammad; Emami, Shahriar Hojjati; Mirzadeh, Hamid; Mobedi, Hamid; Karbasi, Saeed

    2009-04-01

    In situ forming biodegradable polymeric systems were prepared from Poly (DL-lactide-co-glycolide), RG504H (50:50, lactide:glycolide), RG756 (75:25) and mixture of them. They were dissolved in N-methyl-2-pyrrolidone (33% w/w) and mixed with betamethasone acetate (BTMA, 5 and 10% w/w) and ethyl heptanoate (5% w/w, as an additive). The effects of gamma irradiation, drug loading, type of polymers and solvent removal were evaluated on release profiles. Scanning electron microscopy (SEM) of RG756 samples loaded by BTMA did not show any degradation until two weeks. Differential scanning calorimeter (DSC) experiments confirmed insignificant decrease in T(g), and consequently release rate. Declining T(g) of RG504H and RG756 after gamma irradiation was about 0.4 and 1.46 degrees C, respectively. High performance liquid chromatography (HPLC) revealed that BTMA release is more rapid from the formulations prepared using the RG504H with lower molecular weight. The formulations prepared by RG756 had lower burst release (2.5-41%) than the samples based on RG504H (60-67%) and mixture of them (30-33%). Regarding this research three different kinds of steriled in situ forming systems were developed which can release BTMA for 24, 90 and 60 days.

  6. Executive Summary of the Guidelines for the Use of interferon-gamma Release Assays in the Diagnosis of Tuberculosis Infection.

    PubMed

    Santin, Miguel; García-García, José-María; Rigau, David; Altet, Neus; Anibarro, Luis; Casas, Irma; Díez, Nuria; García-Gasalla, Mercedes; Martínez-Lacasa, Xavier; Penas, Antón; Pérez-Escolano, Elvira; Sánchez, Francisca; Domínguez, José

    2016-09-01

    Interferon-gamma release assays are widely used for the diagnosis of tuberculosis infection in Spain. However, there is no consensus on their application in specific clinical scenarios. To develop a guide-line for their use, a panel of experts comprising specialists in infectious diseases, respiratory diseases, microbiology, pediatrics and preventive medicine, together with a methodologist, conducted a systematic literature search, summarized the findings, rated the quality of the evidence, and formulated recommendations following the Grading of Recommendations of Assessment Development and Evaluations methodology. This document provides evidence-based guidance on the use of interferon-gamma release assays for the diagnosis of tuberculosis infection in patients at risk of tuberculosis or suspected of having active disease. The guidelines will be applicable to specialist and primary care, and public health. Copyright © 2016 SEPAR. Publicado por Elsevier España, S.L.U. All rights reserved.

  7. Constraining heavy decaying dark matter with the high energy gamma-ray limits

    NASA Astrophysics Data System (ADS)

    Kalashev, O. E.; Kuznetsov, M. Yu.

    2016-09-01

    We consider decaying dark matter with masses 1 07≲M ≲1 016 GeV as a source of ultrahigh energy (UHE) gamma rays. Using recent limits on UHE gamma-ray flux for energies Eγ>2 ×1 014 eV , provided by extensive air shower observatories, we put limits on masses and lifetimes of the dark matter. We also discuss possible dark matter decay origin of tentative 100 PeV photon flux detected with the EAS-MSU experiment.

  8. THE HIGH-ENERGY, ARCMINUTE-SCALE GALACTIC CENTER GAMMA-RAY SOURCE

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

    Chernyakova, M.; Malyshev, D.; Aharonian, F. A.

    2011-01-10

    Employing data collected during the first 25 months of observations by the Fermi-LAT, we describe and subsequently seek to model the very high energy (>300 MeV) emission from the central few parsecs of our Galaxy. We analyze the morphological, spectral, and temporal characteristics of the central source, 1FGL J1745.6-2900. The data show a clear, statistically significant signal at energies above 10 GeV, where the Fermi-LAT has angular resolution comparable to that of HESS at TeV energies. This makes a meaningful joint analysis of the data possible. Our analysis of the Fermi data (alone) does not uncover any statistically significant variabilitymore » of 1FGL J1745.6-2900 at GeV energies on the month timescale. Using the combination of Fermi data on 1FGL J1745.6-2900 and HESS data on the coincident, TeV source HESS J1745-290, we show that the spectrum of the central gamma-ray source is inflected with a relatively steep spectral region matching between the flatter spectrum found at both low and high energies. We model the gamma-ray production in the inner 10 pc of the Galaxy and examine cosmic ray (CR) proton propagation scenarios that reproduce the observed spectrum of the central source. We show that a model that instantiates a transition from diffusive propagation of the CR protons at low energy to almost rectilinear propagation at high energies can explain well the spectral phenomenology. We find considerable degeneracy between different parameter choices which will only be broken with the addition of morphological information that gamma-ray telescopes cannot deliver given current angular resolution limits. We argue that a future analysis performed in combination with higher-resolution radio continuum data holds out the promise of breaking this degeneracy.« less

  9. Low-temperature high-Z gamma-detectors with very high energy resolution

    NASA Astrophysics Data System (ADS)

    Pobes, Carlos; Brofferio, Chiara; Bucci, Carlo; Cremonesi, Oliviero; Fiorini, Ettore; Giuliani, Andrea; Nucciotti, Angelo; Pavan, Maura; Pedretti, Marisa; Pessina, Gianluigi; Pirro, Stefano; Previtali, Ezio; Sisti, Monica; Vanzini, Marco; Zanotti, Luigi

    2001-12-01

    High-Z low-temperature calorimeters are developed by an Italian collaboration (Milano-Como-Gran Sasso Underground Laboratories) in order to search for rare nuclear events and Dark Matter massive candidates. They exhibit an excellent energy resolution, close to that of Ge-diodes, but a much higher efficiency. Different high-Z materials were initially employed . A many-years optimisation work on tellurium oxide (TeO2) lead to impressive results: devices with total masses around 750 g present FWHM energy resolutions on gamma-ray peaks ranging from 1 KeV (close to the 5 KeV energy threshold) to 2.6 KeV at 2615 KeV (208Tl gamma line). A 3.2 KeV FWHM energy resolution was obtained at 5.4 MeV (210Po alpha line), which is by far the best one ever achieved with any alpha detector. These devices, operated at about 10 mK, consist of a TeO2 single crystal thermally coupled to a 50 mg Neutron Transmutation Doped (NTD) Ge crystal working as a temperature sensor. Special care was devoted to methods for response linearization and temporal stabilisation. Devices based on the same principle and specifically optimised could find applications in several fields like gamma-ray astrophysics, nuclear physics searches, environmental monitoring and radiation metrology.

  10. Observations of Spin-Powered Pulsars with the AGILE Gamma-Ray Telescope

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

    Pellizzoni, A.; Pilia, M.; Possenti, M.

    2008-12-24

    AGILE is a small gamma-ray astronomy satellite mission of the Italian Space Agency dedicated to high-energy astrophysics launched in 2007 April. It provides large sky exposure levels (> or approx. 10{sup 9} cm{sup 2} s per year on the Galactic Plane) with sensitivity peaking at E{approx}400 MeV(and simultaneous X-ray monitoring in the 18-60 keV band) where the bulk of pulsar energy output is typically released. Its {approx}1 {mu}s is absolute time tagging capability makes it perfectly suited for the study of gamma-ray pulsars following up on the CGRO/EGRET heritage. In this paper we summarize the timing results obtained during themore » first year of AGILE observations of the known gamma-ray pulsars Vela, Crab, Geminga and B 1706-4. AGILE collected a large number of gamma-ray photons from EGRET pulsars ({approx}10,000 pulsed counts for Vela) in only few months of observations unveiling new interesting features at sub-millisecond level in the pulsars' high-energy light-curves and paving the way to the discovery of new gamma-ray pulsars.« less

  11. Cosmological gamma-ray bursts

    NASA Technical Reports Server (NTRS)

    Paczynski, Bohdan

    1991-01-01

    The distribution in angle and flux of gamma-ray bursts indicates that the majority of gamma-ray bursters are at cosmological distances, i.e., at z of about 1. The rate is then about 10 exp -8/yr in a galaxy like the Milky Way, i.e., orders of magnitude lower than the estimated rate for collisions between neutron stars in close binary systems. The energy per burst is about 10 exp 51 ergs, assuming isotropic emission. The events appear to be less energetic and more frequent if their emission is strongly beamed. Some tests for the distance scale are discussed: a correlation between the burst's strength and its spectrum; the absorption by the Galactic gas below about 2 keV; the X-ray tails caused by forward scattering by the Galactic dust; about 1 month recurrence of some bursts caused by gravitational lensing by foreground galaxies; and a search for gamma-ray bursts in M31. The bursts appear to be a manifestation of something exotic, but conventional compact objects can provide an explanation. The best possibility is offered by a decay of a bindary composed of a spinning-stellar-mass black-hole primary and a neutron or a strange-quark star secondary. In the final phase the secondary is tidally disrupted, forms an accretion disk, and up to 10 exp 54 ergs are released. A very small fraction of this energy powers the gamma-ray burst.

  12. Recent high energy gamma-ray results from SAS-2

    NASA Technical Reports Server (NTRS)

    Thompson, D. J.; Fichtel, C. E.; Hartman, R. C.; Kniffen, D. A.; Bignami, G. F.; Ogelman, H. B.; Ozel, M. E.; Tumer, T.; Lamb, R. C.

    1977-01-01

    Recent developments in gamma-ray astronomy due to the results from SAS-2 have focused on two areas. First, the emission from the plane of the Galaxy is the dominant feature in the gamma-ray sky. The galactic latitude and longitude distributions are consistent with the concept that the high-energy radiation originates from cosmic rays interacting with interstellar matter, and the measurements support a galactic origin for cosmic rays. Second, searches of the SAS-2 data for emission from localized sources have shown three strong discrete gamma-ray sources: the Crab nebula and PSR 0531 + 21, the Vela supernova remnant and PSR 0833-45, and a source near galactic coordinates 193 deg longitude, +3 deg latitude, which does not appear to be associated with other known celestial objects. Evidence has also been found for pulsed gamma-ray emission from two other radio pulsars, PSR 1818-04 and PSR 1747-46. A localized source near longitudes 76-80 deg may be associated with the X-ray source Cyg X-3.

  13. Statistical measurement of the gamma-ray source-count distribution as a function of energy

    DOE PAGES

    Zechlin, Hannes-S.; Cuoco, Alessandro; Donato, Fiorenza; ...

    2016-07-29

    Statistical properties of photon count maps have recently been proven as a new tool to study the composition of the gamma-ray sky with high precision. Here, we employ the 1-point probability distribution function of six years of Fermi-LAT data to measure the source-count distribution dN/dS and the diffuse components of the high-latitude gamma-ray sky as a function of energy. To that aim, we analyze the gamma-ray emission in five adjacent energy bands between 1 and 171 GeV. It is demonstrated that the source-count distribution as a function of flux is compatible with a broken power law up to energies of ~50 GeV. Furthermore, the index below the break is between 1.95 and 2.0. For higher energies, a simple power-law fits the data, with an index ofmore » $${2.2}_{-0.3}^{+0.7}$$ in the energy band between 50 and 171 GeV. Upper limits on further possible breaks as well as the angular power of unresolved sources are derived. We find that point-source populations probed by this method can explain $${83}_{-13}^{+7}$$% ($${81}_{-19}^{+52}$$%) of the extragalactic gamma-ray background between 1.04 and 1.99 GeV (50 and 171 GeV). Our method has excellent capabilities for constraining the gamma-ray luminosity function and the spectra of unresolved blazars.« less

  14. Statistical measurement of the gamma-ray source-count distribution as a function of energy

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

    Zechlin, Hannes-S.; Cuoco, Alessandro; Donato, Fiorenza

    Statistical properties of photon count maps have recently been proven as a new tool to study the composition of the gamma-ray sky with high precision. Here, we employ the 1-point probability distribution function of six years of Fermi-LAT data to measure the source-count distribution dN/dS and the diffuse components of the high-latitude gamma-ray sky as a function of energy. To that aim, we analyze the gamma-ray emission in five adjacent energy bands between 1 and 171 GeV. It is demonstrated that the source-count distribution as a function of flux is compatible with a broken power law up to energies of ~50 GeV. Furthermore, the index below the break is between 1.95 and 2.0. For higher energies, a simple power-law fits the data, with an index ofmore » $${2.2}_{-0.3}^{+0.7}$$ in the energy band between 50 and 171 GeV. Upper limits on further possible breaks as well as the angular power of unresolved sources are derived. We find that point-source populations probed by this method can explain $${83}_{-13}^{+7}$$% ($${81}_{-19}^{+52}$$%) of the extragalactic gamma-ray background between 1.04 and 1.99 GeV (50 and 171 GeV). Our method has excellent capabilities for constraining the gamma-ray luminosity function and the spectra of unresolved blazars.« less

  15. HOW SOFT GAMMA REPEATERS MIGHT MAKE FAST RADIO BURSTS

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

    Katz, J. I., E-mail: katz@wuphys.wustl.edu

    2016-08-01

    There are several phenomenological similarities between soft gamma repeaters (SGRs) and fast radio bursts (FRBs), including duty factors, timescales, and repetition. The sudden release of magnetic energy in a neutron star magnetosphere, as in popular models of SGRs, can meet the energy requirements of FRBs, but requires both the presence of magnetospheric plasma, in order for dissipation to occur in a transparent region, and a mechanism for releasing much of that energy quickly. FRB sources and SGRs are distinguished by long-lived (up to thousands of years) current-carrying coronal arches remaining from the formation of the young neutron star, and theirmore » decay ends the phase of SGR/AXP/FRB activity even though “magnetar” fields may persist. Runaway increases in resistance when the current density exceeds a threshold, releases magnetostatic energy in a sudden burst, and produces high brightness GHz emission of FRB by a coherent process. SGRs are produced when released energy thermalizes as an equlibrium pair plasma. The failures of some alternative FRB models and the non-detection of SGR 1806-20 at radio frequencies are discussed in the appendices.« less

  16. [Neoplastic transformation of mouse fibroblasts under the influence of high-energy protons and gamma-rays].

    PubMed

    Voskanian, K Sh

    2004-01-01

    Oncoginic transformations of mouse fibroblasts C3H10T1/2 after exposure to proton energies 150 and 584 MeV were compared with fibroblast effects of gamma-radiation. Prior to exposure, cell populations (2.7 x 10(3) cells/cm2) were inoculated in plastic vials with the surface area of 75 cm2 and cultivated 11 days. Survivability was determined by comparing the number of cell colonies in irradiated and non-irradiated (control) vials. Transformation rate was calculated by dividing the total transformation focus number by the number of survived cells in a vial. Rate of oncogenic transformations after gamma- and proton (584 MeV) irradiation was essentially identical, i.e. the parameter grew rapidly at the doses < 1 Gy and slowed down at the doses > 1 Gy. In the dose interval between 1 and 5 Gy, transformation rate for proton energy 150 MeV was found low compared with gamma-radiation and proton energy 584 MeV. It is hypothesized that the different transformation rate after exposure to proton energy 150 MeV is linked with the high linear energy transfer as compared with the proton energy of 584 MeV and gamma-radiation.

  17. Multiwavelength observations of unidentified high energy gamma ray sources

    NASA Technical Reports Server (NTRS)

    Halpern, Jules P.

    1993-01-01

    As was the case for COS B, the majority of high-energy (greater than 100 MeV) gamma-ray sources detected by the EGRET instrument on GRO are not immediately identifiable with cataloged objects at other wavelengths. These persistent gamma-ray sources are, next to the gamma-ray bursts, the least understood objects in the universe. Even a rudimentary understanding of their nature awaits identifications and follow-up work at other wavelengths to tell us what they are. The as yet unidentified sources are potentially the most interesting, since they may represent unrecognized new classes of astronomical objects, such as radio-quiet pulsars or new types of active galactic nuclei (AGN's). This two-year investigation is intended to support the analysis, correlation, and theoretical interpretation of data that we are obtaining at x ray, optical, and radio wavelengths in order to render the gamma-ray data interpretable. According to plan, in the first year concentration was on the identification and study of Geminga. The second year will be devoted to studies of similar unidentified gamma-ray sources which will become available in the first EGRET catalogs. The results obtained so far are presented in the two papers which are reproduced in the Appendix. In these papers, we discuss the pulse profiles of Geminga, the geometry and efficiency of the magnetospheric accelerator, the distance to Geminga, the implications for theories of polar cap heating, the effect of the magnetic field on the surface emission and environment of the neutron star, and possible interpretations of a radio-quiet Geminga. The implications of the other gamma-ray pulsars which were discovered to have high gamma-ray efficiency are also discussed, and the remaining unidentified COS B sources are attributed to a population of efficient gamma-ray sources, some of which may be radio quiet.

  18. The main beam correction term in kinetic energy release from metastable peaks.

    PubMed

    Petersen, Allan Christian

    2017-12-01

    The correction term for the precursor ion signal width in determination of kinetic energy release is reviewed, and the correction term is formally derived. The derived correction term differs from the traditionally applied term. An experimental finding substantiates the inaccuracy in the latter. The application of the "T-value" to study kinetic energy release is found preferable to kinetic energy release distributions when the metastable peaks are slim and simple Gaussians. For electronically predissociated systems, a "borderline zero" kinetic energy release can be directly interpreted in reaction dynamics with strong curvature in the reaction coordinate. Copyright © 2017 John Wiley & Sons, Ltd.

  19. A Microelectromechanical High-Density Energy Storage/Rapid Release System

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

    Rodgers, M. Steven; Allen, Jim J.; Meeks, Kent D.

    1999-07-21

    One highly desirable characteristic of electrostatically driven microelectromechanical systems (MEMS) is that they consume very little power. The corresponding drawback is that the force they produce may be inadequate for many applications. It has previously been demonstrated that gear reduction units or microtransmissions can substantially increase the torque generated by microengines. Operating speed, however, is also reduced by the transmission gear ratio. Some applications require both high speed and high force. If this output is only required for a limited period of time, then energy could be stored in a mechanical system and rapidly released upon demand. We have designed,more » fabricated, and demonstrated a high-density energy storage/rapid release system that accomplishes this task. Built using a 5-level surface micromachining technology, the assembly closely resembles a medieval crossbow. Energy releases on the order of tens of nanojoules have already been demonstrated, and significantly higher energy systems are under development.« less

  20. Blazar 3C 66A: Another extragalactic source of ultra-high-energy gamma-ray photons

    NASA Astrophysics Data System (ADS)

    Neshpor, Yu. I.; Stepanyan, A. A.; Kalekin, O. P.; Fomin, V. P.; Chalenko, N. N.; Shitov, V. G.

    1998-03-01

    he observations of the object 3C 66A which were carried out with the GT-48 gamma-ray telescope at the Crimean Astrophysical Observatory in November-December 1996 revealed a flux of ultra-high-energy (>10^12 eV) gamma-ray photons from this blazar. According to preliminary estimates, the photon flux is (31) 10^11 photons cm^-2 s^-1. The blazar 3C 66A is the third extragalactic object from which a flux of ultra- high-energy gamma-ray photons was detected. Fluxes of gamma-ray photons were previously detected from the galaxies Mk 421 and Mk 501 at the Whipple observatory. This result provides further evidence that active processes proceed in blazars which are accompanied by the generation of cosmic rays responsible for the emission of gamma-ray photons.

  1. Some problems of the detection of the high energy gamma-radiation in space

    NASA Astrophysics Data System (ADS)

    Fradkin, M. I.; Ginzburg, V. L.; Kurnosova, L. V.; Labensky, A. G.; Razorenov, L. A.; Rusakovich, M. A.; Topchiev, N. P.; Kaplin, V. A.; Runtso, M. F.; Gorchakov, E. V.; Ignatiev, P. P.

    1995-05-01

    Diffuse gamma radiation in the Galaxy has been measured with instruments onboard the COS-B and Compton Gamma Ray Observatory (CGRO) satellites from the tens of keV up to about 30 GeV. There is no experimental data at higher energies, but this data is very important for the spectrum of primary cosmic rays and the existence of neutralinos (hypothetical supersymmetrical particles which are supposed to constitute dark matter in the Galaxy and create gamma-quanta in the process of annihilation). The GAMMA-400 collaboration is working on the design of a telescope for gamma-ray measurements in the 10-1000 GeV range. The electronics of the GAMMA-400 eliminate some hindering effects, in particular the influence of backscattered gammas emitted by the very massive calorimeter (calorimeter albedo). The GAMMA-400 project may be realized in the near future if economic conditions in Russia are favorable.

  2. Unfolding the fission prompt gamma-ray energy and multiplicity distribution measured by DANCE

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

    Chyzh, A; Wu, C Y; Bredeweg, T

    2010-10-16

    The nearly energy independence of the {gamma}-ray efficiency and multiplicity response for the DANCE array, the unusual characteristic elucidated in our early technical report (LLNL-TR-452298), gives one a unique opportunity to derive the true prompt {gamma}-ray energy and multiplicity distribution in fission from the measurement. This unfolding procedure for the experimental data will be described in details and examples will be given to demonstrate the feasibility of reconstruction of the true distribution.

  3. High energy gamma-ray astronomy observations of Geminga with the VERITAS array

    NASA Astrophysics Data System (ADS)

    Finnegan, Gary Marvin

    The closest known supernova remnant and pulsar is Geminga. The Geminga pulsar is the first pulsar to have ever been detected initially by gamma rays and the first pulsar in a class of radio-quiet pulsars. In 2007, the Milagro collaboration detected a large angularly extended (˜ 2.6°) emission of high energy gamma rays (˜ 20 TeV ) that was positionally coincident with Geminga. The Very Energetic Radiation Imaging Telescope Array System (VERITAS) is a ground- based observatory with four imaging Cherenkov telescopes with an energy range between 100 GeV to more than 30 TeV. The imaging Cherenkov telescopes detect the Cherenkov light from charged particles in electromagnetic air showers initiated by high energy particles such as gamma rays and cosmic rays. Most gamma-ray sources detected by VERITAS are point like sources, which have an angular extension smaller than the angular resolution of the telescopes (˜ 0.1°). For a point source, the background noise can be measured in the same field of view (FOV) as the source. For an angularly extended object, such as Geminga, an external FOV from the source region must be used to estimate the background noise, to avoid contamination from the extended source region. In this dissertation, I describe a new analysis procedure that is designed to increase the observation sensitivity of angularly extended objects like Geminga. I apply this procedure to a known extended gamma-ray source, Boomerang, as well as Geminga. The results indicate the detection of very high energy emission from the Geminga region at the level of 4% of the Crab nebula with a weighted average spectral index of -2.8 ± 0.2. A possible extension less than one degree wide is shown. This detection, however, awaits a confirmation by the VERITAS collaboration. The luminosity of the Geminga extended source, the Vela Nebula, and the Crab nebula was calculated for energies greater than 1 TeV. The data suggest that older pulsars, such as Geminga and Vela, convert the

  4. Dark Energy Survey releases early data | News

    Science.gov Websites

    released to the public. Astronomers and astronomy buffs can download the data from the website for the of all the images taken for the Dark Energy Survey. This is good news for the astronomy community, as Optical Astronomy Observatory's Cerro Tololo Inter-American Observatory in Chile. The Dark Energy Survey

  5. Dike propagation energy balance from deformation modeling and seismic release

    NASA Astrophysics Data System (ADS)

    Bonaccorso, Alessandro; Aoki, Yosuke; Rivalta, Eleonora

    2017-06-01

    Magma is transported in the crust mainly by dike intrusions. In volcanic areas, dikes can ascend toward the free surface and also move by lateral propagation, eventually feeding flank eruptions. Understanding dike mechanics is a key to forecasting the expected propagation and associated hazard. Several studies have been conducted on dike mechanisms and propagation; however, a less in-depth investigated aspect is the relation between measured dike-induced deformation and the seismicity released during its propagation. We individuated a simple x that can be used as a proxy of the expected mechanical energy released by a propagating dike and is related to its average thickness. For several intrusions around the world (Afar, Japan, and Mount Etna), we correlate such mechanical energy to the seismic moment released by the induced earthquakes. We obtain an empirical law that quantifies the expected seismic energy released before arrest. The proposed approach may be helpful to predict the total seismic moment that will be released by an intrusion and thus to control the energy status during its propagation and the time of dike arrest.Plain Language SummaryDike propagation is a dominant mechanism for magma ascent, transport, and eruptions. Besides being an intriguing physical process, it has critical hazard implications. After the magma intrusion starts, it is difficult to predict when and where a specific horizontal dike is going to halt and what its final length will be. In our study, we singled an equation that can be used as a proxy of the expected mechanical <span class="hlt">energy</span> to be <span class="hlt">released</span> by the opening dike. We related this expected <span class="hlt">energy</span> to the seismic moment of several eruptive intrusions around the world (Afar region, Japanese volcanoes, and Mount Etna). The proposed novel approach is helpful to estimate the total seismic moment to be <span class="hlt">released</span>, therefore allowing potentially predicting when the dike will end its propagation</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/6921407-imaging-observations-sn1987a-gamma-ray-energies','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/6921407-imaging-observations-sn1987a-gamma-ray-energies"><span>Imaging observations of SN1987A at <span class="hlt">gamma</span>-ray <span class="hlt">energies</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Cook, W.R.; Palmer, D.M.; Prince, T.A.</p> <p>1988-09-25</p> <p>The Caltech imaging ..<span class="hlt">gamma</span>..-ray telescope was launched by balloon from Alice Springs, NT, Australia for observations of SN1987A during the period 18.60--18.87 November 1987 UT. The preliminary results presented here are derived from 8200 seconds of instrument livetime on the supernova and 2500 seconds on the Crab Nebula and pulsar at a float altitude of 37 km. We have obtained the first images of the SN1987A region at ..<span class="hlt">gamma</span>..-ray <span class="hlt">energies</span> confirming that the bulk of the ..<span class="hlt">gamma</span>..-ray emission comes from the supernova and not from LMC X-1. A count excess is detected between 300 and 1300 keV from the directionmore » of the supernova, one third of which comes from <span class="hlt">energy</span> bands of width 80 and 92 keV centered on 847 and 1238 keV, respectively. The excess can be interpreted as a line photon flux plus scattered photon continuum from the radioactive decay of /sup 56/Co synthesized in the supernova explosion. We compare our data to recent predictions and find it to be consistent with models invoking moderate mixing of core material into the envelope.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018uhec.confa1021C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018uhec.confa1021C"><span>A Novel Study Connecting Ultra-High <span class="hlt">Energy</span> Cosmic Rays, Neutrinos, and <span class="hlt">Gamma</span>-Rays</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Coenders, Stefan; Resconi, Elisa; Padovani, Paolo; Giommi, Paolo; Caccianiga, Lorenzo</p> <p></p> <p>We present a novel study connecting ultra-high <span class="hlt">energy</span> cosmic rays, neutrinos, and <span class="hlt">gamma</span>-rays with the objective to identify common counterparts of the three astrophysical messengers. In the test presented here, we first identify potential hadronic sources by filtering <span class="hlt">gamma</span>-ray emitters that are in spatial coincidence with IceCube neutrinos. Subsequently, these objects are correlated against ultra-high <span class="hlt">energy</span> cosmic rays detected by the Pierre Auger Observatory and the Telescope Array, scanning in <span class="hlt">gamma</span>-ray flux and angular separation between sources and cosmic rays. A maximal excess of 80 cosmic rays (41.9 expected) is observed for the second catalog of hard Fermi-LAT objects of blazars of the high synchrotron peak type. This corresponds to a deviation from the null-hypothesis of 2.94σ . No excess is observed for objects not in spatial connection with neutrinos. The <span class="hlt">gamma</span>-ray sources that make up the excess are blazars of the high synchrotron peak type.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19800029756&hterms=palestine&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dpalestine','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19800029756&hterms=palestine&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dpalestine"><span>A search for low <span class="hlt">energy</span> <span class="hlt">gamma</span> rays from CG 195+4</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Haymes, R. C.; Meegan, C. A.; Fishman, G. J.</p> <p>1979-01-01</p> <p>A 13-deg-wide region of sky containing the high-<span class="hlt">energy</span> <span class="hlt">gamma</span>-ray source CG 195+4 was searched for X-ray and <span class="hlt">gamma</span>-ray emission in the <span class="hlt">energy</span> interval from 0.035 to 8.737 MeV. The balloon-altitude measurements were undertaken on October 4, 1977, at Palestine, Texas, and used an actively collimated scintillation counter. As a result of the measurements, low upper limits have been found for the spectrum from the source. Combined with the positive detections made with satellites at high <span class="hlt">energies</span>, the measurements show that the photon number spectrum must have a spectral index harder than 2.0. The data appear inconsistent with models of the source in which the presumed neutron star is surrounded by a cloud thick to X-rays. Negative results of the search for periodicity are discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018ApJ...852...62V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018ApJ...852...62V"><span>High-<span class="hlt">energy</span> Emission from Nonrelativistic Radiative Shocks: Application to <span class="hlt">Gamma</span>-Ray Novae</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Vurm, Indrek; Metzger, Brian D.</p> <p>2018-01-01</p> <p>The observation of GeV <span class="hlt">gamma</span>-rays from novae by Fermi/LAT demonstrates that the nonrelativistic radiative shocks in these systems can accelerate particles to <span class="hlt">energies</span> of at least ∼10 GeV. The low-<span class="hlt">energy</span> extension of the same nonthermal particle distribution inevitably gives rise to emission in the hard X-ray band. Above ≳ 10 {keV}, this radiation can escape the system without significant absorption/attenuation, and can potentially be detected by NuSTAR. We present theoretical models for hard X-ray and <span class="hlt">gamma</span>-ray emission from radiative shocks in both leptonic and hadronic scenarios, accounting for the rapid evolution of the downstream properties due to the fast cooling of thermal plasma. We find that due to strong Coulomb losses, only a fraction of {10}-4{--}{10}-3 of the <span class="hlt">gamma</span>-ray luminosity is radiated in the NuSTAR band; nevertheless, this emission could be detectable simultaneously with the LAT emission in bright <span class="hlt">gamma</span>-ray novae with a ∼50 ks exposure. The spectral slope in hard X-rays is α ≈ 0 for typical nova parameters, thus serving as a testable prediction of the model. Our work demonstrates how combined hard X-ray and <span class="hlt">gamma</span>-ray observations can be used to constrain properties of the nova outflow (velocity, density, and mass outflow rate) and particle acceleration at the shock. A very low X-ray to <span class="hlt">gamma</span>-ray luminosity ratio ({L}{{X}}/{L}γ ≲ 5× {10}-4) would disfavor leptonic models for the <span class="hlt">gamma</span>-ray emission. Our model can also be applied to other astrophysical environments with radiative shocks, including SNe IIn and colliding winds in massive star binaries.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1356471-systematic-search-high-energy-gamma-ray-emission-from-bow-shocks-runaway-stars','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1356471-systematic-search-high-energy-gamma-ray-emission-from-bow-shocks-runaway-stars"><span>Systematic search for high-<span class="hlt">energy</span> <span class="hlt">gamma</span>-ray emission from bow shocks of runaway stars</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Schulz, A.; Ackermann, M.; Buehler, R.; ...</p> <p>2014-05-01</p> <p>Context. It has been suggested that the bow shocks of runaway stars are sources of high-<span class="hlt">energy</span> <span class="hlt">gamma</span> rays (E > 100 MeV). Theoretical models predicting high-<span class="hlt">energy</span> <span class="hlt">gamma</span>-ray emission from these sources were followed by the first detection of non-thermal radio emission from the bow shock of BD+43°3654 and non-thermal X-ray emission from the bow shock of AE Aurigae. Aims. We perform the first systematic search for MeV and GeV emission from 27 bow shocks of runaway stars using data collected by the Large Area Telescope (LAT) onboard the Fermi <span class="hlt">Gamma</span>-ray Space Telescope (Fermi). Methods. We analysed 57 months of Fermi-LATmore » data at the positions of 27 bow shocks of runaway stars extracted from the Extensive stellar BOw Shock Survey catalogue (E-BOSS). A likelihood analysis was performed to search for <span class="hlt">gamma</span>-ray emission that is not compatible with diffuse background or emission from neighbouring sources and that could be associated with the bow shocks. Results. None of the bow shock candidates is detected significantly in the Fermi-LAT <span class="hlt">energy</span> range. We therefore present upper limits on the high-<span class="hlt">energy</span> emission in the <span class="hlt">energy</span> range from 100MeV to 300 GeV for 27 bow shocks of runaway stars in four <span class="hlt">energy</span> bands. For the three cases where models of the high-<span class="hlt">energy</span> emission are published we compare our upper limits to the modelled spectra. Our limits exclude the model predictions for ζ Ophiuchi by a factor ≈ 5.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22038535-gamma-rays-made-earth-have-unexpectedly-high-energies','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22038535-gamma-rays-made-earth-have-unexpectedly-high-energies"><span><span class="hlt">Gamma</span> rays made on Earth have unexpectedly high <span class="hlt">energies</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Miller, Johanna</p> <p></p> <p>Terrestrial <span class="hlt">gamma</span>-ray flashes (TGFs) are the source of the highest-<span class="hlt">energy</span> nonanthropogenic photons produced on Earth. Associated with thunder-storms - and in fact, with individual lightning discharges - they are presumed to be the bremsstrahlung produced when relativistic electrons, accelerated by the storms' strong electric fields, collide with air molecules some 10-20 km above sea level. The TGFs last up to a few milliseconds and contain photons with <span class="hlt">energies</span> on the order of MeV.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/15790849','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/15790849"><span>A new population of very high <span class="hlt">energy</span> <span class="hlt">gamma</span>-ray sources in the Milky Way.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Aharonian, F; Akhperjanian, A G; Aye, K-M; Bazer-Bachi, A R; Beilicke, M; Benbow, W; Berge, D; Berghaus, P; Bernlöhr, K; Boisson, C; Bolz, O; Borgmeier, C; Braun, I; Breitling, F; Brown, A M; Gordo, J Bussons; Chadwick, P M; Chounet, L-M; Cornils, R; Costamante, L; Degrange, B; Djannati-Ataï, A; Drury, L O'C; Dubus, G; Ergin, T; Espigat, P; Feinstein, F; Fleury, P; Fontaine, G; Funk, S; Gallant, Y A; Giebels, B; Gillessen, S; Goret, P; Hadjichristidis, C; Hauser, M; Heinzelmann, G; Henri, G; Hermann, G; Hinton, J A; Hofmann, W; Holleran, M; Horns, D; de Jager, O C; Jung, I; Khélifi, B; Komin, Nu; Konopelko, A; Latham, I J; Le Gallou, R; Lemière, A; Lemoine, M; Leroy, N; Lohse, T; Marcowith, A; Masterson, C; McComb, T J L; de Naurois, M; Nolan, S J; Noutsos, A; Orford, K J; Osborne, J L; Ouchrif, M; Panter, M; Pelletier, G; Pita, S; Pühlhofer, G; Punch, M; Raubenheimer, B C; Raue, M; Raux, J; Rayner, S M; Redondo, I; Reimer, A; Reimer, O; Ripken, J; Rob, L; Rolland, L; Rowell, G; Sahakian, V; Saugé, L; Schlenker, S; Schlickeiser, R; Schuster, C; Schwanke, U; Siewert, M; Sol, H; Steenkamp, R; Stegmann, C; Tavernet, J-P; Terrier, R; Théoret, C G; Tluczykont, M; van der Walt, D J; Vasileiadis, G; Venter, C; Vincent, P; Visser, B; Völk, H J; Wagner, S J</p> <p>2005-03-25</p> <p>Very high <span class="hlt">energy</span> <span class="hlt">gamma</span>-rays probe the long-standing mystery of the origin of cosmic rays. Produced in the interactions of accelerated particles in astrophysical objects, they can be used to image cosmic particle accelerators. A first sensitive survey of the inner part of the Milky Way with the High <span class="hlt">Energy</span> Stereoscopic System (HESS) reveals a population of eight previously unknown firmly detected sources of very high <span class="hlt">energy</span> <span class="hlt">gamma</span>-rays. At least two have no known radio or x-ray counterpart and may be representative of a new class of "dark" nucleonic cosmic ray sources.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.eia.gov/outlooks/archive/aeo10/carbon_dioxide.html','EIAPUBS'); return false;" href="https://www.eia.gov/outlooks/archive/aeo10/carbon_dioxide.html"><span>Accounting for Carbon Dioxide Emissions from Biomass <span class="hlt">Energy</span> Combustion (<span class="hlt">released</span> in AEO2010)</span></a></p> <p><a target="_blank" href="http://www.eia.doe.gov/reports/">EIA Publications</a></p> <p></p> <p>2010-01-01</p> <p>Carbon Dioxide (CO2) emissions from the combustion of biomass to produce <span class="hlt">energy</span> are excluded from the <span class="hlt">energy</span>-related CO2 emissions reported in Annual <span class="hlt">Energy</span> Outlook 2010. According to current international convention, carbon <span class="hlt">released</span> through biomass combustion is excluded from reported <span class="hlt">energy</span>-related emissions. The <span class="hlt">release</span> of carbon from biomass combustion is assumed to be balanced by the uptake of carbon when the feedstock is grown, resulting in zero net emissions over some period of time]. However, analysts have debated whether increased use of biomass <span class="hlt">energy</span> may result in a decline in terrestrial carbon stocks, leading to a net positive <span class="hlt">release</span> of carbon rather than the zero net <span class="hlt">release</span> assumed by its exclusion from reported <span class="hlt">energy</span>-related emissions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22679462-simulation-radiation-energy-release-air-showers','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22679462-simulation-radiation-energy-release-air-showers"><span>Simulation of radiation <span class="hlt">energy</span> <span class="hlt">release</span> in air showers</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Glaser, Christian; Erdmann, Martin; Hörandel, Jörg R.</p> <p>2016-09-01</p> <p>A simulation study of the <span class="hlt">energy</span> <span class="hlt">released</span> by extensive air showers in the form of MHz radiation is performed using the CoREAS simulation code. We develop an efficient method to extract this radiation <span class="hlt">energy</span> from air-shower simulations. We determine the longitudinal profile of the radiation <span class="hlt">energy</span> <span class="hlt">release</span> and compare it to the longitudinal profile of the <span class="hlt">energy</span> deposit by the electromagnetic component of the air shower. We find that the radiation <span class="hlt">energy</span> corrected for the geometric dependence of the geomagnetic emission scales quadratically with the <span class="hlt">energy</span> in the electromagnetic component of the air shower with a second-order dependence on themore » atmospheric density at the position of the maximum shower development X {sub max}. In a measurement where X {sub max} is not accessible, this second order dependence can be approximated using the zenith angle of the incoming direction of the air shower with only a minor loss in accuracy. Our method results in an intrinsic uncertainty of 4% in the determination of the <span class="hlt">energy</span> in the electromagnetic air-shower component, which is well below current experimental uncertainties.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JGRA..123.2513Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JGRA..123.2513Z"><span>Coronal Flux Rope Catastrophe Associated With Internal <span class="hlt">Energy</span> <span class="hlt">Release</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhuang, Bin; Hu, Youqiu; Wang, Yuming; Zhang, Quanhao; Liu, Rui; Gou, Tingyu; Shen, Chenglong</p> <p>2018-04-01</p> <p>Magnetic <span class="hlt">energy</span> during the catastrophe was predominantly studied by the previous catastrophe works since it is believed to be the main <span class="hlt">energy</span> supplier for the solar eruptions. However, the contribution of other types of <span class="hlt">energies</span> during the catastrophe cannot be neglected. This paper studies the catastrophe of the coronal flux rope system in the solar wind background, with emphasis on the transformation of different types of <span class="hlt">energies</span> during the catastrophe. The coronal flux rope is characterized by its axial and poloidal magnetic fluxes and total mass. It is shown that a catastrophe can be triggered by not only an increase but also a decrease of the axial magnetic flux. Moreover, the internal <span class="hlt">energy</span> of the rope is found to be <span class="hlt">released</span> during the catastrophe so as to provide <span class="hlt">energy</span> for the upward eruption of the flux rope. As far as the magnetic <span class="hlt">energy</span> is concerned, it provides only part of the <span class="hlt">energy</span> <span class="hlt">release</span>, or even increases during the catastrophe, so the internal <span class="hlt">energy</span> may act as the dominant or even the unique <span class="hlt">energy</span> supplier during the catastrophe.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2004HEAD....8.1611P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2004HEAD....8.1611P"><span>MEGA: the next generation Medium <span class="hlt">Energy</span> <span class="hlt">Gamma</span>-ray Telescope</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Paciesas, W.; Miller, R. S.; Andritschke, R.; Kanbach, G.; Zoglauer, A.; Bloser, P.; Hunter, S.; Cravens, J.; Cherry, M.; Guzik, T. G.; Stacy, J. G.; Wefel, J. P.; Di Cocco, G.; Hartmann, D.; Kippen, R. M.; Vestrand, W. T.; Kurfess, J.; Phlips, B.; Strickman, M.; Wulf, E.; Macri, J. R.; McConnell, M. L.; Ryan, J. M.; Reglero, V.; Zych, A. D.</p> <p>2004-08-01</p> <p>The MEGA mission would enable a sensitive all-sky survey of the medium-<span class="hlt">energy</span> <span class="hlt">gamma</span>-ray sky (0.3-50 MeV). This mission will bridge the huge sensitivity gap between the COMPTEL and OSSE experiments on the Compton <span class="hlt">Gamma</span> Ray Observatory, the SPI and IBIS instruments on INTEGRAL and the visionary ACT mission. It will, among other things, serve to compile a much larger catalog of sources in this <span class="hlt">energy</span> range, perform far deeper searches for supernovae, better measure the galactic continuum emission as well as identify the components of the cosmic diffuse emission. It will accomplish these goals with a stack of Si-strip detector (SSD) planes surrounded by a dense high-Z calorimeter. At lower photon <span class="hlt">energies</span> (below ˜ 30 MeV), the design is sensitive to Compton interactions, with the SSD system serving as a scattering medium that also detects and measures the Compton recoil <span class="hlt">energy</span> deposit. If the <span class="hlt">energy</span> of the recoil electron is sufficiently high (> 2 MeV), the track of the recoil electron can also be defined. At higher photon <span class="hlt">energies</span> (above ˜ 10 MeV), the design is sensitive to pair production events, with the SSD system measuring the tracks of the electron and positron. We will discuss the various types of event signatures in detail and describe the advantages of this design over previous Compton telescope designs. Effective area, sensitivity and resolving power estimates are also presented along with simulations of expected scientific results and beam calibration results from the prototype instrument.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1993PASP..105..125W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1993PASP..105..125W"><span>A Search for High-<span class="hlt">Energy</span> <span class="hlt">Gamma</span> Rays from Supernova 1987A</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Waldron, Liam Edwin</p> <p>1993-01-01</p> <p>The Australian Defense Force Academy (ADFA) balloon-borne <span class="hlt">gamma</span>-ray astronomy telescope was flown successfully from Alice Springs, Australia, twice during 1987 and 1988 (Flights 87-2-19 and 88-1-5) with the aim of measuring the <span class="hlt">gamma</span>-ray flux, in the <span class="hlt">energy</span> range 50-500 MeV, from Supernova 1987A in the Large Magellanic Cloud. The two flights correspond to day 55 and 407, respectively, of remnant evolution. The instrument was complemented by a hard X-ray proportional counter, designed and constructed by the Istituto di Astrofisica Spaziale, CNR, Frascati, Italy, and sensitive to the 10-250 keV <span class="hlt">energy</span> range. In this thesis, an account is given of the physical processes responsible for the production of <span class="hlt">gamma</span> rays in astrophysical environments and their relation to supernovae and cosmic rays. A description is then given of main features of the <span class="hlt">gamma</span>-ray telescope and its principles of operation, the most important part of the telescope being a spark chamber used to determine the direction of arrival of incident <span class="hlt">gamma</span> rays. Data obtained during each flight were recorded as spark-chamber tracks on the photographic film. A detailed account of the methods of subsequent data reduction and analysis, as carried out by the author, is given. The principal results of this work were that 3-sigma upper limits to the <span class="hlt">gamma</span>-ray flux from SN 1987A of 2.2 and 3.4 X 10^-5 photons cm^-2s^-1 were obtained for days 55 and 407 of remnant evolution, respectively, these limits being somewhat lower than previously reported in the literature from a preliminary analysis of the data. The above two upper limits are consistent with SN 1987A being an atypical Type II supernova. That is, the progenitor was a blue, rather than a red, supergiant. The limits are compared with theoretical predictions related to current models of <span class="hlt">gamma</span>-ray emission from young Type II supernovae. (SECTION: Dissertation Abstracts)</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20070031733','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20070031733"><span>Monitoring the Low-<span class="hlt">Energy</span> <span class="hlt">Gamma</span>-Ray Sky Using Earth Occultation with GLAST GBM</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Case, G.; Wilson-Hodge, C.; Cherry, M.; Kippen, M.; Ling, J.; Radocinski, R.; Wheaton, W.</p> <p>2007-01-01</p> <p>Long term all-sky monitoring of the 20 keV - 2 MeV <span class="hlt">gamma</span>-ray sky using the Earth occultation technique was demonstrated by the BATSE instrument on the Compton <span class="hlt">Gamma</span> Ray Observatory. The principles and techniques used for the development of an end-to-end earth occultation data analysis system for BATSE can be extended to the GLAST <span class="hlt">Gamma</span>-ray Burst Monitor (GBM), resulting in multiband light curves and time-resolved spectra in the <span class="hlt">energy</span> range 8 keV to above 1 MeV for known <span class="hlt">gamma</span>-ray sources and transient outbursts, as well as the discovery of new sources of <span class="hlt">gamma</span>-ray emission. In this paper we describe the application of the technique to the GBM. We also present the expected sensitivity for the GBM.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25430303','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25430303"><span>Extended performance gas Cherenkov detector for <span class="hlt">gamma</span>-ray detection in high-<span class="hlt">energy</span> density experiments.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Herrmann, H W; Kim, Y H; Young, C S; Fatherley, V E; Lopez, F E; Oertel, J A; Malone, R M; Rubery, M S; Horsfield, C J; Stoeffl, W; Zylstra, A B; Shmayda, W T; Batha, S H</p> <p>2014-11-01</p> <p>A new Gas Cherenkov Detector (GCD) with low-<span class="hlt">energy</span> threshold and high sensitivity, currently known as Super GCD (or GCD-3 at OMEGA), is being developed for use at the OMEGA Laser Facility and the National Ignition Facility (NIF). Super GCD is designed to be pressurized to ≤400 psi (absolute) and uses all metal seals to allow the use of fluorinated gases inside the target chamber. This will allow the <span class="hlt">gamma</span> <span class="hlt">energy</span> threshold to be run as low at 1.8 MeV with 400 psi (absolute) of C2F6, opening up a new portion of the <span class="hlt">gamma</span> ray spectrum. Super GCD operating at 20 cm from TCC will be ∼400 × more efficient at detecting DT fusion <span class="hlt">gammas</span> at 16.7 MeV than the <span class="hlt">Gamma</span> Reaction History diagnostic at NIF (GRH-6m) when operated at their minimum thresholds.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19780016089','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19780016089"><span>Observations of medium <span class="hlt">energy</span> <span class="hlt">gamma</span> ray emission from the galactic center region</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kniffen, D. A.; Bertsch, D. L.; Morris, D. J.; Palmeira, R. A. R.; Rao, K. R.</p> <p>1978-01-01</p> <p>Measurements of the <span class="hlt">gamma</span>-ray emission in the medium <span class="hlt">energy</span> range between 15 and 100 MeV, obtained during two ballon flights from Brazil are presented. The importance of this <span class="hlt">energy</span> region in determining whether pi deg - decay of electron bremsstrahlung is the most likely dominant source mechanism is discussed along with the implications of such observations. Specifically, the data from this experiment suggest that emission from the galactic plane is similar to theoretical spectrum calculations including both sources mechanisms, but with the bremsstrahlung component enhanced by a factor of about 2. A spectral distribution of <span class="hlt">gamma</span>-rays produced in the residual atmosphere above the instrument is also presented and compared with other data. A rather smooth spectral variation from high to low <span class="hlt">energies</span> is found for the atmospheric spectrum.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_6");'>6</a></li> <li><a href="#" onclick='return showDiv("page_7");'>7</a></li> <li class="active"><span>8</span></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_8 --> <div id="page_9" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_7");'>7</a></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li class="active"><span>9</span></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="161"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=health+AND+care+AND+expenditures&pg=3&id=EJ1054953','ERIC'); return false;" href="https://eric.ed.gov/?q=health+AND+care+AND+expenditures&pg=3&id=EJ1054953"><span>The Effectiveness of Screening with Interferon-<span class="hlt">Gamma</span> <span class="hlt">Release</span> Assays in a University Health Care Setting with a Diverse Global Population</span></a></p> <p><a target="_blank" href="http://www.eric.ed.gov/ERICWebPortal/search/extended.jsp?_pageLabel=advanced">ERIC Educational Resources Information Center</a></p> <p>Birch, Samantha J.; Golbeck, Amanda L.</p> <p>2015-01-01</p> <p>Objective: This analysis examined the effectiveness of utilizing interferon-<span class="hlt">gamma</span> <span class="hlt">release</span> assay (IGRA) technology in a TB (TB) screening program at a university. Participants: Participants were 2299 students at a Montana university who had presented to the university health center for TB screening during 2012 and 2013. Methods: A retrospective…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013PhDT.......228D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013PhDT.......228D"><span>Low <span class="hlt">energy</span> proton capture study of the 14N(p, <span class="hlt">gamma</span>)15O reaction</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Daigle, Stephen Michael</p> <p></p> <p>The 14N(p,<span class="hlt">gamma</span>)15O reaction regulates the rate of <span class="hlt">energy</span> production for stars slightly more massive than the sun throughout stable hydrogen burning on the main sequence. The 14N(p,<span class="hlt">gamma</span>)15O reaction rate also determines the luminosity for all stars after leaving the main sequence when their cores have exhausted hydrogen fuel, and later when they become red giant stars. The significant role that this reaction plays in stellar evolution has far-reaching consequences, from neutrino production in our Sun, to age estimates of globular clusters in our Galaxy. The weak cross section and inherent coincidence summing in the 15O <span class="hlt">gamma</span>-ray decay scheme make a precision measurement of the astrophysical S-factor especially challenging, particularly for the ground-state transition. The present study, performed in the Laboratory for Experimental Nuclear Astrophysics (LENA), was aimed at measuring the ground-state transition at low <span class="hlt">energy</span> by utilizing a new 24-element, position-sensitive, NaI(Tl) detector array. Because the array is highly segmented, the 14N( p,<span class="hlt">gamma</span>)15O S-factor was evaluated for transitions to the ground, 5.18, 6.18, and 6.79 MeV states without the need for coincidence summing corrections. Additionally, the position-sensitivity of the detector was exploited to measure the angular correlation of the two-photon cascades. Software cuts were made to the data in order to identify single and coincident <span class="hlt">gamma</span>-ray events and a fraction fit analysis technique was used to extract the characteristic 15O peaks from the composite <span class="hlt">gamma</span>-ray spectrum. The results from the current work demonstrated a new approach to measuring weak nuclear cross sections near astrophysically relevant <span class="hlt">energies</span> that, with refinements, has broader applications in <span class="hlt">gamma</span>-ray spectroscopy.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/16002580','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/16002580"><span>Discovery of very high <span class="hlt">energy</span> <span class="hlt">gamma</span> rays associated with an x-ray binary.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Aharonian, F; Akhperjanian, A G; Aye, K-M; Bazer-Bachi, A R; Beilicke, M; Benbow, W; Berge, D; Berghaus, P; Bernlöhr, K; Boisson, C; Bolz, O; Borrel, V; Braun, I; Breitling, F; Brown, A M; Bussons Gordo, J; Chadwick, P M; Chounet, L-M; Cornils, R; Costamante, L; Degrange, B; Dickinson, H J; Djannati-Ataï, A; Drury, L O'c; Dubus, G; Emmanoulopoulos, D; Espigat, P; Feinstein, F; Fleury, P; Fontaine, G; Fuchs, Y; Funk, S; Gallant, Y A; Giebels, B; Gillessen, S; Glicenstein, J F; Goret, P; Hadjichristidis, C; Hauser, M; Heinzelmann, G; Henri, G; Hermann, G; Hinton, J A; Hofmann, W; Holleran, M; Horns, D; Jacholkowska, A; de Jager, O C; Khélifi, B; Komin, Nu; Konopelko, A; Latham, I J; Le Gallou, R; Lemière, A; Lemoine-Goumard, M; Leroy, N; Lohse, T; Marcowith, A; Martin, J-M; Martineau-Huynh, O; Masterson, C; McComb, T J L; de Naurois, M; Nolan, S J; Noutsos, A; Orford, K J; Osborne, J L; Ouchrif, M; Panter, M; Pelletier, G; Pita, S; Pühlhofer, G; Punch, M; Raubenheimer, B C; Raue, M; Raux, J; Rayner, S M; Reimer, A; Reimer, O; Ripken, J; Rob, L; Rolland, L; Rowell, G; Sahakian, V; Saugé, L; Schlenker, S; Schlickeiser, R; Schuster, C; Schwanke, U; Siewert, M; Sol, H; Spangler, D; Steenkamp, R; Stegmann, C; Tavernet, J-P; Terrier, R; Théoret, C G; Tluczykont, M; Vasileiadis, G; Venter, C; Vincent, P; Völk, H J; Wagner, S J</p> <p>2005-07-29</p> <p>X-ray binaries are composed of a normal star in orbit around a neutron star or stellar-mass black hole. Radio and x-ray observations have led to the presumption that some x-ray binaries called microquasars behave as scaled-down active galactic nuclei. Microquasars have resolved radio emission that is thought to arise from a relativistic outflow akin to active galactic nuclei jets, in which particles can be accelerated to large <span class="hlt">energies</span>. Very high <span class="hlt">energy</span> <span class="hlt">gamma</span>-rays produced by the interactions of these particles have been observed from several active galactic nuclei. Using the High <span class="hlt">Energy</span> Stereoscopic System, we find evidence for <span class="hlt">gamma</span>-ray emission of >100 gigaelectron volts from a candidate microquasar, LS 5039, showing that particles are also accelerated to very high <span class="hlt">energies</span> in these systems.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018SPIE10595E..10K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018SPIE10595E..10K"><span><span class="hlt">Energy</span> <span class="hlt">release</span> for the actuation and deployment of muscle-inspired asymmetrically multistable chains</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kidambi, Narayanan; Zheng, Yisheng; Harne, Ryan L.; Wang, K. W.</p> <p>2018-03-01</p> <p>Animal locomotion and movement requires <span class="hlt">energy</span>, and the elastic potential <span class="hlt">energy</span> stored in skeletal muscle can facilitate movements that are otherwise energetically infeasible. A significant proportion of this <span class="hlt">energy</span> is captured and stored in the micro- and nano-scale constituents of muscle near the point of instability between asymmetric equilibrium states. This <span class="hlt">energy</span> may be quickly <span class="hlt">released</span> to enable explosive macroscopic motions or to reduce the metabolic cost of cyclic movements. Inspired by these behaviors, this research explores modular metastructures of bistable element chains and develops methods to <span class="hlt">release</span> the <span class="hlt">energy</span> stored in higher-potential system configurations. Quasi-static investigations reveal the role of state-transition pathways on the overall efficiency of the deployment event. It is shown that sequential, local <span class="hlt">release</span> of <span class="hlt">energy</span> from the bistable elements is more efficient than concurrent <span class="hlt">energy</span> <span class="hlt">release</span> achieved by applying a force at the free end of the structure. From dynamic analyses and experiments, it is shown that that the <span class="hlt">energy</span> <span class="hlt">released</span> from one bistable element can be used to activate the <span class="hlt">release</span> of <span class="hlt">energy</span> from subsequent links, reducing the actuation <span class="hlt">energy</span> required to extend or deploy the chain below that required for quasi-static deployment. This phenomenon is influenced by the level of asymmetry in the bistable constituents and the location of the impulse that initiates the deployment of the structure. The results provide insight into the design and behavior of asymmetrically multistable chains that can leverage stored potential <span class="hlt">energy</span> to enable efficient and effective system deployment and length change.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=1854731','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=1854731"><span>Regulation of the substance P-induced contraction via the <span class="hlt">release</span> of acetylcholine and <span class="hlt">gamma</span>-aminobutyric acid in the guinea-pig urinary bladder.</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Shirakawa, J.; Nakanishi, T.; Taniyama, K.; Kamidono, S.; Tanaka, C.</p> <p>1989-01-01</p> <p>1. The action of substance P (SP) on the <span class="hlt">release</span> of <span class="hlt">gamma</span>-aminobutyric acid (GABA) and acetylcholine (ACh) and on contraction were studied in strips of the guinea-pig urinary bladder. Substance P induced a dose-dependent contraction of strips of guinea-pig urinary bladder (EC50 = 1.2 x 10(-9) M). This contraction was not altered by tetrodotoxin, but with a dose of 10(-9) M and less, there was a complete inhibition by 10(-6) M) atropine. Contractions initiated by 3 x 10(-9) M) SP or more were partly inhibited by atropine. The EC50 value of substance P in the presence of atropine was 7.0 x 10(-9) M. 2. Substance P induced a Ca2+-dependent and tetrodotoxin-resistant <span class="hlt">release</span> of [3H]-acetylcholine (ACh) from strips of urinary bladder preloaded with [3H]-choline (EC50 = 4.9 x 10(-10) M), and this <span class="hlt">release</span> was antagonized by [D-Pro2,D-Trp7,9] substance P. 3. Bicuculline increased the substance P-induced contraction and the <span class="hlt">release</span> of [3H]-ACh from the strips. 4. Substance P induced a Ca2+-dependent and tetrodotoxin-sensitive <span class="hlt">release</span> of [3H]-<span class="hlt">gamma</span>-aminobutyric acid (GABA) from strips preloaded with [3H]-GABA (EC50 = 2.6 x 10(-9) M), and this <span class="hlt">release</span> was antagonized by [D-Pro2,D-Trp7,9] substance P. 5. Therefore, substance P appears to exert excitatory effects on the contractility of urinary bladder predominantly by stimulating its own receptor located on the cholinergic nerve terminals. GABA <span class="hlt">released</span> by substance P inhibits stimulation of the cholinergic neurone. However, the direct action of substance P on the cholinergic neurone is more potent that the indirect action via GABA <span class="hlt">release</span>. PMID:2479440</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20010048764&hterms=CERN&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3DCERN','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20010048764&hterms=CERN&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3DCERN"><span>High <span class="hlt">Energy</span> Electron and <span class="hlt">Gamma</span> - Ray Detection with ATIC</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Chang, J.; Schmidt, W. K. H.; Whitaker, Ann F. (Technical Monitor)</p> <p>2001-01-01</p> <p>The Advanced Thin Ionization Calorimeter (ATIC) balloon borne ionization calorimeter is well suited to record and identify high <span class="hlt">energy</span> cosmic ray electrons, and at very high <span class="hlt">energies</span> <span class="hlt">gamma</span>-ray photons as well. We have simulated the performance of the instrument, and compare the simulations with actual high <span class="hlt">energy</span> electron exposures at the CERN accelerator. Simulations and measurements do not compare exactly, in detail, but overall the simulations have predicted actual measured behavior quite well. ATIC has had its first 16 day balloon flight at the turn of the year over Antarctica, and first results obtained using the analysis methods derived from simulations and calibrations will be reported.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20110015330','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20110015330"><span>Development of the Advanced Energetic Pair Telescope (AdEPT) for Medium-<span class="hlt">Energy</span> <span class="hlt">Gamma</span>-Ray Astronomy</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Hunter, Stanley D.; Bloser, Peter F.; Dion, Michael P.; McConnell, Mark L.; deNolfo, Georgia A.; Son, Seunghee; Ryan, James M.; Stecker, Floyd W.</p> <p>2011-01-01</p> <p>Progress in high-<span class="hlt">energy</span> <span class="hlt">gamma</span>-ray science has been dramatic since the launch of INTEGRAL, AGILE and FERMI. These instruments, however, are not optimized for observations in the medium-<span class="hlt">energy</span> (approx.0.3< E(sub <span class="hlt">gamma</span>)< approx.200 MeV) regime where many astrophysical objects exhibit unique, transitory behavior, such as spectral breaks, bursts, and flares. We outline some of the major science goals of a medium-<span class="hlt">energy</span> mission. These science goals are best achieved with a combination of two telescopes, a Compton telescope and a pair telescope, optimized to provide significant improvements in angular resolution and sensitivity. In this paper we describe the design of the Advanced Energetic Pair Telescope (AdEPT) based on the Three-Dimensional Track Imager (3-DTI) detector. This technology achieves excellent, medium-<span class="hlt">energy</span> sensitivity, angular resolution near the kinematic limit, and <span class="hlt">gamma</span>-ray polarization sensitivity, by high resolution 3-D electron tracking. We describe the performance of a 30x30x30 cm3 prototype of the AdEPT instrument.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19790026711&hterms=Media+Brazil&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3DMedia%2BBrazil','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19790026711&hterms=Media+Brazil&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3DMedia%2BBrazil"><span>Observations of medium-<span class="hlt">energy</span> <span class="hlt">gamma</span>-ray emission from the galactic center region</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kniffen, D. A.; Bertsch, D. L.; Morris, D. J.; Palmeira, R. A. R.; Rao, K. R.</p> <p>1978-01-01</p> <p>Measurements of the <span class="hlt">gamma</span>-ray emission in the medium-<span class="hlt">energy</span> range between 15 and 100 MeV, obtained during two balloon flights from Brazil, are presented. The importance of this <span class="hlt">energy</span> region in determining whether neutral-pion decay or electron bremsstrahlung is the most likely dominant source mechanism is discussed, along with the implications of such observations. Specifically, the data from this experiment suggest that emission from the galactic plane is similar to the theoretical spectrum calculated by Fichtel et al. (1976), including both source mechanisms but with the bremsstrahlung component enhanced by a factor of about 2. A spectral distribution of <span class="hlt">gamma</span>-rays produced in the residual atmosphere above the instrument is also presented and compared with other data. A rather smooth spectral variation from high to low <span class="hlt">energies</span> is found for the atmospheric spectrum.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AIPC.1792g0020Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AIPC.1792g0020Z"><span>Statistical measurement of the <span class="hlt">gamma</span>-ray source-count distribution as a function of <span class="hlt">energy</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zechlin, H.-S.; Cuoco, A.; Donato, F.; Fornengo, N.; Regis, M.</p> <p>2017-01-01</p> <p>Photon counts statistics have recently been proven to provide a sensitive observable for characterizing <span class="hlt">gamma</span>-ray source populations and for measuring the composition of the <span class="hlt">gamma</span>-ray sky. In this work, we generalize the use of the standard 1-point probability distribution function (1pPDF) to decompose the high-latitude <span class="hlt">gamma</span>-ray emission observed with Fermi-LAT into: (i) point-source contributions, (ii) the Galactic foreground contribution, and (iii) a diffuse isotropic background contribution. We analyze <span class="hlt">gamma</span>-ray data in five adjacent <span class="hlt">energy</span> bands between 1 and 171 GeV. We measure the source-count distribution dN/dS as a function of <span class="hlt">energy</span>, and demonstrate that our results extend current measurements from source catalogs to the regime of so far undetected sources. Our method improves the sensitivity for resolving point-source populations by about one order of magnitude in flux. The dN/dS distribution as a function of flux is found to be compatible with a broken power law. We derive upper limits on further possible breaks as well as the angular power of unresolved sources. We discuss the composition of the <span class="hlt">gamma</span>-ray sky and capabilities of the 1pPDF method.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012A%26A...545A..94D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012A%26A...545A..94D"><span>Exploring the nature of the unidentified very-high-<span class="hlt">energy</span> <span class="hlt">gamma</span>-ray source HESS J1507-622</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Domainko, W.; Ohm, S.</p> <p>2012-09-01</p> <p>Context. Several extended sources of very-high-<span class="hlt">energy</span> (VHE; E > 100 GeV) <span class="hlt">gamma</span> rays have been found that lack counterparts belonging to an established class of VHE <span class="hlt">gamma</span>-ray emitters. Aims: The nature of the first unidentified VHE <span class="hlt">gamma</span>-ray source with significant angular offset from the Galactic plane of 3.5°, HESS J1507-622, is explored. Methods.Fermi-LAT data in the high-<span class="hlt">energy</span> (HE, 100 MeV < E < 100 GeV) <span class="hlt">gamma</span>-ray range collected over 34 month are used to describe the spectral <span class="hlt">energy</span> distribution (SED) of the source. Additionally, implications of the off-plane location of the source for a leptonic and hadronic <span class="hlt">gamma</span>-ray emission model are investigated. Results: HESS J1507-622 is detected in the Fermi <span class="hlt">energy</span> range and its spectrum is best described by a power law in <span class="hlt">energy</span> with Γ = 1.7 ± 0.1stat ± 0.2sys and integral flux between (0.3-300) GeV of F = (2.0 ± 0.5stat ± 1.0sys) × 10-9 cm-2 s-1. The SED constructed from the Fermi and H.E.S.S. data for this source does not support a smooth power-law continuation from the VHE to the HE <span class="hlt">gamma</span>-ray range. With the available data it is not possible to discriminate between a hadronic and a leptonic scenario for HESS J1507-622. The location and compactness of the source indicate a considerable physical offset from the Galactic plane for this object. In case of a multiple-kpc distance, this challenges a pulsar wind nebula (PWN) origin for HESS J1507-622 since the time of travel for a pulsar born in the Galactic disk to reach such a location would exceed the inverse Compton (IC) cooling time of electrons that are energetic enough to produce VHE <span class="hlt">gamma</span>-rays. However, an origin of this <span class="hlt">gamma</span>-ray source connected to a pulsar that was born off the Galactic plane in the explosion of a hypervelocity star cannot be excluded. Conclusions: The nature of HESS J1507-622 is still unknown to date, and a PWN scenario cannot be ruled out in general. On the contrary HESS J1507-622 could be the first discovered representative of a</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014HEAD...1410619B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014HEAD...1410619B"><span>Sneaky <span class="hlt">Gamma</span>-Rays: Using Gravitational Lensing to Avoid <span class="hlt">Gamma-Gamma</span>-Absorption</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Boettcher, Markus; Barnacka, Anna</p> <p>2014-08-01</p> <p>It has recently been suggested that gravitational lensing studies of <span class="hlt">gamma</span>-ray blazars might be a promising avenue to probe the location of the <span class="hlt">gamma</span>-ray emitting region in blazars. Motivated by these prospects, we have investigated potential <span class="hlt">gamma-gamma</span> absorption signatures of intervening lenses in the very-high-<span class="hlt">energy</span> <span class="hlt">gamma</span>-ray emission from lensedblazars. We considered intervening galaxies and individual stars within these galaxies. We find that the collective radiation field of galaxies acting as sources of macrolensing are not expected to lead to significant <span class="hlt">gamma-gamma</span> absorption. Individual stars within intervening galaxies could, in principle, cause a significant opacity to <span class="hlt">gamma-gamma</span> absorption for VHE <span class="hlt">gamma</span>-rays if the impact parameter (the distance of closest approach of the <span class="hlt">gamma</span>-ray to the center of the star) is small enough. However, we find that the curvature of the photon path due to gravitational lensing will cause <span class="hlt">gamma</span>-ray photons to maintain a sufficiently large distance from such stars to avoid significant <span class="hlt">gamma-gamma</span> absorption. This re-inforces the prospect of gravitational-lensing studies of <span class="hlt">gamma</span>-ray blazars without interference due to <span class="hlt">gamma-gamma</span> absorption due to the lensing objects.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20140005980','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20140005980"><span>Design and Performance of the <span class="hlt">GAMMA</span>-400 <span class="hlt">Gamma</span>-Ray Telescope for Dark Matter Searches</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Galper, A.M.; Adriani, O.; Aptekar, R. L.; Arkhangelskaja, I. V.; Arkhangelskiy, A.I.; Boezio, M.; Bonvicini, V.; Boyarchuk, K. A.; Fradkin, M. I.; Gusakov, Yu. V.; <a style="text-decoration: none; " href="javascript:void(0); " onClick="displayelement('author_20140005980'); toggleEditAbsImage('author_20140005980_show'); toggleEditAbsImage('author_20140005980_hide'); "> <img style="display:inline; width:12px; height:12px; " src="images/arrow-up.gif" width="12" height="12" border="0" alt="hide" id="author_20140005980_show"> <img style="width:12px; height:12px; display:none; " src="images/arrow-down.gif" width="12" height="12" border="0" alt="hide" id="author_20140005980_hide"></p> <p>2012-01-01</p> <p>The <span class="hlt">GAMMA</span>-400 <span class="hlt">gamma</span>-ray telescope is designed to measure the fluxes of <span class="hlt">gamma</span>-rays and cosmic-ray electrons + positrons, which can be produced by annihilation or decay of the dark matter particles, as well as to survey the celestial sphere in order to study point and extended sources of <span class="hlt">gamma</span>-rays, measure <span class="hlt">energy</span> spectra of Galactic and extragalactic diffuse <span class="hlt">gamma</span>-ray emission, <span class="hlt">gamma</span>-ray bursts, and <span class="hlt">gamma</span>-ray emission from the Sun. <span class="hlt">GAMMA</span>-400 covers the <span class="hlt">energy</span> range from 100 MeV to 3000 GeV. Its angular resolution is approx. 0.01 deg (E(sub <span class="hlt">gamma</span>) > 100 GeV), the <span class="hlt">energy</span> resolution approx. 1% (E(sub <span class="hlt">gamma</span>) > 10 GeV), and the proton rejection factor approx 10(exp 6). <span class="hlt">GAMMA</span>-400 will be installed on the Russian space platform Navigator. The beginning of observations is planned for 2018.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1992PhDT........69W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1992PhDT........69W"><span>A Search for High-<span class="hlt">Energy</span> <span class="hlt">Gamma</span>-Rays from Supernova SN1987A.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Waldron, Liam Edwin</p> <p>1992-01-01</p> <p>The Australian Defence Force Academy (ADFA) balloon -borne <span class="hlt">gamma</span>-ray astronomy telescope was flown successfully from Alice Springs Australia twice during 1987 and 1988 (flights 87-2-19 and 88-1-5) with the aim of measuring the <span class="hlt">gamma</span>-ray flux, in the <span class="hlt">energy</span> range 50 to 500 MeV, from Supernova SN1987A in the Large Magellanic Cloud. The two flights corresponded to day 55 and day 407 respectively of remnant evolution. The instrument was complemented by a hard X-ray proportional counter, designed and constructed by the Istituto di Astrofisica Spaziale, CNR, Frascati Italy, and sensitive to the 10 to 250 KeV <span class="hlt">energy</span> range. In this thesis, an account is given of the physical processes responsible for the production of <span class="hlt">gamma</span>-rays astrophysical environments and their relation to supernovae and cosmic-rays. A description is then given of the main features of the <span class="hlt">gamma</span>-ray telescope and its principle of operation, the most important part of the telescope being a spark-chamber used to determine the direction of arrival of incident <span class="hlt">gamma</span>-rays. Data obtained during each flight was recorded as spark-chamber tacks on photographic film. A detailed account of the methods of subsequent data reduction and analysis, as carried out by the author, are given. The principal results of this work were that 3-sigma upper limits to the <span class="hlt">gamma</span>-ray flux from Supernova SN1987A of 2.2 times 10^ {-5} photons cm^{ -2} s^{-1} and 3.4 times 10^{-5} photons cm^{-2} s^ {-1} were obtained for days 55 and 407 of remnant evolution respectively, these limits being somewhat lower than previously reported in the literature from a preliminary analysis of the data. The above two upper limits are consistent with Supernova SN1987A being an atypical Type-II supernova. That is, the progenitor was a blue, rather than a red, supergiant. The limits are compared with theoretical predictions related to current models of <span class="hlt">gamma</span>-ray emission from young Type -II supernovae.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/863846','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/863846"><span>Directional <span class="hlt">gamma</span> detector</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>LeVert, Francis E.; Cox, Samson A.</p> <p>1981-01-01</p> <p>An improved directional <span class="hlt">gamma</span> radiation detector has a collector sandwiched etween two layers of insulation of varying thicknesses. The collector and insulation layers are contained within an evacuated casing, or emitter, which <span class="hlt">releases</span> electrons upon exposure to <span class="hlt">gamma</span> radiation. Delayed electrons and electrons entering the collector at oblique angles are attenuated as they pass through the insulation layers on route to the collector.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AIPC.1792f0005L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AIPC.1792f0005L"><span>Constraining the redshift distribution of ultrahigh-<span class="hlt">energy</span>-cosmic-ray sources by isotropic <span class="hlt">gamma</span>-ray background</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Liu, Ruo-Yu; Taylor, Andrew; Wang, Xiang-Yu; Aharonian, Felix</p> <p>2017-01-01</p> <p>By interacting with the cosmic background photons during their propagation through intergalactic space, ultrahigh <span class="hlt">energy</span> cosmic rays (UHECRs) produce energetic electron/positron pairs and photons which will initiate electromagnetic cascades, contributing to the isotropic <span class="hlt">gamma</span>-ray background (IGRB). The generated <span class="hlt">gamma</span>-ray flux level highly depends on the redshift evolution of the UHECR sources. Recently, the Fermi-LAT collaboration reported that 86-14+16 of the total extragalactic <span class="hlt">gamma</span>-ray flux comes from extragalactic point sources including those unresolved ones. This leaves a limited room for the diffusive <span class="hlt">gamma</span> ray generated via UHECR propagation, and subsequently constrains their source distribution in the Universe. Normalizing the total cosmic ray <span class="hlt">energy</span> budget with the observed UHECR flux in the <span class="hlt">energy</span> band of (1-4)×1018 eV, we calculate the diffuse <span class="hlt">gamma</span>-ray flux generated through UHECR propagation. We find that in order to not overshoot the new IGRB limit, these sub-ankle UHECRs should be produced mainly by nearby sources, with a possible non-negligible contribution from our Galaxy. The distance for the majority of UHECR sources can be further constrained if a given fraction of the observed IGRB at 820 GeV originates from UHECR. We note that our result should be conservative since there may be various other contributions to the IGRB that is not included here.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20000024863','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20000024863"><span>Development of a Broad High-<span class="hlt">Energy</span> <span class="hlt">Gamma</span>-Ray Telescope using Silicon Strip Detectors</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Michelson, Peter F.</p> <p>1998-01-01</p> <p>The research effort has led to the development and demonstration of technology to enable the design and construction of a next-generation high-<span class="hlt">energy</span> <span class="hlt">gamma</span>-ray telescope that operates in the pair-production regime (E greater than 10 MeV). In particular, the technology approach developed is based on silicon-strip detector technology. A complete instrument concept based on this technology for the pair-conversion tracker and the use of CsI(T1) crystals for the calorimeter is now the baseline instrument concept for the <span class="hlt">Gamma</span>-ray Large Area Space Telescope (GLAST) mission. GLAST is NASA's proposed high-<span class="hlt">energy</span> <span class="hlt">gamma</span>-ray mission designed to operate in the <span class="hlt">energy</span> range from 10 MeV to approximately 300 GeV. GLAST, with nearly 100 times the sensitivity of EGRET, operates through pair conversion of <span class="hlt">gamma</span>-rays and measurement of the direction and <span class="hlt">energy</span> of the resulting e (+) - e (-) shower. The baseline design, developed with support from NASA includes a charged particle anticoincidence shield, a tracker/converter made of thin sheets of high-Z material interspersed with Si strip detectors, a CsI calorimeter and a programmable data trigger and acquisition system. The telescope is assembled as an array of modules or towers. Each tower contains elements of the tracker, calorimeter, and anticoincidence system. As originally proposed, the telescope design had 49 modules. In the more optimized design that emerged at the end of the grant period the individual modules are larger and the total number in the GLAST array is 25. Also the calorimeter design was advanced substantially to the point that it has a self-contained imaging capability, albeit much cruder than the tracker.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20150001466','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20150001466"><span>Design and Performance of the <span class="hlt">GAMMA</span>-400 <span class="hlt">Gamma</span>-Ray Telescope for Dark Matter Searches</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Galper, A. M.; Adriani, O.; Aptekar, R. L.; Arkhangelskaja, I. V.; Arkhangelskiy, A. I.; Boezio, M.; Bonvicini, V.; Boyarchuk, K. A.; Fradkin, M. I.; Gusakov, Yu V.; <a style="text-decoration: none; " href="javascript:void(0); " onClick="displayelement('author_20150001466'); toggleEditAbsImage('author_20150001466_show'); toggleEditAbsImage('author_20150001466_hide'); "> <img style="display:inline; width:12px; height:12px; " src="images/arrow-up.gif" width="12" height="12" border="0" alt="hide" id="author_20150001466_show"> <img style="width:12px; height:12px; display:none; " src="images/arrow-down.gif" width="12" height="12" border="0" alt="hide" id="author_20150001466_hide"></p> <p>2012-01-01</p> <p>The <span class="hlt">GAMMA</span>-400 <span class="hlt">gamma</span>-ray telescope is designed to measure the fluxes of <span class="hlt">gamma</span>-rays and cosmic-ray electrons (+) positrons, which can be produced by annihilation or decay of the dark matter particles, as well as to survey the celestial sphere in order to study point and extended sources of <span class="hlt">gamma</span>-rays, measure <span class="hlt">energy</span> spectra of Galactic and extragalactic diffuse <span class="hlt">gamma</span>-ray emission, <span class="hlt">gamma</span>-ray bursts, and <span class="hlt">gamma</span>-ray emission from the Sun. <span class="hlt">GAMMA</span>-400 covers the <span class="hlt">energy</span> range from 100 MeV to 3000 GeV. Its angular resolution is approximately 0.01deg (E(sub <span class="hlt">gamma</span>) greater than 100 GeV), the <span class="hlt">energy</span> resolution approximately 1% (E(sub <span class="hlt">gamma</span>) greater than 10 GeV), and the proton rejection factor approximately 10(exp 6). <span class="hlt">GAMMA</span>-400 will be installed on the Russian space platform Navigator. The beginning of observations is planned for 2018.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AIPC.1516..288G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AIPC.1516..288G"><span>Design and performance of the <span class="hlt">GAMMA</span>-400 <span class="hlt">gamma</span>-ray telescope for dark matter searches</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Galper, A. M.; Adriani, O.; Aptekar, R. L.; Arkhangelskaja, I. V.; Arkhangelskiy, A. I.; Boezio, M.; Bonvicini, V.; Boyarchuk, K. A.; Fradkin, M. I.; Gusakov, Yu. V.; Kaplin, V. A.; Kachanov, V. A.; Kheymits, M. D.; Leonov, A. A.; Longo, F.; Mazets, E. P.; Maestro, P.; Marrocchesi, P.; Mereminskiy, I. A.; Mikhailov, V. V.; Moiseev, A. A.; Mocchiutti, E.; Mori, N.; Moskalenko, I. V.; Naumov, P. Yu.; Papini, P.; Picozza, P.; Rodin, V. G.; Runtso, M. F.; Sparvoli, R.; Spillantini, P.; Suchkov, S. I.; Tavani, M.; Topchiev, N. P.; Vacchi, A.; Vannuccini, E.; Yurkin, Yu. T.; Zampa, N.; Zverev, V. G.; Zirakashvili, V. N.</p> <p>2013-02-01</p> <p>The <span class="hlt">GAMMA</span>-400 <span class="hlt">gamma</span>-ray telescope is designed to measure the fluxes of <span class="hlt">gamma</span>-rays and cosmic-ray electrons + positrons, which can be produced by annihilation or decay of the dark matter particles, as well as to survey the celestial sphere in order to study point and extended sources of <span class="hlt">gamma</span>-rays, measure <span class="hlt">energy</span> spectra of Galactic and extragalactic diffuse <span class="hlt">gamma</span>-ray emission, <span class="hlt">gamma</span>-ray bursts, and <span class="hlt">gamma</span>-ray emission from the Sun. <span class="hlt">GAMMA</span>-400 covers the <span class="hlt">energy</span> range from 100 MeV to 3000 GeV. Its angular resolution is ~0.01° (Eγ > 100 GeV), the <span class="hlt">energy</span> resolution ~1% (Eγ > 10 GeV), and the proton rejection factor ~106. <span class="hlt">GAMMA</span>-400 will be installed on the Russian space platform Navigator. The beginning of observations is planned for 2018.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19850025618','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19850025618"><span>Ultra high <span class="hlt">energy</span> <span class="hlt">gamma</span> rays, cosmic rays and neutrinos from accreting degenerate stars</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Brecher, K.; Chanmugam, G.</p> <p>1985-01-01</p> <p>Super-Eddington accretion for a recently proposed unipolar induction model of cosmic ray acceleration in accreting binary star systems containing magnetic white dwarfs or neutron stars is considered. For sufficiently high accretion rates and low magnetic fields, the model can account for: (1) acceleration of cosmic ray nuclei up to <span class="hlt">energies</span> of 10 to the 19th power eV; (2) production of more or less normal solar cosmic ray composition; (3) the bulk of cosmic rays observed with <span class="hlt">energies</span> above 1 TeV, and probably even down to somewhat lower <span class="hlt">energies</span> as well; and (4) possibly the observed antiproton cosmic ray flux. It can also account for the high ultra high <span class="hlt">energy</span> (UHE) <span class="hlt">gamma</span> ray flux observed from several accreting binary systems (including Cygnus X-3), while allowing the possibility of an even higher neutrino flux from these sources, with L sub nu/L sub <span class="hlt">gamma</span> is approximately 100.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19840009035','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19840009035"><span>High resolution X- and <span class="hlt">gamma</span>-ray spectroscopy of solar flares</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Lin, R. P.</p> <p>1984-01-01</p> <p>A balloon-borne X- and <span class="hlt">gamma</span>-ray instrument was developed, fabricated, and flown. This instrument has the highest <span class="hlt">energy</span> resolution of any instrument flown to date for measurements of solar and cosmic X-ray and <span class="hlt">gamma</span>-ray emission in the 13 to 600 keV <span class="hlt">energy</span> range. The purpose of the solar measurements was to study electron acceleration and solar flare <span class="hlt">energy</span> <span class="hlt">release</span> processes. The cosmic observations were to search for cyclotron line features from neutron stars and for low <span class="hlt">energy</span> <span class="hlt">gamma</span>-ray lines from nucleosynthesis. The instrument consists of four 4 cm diameter, 1.3 cm thick, planar intrinsic germanium detectors cooled by liquid nitrogen and surrounded by CsI and NaI anti-coincidence scintillation crystals. A graded z collimator limited the field of view to 3 deg x 6 deg and a gondola pointing system provided 0.3 deg pointing accuracy. A total of four flights were made with this instrument. Additional funding was obtained from NSF for the last three flights, which had primarily solar objectives. A detailed instrument description is given. The main scientific results and the data analysis are discussed. Current work and indications for future work are summarized. A bibliography of publications resulting from this work is given.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_7");'>7</a></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li class="active"><span>9</span></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_9 --> <div id="page_10" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li class="active"><span>10</span></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="181"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19850026455','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19850026455"><span>High <span class="hlt">energy</span> neutron and <span class="hlt">gamma</span>-radiation generated during the solar flares</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kocharov, G. E.; Mandzhavidze, N. Z.</p> <p>1985-01-01</p> <p>The problem of high <span class="hlt">energy</span> neutrons and <span class="hlt">gamma</span> rays generation in the solar conditions is considered. It is shown that due to a peculiarity of generation and propagation of neutrons corresponding solar flares should be localized at high helio-longitudes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19850027614','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19850027614"><span>Size distributions of air showers accompanied with high <span class="hlt">energy</span> <span class="hlt">gamma</span> ray bundles observed at Mt. Chacaltaya</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Matano, T.; Machida, M.; Tsuchima, I.; Kawasumi, N.; Honda, K.; Hashimoto, K.; Martinic, N.; Zapata, J.; Navia, C. E.; Aquirre, C.</p> <p>1985-01-01</p> <p>Size distributions of air showers accompanied with bundle of high <span class="hlt">energy</span> <span class="hlt">gamma</span> rays and/or large size bursts under emulsion chambers, to study the composition of primary cosmic rays and also characteristics of high <span class="hlt">energy</span> nuclear interaction. Air showers initiated by particles with a large cross section of interaction may develop from narrow region of the atmosphere near the top. Starting levels of air showers by particles with smaller cross section fluctuate in wider region of the atmosphere. Air showers of extremely small size accompanied with bundle of <span class="hlt">gamma</span> rays may be ones initiated by protons at lower level after penetrating deep atmosphere without interaction. It is determined that the relative size distribution according to the total <span class="hlt">energy</span> of bundle of <span class="hlt">gamma</span> rays and the total burst size observed under 15 cm lead absorber.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22679360-searches-correlation-between-uhecr-events-high-energy-gamma-ray-fermi-lat-data','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22679360-searches-correlation-between-uhecr-events-high-energy-gamma-ray-fermi-lat-data"><span>Searches for correlation between UHECR events and high-<span class="hlt">energy</span> <span class="hlt">gamma</span>-ray Fermi-LAT data</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Álvarez, Ezequiel; Cuoco, Alessandro; Mirabal, Nestor</p> <p></p> <p>The astrophysical sources responsible for ultra high-<span class="hlt">energy</span> cosmic rays (UHECRs) continue to be one of the most intriguing mysteries in astrophysics. We present a comprehensive search for correlations between high-<span class="hlt">energy</span> (∼> 1 GeV) <span class="hlt">gamma</span>-ray events from the Fermi Large Area Telescope (LAT) and UHECRs (∼> 60 EeV) detected by the Telescope Array and the Pierre Auger Observatory. We perform two separate searches. First, we conduct a standard cross-correlation analysis between the arrival directions of 148 UHECRs and 360 <span class="hlt">gamma</span>-ray sources in the Second Catalog of Hard Fermi-LAT sources (2FHL). Second, we search for a possible correlation between UHECR directions andmore » unresolved Fermi -LAT <span class="hlt">gamma</span>-ray emission. For the latter, we use three different methods: a stacking technique with both a model-dependent and model-independent background estimate, and a cross-correlation function analysis. We also test for statistically significant excesses in <span class="hlt">gamma</span> rays from signal regions centered on Cen A and the Telescope Array hotspot. No significant correlation is found in any of the analyses performed, except a weak (∼< 2σ) hint of signal with the correlation function method on scales ∼ 1°. Upper limits on the flux of possible power-law <span class="hlt">gamma</span>-ray sources of UHECRs are derived.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/20348336','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/20348336"><span><span class="hlt">Gamma</span>-amino butyric acid (GABA) <span class="hlt">release</span> in the ciliated protozoon Paramecium occurs by neuronal-like exocytosis.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Ramoino, P; Milanese, M; Candiani, S; Diaspro, A; Fato, M; Usai, C; Bonanno, G</p> <p>2010-04-01</p> <p>Paramecium primaurelia expresses a significant amount of <span class="hlt">gamma</span>-amino butyric acid (GABA). Paramecia possess both glutamate decarboxylase (GAD)-like and vesicular GABA transporter (vGAT)-like proteins, indicating the ability to synthesize GABA from glutamate and to transport GABA into vesicles. Using antibodies raised against mammalian GAD and vGAT, bands with an apparent molecular weight of about 67 kDa and 57 kDa were detected. The presence of these bands indicated a similarity between the proteins in Paramecium and in mammals. VAMP, syntaxin and SNAP, putative proteins of the <span class="hlt">release</span> machinery that form the so-called SNARE complex, are present in Paramecium. Most VAMP, syntaxin and SNAP fluorescence is localized in spots that vary in size and density and are primarily distributed near the plasma membrane. Antibodies raised against mammal VAMP-3, sintaxin-1 or SNAP-25 revealed protein immunoblot bands having molecular weights consistent with those observed in mammals. Moreover, P. primaurelia spontaneously <span class="hlt">releases</span> GABA into the environment, and this neurotransmitter <span class="hlt">release</span> significantly increases after membrane depolarization. The depolarization-induced GABA <span class="hlt">release</span> was strongly reduced not only in the absence of extracellular Ca(2+) but also by pre-incubation with bafilomycin A1 or with botulinum toxin C1 serotype. It can be concluded that GABA occurs in Paramecium, where it is probably stored in vesicles capable of fusion with the cell membrane; accordingly, GABA can be <span class="hlt">released</span> from Paramecium by stimulus-induced, neuronal-like exocytotic mechanisms.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1357545-fermi-observations-high-energy-gamma-ray-emission-from-grb','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1357545-fermi-observations-high-energy-gamma-ray-emission-from-grb"><span>FERMI observations of high-<span class="hlt">energy</span> <span class="hlt">gamma</span>-ray emission from GRB 090217A</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Ackermann, M.; Ajello, M.; Baldini, L.; ...</p> <p>2010-06-22</p> <p>The Fermi observatory is advancing our knowledge of <span class="hlt">gamma</span>-ray bursts (GRBs) through pioneering observations at high <span class="hlt">energies</span>, covering more than seven decades in <span class="hlt">energy</span> with the two on-board detectors, the Large Area Telescope (LAT) and the <span class="hlt">Gamma</span>-ray Burst Monitor (GBM). Here, we report on the observation of the long GRB 090217A which triggered the GBM and has been detected by the LAT with a significance greater than 9σ. We present the GBM and LAT observations and on-ground analyses, including the time-resolved spectra and the study of the temporal profile from 8 keV up to ~1 GeV. All spectra are wellmore » reproduced by a Band model. We compare these observations to the first two LAT-detected, long bursts GRB 080825C and GRB 080916C. These bursts were found to have time-dependent spectra and exhibited a delayed onset of the high-<span class="hlt">energy</span> emission, which are not observed in the case of GRB 090217A. We discuss some theoretical implications for the high-<span class="hlt">energy</span> emission of GRBs.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017NIMPA.874..137G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017NIMPA.874..137G"><span>Silicon photomultipliers in scintillation detectors used for <span class="hlt">gamma</span> ray <span class="hlt">energies</span> up to 6.1 MeV</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Grodzicka-Kobylka, M.; Szczesniak, T.; Moszyński, M.; Swiderski, L.; Szawłowski, M.</p> <p>2017-12-01</p> <p>Majority of papers concerning scintillation detectors with light readout by means of silicon photomultipliers refer to nuclear medicine or radiation monitoring devices where <span class="hlt">energy</span> of detected <span class="hlt">gamma</span> rays do not exceed 2 MeV. Detection of <span class="hlt">gamma</span> radiation with higher <span class="hlt">energies</span> is of interest to e.g. high <span class="hlt">energy</span> physics and plasma diagnostics. The aim of this paper is to study applicability (usefulness) of SiPM light readout in detection of <span class="hlt">gamma</span> rays up to 6.1 MeV in combination with various scintillators. The reported measurements were made with 3 samples of one type of Hamamatsu TSV (Through-Silicon Via technology) MPPC arrays. These 4x4 channel arrays have a 50 × 50 μm2 cell size and 12 × 12 mm2 effective active area. The following scintillators were used: CeBr3, NaI:Tl, CsI:Tl. During all the tests detectors were located in a climatic chamber. The studies are focused on optimization of the MPPC performance for practical use in detection of high <span class="hlt">energy</span> <span class="hlt">gamma</span> rays. The optimization includes selection of the optimum operating voltage in respect to the required <span class="hlt">energy</span> resolution, dynamic range, linearity and pulse amplitude. The presented temperature tests show breakdown voltage dependence on the temperature change and define requirements for a power supply and gain stabilization method. The <span class="hlt">energy</span> spectra for <span class="hlt">energies</span> between 511 keV and 6.1 MeV are also presented and compared with data acquired with a classic photomultiplier XP5212B readout. Such a comparison allowed study of nonlinearity of the tested MPPCs, correction of the <span class="hlt">energy</span> spectra and proper analysis of the <span class="hlt">energy</span> resolution.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28521230','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28521230"><span><span class="hlt">Energy</span> consumption and water-soluble protein <span class="hlt">release</span> by cell wall disruption of Nannochloropsis gaditana.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Safi, C; Cabas Rodriguez, L; Mulder, W J; Engelen-Smit, N; Spekking, W; van den Broek, L A M; Olivieri, G; Sijtsma, L</p> <p>2017-09-01</p> <p>Several cell disruption methods were tested on Nannochloropsis gaditana, to evaluate their efficiency in terms of cell disintegration, <span class="hlt">energy</span> input and <span class="hlt">release</span> of soluble proteins. High-pressure homogenization (HPH) and bead milling were the most efficient with >95% cell disintegration, ±50% (w/w) <span class="hlt">release</span> of total proteins and low <span class="hlt">energy</span> input (<0.5kWh.kg -1 biomass ). Enzymatic treatment required low <span class="hlt">energy</span> input (<0.34kWh.kg -1 biomass ), but it only <span class="hlt">released</span> ±35% protein (w/w). Pulsed Electric Field (PEF) was neither <span class="hlt">energy</span>-efficient (10.44kWh.kg -1 biomass ) nor successful for protein <span class="hlt">release</span> (only 10% proteins w/w) and cell disintegration. The <span class="hlt">release</span> of proteins after applying HPH and bead milling always required less intensive operating conditions for cell disruption. The <span class="hlt">energy</span> cost per unit of <span class="hlt">released</span> protein ranged from 0.15-0.25 €.kg Protein -1 in case of HPH, and up to 2-20 €.kg Protein -1 in case of PEF. Copyright © 2017 Elsevier Ltd. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19920052007&hterms=Magnetic+energy&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3DMagnetic%2Benergy','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19920052007&hterms=Magnetic+energy&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3DMagnetic%2Benergy"><span>High-<span class="hlt">energy</span> <span class="hlt">gamma</span>-ray emission from pion decay in a solar flare magnetic loop</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Mandzhavidze, Natalie; Ramaty, Reuven</p> <p>1992-01-01</p> <p>The production of high-<span class="hlt">energy</span> <span class="hlt">gamma</span> rays resulting from pion decay in a solar flare magnetic loop is investigated. Magnetic mirroring, MHD pitch-angle scattering, and all of the relevant loss processes and photon production mechanisms are taken into account. The transport of both the primary ions and the secondary positrons resulting from the decay of the positive pions, as well as the transport of the produced <span class="hlt">gamma</span>-ray emission are considered. The distributions of the <span class="hlt">gamma</span> rays as a function of atmospheric depth, time, emission angle, and photon <span class="hlt">energy</span> are calculated and the dependence of these distributions on the model parameters are studied. The obtained angular distributions are not sufficiently anisotropic to account for the observed limb brightening of the greater than 10 MeV flare emission, indicating that the bulk of this emission is bremsstrahlung from primary electrons.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19850045251&hterms=oso&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Doso','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19850045251&hterms=oso&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Doso"><span>High <span class="hlt">energy</span> X-ray observations of COS-B <span class="hlt">gamma</span>-ray sources from OSO-8</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Dolan, J. F.; Crannell, C. J.; Dennis, B. R.; Frost, K. J.; Orwig, L. E.; Caraveo, P. A.</p> <p>1985-01-01</p> <p>During the three years between satellite launch in June 1975 and turn-off in October 1978, the high <span class="hlt">energy</span> X-ray spectrometer on board OSO-8 observed nearly all of the COS-B <span class="hlt">gamma</span>-ray source positions given in the 2CG catalog (Swanenburg et al., 1981). An X-ray source was detected at <span class="hlt">energies</span> above 20 keV at the 6-sigma level of significance in the <span class="hlt">gamma</span>-ray error box containing 2CG342 - 02 and at the 3-sigma level of significance in the error boxes containing 2CG065 + 00, 2CG195 + 04, and 2CG311 - 01. No definite association between the X-ray and <span class="hlt">gamma</span>-ray sources can be made from these data alone. Upper limits are given for the 2CG sources from which no X-ray flux was detected above 20 keV.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014bsee.confP..54P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014bsee.confP..54P"><span>Observations of short-duration <span class="hlt">gamma</span>-ray bursts</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pozanenko, Alexei; Volnova, Alina; Tungalag, Namkhai; Elenin, Leonid; Molotov, Igor; Voropaev, Victor; Schmalz, Sergey</p> <p>2014-09-01</p> <p><span class="hlt">Gamma</span>-ray bursts (GRB) are the most powerful cosmological catastrophes in the Universe, with <span class="hlt">energy</span> <span class="hlt">releases</span> of 1048 - 1053 erg within a few tens of seconds. It is widely believed that progenitors of the short-duration class of GRB can be merging relativistic binary systems such as a neutron star (NS) and a black hole (BH) or NS-NS. We review the physics of GRBs, their phenomenological properties and observational evidence of GRBs, emphasizing optical observations of GRBs from Mongolia.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3910908','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3910908"><span><span class="hlt">Gamma</span> Interferon <span class="hlt">Release</span> Assays for Detection of Mycobacterium tuberculosis Infection</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Denkinger, Claudia M.; Kik, Sandra V.; Rangaka, Molebogeng X.; Zwerling, Alice; Oxlade, Olivia; Metcalfe, John Z.; Cattamanchi, Adithya; Dowdy, David W.; Dheda, Keertan; Banaei, Niaz</p> <p>2014-01-01</p> <p>SUMMARY Identification and treatment of latent tuberculosis infection (LTBI) can substantially reduce the risk of developing active disease. However, there is no diagnostic gold standard for LTBI. Two tests are available for identification of LTBI: the tuberculin skin test (TST) and the <span class="hlt">gamma</span> interferon (IFN-γ) <span class="hlt">release</span> assay (IGRA). Evidence suggests that both TST and IGRA are acceptable but imperfect tests. They represent indirect markers of Mycobacterium tuberculosis exposure and indicate a cellular immune response to M. tuberculosis. Neither test can accurately differentiate between LTBI and active TB, distinguish reactivation from reinfection, or resolve the various stages within the spectrum of M. tuberculosis infection. Both TST and IGRA have reduced sensitivity in immunocompromised patients and have low predictive value for progression to active TB. To maximize the positive predictive value of existing tests, LTBI screening should be reserved for those who are at sufficiently high risk of progressing to disease. Such high-risk individuals may be identifiable by using multivariable risk prediction models that incorporate test results with risk factors and using serial testing to resolve underlying phenotypes. In the longer term, basic research is necessary to identify highly predictive biomarkers. PMID:24396134</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1402583-miniature-bulge-test-energy-release-rate-hiped-aluminum-aluminum-interfacial-fracture','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1402583-miniature-bulge-test-energy-release-rate-hiped-aluminum-aluminum-interfacial-fracture"><span>Miniature bulge test and <span class="hlt">energy</span> <span class="hlt">release</span> rate in HIPed aluminum/aluminum interfacial fracture</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Liu, C.; Lovato, M. L.; Clarke, K. D.</p> <p></p> <p>We summarize the development of a technique of using miniature bulge test combined with three-dimensional digital image correlation (3D-DIC) for measuring <span class="hlt">energy</span> <span class="hlt">release</span> rate or fracture toughness of bimaterial interface of thin metal foils. Furthermore, the <span class="hlt">energy</span> <span class="hlt">release</span> rate associated with the HIPed aluminum/aluminum interfacial delamination is determined experimentally using the proposed technique. Detailed discussions of the schemes of preparing and conducting the bulge test, and computing various quantities required for the determination of the <span class="hlt">energy</span> <span class="hlt">release</span> rate are presented.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1402583-miniature-bulge-test-energy-release-rate-hiped-aluminum-aluminum-interfacial-fracture','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1402583-miniature-bulge-test-energy-release-rate-hiped-aluminum-aluminum-interfacial-fracture"><span>Miniature bulge test and <span class="hlt">energy</span> <span class="hlt">release</span> rate in HIPed aluminum/aluminum interfacial fracture</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Liu, C.; Lovato, M. L.; Clarke, K. D.; ...</p> <p>2017-10-13</p> <p>We summarize the development of a technique of using miniature bulge test combined with three-dimensional digital image correlation (3D-DIC) for measuring <span class="hlt">energy</span> <span class="hlt">release</span> rate or fracture toughness of bimaterial interface of thin metal foils. Furthermore, the <span class="hlt">energy</span> <span class="hlt">release</span> rate associated with the HIPed aluminum/aluminum interfacial delamination is determined experimentally using the proposed technique. Detailed discussions of the schemes of preparing and conducting the bulge test, and computing various quantities required for the determination of the <span class="hlt">energy</span> <span class="hlt">release</span> rate are presented.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22265959-effective-atomic-numbers-blue-topaz-different-gamma-rays-energies-obtained-from-compton-scattering-technique','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22265959-effective-atomic-numbers-blue-topaz-different-gamma-rays-energies-obtained-from-compton-scattering-technique"><span>Effective atomic numbers of blue topaz at different <span class="hlt">gamma</span>-rays <span class="hlt">energies</span> obtained from Compton scattering technique</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Tuschareon, S., E-mail: tuscharoen@hotmail.com; Limkitjaroenporn, P., E-mail: tuscharoen@hotmail.com; Kaewkhao, J., E-mail: tuscharoen@hotmail.com</p> <p>2014-03-24</p> <p>Topaz occurs in a wide range of colors, including yellow, orange, brown, pink-to-violet and blue. All of these color differences are due to color centers. In order to improve the color of natural colorless topaz, the most commonly used is irradiated with x- or <span class="hlt">gamma</span>-rays, indicated that attenuation parameters is important to enhancements by irradiation. In this work, the mass attenuation coefficients of blue topaz were measured at the different <span class="hlt">energy</span> of γ-rays using the Compton scattering technique. The results show that, the experimental values of mass attenuation coefficient are in good agreement with the theoretical values. The mass attenuationmore » coefficients increase with the decrease in <span class="hlt">gamma</span> rays <span class="hlt">energies</span>. This may be attributed to the higher photon interaction probability of blue topaz at lower <span class="hlt">energy</span>. This result is a first report of mass attenuation coefficient of blue topaz at different <span class="hlt">gamma</span> rays <span class="hlt">energies</span>.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/1386873','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/1386873"><span>Identification of the low affinity receptor for immunoglobulin E on mouse mast cells and macrophages as Fc <span class="hlt">gamma</span> RII and Fc <span class="hlt">gamma</span> RIII.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Takizawa, F; Adamczewski, M; Kinet, J P</p> <p>1992-08-01</p> <p>In addition to their well characterized high affinity immunoglobulin E (IgE) receptors (Fc epsilon RI) mast cells have long been suspected to express undefined Fc receptors capable of binding IgE with low affinity. In this paper, we show that Fc <span class="hlt">gamma</span> RII and Fc <span class="hlt">gamma</span> RIII, but not Mac-2, on mouse mast cells and macrophages bind IgE-immune complexes. This binding is efficiently competed by 2.4G2, a monoclonal antibody against the extracellular homologous region of both Fc <span class="hlt">gamma</span> RII and Fc <span class="hlt">gamma</span> RIII. Furthermore, IgE-immune complexes bind specifically to Fc <span class="hlt">gamma</span> RII or Fc <span class="hlt">gamma</span> RIII transfected into COS-7 cells. The association constants of IgE binding estimated from competition experiments are about 3.1 x 10(5) M-1 for Fc <span class="hlt">gamma</span> RII, and 4.8 x 10(5) M-1 for Fc <span class="hlt">gamma</span> RIII. Engagement of Fc <span class="hlt">gamma</span> RII and Fc <span class="hlt">gamma</span> RIII with IgE-immune complexes (after blocking access to Fc epsilon RI) or with IgG-immune complexes triggers C57.1 mouse mast cells to <span class="hlt">release</span> serotonin. This <span class="hlt">release</span> is inhibited by 2.4G2, and at maximum, reaches 30-40% of the intracellular content, about half of the maximal <span class="hlt">release</span> (60-80%) obtained after Fc epsilon RI engagement. These data demonstrate that mouse Fc <span class="hlt">gamma</span> RII and Fc <span class="hlt">gamma</span> RIII are not isotype specific, and that the binding of IgE-immune complexes to these receptors induces cell activation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1357420-fermi-observations-high-energy-gamma-ray-emission-from-grb','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1357420-fermi-observations-high-energy-gamma-ray-emission-from-grb"><span>FERMI Observations of High-<span class="hlt">Energy</span> <span class="hlt">Gamma</span>-Ray Emission from GRB 080825C</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Abdo, A. A.; Ackermann, M.; Asano, K.; ...</p> <p>2009-11-24</p> <p>The Fermi <span class="hlt">Gamma</span>-ray Space Telescope has opened a new high-<span class="hlt">energy</span> window in the study of <span class="hlt">gamma</span>-ray bursts (GRBs). Here in this paper, we present a thorough analysis of GRB 080825C, which triggered the Fermi <span class="hlt">Gamma</span>-ray Burst Monitor (GBM), and was the first firm detection of a GRB by the Fermi Large Area Telescope (LAT). We discuss the LAT event selections, background estimation, significance calculations, and localization for Fermi GRBs in general and GRB 080825C in particular. We show the results of temporal and time-resolved spectral analysis of the GBM and LAT data. Finally, we also present some theoretical interpretation ofmore » GRB 080825C observations as well as some common features observed in other LAT GRBs.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19870052744&hterms=Magnetic+energy&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3DMagnetic%2Benergy','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19870052744&hterms=Magnetic+energy&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3DMagnetic%2Benergy"><span>Observed form and action of the magnetic <span class="hlt">energy</span> <span class="hlt">release</span> in flares</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Machado, Marcos E.; Moore, Ronald L.</p> <p>1986-01-01</p> <p>The observable spatio-temporal characteristics of the <span class="hlt">energy</span> <span class="hlt">release</span> in flares and their association with the magnetic environment and tracers of field dynamics are reviewed. The observations indicate that impulsive phase manifestations, like particle acceleration, may be related to the formation of neutral sheets at the interface between interacting bipoles, but that the site for the bulk of the <span class="hlt">energy</span> <span class="hlt">release</span> is within closed loops rather than at the interaction site.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20120013458','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20120013458"><span>Future <span class="hlt">Gamma</span>-Ray Imaging of Solar Eruptive Events</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Shih, Albert</p> <p>2012-01-01</p> <p>Solar eruptive events, the combination of large solar flares and coronal mass ejections (CMEs), accelerate ions to tens of Gev and electrons to hundreds of MeV. The <span class="hlt">energy</span> in accelerated particles can be a significant fraction (up to tens of percent) of the <span class="hlt">released</span> <span class="hlt">energy</span> and is roughly equipartitioned between ions and electrons. Observations of the <span class="hlt">gamma</span>-ray signatures produced by these particles interacting with the ambient solar atmosphere probes the distribution and composition of the accelerated population, as well as the atmospheric parameters and abundances of the atmosphere, ultimately revealing information about the underlying physics. <span class="hlt">Gamma</span>-ray imaging provided by RHESSI showed that the interacting approx.20 MeV/nucleon ions are confined to flare magnetic loops rather than precipitating from a large CME-associated shock. Furthermore, RHESSI images show a surprising, significant spatial separation between the locations where accelerated ions and electrons are interacting, thus indicating a difference in acceleration or transport processes for the two types of particles. Future <span class="hlt">gamma</span>-ray imaging observations, with higher sensitivity and greater angular resolution, can investigate more deeply the nature of ion acceleration. The technologies being proven on the <span class="hlt">Gamma</span>-Ray Imager/Polarimeter for Solar flares (GRIPS), a NASA balloon instrument, are possible approaches for future instrumentation. We discuss the GRIPS instrument and the future of studying this aspect of solar eruptive events.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016cosp...41E..89A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016cosp...41E..89A"><span>Registered particles onboard identification in the various apertures of <span class="hlt">GAMMA</span>-400 space <span class="hlt">gamma</span>-telescope</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Arkhangelskaja, Irene</p> <p>2016-07-01</p> <p><span class="hlt">GAMMA</span>-400 (<span class="hlt">Gamma</span> Astronomical Multifunctional Modular Apparatus) will be the <span class="hlt">gamma</span>-telescope onboard international satellite <span class="hlt">gamma</span>-observatory designed for particle registration in the wide <span class="hlt">energy</span> band. Its parameters are optimized for detection of <span class="hlt">gamma</span>-quanta with the <span class="hlt">energy</span> ˜ 100 GeV in the main aperture. The main scientific goals of <span class="hlt">GAMMA</span>-400 are to investigate fluxes of γ-rays and the electron-positron cosmic ray component possibly generated by dark matter particles decay or annihilation and to search for and study in detail discrete γ-ray sources, to investigate the <span class="hlt">energy</span> spectra of Galactic and extragalactic diffuse γ-rays, and to study γ-ray bursts and γ-emission from the active Sun. This article presents analysis of detected events identification procedures and <span class="hlt">energy</span> resolution in three apertures provide particles registration both from upper and lateral directions based on <span class="hlt">GAMMA</span>-400 modeling due special designed software. Time and segmentation methods are used to reject backsplash (backscattering particles created when high <span class="hlt">energy</span> γ-rays interact with the calorimeter's matter and move in the opposite direction) in the main aperture while only <span class="hlt">energy</span> deposition analysis allows to reject this effect in the additional and lateral ones. The main aperture provides the best angular (all strip layers information analysis) and <span class="hlt">energy</span> (<span class="hlt">energy</span> deposition in the all detectors studying) resolution in the <span class="hlt">energy</span> range 0.1 - 3 × 10^{3} GeV. The <span class="hlt">energy</span> resolution in this band is 1%. Triggers in the main aperture will be formed using information about particle direction provided by time of flight system and presence of charged particle or backsplash signal formed according to analysis of <span class="hlt">energy</span> deposition in combination of all two-layers anticoincidence systems individual detectors. In the additional aperture <span class="hlt">gamma</span>-telescope allows to register events in the <span class="hlt">energy</span> band 10 × 10^{-3} - 3 × 10^{3} GeV. The additional aperture <span class="hlt">energy</span> resolution provides due to</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1038005','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1038005"><span>Unidentified <span class="hlt">Gamma</span>-Ray Sources: Hunting <span class="hlt">Gamma</span>-Ray Blazars</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Massaro, F.; D'Abrusco, R.; Tosti, G.</p> <p>2012-04-02</p> <p>One of the main scientific objectives of the ongoing Fermi mission is unveiling the nature of the unidentified {<span class="hlt">gamma</span>}-ray sources (UGSs). Despite the large improvements of Fermi in the localization of {<span class="hlt">gamma</span>}-ray sources with respect to the past {<span class="hlt">gamma</span>}-ray missions, about one third of the Fermi-detected objects are still not associated to low <span class="hlt">energy</span> counterparts. Recently, using the Wide-field Infrared Survey Explorer (WISE) survey, we discovered that blazars, the rarest class of Active Galactic Nuclei and the largest population of {<span class="hlt">gamma</span>}-ray sources, can be recognized and separated from other extragalactic sources on the basis of their infrared (IR) colors. Basedmore » on this result, we designed an association method for the {<span class="hlt">gamma</span>}-ray sources to recognize if there is a blazar candidate within the positional uncertainty region of a generic {<span class="hlt">gamma</span>}-ray source. With this new IR diagnostic tool, we searched for {<span class="hlt">gamma</span>}-ray blazar candidates associated to the UGS sample of the second Fermi {<span class="hlt">gamma</span>}-ray catalog (2FGL). We found that our method associates at least one {<span class="hlt">gamma</span>}-ray blazar candidate as a counterpart each of 156 out of 313 UGSs analyzed. These new low-<span class="hlt">energy</span> candidates have the same IR properties as the blazars associated to {<span class="hlt">gamma</span>}-ray sources in the 2FGL catalog.« less</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li class="active"><span>10</span></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_10 --> <div id="page_11" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li class="active"><span>11</span></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="201"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22037062-unidentified-gamma-ray-sources-hunting-gamma-ray-blazars','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22037062-unidentified-gamma-ray-sources-hunting-gamma-ray-blazars"><span>UNIDENTIFIED {<span class="hlt">gamma</span>}-RAY SOURCES: HUNTING {<span class="hlt">gamma</span>}-RAY BLAZARS</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Massaro, F.; Ajello, M.; D'Abrusco, R.</p> <p>2012-06-10</p> <p>One of the main scientific objectives of the ongoing Fermi mission is unveiling the nature of unidentified {<span class="hlt">gamma</span>}-ray sources (UGSs). Despite the major improvements of Fermi in the localization of {<span class="hlt">gamma</span>}-ray sources with respect to the past {<span class="hlt">gamma</span>}-ray missions, about one-third of the Fermi-detected objects are still not associated with low-<span class="hlt">energy</span> counterparts. Recently, using the Wide-field Infrared Survey Explorer survey, we discovered that blazars, the rarest class of active galactic nuclei and the largest population of {<span class="hlt">gamma</span>}-ray sources, can be recognized and separated from other extragalactic sources on the basis of their infrared (IR) colors. Based on this result, wemore » designed an association method for the {<span class="hlt">gamma</span>}-ray sources to recognize if there is a blazar candidate within the positional uncertainty region of a generic {<span class="hlt">gamma</span>}-ray source. With this new IR diagnostic tool, we searched for {<span class="hlt">gamma</span>}-ray blazar candidates associated with the UGS sample of the second Fermi {<span class="hlt">gamma</span>}-ray LAT catalog (2FGL). We found that our method associates at least one {<span class="hlt">gamma</span>}-ray blazar candidate as a counterpart to each of 156 out of 313 UGSs analyzed. These new low-<span class="hlt">energy</span> candidates have the same IR properties as the blazars associated with {<span class="hlt">gamma</span>}-ray sources in the 2FGL catalog.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20120011795','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20120011795"><span><span class="hlt">Gamma</span>-400 Science Objectives Built on the Current HE <span class="hlt">Gamma</span>-Ray and CR Results</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Moiseev, Alexander; Mitchell, John; Thompson, David</p> <p>2012-01-01</p> <p>The main scientific interest of the Russian <span class="hlt">Gamma</span>-400 team: Observe <span class="hlt">gamma</span>-rays above approximately 50 GeV with excellent <span class="hlt">energy</span> and angular resolution with the goals of: (1) Studying the fine spectral structure of the isotropic high-<span class="hlt">energy</span> <span class="hlt">gamma</span>-radiation, (2) Attempting to identify the many still-unidentified Fermi-LAT <span class="hlt">gamma</span>-ray sources. <span class="hlt">Gamma</span>-400 will likely be the only space-based <span class="hlt">gamma</span>-ray observatory operating at the end of the decade. In our proposed <span class="hlt">Gamma</span>-400-LE version, it will substantially improve upon the capabilities of Fermi LAT and AGILE in both LE and HE <span class="hlt">energy</span> range. Measuring <span class="hlt">gamma</span>-rays from approx 20 MeV to approx 1 TeV for at least 7 years, <span class="hlt">Gamma</span>-400-LE will address the topics of dark matter, cosmic ray origin and propagation, neutron stars, flaring pulsars, black holes, AGNs, GRBs, and actively participate in multiwavelength campaigns.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5469356','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5469356"><span>Reproducibility of Interferon <span class="hlt">Gamma</span> (IFN-γ) <span class="hlt">Release</span> Assays. A Systematic Review</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Tagmouti, Saloua; Slater, Madeline; Benedetti, Andrea; Kik, Sandra V.; Banaei, Niaz; Cattamanchi, Adithya; Metcalfe, John; Dowdy, David; van Zyl Smit, Richard; Dendukuri, Nandini</p> <p>2014-01-01</p> <p>Rationale: Interferon <span class="hlt">gamma</span> (IFN-γ) <span class="hlt">release</span> assays for latent tuberculosis infection result in a larger-than-expected number of conversions and reversions in occupational screening programs, and reproducibility of test results is a concern. Objectives: Knowledge of the relative contribution and extent of the individual sources of variability (immunological, preanalytical, or analytical) could help optimize testing protocols. Methods: We performed a systematic review of studies published by October 2013 on all potential sources of variability of commercial IFN-γ <span class="hlt">release</span> assays (QuantiFERON-TB Gold In-Tube and T-SPOT.TB). The included studies assessed test variability under identical conditions and under different conditions (the latter both overall and stratified by individual sources of variability). Linear mixed effects models were used to estimate within-subject SD. Measurements and Main Results: We identified a total of 26 articles, including 7 studies analyzing variability under the same conditions, 10 studies analyzing variability with repeat testing over time under different conditions, and 19 studies reporting individual sources of variability. Most data were on QuantiFERON (only three studies on T-SPOT.TB). A considerable number of conversions and reversions were seen around the manufacturer-recommended cut-point. The estimated range of variability of IFN-γ response in QuantiFERON under identical conditions was ±0.47 IU/ml (coefficient of variation, 13%) and ±0.26 IU/ml (30%) for individuals with an initial IFN-γ response in the borderline range (0.25–0.80 IU/ml). The estimated range of variability in noncontrolled settings was substantially larger (±1.4 IU/ml; 60%). Blood volume inoculated into QuantiFERON tubes and preanalytic delay were identified as key sources of variability. Conclusions: This systematic review shows substantial variability with repeat IFN-γ <span class="hlt">release</span> assays testing even under identical conditions, suggesting that reversions</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20180001167','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20180001167"><span>A Comparison of High-<span class="hlt">Energy</span> Electron and Cobalt-60 <span class="hlt">Gamma</span>-Ray Radiation Testing</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Boutte, Alvin J.; Campola, Michael J.; Carts, Martin A.; Wilcox, Edward P.; Marshall, Cheryl J.; Phan, Anthony M.; Pellish, Jonathan A.; Powell, Wesley A.; Xapsos, Michael A.</p> <p>2012-01-01</p> <p>In this paper, a comparison between the effects of irradiating microelectronics with high <span class="hlt">energy</span> electrons and Cobalt-60 <span class="hlt">gamma</span>-rays is examined. Additionally, the effect of electron <span class="hlt">energy</span> is also discussed. A variety of part types are investigated, including discrete bipolar transistors, hybrids, and junction field effect transistors</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/21367334-discovery-very-high-energy-gamma-rays-from-blazar-s5','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/21367334-discovery-very-high-energy-gamma-rays-from-blazar-s5"><span>DISCOVERY OF VERY HIGH <span class="hlt">ENERGY</span> <span class="hlt">gamma</span>-RAYS FROM THE BLAZAR S5 0716+714</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Anderhub, H.; Biland, A.; Antonelli, L. A.</p> <p></p> <p>The MAGIC Collaboration reports the detection of the blazar S5 0716+714 (z = 0.31 +- 0.08) in very high <span class="hlt">energy</span> <span class="hlt">gamma</span> rays. The observations were performed in 2007 November and in 2008 April, and were triggered by the Kungliga Vetenskapliga Akademi telescope due to the high optical state of the object. An overall significance of the signal accounts to S = 5.8sigma for 13.1 hr of data. Most of the signal (S = 6.9sigma) comes from the 2008 April data sample during a higher optical state of the object suggesting a possible correlation between the Very High <span class="hlt">Energy</span> <span class="hlt">gamma</span>-ray andmore » optical emissions. The differential <span class="hlt">energy</span> spectrum of the 2008 data sample follows a power law with a photon index of <span class="hlt">GAMMA</span> = 3.45 +- 0.54{sub stat} +- 0.2{sub syst}, and the integral flux above 400 GeV is at the level of (7.5 +- 2.2{sub stat} +- 2.3{sub syst}) x 10{sup -12} cm{sup -2} s{sup -1}, corresponding to a 9% Crab Nebula flux. Modeling of the broadband spectral <span class="hlt">energy</span> distribution indicates that a structured jet model appears to be more promising in describing the available data than a simple one-zone synchrotron self-Compton model.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19930073703&hterms=place+identity&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dplace%2Bidentity','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19930073703&hterms=place+identity&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dplace%2Bidentity"><span>Nonthermal processes around collapsed objects: High <span class="hlt">energy</span> <span class="hlt">gamma</span> ray sources in the radio sky</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Helfand, David J.; Ruderman, Malvin; Applegate, James H.; Becker, Robert H.</p> <p>1993-01-01</p> <p>In our proposal responding to the initial Guest Observer NRA for the Compton <span class="hlt">Gamma</span> Ray Observatory, 'Nonthermal Processes Around Collapsed Objects: High <span class="hlt">Energy</span> <span class="hlt">Gamma</span> Ray Sources in the Radio Sky', we stated that 'At high <span class="hlt">energies</span> - the identity of the principal Galactic source population remains unknown' although the 'one certain source of high <span class="hlt">energy</span> emission is young radio pulsars'. These two statements remain true, although at this writing, eighteen months after the beginning of the Compton allsky survey, much of the <span class="hlt">gamma</span>-ray data required to greatly extend our knowledge of the Galaxy's high <span class="hlt">energy</span> emission has been collected. The thrust of the program supported by our grant was to collect and analyze a complementary set of data on the Milky Way at radio wavelengths in order to help identify the dominant Pop 1 component of the Galaxy's <span class="hlt">gamma</span> ray sources, and to pursue theoretical investigations on the origins and emission mechanisms of young pulsars, the one component of this population identified to date. We summarize here our accomplishments under the grant. In Section 2, we describe our VLA surveys of the Galactic Plane along with the current status of the radio source catalogs derived therefrom; unfortunately, owing to the TDRSS antenna problem and subsequent extension of the Sky Survey, we were not able to carry out a comparison with the EGRET data directly, although everything is now in place to do so as soon as it becomes available. In Section 2, we summarize our progress on the theoretical side, including the substantial completion of a dissertation on pulsar origins and work on the high <span class="hlt">energy</span> emission mechanisms of isolated pulsars. We list the personnel supported by the grant in section 4 and provide a complete bibliography of publications supported in whole or in part by the grant in the final section.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1083194','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/1083194"><span>Gadolinium-doped water cerenkov-based neutron and high <span class="hlt">energy</span> <span class="hlt">gamma</span>-ray detector and radiation portal monitoring system</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Dazeley, Steven A; Svoboda, Robert C; Bernstein, Adam; Bowden, Nathaniel</p> <p>2013-02-12</p> <p>A water Cerenkov-based neutron and high <span class="hlt">energy</span> <span class="hlt">gamma</span> ray detector and radiation portal monitoring system using water doped with a Gadolinium (Gd)-based compound as the Cerenkov radiator. An optically opaque enclosure is provided surrounding a detection chamber filled with the Cerenkov radiator, and photomultipliers are optically connected to the detect Cerenkov radiation generated by the Cerenkov radiator from incident high <span class="hlt">energy</span> <span class="hlt">gamma</span> rays or <span class="hlt">gamma</span> rays induced by neutron capture on the Gd of incident neutrons from a fission source. The PMT signals are then used to determine time correlations indicative of neutron multiplicity events characteristic of a fission source.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19760022030&hterms=cfa&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dcfa','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19760022030&hterms=cfa&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dcfa"><span>Very high <span class="hlt">energy</span> <span class="hlt">gamma</span> ray astronomy</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Grindlay, J. E.</p> <p>1976-01-01</p> <p>Recent results in ground based very high <span class="hlt">energy</span> <span class="hlt">gamma</span> ray astronomy are reviewed. The various modes of the atmospheric Cerenkov technique are described, and the importance of cosmic ray rejection methods is stressed. The positive detections of the Crab pulsar that suggest a very flat spectrum and time-variable pulse phase are discussed. Observations of other pulsars (particularly Vela) suggest these features may be general. Evidence that a 4.8 hr modulated effect was detected from Cyg X-3 is strengthened in that the exact period originally proposed agrees well with a recent determination of the X-ray period. The southern sky observations are reviewed, and the significance of the detection of an active galaxy (NGC 5128) is considered for source models and future observations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28800285','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28800285"><span>Cytogenetic Reconstruction of <span class="hlt">Gamma</span>-Ray Doses Delivered to Atomic Bomb Survivors: Dealing with Wide Distributions of Photon <span class="hlt">Energies</span> and Contributions from Hematopoietic Stem/Progenitor Cells.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Nakamura, Nori; Hirai, Yuko; Kodama, Yoshiaki; Hamasaki, Kanya; Cullings, Harry M; Cordova, Kismet A; Awa, Akio</p> <p>2017-10-01</p> <p>Retrospective estimation of the doses received by atomic bomb (A-bomb) survivors by cytogenetic methods has been hindered by two factors: One is that the photon <span class="hlt">energies</span> <span class="hlt">released</span> from the bomb were widely distributed, and since the aberration yield varies depending on the <span class="hlt">energy</span>, the use of monoenergetic 60 Co <span class="hlt">gamma</span> radiation to construct a calibration curve may bias the estimate. The second problem is the increasing proportion of newly formed lymphocytes entering into the lymphocyte pool with increasing time intervals since the exposures. These new cells are derived from irradiated precursor/stem cells whose radiosensitivity may differ from that of blood lymphocytes. To overcome these problems, radiation doses to tooth enamel were estimated using the electron spin resonance (ESR; or EPR, electron paramagnetic resonance) method and compared with the cytogenetically estimated doses from the same survivors. The ESR method is only weakly dependent on the photon <span class="hlt">energy</span> and independent of the years elapsed since an exposure. Both ESR and cytogenetic doses were estimated from 107 survivors. The latter estimates were made by assuming that although a part of the cells examined could be lymphoid stem or precursor cells at the time of exposure, all the cells had the same radiosensitivity as blood lymphocytes, and that the A-bomb <span class="hlt">gamma</span>-ray spectrum was the same as that of the 60 Co <span class="hlt">gamma</span> rays. Subsequently, ESR and cytogenetic endpoints were used to estimate the kerma doses using individual DS02R1 information on shielding conditions. The results showed that the two sets of kerma doses were in close agreement, indicating that perhaps no correction is needed in estimating atomic bomb <span class="hlt">gamma</span>-ray doses from the cytogenetically estimated 60 Co <span class="hlt">gamma</span>-ray equivalent doses. The present results will make it possible to directly compare cytogenetic doses with the physically estimated doses of the survivors, which would pave the way for testing whether or not there are any systematic</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008RaPC...77..352L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008RaPC...77..352L"><span>Effect of <span class="hlt">gamma</span> irradiation on viscosity reduction of cereal porridges for improving <span class="hlt">energy</span> density</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lee, Ju-Woon; Kim, Jae-Hun; Oh, Sang-Hee; Byun, Eui-Hong; Yook, Hong-Sun; Kim, Mee-Ree; Kim, Kwan-Soo; Byun, Myung-Woo</p> <p>2008-03-01</p> <p>Cereal porridges have low <span class="hlt">energy</span> and nutrient density because of its viscosity. The objective of the present study was to evaluate the effect of irradiation on the reduction of viscosity and on the increasing solid content of cereal porridge. Four cereals, wheat, rice, maize (the normal starchy type) and waxy rice, were used in this study. The porridge with 3000 cP was individually prepared from cereal flour, <span class="hlt">gamma</span>-irradiated at 20 kGy and tested. <span class="hlt">Gamma</span> irradiation of 20 kGy was allowed that the high viscous and rigid cereal porridges turned into semi-liquid consistencies. The solid contents of all porridges could increase by irradiation, compared with non-irradiated ones. No significant differences of starch digestibility were observed in all cereal porridge samples. The results indicated that <span class="hlt">gamma</span> irradiation might be helpful for improving <span class="hlt">energy</span> density of cereal porridge with acceptable consistency.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/21535632','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/21535632"><span>Levels of 2-dodecylcyclobutanone in ground beef patties irradiated by low-<span class="hlt">energy</span> X-ray and <span class="hlt">gamma</span> rays.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Hijaz, Faraj M; Smith, J Scott</p> <p>2010-01-01</p> <p>Food irradiation improves food safety and maintains food quality by controlling microorganisms and extending shelf life. However, acceptance and commercial adoption of food irradiation is still low. Consumer groups such as Public Citizen and the Food and Water Watch have opposed irradiation because of the formation of 2-alkylcyclobutanones (2-ACBs) in irradiated, lipid-containing foods. The objectives of this study were to measure and to compare the level of 2-dodecylcyclobutanone (2-DCB) in ground beef irradiated by low-<span class="hlt">energy</span> X-rays and <span class="hlt">gamma</span> rays. Beef patties were irradiated by low-<span class="hlt">energy</span> X-rays and <span class="hlt">gamma</span> rays (Cs-137) at 3 targeted absorbed doses of 1.5, 3.0, and 5.0 kGy. The samples were extracted with n-hexane using a Soxhlet apparatus, and the 2-DCB concentration was determined with gas chromatography-mass spectrometry. The 2-DCB concentration increased linearly (P < 0.05) with irradiation dose for <span class="hlt">gamma</span>-ray and low-<span class="hlt">energy</span> X-ray irradiated patties. There was no significant difference in 2-DCB concentration between <span class="hlt">gamma</span>-ray and low-<span class="hlt">energy</span> X-ray irradiated patties (P > 0.05) at all targeted doses. © 2010 Institute of Food Technologists®</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1355719','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1355719"><span>Searches for correlation between UHECR events and high-<span class="hlt">energy</span> <span class="hlt">gamma</span>-ray Fermi-LAT data</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Álvarez, Ezequiel; Cuoco, Alessandro; Mirabal, Nestor</p> <p></p> <p>The astrophysical sources responsible for ultra high-<span class="hlt">energy</span> cosmic rays (UHECRs) continue to be one of the most intriguing mysteries in astrophysics. Here, we present a comprehensive search for correlations between high-<span class="hlt">energy</span> (≳ 1 GeV) <span class="hlt">gamma</span>-ray events from the Fermi Large Area Telescope (LAT) and UHECRs (≳ 60 EeV) detected by the Telescope Array and the Pierre Auger Observatory. We perform two separate searches. First, we conduct a standard cross-correlation analysis between the arrival directions of 148 UHECRs and 360 <span class="hlt">gamma</span>-ray sources in the Second Catalog of Hard Fermi-LAT sources (2FHL). Second, we search for a possible correlation between UHECR directionsmore » and unresolved Fermi-LAT <span class="hlt">gamma</span>-ray emission. For the latter, we use three different methods: a stacking technique with both a model-dependent and model-independent background estimate, and a cross-correlation function analysis. We also test for statistically significant excesses in <span class="hlt">gamma</span> rays from signal regions centered on Cen A and the Telescope Array hotspot. There was no significant correlation is found in any of the analyses performed, except a weak (≲ 2σ) hint of signal with the correlation function method on scales ~ 1°. Upper limits on the flux of possible power-law <span class="hlt">gamma</span>-ray sources of UHECRs are derived.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1355719-searches-correlation-between-uhecr-events-high-energy-gamma-ray-fermi-lat-data','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1355719-searches-correlation-between-uhecr-events-high-energy-gamma-ray-fermi-lat-data"><span>Searches for correlation between UHECR events and high-<span class="hlt">energy</span> <span class="hlt">gamma</span>-ray Fermi-LAT data</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Álvarez, Ezequiel; Cuoco, Alessandro; Mirabal, Nestor; ...</p> <p>2016-12-13</p> <p>The astrophysical sources responsible for ultra high-<span class="hlt">energy</span> cosmic rays (UHECRs) continue to be one of the most intriguing mysteries in astrophysics. Here, we present a comprehensive search for correlations between high-<span class="hlt">energy</span> (≳ 1 GeV) <span class="hlt">gamma</span>-ray events from the Fermi Large Area Telescope (LAT) and UHECRs (≳ 60 EeV) detected by the Telescope Array and the Pierre Auger Observatory. We perform two separate searches. First, we conduct a standard cross-correlation analysis between the arrival directions of 148 UHECRs and 360 <span class="hlt">gamma</span>-ray sources in the Second Catalog of Hard Fermi-LAT sources (2FHL). Second, we search for a possible correlation between UHECR directionsmore » and unresolved Fermi-LAT <span class="hlt">gamma</span>-ray emission. For the latter, we use three different methods: a stacking technique with both a model-dependent and model-independent background estimate, and a cross-correlation function analysis. We also test for statistically significant excesses in <span class="hlt">gamma</span> rays from signal regions centered on Cen A and the Telescope Array hotspot. There was no significant correlation is found in any of the analyses performed, except a weak (≲ 2σ) hint of signal with the correlation function method on scales ~ 1°. Upper limits on the flux of possible power-law <span class="hlt">gamma</span>-ray sources of UHECRs are derived.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015SPIE.9593E..0SM','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015SPIE.9593E..0SM"><span>Radiation anomaly detection algorithms for field-acquired <span class="hlt">gamma</span> <span class="hlt">energy</span> spectra</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mukhopadhyay, Sanjoy; Maurer, Richard; Wolff, Ron; Guss, Paul; Mitchell, Stephen</p> <p>2015-08-01</p> <p>The Remote Sensing Laboratory (RSL) is developing a tactical, networked radiation detection system that will be agile, reconfigurable, and capable of rapid threat assessment with high degree of fidelity and certainty. Our design is driven by the needs of users such as law enforcement personnel who must make decisions by evaluating threat signatures in urban settings. The most efficient tool available to identify the nature of the threat object is real-time <span class="hlt">gamma</span> spectroscopic analysis, as it is fast and has a very low probability of producing false positive alarm conditions. Urban radiological searches are inherently challenged by the rapid and large spatial variation of background <span class="hlt">gamma</span> radiation, the presence of benign radioactive materials in terms of the normally occurring radioactive materials (NORM), and shielded and/or masked threat sources. Multiple spectral anomaly detection algorithms have been developed by national laboratories and commercial vendors. For example, the <span class="hlt">Gamma</span> Detector Response and Analysis Software (GADRAS) a one-dimensional deterministic radiation transport software capable of calculating <span class="hlt">gamma</span> ray spectra using physics-based detector response functions was developed at Sandia National Laboratories. The nuisance-rejection spectral comparison ratio anomaly detection algorithm (or NSCRAD), developed at Pacific Northwest National Laboratory, uses spectral comparison ratios to detect deviation from benign medical and NORM radiation source and can work in spite of strong presence of NORM and or medical sources. RSL has developed its own wavelet-based <span class="hlt">gamma</span> <span class="hlt">energy</span> spectral anomaly detection algorithm called WAVRAD. Test results and relative merits of these different algorithms will be discussed and demonstrated.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19910063866&hterms=procedure+whipple&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3Dprocedure%2Bwhipple','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19910063866&hterms=procedure+whipple&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3Dprocedure%2Bwhipple"><span>Locating very high <span class="hlt">energy</span> <span class="hlt">gamma</span>-ray sources with arcminute accuracy</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Akerlof, C. W.; Cawley, M. F.; Chantell, M.; Harris, K.; Lawrence, M. A.; Fegan, D. J.; Lang, M. J.; Hillas, A. M.; Jennings, D. G.; Lamb, R. C.</p> <p>1991-01-01</p> <p>The angular accuracy of <span class="hlt">gamma</span>-ray detectors is intrinsically limited by the physical processes involved in photon detection. Although a number of pointlike sources were detected by the COS B satellite, only two have been unambiguously identified by time signature with counterparts at longer wavelengths. By taking advantage of the extended longitudinal structure of VHE <span class="hlt">gamma</span>-ray showers, measurements in the TeV <span class="hlt">energy</span> range can pinpoint source coordinates to arcminute accuracy. This has now been demonstrated with new data analysis procedures applied to observations of the Crab Nebula using Cherenkov air shower imaging techniques. With two telescopes in coincidence, the individual event circular probable error will be 0.13 deg. The half-cone angle of the field of view is effectively 1 deg.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/9351512','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/9351512"><span>Effect of chronic treatment with the GABA transaminase inhibitors <span class="hlt">gamma</span>-vinyl GABA and ethanolamine O-sulphate on the in vitro GABA <span class="hlt">release</span> from rat hippocampus.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Qume, M; Fowler, L J</p> <p>1997-10-01</p> <p>1. The effects of 2, 8 and 21 day oral treatment with the specific <span class="hlt">gamma</span>-aminobutyric acid transaminase (GABA-T) inhibitors <span class="hlt">gamma</span>-vinyl GABA (GVG) and ethanolamine O-sulphate (EOS) on brain GABA levels, GABA-T activity, and basal and stimulated GABA <span class="hlt">release</span> from rat cross-chopped brain hippocampal slices was investigated. 2. Treatment with GABA-T inhibitors lead to a reduction in brain GABA-T activity by 65-80% compared with control values, with a concomitant increase in brain GABA content of 40-100%. 3. Basal hippocampal GABA <span class="hlt">release</span> was increased to 250-450% of control levels following inhibition of GABA-T activity. No Ca2+ dependence was observed in either control or treated tissues. 4. GVG and EOS administration led to a significant elevation in the potassium stimulated <span class="hlt">release</span> of GABA from cross-chopped hippocampal slices compared with that of controls. Although stimulated GABA <span class="hlt">release</span> from control tissues was decreased in the presence of a low Ca2+ medium, GVG and EOS treatment abolished this Ca2+ dependency. 5. GABA compartmentalization, Na+ and Cl- coupled GABA uptake carriers and glial <span class="hlt">release</span> may provide explanations for the loss of the Ca2+ dependency of stimulated GABA <span class="hlt">release</span> observed following GVG and EOS treatment. 6. Administration of GABA-T inhibitors led to increases in both basal and stimulated hippocampal GABA <span class="hlt">release</span>. However, it is not clear which is the most important factor in the anticonvulsant activity of these drugs, the increased GABA content 'leaking' out of neurones and glia leading to widespread inhibition, or the increase in stimulated GABA <span class="hlt">release</span> which may occur following depolarization caused by an epileptic discharge.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013CMaPh.324..215B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013CMaPh.324..215B"><span>Log-<span class="hlt">Gamma</span> Polymer Free <span class="hlt">Energy</span> Fluctuations via a Fredholm Determinant Identity</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Borodin, Alexei; Corwin, Ivan; Remenik, Daniel</p> <p>2013-11-01</p> <p>We prove that under n 1/3 scaling, the limiting distribution as n → ∞ of the free <span class="hlt">energy</span> of Seppäläinen’s log-<span class="hlt">Gamma</span> discrete directed polymer is GUE Tracy-Widom. The main technical innovation we provide is a general identity between a class of n-fold contour integrals and a class of Fredholm determinants. Applying this identity to the integral formula proved in Corwin et al. (Tropical combinatorics and Whittaker functions. http://arxiv.org/abs/1110.3489v3 [math.PR], 2012) for the Laplace transform of the log-<span class="hlt">Gamma</span> polymer partition function, we arrive at a Fredholm determinant which lends itself to asymptotic analysis (and thus yields the free <span class="hlt">energy</span> limit theorem). The Fredholm determinant was anticipated in Borodin and Corwin (Macdonald processes. http://arxiv.org/abs/1111.4408v3 [math.PR], 2012) via the formalism of Macdonald processes yet its rigorous proof was so far lacking because of the nontriviality of certain decay estimates required by that approach.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016cosp...41E1734S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016cosp...41E1734S"><span>Observations of <span class="hlt">gamma</span>-ray pulsars at the highest <span class="hlt">energies</span> with the Fermi Large Area Telescope</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Saz Parkinson, Pablo</p> <p>2016-07-01</p> <p>One of the most exciting developments in pulsar astrophysics in recent years has been the detection, with ground-based instruments (VERITAS, MAGIC), of pulsed <span class="hlt">gamma</span>-ray emission from the Crab at very high <span class="hlt">energies</span> (VHE, E>100 GeV). The Large Area Telescope (LAT) on board the Fermi satellite has detected over 160 pulsars above 100 MeV. Twenty-eight of these have been shown to emit pulsations above 10 GeV and approximately a dozen show emission above 25 GeV. While most <span class="hlt">gamma</span>-ray pulsars are well-fitted in the GeV range by a power law with an exponential cut-off at around a few GeV, some emission models predict emission at <span class="hlt">energies</span> above 100 GeV, either through a power-law extrapolation of the low-<span class="hlt">energy</span> spectrum, or via a new (e.g. Inverse Compton) component. We will present results of our search for high-<span class="hlt">energy</span> emission from LAT-detected <span class="hlt">gamma</span>-ray pulsars using the latest Pass 8 data and discuss the prospects of finding the next VHE pulsar, providing a good target (or targets) for follow-up observations with current and future ground-based observatories, like CTA.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/6302969-kosmos-kosmos-measurements-high-energy-diffuse-gamma-rays','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/6302969-kosmos-kosmos-measurements-high-energy-diffuse-gamma-rays"><span>Kosmos 856 and Kosmos 914 measurements of high-<span class="hlt">energy</span> diffuse <span class="hlt">gamma</span> rays</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Kalinkin, L.F.; Nagornykh, Y.I.</p> <p>1982-09-01</p> <p>The measurements by the Kosmos 856 and Kosmos 914 satellites of diffuse cosmic ..<span class="hlt">gamma</span>.. rays with photon <span class="hlt">energies</span> above 100 MeV are discussed. Integrated <span class="hlt">energy</span> spectra for the 100--4000 MeV <span class="hlt">energy</span> range are given for galactic lattitudes Vertical BarbVertical Bar< or =30/sup 0/ and Vertical BarbVertical Bar>30/sup 0/. The form of the spectra suggests that at high lattitudes there may still be some contribution from the galactic component.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2119311','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2119311"><span>Identification of the low affinity receptor for immunoglobulin E on mouse mast cells and macrophages as Fc <span class="hlt">gamma</span> RII and Fc <span class="hlt">gamma</span> RIII</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p></p> <p>1992-01-01</p> <p>In addition to their well characterized high affinity immunoglobulin E (IgE) receptors (Fc epsilon RI) mast cells have long been suspected to express undefined Fc receptors capable of binding IgE with low affinity. In this paper, we show that Fc <span class="hlt">gamma</span> RII and Fc <span class="hlt">gamma</span> RIII, but not Mac-2, on mouse mast cells and macrophages bind IgE-immune complexes. This binding is efficiently competed by 2.4G2, a monoclonal antibody against the extracellular homologous region of both Fc <span class="hlt">gamma</span> RII and Fc <span class="hlt">gamma</span> RIII. Furthermore, IgE-immune complexes bind specifically to Fc <span class="hlt">gamma</span> RII or Fc <span class="hlt">gamma</span> RIII transfected into COS-7 cells. The association constants of IgE binding estimated from competition experiments are about 3.1 x 10(5) M-1 for Fc <span class="hlt">gamma</span> RII, and 4.8 x 10(5) M-1 for Fc <span class="hlt">gamma</span> RIII. Engagement of Fc <span class="hlt">gamma</span> RII and Fc <span class="hlt">gamma</span> RIII with IgE-immune complexes (after blocking access to Fc epsilon RI) or with IgG-immune complexes triggers C57.1 mouse mast cells to <span class="hlt">release</span> serotonin. This <span class="hlt">release</span> is inhibited by 2.4G2, and at maximum, reaches 30-40% of the intracellular content, about half of the maximal <span class="hlt">release</span> (60-80%) obtained after Fc epsilon RI engagement. These data demonstrate that mouse Fc <span class="hlt">gamma</span> RII and Fc <span class="hlt">gamma</span> RIII are not isotype specific, and that the binding of IgE-immune complexes to these receptors induces cell activation. PMID:1386873</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li class="active"><span>11</span></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_11 --> <div id="page_12" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li class="active"><span>12</span></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="221"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014SPIE.9213E..18N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014SPIE.9213E..18N"><span>Xenon detector with high <span class="hlt">energy</span> resolution for <span class="hlt">gamma</span>-ray line emission registration</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Novikov, Alexander S.; Ulin, Sergey E.; Chernysheva, Irina V.; Dmitrenko, Valery V.; Grachev, Victor M.; Petrenko, Denis V.; Shustov, Alexander E.; Uteshev, Ziyaetdin M.; Vlasik, Konstantin F.</p> <p>2014-09-01</p> <p>A description of the xenon detector (XD) for <span class="hlt">gamma</span>-ray line emission registration is presented. The detector provides high <span class="hlt">energy</span> resolution and is able to operate under extreme environmental conditions (wide temperature range and unfavorable acoustic action). Resistance to acoustic noise as well as improvement in <span class="hlt">energy</span> resolution has been achieved by means of real-time digital pulse processing. Another important XD feature is the ionization chamber's thin wall with composite housing, which significantly decreases the mass of the device and expands its <span class="hlt">energy</span> range, especially at low <span class="hlt">energies</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014SPIE.9144E..0OM','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014SPIE.9144E..0OM"><span>POET: a SMEX mission for <span class="hlt">gamma</span> ray burst polarimetry</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>McConnell, Mark L.; Baring, Matthew; Bloser, Peter; Dwyer, Joseph F.; Emslie, A. Gordon; Ertley, Camden D.; Greiner, Jochen; Harding, Alice K.; Hartmann, Dieter H.; Hill, Joanne E.; Kaaret, Philip; Kippen, R. M.; Mattingly, David; McBreen, Sheila; Pearce, Mark; Produit, Nicolas; Ryan, James M.; Ryde, Felix; Sakamoto, Takanori; Toma, Kenji; Vestrand, W. Thomas; Zhang, Bing</p> <p>2014-07-01</p> <p>Polarimeters for Energetic Transients (POET) is a mission concept designed to t within the envelope of a NASA Small Explorer (SMEX) mission. POET will use X-ray and <span class="hlt">gamma</span>-ray polarimetry to uncover the <span class="hlt">energy</span> <span class="hlt">release</span> mechanism associated with the formation of stellar-mass black holes and investigate the physics of extreme magnetic ields in the vicinity of compact objects. Two wide-FoV, non-imaging polarimeters will provide polarization measurements over the broad <span class="hlt">energy</span> range from about 2 keV up to about 500 keV. A Compton scatter polarimeter, using an array of independent scintillation detector elements, will be used to collect data from 50 keV up to 500 keV. At low <span class="hlt">energies</span> (2{15 keV), data will be provided by a photoelectric polarimeter based on the use of a Time Projection Chamber for photoelectron tracking. During a two-year baseline mission, POET will be able to collect data that will allow us to distinguish between three basic models for the inner jet of <span class="hlt">gamma</span>-ray bursts.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19850022925','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19850022925"><span>Residual thermal and moisture influences on the strain <span class="hlt">energy</span> <span class="hlt">release</span> rate analysis of edge delamination</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Obrien, T. K.; Raju, I. S.; Garber, D. P.</p> <p>1985-01-01</p> <p>A laminated plate theory analysis is developed to calculate the strain <span class="hlt">energy</span> <span class="hlt">release</span> rate associated with edge delamination growth in a composite laminate. The analysis includes the contribution of residual thermal and moisture stresses to the strain <span class="hlt">energy</span> <span class="hlt">released</span>. The strain <span class="hlt">energy</span> <span class="hlt">release</span> rate, G, increased when residual thermal effects were combined with applied mechanical strains, but then decreased when increasing moisture content was included. A quasi-three-dimensional finite element analysis indicated identical trends and demonstrated these same trends for the individual strain <span class="hlt">energy</span> <span class="hlt">release</span> rate components, G sub I and G sub II, associated with interlaminar tension and shear. An experimental study indicated that for T300/5208 graphite-epoxy composites, the inclusion of residual thermal and moisture stresses did not significantly alter the calculation of interlaminar fracture toughness from strain <span class="hlt">energy</span> <span class="hlt">release</span> rate analysis of edge delamination data taken at room temperature, ambient conditions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20110013261','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20110013261"><span>The Advanced Energetic Pair Telescope (AdEPT}: A Future Medium-<span class="hlt">Energy</span> <span class="hlt">Gamma</span>-Ray Balloon (and Explorer?) Mission</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Hunter, Stanley D.</p> <p>2011-01-01</p> <p><span class="hlt">Gamma</span>-ray astrophysics probes the highest <span class="hlt">energy</span>, exotic phenomena in astrophysics. In the medium-<span class="hlt">energy</span> regime, 0.1-200 MeV, many astrophysical objects exhibit unique and transitory behavior such as the transition from electron dominated to hadron dominated processes, spectral breaks, bursts, and flares. Medium-<span class="hlt">energy</span> <span class="hlt">gamma</span>-ray imaging however, continues to be a major challenge particularly because of high background, low effective area, and low source intensities. The sensitivity and angular resolution required to address these challenges requires a leap in technology. The Advance Energetic Pair Telescope (AdEPT) being developed at GSFC is designed to image <span class="hlt">gamma</span> rays above 5 MeV via pair production with angular resolution of 1-10 deg. In addition AdEPT will, for the first time, provide high polarization sensitivity in this <span class="hlt">energy</span> range. This performance is achieved by reducing the effective area in favor of enhanced angular resolution through the use of a low-density gaseous conversion medium. AdEPT is based on the Three-Dimensional Track Imager (3-DTI) technology that combines a large volume Negative Ion Time Projection Chamber (NITPC) with 2-D Micro-Well Detector (MWD) readout. I will review the major science topics addressable with medium-<span class="hlt">energy</span> <span class="hlt">gamma</span>-rays and discuss the current status of the AdEPT technology, a proposed balloon instrument, and the design of a future satellite mission.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/15858567','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/15858567"><span>A giant <span class="hlt">gamma</span>-ray flare from the magnetar SGR 1806-20.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Palmer, D M; Barthelmy, S; Gehrels, N; Kippen, R M; Cayton, T; Kouveliotou, C; Eichler, D; Wijers, R A M J; Woods, P M; Granot, J; Lyubarsky, Y E; Ramirez-Ruiz, E; Barbier, L; Chester, M; Cummings, J; Fenimore, E E; Finger, M H; Gaensler, B M; Hullinger, D; Krimm, H; Markwardt, C B; Nousek, J A; Parsons, A; Patel, S; Sakamoto, T; Sato, G; Suzuki, M; Tueller, J</p> <p>2005-04-28</p> <p>Two classes of rotating neutron stars-soft <span class="hlt">gamma</span>-ray repeaters (SGRs) and anomalous X-ray pulsars-are magnetars, whose X-ray emission is powered by a very strong magnetic field (B approximately 10(15) G). SGRs occasionally become 'active', producing many short X-ray bursts. Extremely rarely, an SGR emits a giant flare with a total <span class="hlt">energy</span> about a thousand times higher than in a typical burst. Here we report that SGR 1806-20 emitted a giant flare on 27 December 2004. The total (isotropic) flare <span class="hlt">energy</span> is 2 x 10(46) erg, which is about a hundred times higher than the other two previously observed giant flares. The <span class="hlt">energy</span> <span class="hlt">release</span> probably occurred during a catastrophic reconfiguration of the neutron star's magnetic field. If the event had occurred at a larger distance, but within 40 megaparsecs, it would have resembled a short, hard <span class="hlt">gamma</span>-ray burst, suggesting that flares from extragalactic SGRs may form a subclass of such bursts.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/8104180','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/8104180"><span>Escherichia coli K-12 can utilize an exogenous <span class="hlt">gamma</span>-glutamyl peptide as an amino acid source, for which <span class="hlt">gamma</span>-glutamyltranspeptidase is essential.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Suzuki, H; Hashimoto, W; Kumagai, H</p> <p>1993-09-01</p> <p>Escherichia coli K-12 can utilize a <span class="hlt">gamma</span>-glutamyl peptide as an amino acid source, for which <span class="hlt">gamma</span>-glutamyltranspeptidase (EC 2.3.2.2) is essential. We suggest that the <span class="hlt">gamma</span>-glutamyl linkage of a <span class="hlt">gamma</span>-glutamyl peptide is hydrolyzed by <span class="hlt">gamma</span>-glutamyltranspeptidase located in the periplasmic space, and the <span class="hlt">released</span> amino acid is taken up and utilized by E. coli.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22590949-high-low-energy-gamma-beam-dump-designs-gamma-beam-delivery-system-eli-np','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22590949-high-low-energy-gamma-beam-dump-designs-gamma-beam-delivery-system-eli-np"><span>High and low <span class="hlt">energy</span> <span class="hlt">gamma</span> beam dump designs for the <span class="hlt">gamma</span> beam delivery system at ELI-NP</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Yasin, Zafar, E-mail: zafar.yasin@eli-np.ro; Matei, Catalin; Ur, Calin A.</p> <p></p> <p>The Extreme Light Infrastructure - Nuclear Physics (ELI-NP) is under construction in Magurele, Bucharest, Romania. The facility will use two 10 PW lasers and a high intensity, narrow bandwidth <span class="hlt">gamma</span> beam for stand-alone and combined laser-<span class="hlt">gamma</span> experiments. The accurate estimation of particle doses and their restriction within the limits for both personel and general public is very important in the design phase of any nuclear facility. In the present work, Monte Carlo simulations are performed using FLUKA and MCNPX to design 19.4 and 4 MeV <span class="hlt">gamma</span> beam dumps along with shielding of experimental areas. Dose rate contour plots from both FLUKAmore » and MCNPX along with numerical values of doses in experimental area E8 of the facility are performed. The calculated doses are within the permissible limits. Furthermore, a reasonable agreement between both codes enhances our confidence in using one or both of them for future calculations in beam dump designs, radiation shielding, radioactive inventory, and other calculations releated to radiation protection. Residual dose rates and residual activity calculations are also performed for high-<span class="hlt">energy</span> beam dump and their effect is negligible in comparison to contributions from prompt radiation.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1418771-total-kinetic-energy-release-fast-neutron-induced-fission','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1418771-total-kinetic-energy-release-fast-neutron-induced-fission"><span>The total kinetic <span class="hlt">energy</span> <span class="hlt">release</span> in the fast neutron-induced fission of 232Th</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>King, Jonathan; Yanez, Ricardo; Loveland, Walter</p> <p></p> <p>Here, the post-emission total kinetic <span class="hlt">energy</span> <span class="hlt">release</span> (TKE) in the neutron-induced fission of 232Th was measured (using white spectrum neutrons from LANSCE) for neutron <span class="hlt">energies</span> from E n=3 to 91MeV. In this <span class="hlt">energy</span> range the average post-neutron total kinetic <span class="hlt">energy</span> <span class="hlt">release</span> decreases from 162.3±0.3 at E n=3 MeV to 154.9±0.3 MeV at E n=91 MeV. Analysis of the fission mass distributions indicates that the decrease in TKE with increasing neutron <span class="hlt">energy</span> is a combination of increasing yields of symmetric fission (which has a lower associated TKE) and a decrease in the TKE <span class="hlt">release</span> in asymmetric fission.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1418771-total-kinetic-energy-release-fast-neutron-induced-fission','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1418771-total-kinetic-energy-release-fast-neutron-induced-fission"><span>The total kinetic <span class="hlt">energy</span> <span class="hlt">release</span> in the fast neutron-induced fission of 232Th</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>King, Jonathan; Yanez, Ricardo; Loveland, Walter; ...</p> <p>2017-12-15</p> <p>Here, the post-emission total kinetic <span class="hlt">energy</span> <span class="hlt">release</span> (TKE) in the neutron-induced fission of 232Th was measured (using white spectrum neutrons from LANSCE) for neutron <span class="hlt">energies</span> from E n=3 to 91MeV. In this <span class="hlt">energy</span> range the average post-neutron total kinetic <span class="hlt">energy</span> <span class="hlt">release</span> decreases from 162.3±0.3 at E n=3 MeV to 154.9±0.3 MeV at E n=91 MeV. Analysis of the fission mass distributions indicates that the decrease in TKE with increasing neutron <span class="hlt">energy</span> is a combination of increasing yields of symmetric fission (which has a lower associated TKE) and a decrease in the TKE <span class="hlt">release</span> in asymmetric fission.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007APS..SHK.Q7003Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007APS..SHK.Q7003Z"><span>Post-Detonation <span class="hlt">Energy</span> <span class="hlt">Release</span> from TNT-Aluminum Explosives</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhang, Fan; Anderson, John; Yoshinaka, Akio</p> <p>2007-06-01</p> <p>Detonation and post-detonation <span class="hlt">energy</span> <span class="hlt">release</span> from TNT and TNT-aluminum composite have been experimentally studied in an air-filled chamber, 26 m^3 in volume and 3 m in diameter. While TNT has a high oxygen deficiency, experiments with 1.1 kg to 4 kg charges yield <span class="hlt">energy</span> <span class="hlt">releases</span> reaching only 86% of theoretical equilibrium values, possibly due to the non-uniform mixing between the detonation products and air. In order to improve mixing and further increase afterburning <span class="hlt">energy</span>, large mass fractions of large aluminum particles are combined with TNT. The effect of particle distribution is also investigated in two composite configurations, whereby the aluminum particles are uniformly mixed in cast TNT or arranged in a shell surrounding a TNT cylinder. It is shown that the TNT-aluminum composite outperforms pure TNT, while improved performance is achieved for the shell configuration due to enhanced spatial mixing of hot fuels with oxidizing gases. Comparisons with the equilibrium theory and a liquid-based aluminized composite explosive (with an oxygen deficiency less than that of TNT) are conducted to further explore the mixing and afterburning mechanism.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20120013189','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20120013189"><span>Constraining the High-<span class="hlt">Energy</span> Emission from <span class="hlt">Gamma</span>-Ray Bursts with Fermi</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Gehrels, Neil; Harding, A. K.; Hays, E.; Racusin, J. L.; Sonbas, E.; Stamatikos, M.; Guirec, S.</p> <p>2012-01-01</p> <p>We examine 288 GRBs detected by the Fermi <span class="hlt">Gamma</span>-ray Space Telescope's <span class="hlt">Gamma</span>-ray Burst Monitor (GBM) that fell within the field-of-view of Fermi's Large Area Telescope (LAT) during the first 2.5 years of observations, which showed no evidence for emission above 100 MeV. We report the photon flux upper limits in the 0.1-10 GeV range during the prompt emission phase as well as for fixed 30 s and 100 s integrations starting from the trigger time for each burst. We compare these limits with the fluxes that would be expected from extrapolations of spectral fits presented in the first GBM spectral catalog and infer that roughly half of the GBM-detected bursts either require spectral breaks between the GBM and LAT <span class="hlt">energy</span> bands or have intrinsically steeper spectra above the peak of the nuF(sub v) spectra (E(sub pk)). In order to distinguish between these two scenarios, we perform joint GBM and LAT spectral fits to the 30 brightest GBM-detected bursts and find that a majority of these bursts are indeed softer above E(sub pk) than would be inferred from fitting the GBM data alone. Approximately 20% of this spectroscopic subsample show statistically significant evidence for a cut-off in their high-<span class="hlt">energy</span> spectra, which if assumed to be due to <span class="hlt">gamma</span> <span class="hlt">gamma</span> attenuation, places limits on the maximum Lorentz factor associated with the relativistic outflow producing this emission. All of these latter bursts have maximum Lorentz factor estimates that are well below the minimum Lorentz factors calculated for LAT-detected GRBs, revealing a wide distribution in the bulk Lorentz factor of GRB outflows and indicating that LAT-detected bursts may represent the high end of this distribution.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/296742','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/296742"><span>Toward a next-generation high-<span class="hlt">energy</span> <span class="hlt">gamma</span>-ray telescope. Proceedings</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Bloom, E.D.; Evans, L.L.</p> <p></p> <p>It has been some time between the time of the first <span class="hlt">Gamma</span>-ray Large Area Space Telescope (GLAST) workshop, Towards a Next Generation High-<span class="hlt">Energy</span> <span class="hlt">Gamma</span>-Ray Telescope, in late August 1994, and the publication of a partial proceedings of that meeting. Since then there has been considerable progress in both the technical and project development of GLAST. From its origins at SLAC/Stanford in early 1992, the collaboration has currently grown to more than 20 institutions from France, Germany, Italy, Japan, and the US, and is still growing. About half of these are astrophysics/astronomy institutions; the other half are high-<span class="hlt">energy</span> physics institutions. Aboutmore » 100 astronomers, astrophysicists, and particle physicists are currently spending some fraction of their time on the GLAST R and D program. The late publication date of this proceedings has resulted in some additions to the original content of the meeting. The first paper is actually a brochure prepared for NASA by Peter Michelson in early 1996. Except for the appendix, the other papers in the proceedings were presented at the conference, and written up over the following two years. Some presentations were never written up.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/6741811-energy-calibration-organic-scintillation-detectors-gamma-rays','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/6741811-energy-calibration-organic-scintillation-detectors-gamma-rays"><span><span class="hlt">Energy</span> calibration of organic scintillation detectors for. <span class="hlt">gamma</span>. rays</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Gu Jiahui; Xiao Genlai; Liu Jingyi</p> <p>1988-10-01</p> <p>An experimental method of calibrating organic detectors is described. A NaI(T1) detector has some advantages of high detection efficiency, good <span class="hlt">energy</span> resolution, and definite position of the back-scattering peak. The precise position of the Compton edge can be determined by coincidence measurement between the pulse of an organic scintillation detector and the pulse of the back-scattering peak from NaI(T1) detector. It can be used to calibrate various sizes and shapes of organic scintillation detectors simply and reliably. The home-made plastic and organic liquid scintillation detectors are calibrated and positions of the Compton edge as a function of ..<span class="hlt">gamma</span>..-ray <span class="hlt">energies</span> aremore » obtained.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015PhPro..74..238K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015PhPro..74..238K"><span>Magnetometer Application for <span class="hlt">GAMMA</span>-400 Telescope Switching into the Mode with Increased Low <span class="hlt">Energy</span> Charged Particles Intensity Registration</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Khyzhniak, E. V.; Arkhangelskaja, I. V.; Chasovikov, E. N.; Arkhangelskiy, A. I.; Topchiev, N. P.</p> <p></p> <p><span class="hlt">GAMMA</span>-400 is an international project of a high apogee orbital astrophysical observatory for studying the characteristics of high-<span class="hlt">energy</span> <span class="hlt">gamma</span>-emission, electrons/positrons and light nuclei fluxes. The <span class="hlt">energy</span> range for γ-rays and electrons/positrons registration in the main aperture is from ∼0.1 GeV to ∼3.0 TeV. Also, this aperture allows high <span class="hlt">energy</span> light nuclei fluxes characteristics investigation. Moreover, special aperture configuration allows registering of <span class="hlt">gamma</span>-quanta, electrons (positrons) and light nuclei from the lateral directions too. The spacecraft <span class="hlt">GAMMA</span>-400 orbit will be located in the Earth's magnetosphere and will pass front shock wave from magnetosphere interaction with the solar wind, turbulent-transition region, magnetopause and so on. During the satellite's movement through various Earth's magnetosphere regions its anticoincidence detectors will register high intensity fluxes of low <span class="hlt">energy</span> charged particles captured by the magnetic field. The working area sections of <span class="hlt">GAMMA</span>-400 detector systems used as anticoincidence shield are about 1 m2 each. The high intensity low <span class="hlt">energy</span> charged particles flux influence on anticoincidence detectors should be taken into account during particle identification. This article presents a comparison between Earth's magnetosphere theoretical model according to SPENVIIS package and real data measured by detectors onboard THEMIS series satellites. The differences between these two datasets indicate that the calculated data are not sufficient to make short time predictions of variations of magnetic induction in the outer magnetosphere. A special trigger marker flag will be produced by <span class="hlt">GAMMA</span>-400 counting and triggers signals formation system accordingly to the data of two onboard magnetometers. This flag's presence leads to special algorithms execution start, putting the plastic detectors into a dedicated working mode taking into account possible high count rates of external detector layers.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=1192899','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=1192899"><span>Substance P provoked <span class="hlt">gamma</span>-aminobutyric acid <span class="hlt">release</span> from the myenteric plexus of the guinea-pig small intestine.</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Tanaka, C; Taniyama, K</p> <p>1985-01-01</p> <p>The <span class="hlt">release</span> of [3H]<span class="hlt">gamma</span>-aminobutyric acid (GABA) from the isolated small intestine of the guinea-pig pre-loaded with [3H]GABA was measured in the presence of substance P and vasoactive intestinal polypeptide (VIP). Substance P (10(-10)-10(-7) M) produced a dose-dependent increase in the fractional rate of [3H]GABA <span class="hlt">release</span>. VIP, even at 10(-7) M, did not affect the spontaneous [3H]GABA <span class="hlt">release</span> nor the <span class="hlt">release</span> of [3H]GABA evoked by electrical transmural stimulation (0.5 ms, 15 V, 10 Hz for 30 s). The <span class="hlt">release</span> of endogenous GABA from the isolated small intestine was measured in the presence of substance P (10(-9) M). After 60 min superfusion, the spontaneous <span class="hlt">release</span> of GABA was 4.61 +/- 0.14 pmol min-1 g-1 wet wt. (n = 20). Substance P (10(-9) M) produced an approximate 2-fold spontaneous <span class="hlt">release</span> of endogeneous GABA (8.74 +/- 0.21 pmol min-1 g-1 wet wt. (n = 10)). Perfusion with Ca-free medium containing 1 mM-EGTA and tetrodotoxin (3 X 10(-7) M) inhibited the <span class="hlt">release</span> of endogenous GABA evoked by substance P (10(-9) M). (D-Pro2, D-Trp7,9) substance P (10(-6) M) antagonized the <span class="hlt">release</span> of endogenous GABA evoked by substance P (10(-9) M). These results indicate that substance P induces a neuronal <span class="hlt">release</span> of GABA through its receptor located in the guinea-pig small intestine. Substance P (10(-11)-10(-7) M) produced a dose-dependent increase in the fractional rate of [3H]acetylcholine (ACh) <span class="hlt">release</span> from the isolated small intestine pre-loaded with [3H]choline. The <span class="hlt">release</span> of [3H]ACh evoked by substance P (10(-9) M) was inhibited by perfusion with Ca-free medium containing 1 mM-EGTA, tetrodotoxin (3 X 10(-7) M) and (D-Pro2, D-Trp7,9)substance P (10(-6) M). Bicuculline (10(-6) M) inhibited the <span class="hlt">release</span> of [3H]ACh evoked by substance P (10(-9) M) by 68.1 +/- 4.6% (n = 5), thereby suggesting that the substance P-evoked ACh <span class="hlt">release</span> is partly mediated through the endogenous GABA <span class="hlt">released</span> by substance P. These results provide evidence for the neurotransmitter role of GABA and a</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19770032148&hterms=potential+kinetic+energy&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dpotential%2Bkinetic%2Benergy','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19770032148&hterms=potential+kinetic+energy&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dpotential%2Bkinetic%2Benergy"><span>Growth kinetics of <span class="hlt">gamma</span>-prime precipitates in a directionally solidified eutectic, <span class="hlt">gamma/gamma</span>-prime-delta</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Tewari, S. N.</p> <p>1976-01-01</p> <p>A directionally solidified eutectic alloy (DSEA), of those viewed as potential candidates for the next generation of aircraft gas turbine blade materials, is studied for the <span class="hlt">gamma</span>-prime growth kinetics, in the system Ni-Nb-Cr-Al, specifically: Ni-20 w/o Nb-6 w/o Cr-2.5 w/o Al <span class="hlt">gamma/gamma</span>-prime-delta DSEA. Heat treatment, polishing and etching, and preparation for electron micrography are described, and the size distribution of <span class="hlt">gamma</span>-prime phase following various anneals is plotted, along with <span class="hlt">gamma</span>-prime growth kinetics in this specific DSEA, and the cube of <span class="hlt">gamma</span>-prime particle size vs anneal time. Activation <span class="hlt">energies</span> and coarsening kinetics are studied.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014RaPC..103...67L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014RaPC..103...67L"><span><span class="hlt">Gamma</span>-rays attenuation of zircons from Cambodia and South Africa at different <span class="hlt">energies</span>: A new technique for identifying the origin of gemstone</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Limkitjaroenporn, P.; Kaewkhao, J.</p> <p>2014-10-01</p> <p>In this work, the <span class="hlt">gamma</span>-rays interaction properties of zircons from Cambodia and South Africa have been studied. The densities of Cambodian and South African's zircons are 4.6716±0.0040 g/cm3 and 4.5505±0.0018 g/cm3, respectively. The mass attenuation coefficient and the effective atomic number of gemstones were measured with the <span class="hlt">gamma</span>-ray in <span class="hlt">energies</span> range 223-662 keV using the Compton scattering technique. The mass attenuation coefficients of both zircons decreased with the increasing of <span class="hlt">gamma</span>-rays <span class="hlt">energies</span>. The different mass attenuation coefficients between the two zircons observed at <span class="hlt">gamma</span>-ray <span class="hlt">energies</span> below 400 keV are attributed to the differences in the photoelectric interaction. The effective atomic number of zircons was decreased with the increasing of <span class="hlt">gamma</span>-ray <span class="hlt">energies</span> and showed totally different values between the Cambodia and South Africa sources. The origins of the two zircons could be successfully identified by the method based on <span class="hlt">gamma</span>-rays interaction with matter with advantage of being a non-destructive testing.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19880056315&hterms=KOSMOS&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3DKOSMOS','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19880056315&hterms=KOSMOS&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3DKOSMOS"><span>The origin and location of the 5 March 1979 <span class="hlt">gamma</span>-ray burst</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kazanas, Demosthenes</p> <p>1988-01-01</p> <p>Evidence and arguments concerning the origin and location of the <span class="hlt">gamma</span>-ray burst (GRB) of March 5, 1979 are reviewed. This GRB has been positionally identified with the SNR 49 in the LMC. Such an association would fix the GRB's distance at 55 kpc, and the observed flux from the GRB would require prodigious <span class="hlt">energy</span> and luminosity, casting doubt on the GRB's distance and its association with the LMC. Some Kosmos 856 observations which may provide more direct evidence on the <span class="hlt">energy</span> <span class="hlt">released</span> are discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/18197526','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/18197526"><span>Cyclodextrin controlled <span class="hlt">release</span> of poorly water-soluble drugs from hydrogels.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Woldum, Henriette Sie; Larsen, Kim Lambertsen; Madsen, Flemming</p> <p>2008-01-01</p> <p>The effect of 2-hydroxypropyl-beta-cyclodextrin and <span class="hlt">gamma</span>-cyclodextrin on the <span class="hlt">release</span> of ibuprofen, ketoprofen and prednisolone was studied. Stability constants calculated for inclusion complexes show size dependence for complexes with both cyclodextrins. Hydrogels were prepared by ultraviolet irradiation and <span class="hlt">release</span> of each model drug was studied. For drugs formulated using cyclodextrins an increase in the achievable concentration and in the <span class="hlt">release</span> from hydrogels was obtained due to increased solubility, although the solubility of all <span class="hlt">gamma</span>-cyclodextrin complexes was limited. The load also was increased by adjusting pH for the acidic drugs and this exceeds the increase obtained with <span class="hlt">gamma</span>-cyclodextrin addition.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27762047','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27762047"><span>A Responsive Battery with Controlled <span class="hlt">Energy</span> <span class="hlt">Release</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Wang, Xiaopeng; Gao, Jian; Cheng, Zhihua; Chen, Nan; Qu, Liangti</p> <p>2016-11-14</p> <p>A new type of responsive battery with the fascinating feature of pressure perceptibility has been developed, which can spontaneously, timely and reliably control the power outputs (e.g., current and voltage) in response to pressure changes. The device design is based on the structure of the Zn-air battery, in which graphene-coated sponge serves as pressure-sensitive air cathode that endows the whole system with the capability of self-controlled <span class="hlt">energy</span> <span class="hlt">release</span>. The responsive batteries exhibit superior battery performance with high open-circuit voltage (1.3 V), and competitive areal capacity of 1.25 mAh cm -2 . This work presents an important move towards next-generation intelligent <span class="hlt">energy</span> storage devices with <span class="hlt">energy</span> management function. © 2016 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li class="active"><span>12</span></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_12 --> <div id="page_13" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li class="active"><span>13</span></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="241"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018AAS...23121901C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018AAS...23121901C"><span>The Dark <span class="hlt">Energy</span> Survey First Data <span class="hlt">Release</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Carrasco Kind, Matias</p> <p>2018-01-01</p> <p>In this talk I will announce and highlight the main components of the first public data <span class="hlt">release</span> (DR1) coming from the Dark <span class="hlt">Energy</span> Survey (DES).In January 2016, the DES survey made available, in a simple unofficial <span class="hlt">release</span> to the astronomical community, the first set of products. This data was taken and studied during the DES Science Verification period consisting on roughly 250 sq. degrees and 25 million objects at a mean depth of i=23.7 that led to over 80 publications from DES scientist.The DR1 <span class="hlt">release</span> is the first official <span class="hlt">release</span> from the main survey and it consists on the observations taken during the first 3 seasons from August 2013 to February 2016 (about 100 nights each season) of the survey which cover the entire DES footprint. All of the Single Epoch Images and the Year 3 Coadded images distributed in 10223 tiles are available for download in this <span class="hlt">release</span>. The catalogs provide astrometry, photometry and basic classification for near 400M objects in roughly 5000 sq. degrees on the southern hemisphere with a approximate mean depth of i=23.3. Complementary footprint, masking and depth information is also available. All of the software used during the generation of these products are open sourced and have been made available through the Github DES Organization. Images, data and other sub products have been possible through the international and collaborative effort of all 25 institutions involved in DES and are available for exploration and download through the interfaces provided by a partnership between NCSA, NOAO and LIneA.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/20400524','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/20400524"><span>Localized cerebral <span class="hlt">energy</span> failure in DNA polymerase <span class="hlt">gamma</span>-associated encephalopathy syndromes.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Tzoulis, Charalampos; Neckelmann, Gesche; Mørk, Sverre J; Engelsen, Bernt E; Viscomi, Carlo; Moen, Gunnar; Ersland, Lars; Zeviani, Massimo; Bindoff, Laurence A</p> <p>2010-05-01</p> <p> with and without electroencephalographic evidence of concurrent epileptic activity, and have diffusion, spectroscopic and histological profiles strongly suggestive of neuronal <span class="hlt">energy</span> failure. We suggest therefore that both infantile and later onset polymerase <span class="hlt">gamma</span> related encephalopathies are part of a continuum.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19830009173','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19830009173"><span>Measurements of galactic plane <span class="hlt">gamma</span> ray emission in the <span class="hlt">energy</span> range from 10 - 80 MeV</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Bertsch, D. L.; Kniffen, D. A.</p> <p>1982-01-01</p> <p>A spark chamber <span class="hlt">gamma</span> ray telescope was developed and flown to observe diffuse <span class="hlt">gamma</span> ray emission from the central region of the galaxy. The extension of observations down to 10 MeV provides important new data indicating that the galactic diffuse <span class="hlt">gamma</span> ray spectrum continues as a power law down to about 10 MeV, an observation in good agreement with recent theoretical predictions. Data from other experiments in the range from 100 keV to 10 MeV show a significant departure from the extension of the power-law fit to the medium <span class="hlt">energy</span> observations reported here, possibly indicating that a different mechanism may be responsible for the emissions below and above a few MeV. The intensity of the spectrum above 10 MeV implies a galactic electron spectrum which is also very intense down to about 10 MeV. Electrons in this <span class="hlt">energy</span> range cannot be observed in the solar cavity because of solar modulation effects. The galactic <span class="hlt">gamma</span> ray data are compared with recent theoretical predictions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28508907','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28508907"><span>An effective trigger for <span class="hlt">energy</span> <span class="hlt">release</span> of vinylheptafulvene-based solar heat batteries.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Cacciarini, Martina; Vlasceanu, Alexandru; Jevric, Martyn; Nielsen, Mogens Brøndsted</p> <p>2017-05-30</p> <p>Stoichiometric copper(i) tetrakis(acetonitrile) is found to activate the thermal ring-closure reaction of a series of high-<span class="hlt">energy</span> vinylheptafulvene isomers to the corresponding low-<span class="hlt">energy</span> and photoactive dihydroazulenes, allowing the <span class="hlt">release</span> of <span class="hlt">energy</span> upon request.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008SPIE.7011E..1SN','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008SPIE.7011E..1SN"><span>CdZnTe detector for hard x-ray and low <span class="hlt">energy</span> <span class="hlt">gamma</span>-ray focusing telescope</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Natalucci, L.; Alvarez, J. M.; Barriere, N.; Caroli, E.; Curado da Silva, R. M.; Del Sordo, S.; Di Cosimo, S.; Frutti, M.; Hernanz, M.; Lozano, M.; Quadrini, E.; Pellegrini, G.; Stephen, J. B.; Ubertini, P.; Uslenghi, M. C.; Zoglauer, A.</p> <p>2008-07-01</p> <p>The science drivers for a new generation soft <span class="hlt">gamma</span>-ray mission are naturally focused on the detailed study of the acceleration mechanisms in a variety of cosmic sources. Through the development of high <span class="hlt">energy</span> optics in the <span class="hlt">energy</span> <span class="hlt">energy</span> range 0.05-1 MeV it will be possible to achieve a sensitivity about two orders of magnitude better than the currently operating <span class="hlt">gamma</span>-ray telescopes. This will open a window for deep studies of many classes of sources: from Galactic X-ray binaries to magnetars, from supernova remnants to Galaxy clusters, from AGNs (Seyfert, blazars, QSO) to the determination of the origin of the hard X-/<span class="hlt">gamma</span>-ray cosmic background, from the study of antimatter to that of the dark matter. In order to achieve the needed performance, a detector with mm spatial resolution and very high peak efficiency is needed. The instrumental characteristics of this device could eventually allow to detect polarization in a number of objects including pulsars, GRBs and bright AGNs. In this work we focus on the characteristics of the focal plane detector, based on CZT or CdTe semiconductor sensors arranged in multiple planes and viewed by a side detector to enhance <span class="hlt">gamma</span>-ray absorption in the Compton regime. We report the preliminary results of an optimization study based on simulations and laboratory tests, as prosecution of the former design studies of the GRI mission which constitute the heritage of this activity.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20120013588','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20120013588"><span>The <span class="hlt">Gamma</span>-Ray Imager/Polarimeter for Solar Flares (GRIPS)</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Shih, Albert Y.; Lin, Robert P.; Hurford, Gordon J.; Duncan, Nicole A.; Saint-Hilaire, Pascal; Bain, Hazel M.; Boggs, Steven E.; Zoglauer, Andreas C.; Smith, David M.; Tajima, Hiroyasu; <a style="text-decoration: none; " href="javascript:void(0); " onClick="displayelement('author_20120013588'); toggleEditAbsImage('author_20120013588_show'); toggleEditAbsImage('author_20120013588_hide'); "> <img style="display:inline; width:12px; height:12px; " src="images/arrow-up.gif" width="12" height="12" border="0" alt="hide" id="author_20120013588_show"> <img style="width:12px; height:12px; display:none; " src="images/arrow-down.gif" width="12" height="12" border="0" alt="hide" id="author_20120013588_hide"></p> <p>2012-01-01</p> <p>The balloon-borne <span class="hlt">Gamma</span>-Ray Imager/Polarimeter for Solar flares (GRIPS) instrument will provide a near-optimal combination of high-resolution imaging, spectroscopy, and polarimetry of solar-flare <span class="hlt">gamma</span>-ray/hard X-ray emissions from approximately 20 keV to greater than approximately 10 MeV. GRIPS will address questions raised by recent solar flare observations regarding particle acceleration and <span class="hlt">energy</span> <span class="hlt">release</span>, such as: What causes the spatial separation between energetic electrons producing hard X-rays and energetic ions producing <span class="hlt">gamma</span>-ray lines? How anisotropic are the relativistic electrons, and why can they dominate in the corona? How do the compositions of accelerated and ambient material vary with space and time, and why? The spectrometer/polarimeter consists of sixteen 3D position-sensitive germanium detectors (3D-GeDs), where each <span class="hlt">energy</span> deposition is individually recorded with an <span class="hlt">energy</span> resolution of a few keV FWHM and a spatial resolution of less than 0.1 cubic millimeter. Imaging is accomplished by a single multi-pitch rotating modulator (MPRM), a 2.5-centimeter thick tungsten alloy slit/slat grid with pitches that range quasi-continuously from 1 to 13 millimeters. The MPRM is situated 8 meters from the spectrometer to provide excellent image quality and unparalleled angular resolution at <span class="hlt">gamma</span>-ray <span class="hlt">energies</span> (12.5 arcsec FWHM), sufficient to separate 2.2 MeV footpoint sources for almost all flares. Polarimetry is accomplished by analyzing the anisotropy of reconstructed Compton scattering in the 3D-GeDs (i.e., as an active scatterer), with an estimated minimum detectable polarization of a few percent at 150-650 keV in an X-class flare. GRIPS is scheduled for a continental-US engineering test flight in fall 2013, followed by long or ultra-long duration balloon flights in Antarctica.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013ApJ...764..190A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013ApJ...764..190A"><span>Limits to the Fraction of High-<span class="hlt">energy</span> Photon Emitting <span class="hlt">Gamma</span>-Ray Bursts</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Akerlof, Carl W.; Zheng, WeiKang</p> <p>2013-02-01</p> <p>After almost four years of operation, the two instruments on board the Fermi <span class="hlt">Gamma</span>-ray Space Telescope have shown that the number of <span class="hlt">gamma</span>-ray bursts (GRBs) with high-<span class="hlt">energy</span> photon emission above 100 MeV cannot exceed roughly 9% of the total number of all such events, at least at the present detection limits. In a recent paper, we found that GRBs with photons detected in the Large Area Telescope have a surprisingly broad distribution with respect to the observed event photon number. Extrapolation of our empirical fit to numbers of photons below our previous detection limit suggests that the overall rate of such low flux events could be estimated by standard image co-adding techniques. In this case, we have taken advantage of the excellent angular resolution of the Swift mission to provide accurate reference points for 79 GRB events which have eluded any previous correlations with high-<span class="hlt">energy</span> photons. We find a small but significant signal in the co-added field. Guided by the extrapolated power-law fit previously obtained for the number distribution of GRBs with higher fluxes, the data suggest that only a small fraction of GRBs are sources of high-<span class="hlt">energy</span> photons.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014SPPhy.145...59Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014SPPhy.145...59Z"><span>Simulation of High <span class="hlt">Energy</span> Emission from <span class="hlt">Gamma</span>-Ray Bursts</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ziaeepour, Houri</p> <p></p> <p><span class="hlt">Gamma</span>-Ray Bursts (GRBs) are the must violent explosions after the Big-Bang. Their high <span class="hlt">energy</span> radiation can potentially carry information about the most inner part of the accretion disk of a collapsing star, ionize the surrounding material in the host galaxy, and thereby influence the process of star formation specially in the dense environment at high redshifts. They can also have a significant contribution in the formation of high <span class="hlt">energy</span> cosmic-rays. Here we present new simulations of GRBs according to a dynamically consistent relativistic shock model for the prompt emission, with or without the presence of an magnetic field. They show that the properties of observed bursts are well reproduced by this model up to GeV <span class="hlt">energies</span>. They help to better understand GRB phenomenon, and provide an insight into characteristics of relativistic jets and particle acceleration which cannot yet be simulated with enough precision from first principles.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017NewA...56..102K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017NewA...56..102K"><span>CORONAS-F observation of <span class="hlt">gamma</span>-ray emission from the solar flare on 2003 October 29</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kurt, Victoria G.; Yushkov, Boris Yu.; Galkin, Vladimir I.; Kudela, Karel; Kashapova, Larisa K.</p> <p>2017-10-01</p> <p>Appreciable hard X-ray (HXR) and <span class="hlt">gamma</span>-ray emissions in the 0.04-150 MeV <span class="hlt">energy</span> range associated with the 2003 October 29 solar flare (X10/3B) were observed at 20:38-20:58 UT by the SONG instrument onboard the CORONAS-F mission. To restore flare <span class="hlt">gamma</span>-ray spectra we fitted the SONG <span class="hlt">energy</span> loss spectra with a three-component model of the incident spectrum: (1) a power law in <span class="hlt">energy</span>, assumed to be due to electron bremsstrahlung; (2) a broad continuum produced by prompt nuclear de-excitation <span class="hlt">gamma</span>-lines; and (3) a broad <span class="hlt">gamma</span>-line generated from pion-decay. We also restored spectra from the RHESSI data, compared them with the SONG spectra and found a reasonable agreement between these spectra in the 0.1-10 MeV <span class="hlt">energy</span> range. The pion-decay emission was observed from 20:44:20 UT and had its maximum at 20:48-20:51 UT. The power-law spectral index of accelerated protons estimated from the ratio between intensities of different components of <span class="hlt">gamma</span> rays changed with time. The hardest spectrum with a power-law index S = -3.5 - 3.6 was observed at 20:48-20:51 UT. Time histories of the pion-decay emission and proton spectrum were compared with changes of the locations of flare <span class="hlt">energy</span> <span class="hlt">release</span> as shown by RHESSI hard X-ray images and remote and remote Hα brightenings. An apparent temporal correlation between processes of particle acceleration and restructuring of flare magnetic field was found. In particular, the protons were accelerated to subrelativistic <span class="hlt">energies</span> after radical change of the character of footpoint motion from a converging motion to a separation motion.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017MPLA...3250027S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017MPLA...3250027S"><span><span class="hlt">Gamma</span>-ray bursts generated from phase transition of neutron stars to quark stars</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Shu, Xiao-Yu; Huang, Yong-Feng; Zong, Hong-Shi</p> <p>2017-02-01</p> <p>The evolution of compact stars is believed to be able to produce various violent phenomena in our universe. In this paper, we discuss the possibility that <span class="hlt">gamma</span>-ray bursts (GRBs) might result from the phase transition of a neutron star to a quark star and calculate the <span class="hlt">energy</span> <span class="hlt">released</span> from the conversion. In our study, we utilize the relativistic mean field (RMF) theory to describe the hadronic phase of neutron stars, while an improved quasi-particle model is adopted to describe the quark phase of quark stars. With quark matter equation-of-state (EOS) more reliable than models used before, it is found that the <span class="hlt">energy</span> <span class="hlt">released</span> is of the order of 1052 erg, which confirms the validity of the phase transition model.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20140001072','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20140001072"><span>The Role of Compressibility in <span class="hlt">Energy</span> <span class="hlt">Release</span> by Magnetic Reconnection</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Birn, J.; Borovosky, J. E.; Hesse, M.</p> <p>2012-01-01</p> <p>Using resistive compressible magnetohydrodynamics, we investigate the <span class="hlt">energy</span> <span class="hlt">release</span> and transfer by magnetic reconnection in finite (closed or periodic) systems. The emphasis is on the magnitude of <span class="hlt">energy</span> <span class="hlt">released</span> and transferred to plasma heating in configurations that range from highly compressible to incompressible, based on the magnitude of the background beta (ratio of plasma pressure over magnetic pressure) and of a guide field in two-dimensional reconnection. As expected, the system becomes more incompressible, and the role of compressional heating diminishes, with increasing beta or increasing guide field. Nevertheless, compressional heating may dominate over Joule heating for values of the guide field of 2 or 3 (in relation to the reconnecting magnetic field component) and beta of 5-10. This result stems from the strong localization of the dissipation near the reconnection site, which is modeled based on particle simulation results. Imposing uniform resistivity, corresponding to a Lundquist number of 10(exp 3) to 10(exp 4), leads to significantly larger Ohmic heating. Increasing incompressibility greatly reduces the magnetic flux transfer and the amount of <span class="hlt">energy</span> <span class="hlt">released</span>, from approx. 10% of the <span class="hlt">energy</span> associated with the reconnecting field component, for zero guide field and low beta, to approx. 0.2%-0.4% for large values of the guide field B(sub y0) > 5 or large beta. The results demonstrate the importance of taking into account plasma compressibility and localization of dissipation in investigations of heating by turbulent reconnection, possibly relevant for solar wind or coronal heating.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/12826079','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/12826079"><span>Stress-induced <span class="hlt">release</span> of HSC70 from human tumors.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Barreto, Alfonso; Gonzalez, John Mario; Kabingu, Edith; Asea, Alexzander; Fiorentino, Susana</p> <p>2003-04-01</p> <p>In this study, we demonstrate that the pro-inflammatory cytokine interferon-<span class="hlt">gamma</span> (IFN-<span class="hlt">gamma</span>) induces the active <span class="hlt">release</span> of the constitutive form of the 70-kDa heat shock protein (HSC70) from K562 erythroleukemic cells. Treatment of K562 cells with IFN-<span class="hlt">gamma</span> induced the upregulation of the inducible form of the 70-kDa heat shock protein (HSP70), but not the constitutive form of HSC70 within the cytosol, in a proteasome-dependent manner. In addition, IFN-<span class="hlt">gamma</span> induced the downregulation of surface-bound HSC70, but did not significantly alter surface-bound HSP70 expression. These findings indicate that HSC70 can be actively <span class="hlt">released</span> from tumor cells and is indicative of a previously unknown mechanism by which immune modulators stimulate the <span class="hlt">release</span> of intracellular HSC70. This mechanism may account for the potent chaperokine activity of heat shock proteins recently observed during heat shock protein-based immunotherapy against a variety of cancers.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1208907-gamma-ray-output-spectra-from-pu-fission','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1208907-gamma-ray-output-spectra-from-pu-fission"><span><span class="hlt">Gamma</span>-ray Output Spectra from 239 Pu Fission</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Ullmann, John</p> <p>2015-05-25</p> <p>The <span class="hlt">gamma</span>-ray multiplicities, individual <span class="hlt">gamma</span>-ray <span class="hlt">energy</span> spectra, and total <span class="hlt">gamma</span> <span class="hlt">energy</span> spectra following neutron-induced fission of 239Pu were measured using the DANCE detector at Los Alamos. Corrections for detector response were made using a forward-modeling technique based on propagating sets of <span class="hlt">gamma</span> rays generated from a paramaterized model through a GEANT model of the DANCE array and adjusting the parameters for best fit to the measured spectra. The results for the <span class="hlt">gamma</span>-ray spectrum and multiplicity are in general agreement with previous results, but the measured total <span class="hlt">gamma</span>-ray <span class="hlt">energy</span> is about 10% higher. We found that a dependence of the <span class="hlt">gamma</span>-raymore » spectrum on the <span class="hlt">gamma</span>-ray multplicity was also observed. Finally, global model calculations of the multiplicity and <span class="hlt">gamma</span> <span class="hlt">energy</span> distributions are in good agreement with the data, but predict a slightly softer total-<span class="hlt">energy</span> distribution.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007nghe.conf.....M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007nghe.conf.....M"><span>Fourth Workshop on Science with the New Generation of High <span class="hlt">Energy</span> <span class="hlt">Gamma</span>-ray Experiments</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Massai, Marco Maria; Omodei, Nicola; Spandre, Gloria</p> <p></p> <p>I. Space-based telescope. Integral-4 years in orbit / P. Umbertini, P. Caraveo. The Suzaku mission / K. Yamaoka. The Swift mission: two years of operation / A. Moretti. <span class="hlt">Gamma</span>-ray astrophysics with AGILE / F.Longo et al., The AGILE collaboration. The GLAST mission / J.E. McEnery -- II. Ground-based telescope. Recent results from CANGAROO / M. Mori for the CANGAROO team. The H.E.S.S. project / C. Masterson for the H.E.S.S. collaboration. The MAGIC experiment / N. Turini for the MAGIC collaboration. VERITAS: status and performance / J. Holder for the VERITAS collaboration -- III. Galactic variable sources. Galactic variable sky with EGRET and GLAST / S. Digel. Galactic variable sources observed with H.E.S.S. / N. Komin for the H.E.S.S collaboration. <span class="hlt">Gamma</span> ray pulsars in the GLAST era / M. Razzano. Solving the riddle of unidentified high-<span class="hlt">energy</span> <span class="hlt">gamma</span>-ray sources / P. Caraveo. Supernovae and <span class="hlt">gamma</span>-ray burst / M. Della Valle. First cycle of MAGIC galactic observations / J. Cortina for the MAGIC collaboration. <span class="hlt">Gamma</span>-rays and neutrinos from a SNR in the galactic center / V. Cavasinni, D. Grasso, L. Maccione. Solving GRBs and SGRs puzzles by precessing jets / D. Fargion, O. Lanciano, P. Oliva -- IV. Extragalactic sources. Multiwavelength observations and theories of blazers / G. Tosti. AGN observations with the MAGIC telescope / C. Bigongiari for the MAGIC collaboration. <span class="hlt">Gamma</span> ray bursts/ L. Amati. X-rays and GeV flares in GRB light curves / A. Galli ... [et al.]. The highest <span class="hlt">energy</span> emission from <span class="hlt">gamma</span> ray bursts: MILAGRO's constraints and HAWC's potential / B. Dingus for the MILAGRO and HAWC collaborations. Observation of GRB with the MAGIC telescope / N. Galante, P. Piccioli for the MAGIC collaboration. GRB 060218 and the outliers with respect to the E-E correlation / G. Ghirlanda, G. Ghibellini -- V. Poster session. Study of the performance and calibration of the GLAST-LAT silicon tracker / M. Brigida, N. Giglietto, P. Spinelli. The online monitor for the GLAST</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19820014230','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19820014230"><span><span class="hlt">Gamma</span>-ray astronomy</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Ramaty, R.; Lingenfelter, R. E.</p> <p>1982-01-01</p> <p>Cosmic <span class="hlt">gamma</span> rays, the physical processes responsible for their production and the astrophysical sites from which they were seen are reported. The bulk of the observed <span class="hlt">gamma</span> ray emission is in the photon <span class="hlt">energy</span> range from about 0.1 MeV to 1 GeV, where observations are carried out above the atmosphere. There are also, however, <span class="hlt">gamma</span> ray observations at higher <span class="hlt">energies</span> obtained by detecting the Cerenkov light produced by the high <span class="hlt">energy</span> photons in the atmosphere. <span class="hlt">Gamma</span> ray emission was observed from sources as close as the Sun and the Moon and as distant as the quasar 3C273, as well as from various other galactic and extragalactic sites. The radiation processes also range from the well understood, e.g. energetic particle interactions with matter, to the still incompletely researched, such as radiation transfer in optically thick electron positron plasmas in intense neutron star magnetic fields.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20040088233&hterms=ALS&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3DALS','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20040088233&hterms=ALS&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3DALS"><span>Immunoglobulin Fc <span class="hlt">gamma</span> receptor promotes immunoglobulin uptake, immunoglobulin-mediated calcium increase, and neurotransmitter <span class="hlt">release</span> in motor neurons</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Mohamed, Habib A.; Mosier, Dennis R.; Zou, Ling L.; Siklos, Laszlo; Alexianu, Maria E.; Engelhardt, Jozsef I.; Beers, David R.; Le, Wei-dong; Appel, Stanley H.</p> <p>2002-01-01</p> <p>Receptors for the Fc portion of immunoglobulin G (IgG; FcgammaRs) facilitate IgG uptake by effector cells as well as cellular responses initiated by IgG binding. In earlier studies, we demonstrated that amyotrophic lateral sclerosis (ALS) patient IgG can be taken up by motor neuron terminals and transported retrogradely to the cell body and can alter the function of neuromuscular synapses, such as increasing intracellular calcium and spontaneous transmitter <span class="hlt">release</span> from motor axon terminals after passive transfer. In the present study, we examined whether FcgammaR-mediated processes can contribute to these effects of ALS patient immunoglobulins. F(ab')(2) fragments (which lack the Fc portion) of ALS patient IgG were not taken up by motor axon terminals and were not retrogradely transported. Furthermore, in a genetically modified mouse lacking the <span class="hlt">gamma</span> subunit of the FcR, the uptake of whole ALS IgG and its ability to enhance intracellular calcium and acetylcholine <span class="hlt">release</span> were markedly attenuated. These data suggest that FcgammaRs appear to participate in IgG uptake into motor neurons as well as IgG-mediated increases in intracellular calcium and acetylcholine <span class="hlt">release</span> from motor axon terminals. Copyright 2002 Wiley-Liss, Inc.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19980237754','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19980237754"><span>The Third EGRET Catalog of High-<span class="hlt">Energy</span> <span class="hlt">Gamma</span>-Ray Sources</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Hartman, R. C.; Bertsch, D. L.; Bloom, S. D.; Chen, A. W.; Deines-Jones, P.; Esposito, J. A.; Fichtel, C. E.; Friedlander, D. P.; Hunter, S. D.; McDonald, L. M.; <a style="text-decoration: none; " href="javascript:void(0); " onClick="displayelement('author_19980237754'); toggleEditAbsImage('author_19980237754_show'); toggleEditAbsImage('author_19980237754_hide'); "> <img style="display:inline; width:12px; height:12px; " src="images/arrow-up.gif" width="12" height="12" border="0" alt="hide" id="author_19980237754_show"> <img style="width:12px; height:12px; display:none; " src="images/arrow-down.gif" width="12" height="12" border="0" alt="hide" id="author_19980237754_hide"></p> <p>1998-01-01</p> <p>The third catalog of high-<span class="hlt">energy</span> <span class="hlt">gamma</span>-ray sources detected by the EGRET telescope on the Compton <span class="hlt">Gamma</span> Ray Observatory includes data from 1991 April 22 to 1995 October 3 (Cycles 1, 2, 3, and 4 of the mission). In addition to including more data than the second EGRET catalog (Thompson et al. 1995) and its supplement (Thompson et al. 1996), this catalog uses completely reprocessed data (to correct a number of mostly minimal errors and problems). The 271 sources (E greater than 100 MeV) in the catalog include the single 1991 solar flare bright enough to be detected as a source, the Large Magellanic Cloud, five pulsars, one probable radio galaxy detection (Cen A), and 66 high-confidence identifications of blazars (BL Lac objects, flat-spectrum radio quasars, or unidentified flat-spectrum radio sources). In addition, 27 lower-confidence potential blazar identifications are noted. Finally, the catalog contains 170 sources not yet identified firmly with known objects, although potential identifications have been suggested for a number of those. A figure is presented that gives approximate upper limits for <span class="hlt">gamma</span>-ray sources at any point in the sky, as well as information about sources listed in the second catalog and its supplement which do not appear in this catalog.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19990063784','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19990063784"><span>The Third EGRET Catalog of High-<span class="hlt">Energy</span> <span class="hlt">Gamma</span>-Ray Sources</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Hartman, R. C.; Bertsch, D. L.; Bloom, S. D.; Chen, A. W.; Deines-Jones, P.; Esposito, J. A.; Fichtel, C. E.; Friedlander, D. P.; Hunter, S. D.; McDonald, L. M.; <a style="text-decoration: none; " href="javascript:void(0); " onClick="displayelement('author_19990063784'); toggleEditAbsImage('author_19990063784_show'); toggleEditAbsImage('author_19990063784_hide'); "> <img style="display:inline; width:12px; height:12px; " src="images/arrow-up.gif" width="12" height="12" border="0" alt="hide" id="author_19990063784_show"> <img style="width:12px; height:12px; display:none; " src="images/arrow-down.gif" width="12" height="12" border="0" alt="hide" id="author_19990063784_hide"></p> <p>1998-01-01</p> <p>The third catalog of high-<span class="hlt">energy</span> <span class="hlt">gamma</span>-ray sources detected by the EGRET telescope on the Compton <span class="hlt">Gamma</span> Ray Observatory includes data from 1991 April 22 to 1995 October 3 (Cycles 1, 2, 3, and 4 of the mission). In addition to including more data than the second EGRET catalog and its supplement, this catalog uses completely reprocessed data (to correct a number of mostly minimal errors and problems). The 271 sources (E greater than 100 MeV) in the catalog include the single 1991 solar flare bright enough to be detected as a source, the Large Magellanic Cloud, five pulsars, one probable radio galaxy detection (Cen A), and 66 high-confidence identifications of blazars (BL Lac objects, flat-spectrum radio quasars, or unidentified flat-spectrum radio sources). In addition, 27 lower-confidence potential blazar identifications are noted. Finally, the catalog contains 170 sources not yet identified firmly with known objects, although potential identifications have been suggested for a number of those. A figure is presented that gives approximate upper limits for <span class="hlt">gamma</span>-ray sources at any point in the sky, as well as information about sources listed in the second catalog and its supplement which do not appear in this catalog.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22365622-high-energy-emissions-from-gamma-ray-binary-ls','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22365622-high-energy-emissions-from-gamma-ray-binary-ls"><span>High-<span class="hlt">energy</span> emissions from the <span class="hlt">gamma</span>-ray binary LS 5039</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Takata, J.; Leung, Gene C. K.; Cheng, K. S.</p> <p>2014-07-20</p> <p>We study mechanisms of multi-wavelength emissions (X-ray, GeV, and TeV <span class="hlt">gamma</span>-rays) from the <span class="hlt">gamma</span>-ray binary LS 5039. This paper is composed of two parts. In the first part, we report on results of observational analysis using 4 yr data of the Fermi Large Area Telescope. Due to the improvement of instrumental response function and increase of the statistics, the observational uncertainties of the spectrum in the ∼100-300 MeV bands and >10 GeV bands are significantly improved. The present data analysis suggests that the 0.1-100 GeV emissions from LS 5039 contain three different components: (1) the first component contributes to <1more » GeV emissions around superior conjunction, (2) the second component dominates in the 1-10 GeV <span class="hlt">energy</span> bands, and (3) the third component is compatible with the lower-<span class="hlt">energy</span> tail of the TeV emissions. In the second part, we develop an emission model to explain the properties of the phase-resolved emissions in multi-wavelength observations. Assuming that LS 5039 includes a pulsar, we argue that emissions from both the magnetospheric outer gap and the inverse-Compton scattering process of cold-relativistic pulsar wind contribute to the observed GeV emissions. We assume that the pulsar is wrapped by two kinds of termination shock: Shock-I due to the interaction between the pulsar wind and the stellar wind and Shock-II due to the effect of the orbital motion. We propose that the X-rays are produced by the synchrotron radiation at the Shock-I region and the TeV <span class="hlt">gamma</span>-rays are produced by the inverse-Compton scattering process at the Shock-II region.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMMR51B2708M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMMR51B2708M"><span>Strain Rate Dependency of Fracture Toughness, <span class="hlt">Energy</span> <span class="hlt">Release</span> Rate and Geomechanical Attributes of Select Indian Shales</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mahanta, B.; Vishal, V.; Singh, T. N.; Ranjith, P.</p> <p>2016-12-01</p> <p>In addition to modern improved technology, it requires detailed understanding of rock fractures for the purpose of enhanced <span class="hlt">energy</span> extraction through hydraulic fracturing of gas shales and geothermal <span class="hlt">energy</span> systems. The understanding of rock fracture behavior, patterns and properties such as fracture toughness; <span class="hlt">energy</span> <span class="hlt">release</span> rate; strength and deformation attributes during fracturing hold significance. Environmental factors like temperature, pressure, humidity, water vapor and experimental condition such as strain rate influence the estimation of these properties. In this study, the effects of strain rates on fracture toughness, <span class="hlt">energy</span> <span class="hlt">release</span> rate as well as geomechanical properties like uniaxial compressive strength, Young's modulus, failure strain, tensile strength, and brittleness index of gas shales were investigated. In addition to the rock-mechanical parameters, the fracture toughness and the <span class="hlt">energy</span> <span class="hlt">release</span> rates were measured for three different modes viz. mode I, mixed mode (I-II) and mode II. Petrographic and X-ray diffraction (XRD) analyses were performed to identify the mineral composition of the shale samples. Scanning electron microscope (SEM) analyses were conducted to have an insight about the strain rate effects on micro-structure of the rock. The results suggest that the fracture toughness; the <span class="hlt">energy</span> <span class="hlt">release</span> rate as well as other geomechanical properties are a function of strain rates. At high strain rates, the strength and stiffness of shale increases which in turn increases the fracture toughness and the <span class="hlt">energy</span> <span class="hlt">release</span> rate of shale that may be due to stress redistribution during grain fracturing. The fracture toughness and the strain <span class="hlt">energy</span> <span class="hlt">release</span> rates for all the modes (I/I-II/II) are comparable at lower strain rates, but they vary considerably at higher strain rates. In all the cases, mode I and mode II fracturing requires minimum and maximum applied <span class="hlt">energy</span>, respectively. Mode I <span class="hlt">energy</span> <span class="hlt">release</span> rate is maximum, compared to the other modes.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li class="active"><span>13</span></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_13 --> <div id="page_14" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li class="active"><span>14</span></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="261"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018EPJWC.16900018Q','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018EPJWC.16900018Q"><span>Prompt fission <span class="hlt">gamma</span>-ray emission spectral data for 239Pu(n,f) using fast directional neutrons from the LICORNE neutron source</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Qi, L.; Wilson, J. N.; Lebois, M.; Al-Adili, A.; Chatillon, A.; Choudhury, D.; Gatera, A.; Georgiev, G.; Göök, A.; Laurent, B.; Maj, A.; Matea, I.; Oberstedt, A.; Oberstedt, S.; Rose, S. J.; Schmitt, C.; Wasilewska, B.; Zeiser, F.</p> <p>2018-03-01</p> <p>Prompt fission <span class="hlt">gamma</span>-ray spectra (PFGS) have been measured for the 239Pu(n,f) reaction using fast neutrons at Ēn=1.81 MeV produced by the LICORNE directional neutron source. The setup makes use of LaBr3 scintillation detectors and PARIS phoswich detectors to measure the emitted prompt fission <span class="hlt">gamma</span> rays (PFG). The mean multiplicity, average total <span class="hlt">energy</span> <span class="hlt">release</span> per fission and average <span class="hlt">energy</span> of photons are extracted from the unfolded PFGS. These new measurements provide complementary information to other recent work on thermal neutron induced fission of 239Pu and spontaneous fission of 252Cf.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1990AIPC..211..200H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1990AIPC..211..200H"><span>New drift chamber technology for high <span class="hlt">energy</span> <span class="hlt">gamma</span>-ray telescopes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hunter, Stanley D.; Cuddapah, Rajani</p> <p>1990-08-01</p> <p>Work to develop a low-power amplifier and discriminator for use on space qualifiable drift chambers is discussed. Consideration is given to the goals of the next generation of high-<span class="hlt">energy</span> <span class="hlt">gamma</span>-ray telescope design and to how the goals can be achieved using xenon gas drift chambers. The design and construction of a low power drift chamber amplifier and discriminator are described, and the design of a quad-time-to-amplitude converter is outlined.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25811252','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25811252"><span>Normalization of <span class="hlt">energy</span>-dependent <span class="hlt">gamma</span> survey data.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Whicker, Randy; Chambers, Douglas</p> <p>2015-05-01</p> <p>Instruments and methods for normalization of <span class="hlt">energy</span>-dependent <span class="hlt">gamma</span> radiation survey data to a less <span class="hlt">energy</span>-dependent basis of measurement are evaluated based on relevant field data collected at 15 different sites across the western United States along with a site in Mongolia. Normalization performance is assessed relative to measurements with a high-pressure ionization chamber (HPIC) due to its "flat" <span class="hlt">energy</span> response and accurate measurement of the true exposure rate from both cosmic and terrestrial radiation. While analytically ideal for normalization applications, cost and practicality disadvantages have increased demand for alternatives to the HPIC. Regression analysis on paired measurements between <span class="hlt">energy</span>-dependent sodium iodide (NaI) scintillation detectors (5-cm by 5-cm crystal dimensions) and the HPIC revealed highly consistent relationships among sites not previously impacted by radiological contamination (natural sites). A resulting generalized data normalization factor based on the average sensitivity of NaI detectors to naturally occurring terrestrial radiation (0.56 nGy hHPIC per nGy hNaI), combined with the calculated site-specific estimate of cosmic radiation, produced reasonably accurate predictions of HPIC readings at natural sites. Normalization against two to potential alternative instruments (a tissue-equivalent plastic scintillator and <span class="hlt">energy</span>-compensated NaI detector) did not perform better than the sensitivity adjustment approach at natural sites. Each approach produced unreliable estimates of HPIC readings at radiologically impacted sites, though normalization against the plastic scintillator or <span class="hlt">energy</span>-compensated NaI detector can address incompatibilities between different <span class="hlt">energy</span>-dependent instruments with respect to estimation of soil radionuclide levels. The appropriate data normalization method depends on the nature of the site, expected duration of the project, survey objectives, and considerations of cost and practicality.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20050131831','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20050131831"><span>Observation and Simulations of the Backsplash Effects in High-<span class="hlt">Energy</span> <span class="hlt">Gamma</span>-Ray Telescopes Containing a Massive Calorimeter</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Moiseev, Alexander A.; Ormes, Jonathan F.; Hartman, Robert C.; Johnson, Thomas E.; Mitchell, John W.; Thompson, David J.</p> <p>1999-01-01</p> <p>Beam test and simulation results are presented for a study of the backsplash effects produced in a high-<span class="hlt">energy</span> <span class="hlt">gamma</span>-ray detector containing a massive calorimeter. An empirical formula is developed to estimate the probability (per unit area) of backsplash for different calorimeter materials and thicknesses, different incident particle <span class="hlt">energies</span>, and at different distances from the calorimeter. The results obtained are applied to the design of Anti-Coincidence Detector (ACD) for the Large Area Telescope (LAT) on the <span class="hlt">Gamma</span>-ray Large Area Space Telescope (GLAST).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19730057131&hterms=whales&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3Dwhales','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19730057131&hterms=whales&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3Dwhales"><span>Geophysical disturbance environment during the NASA/MPE barium <span class="hlt">release</span> at 5 earth radii on September 21, 1971.</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Davis, T. N.; Stanley, G. M.; Boyd, J. S.</p> <p>1973-01-01</p> <p>The geophysical disturbance environment was quiet during the NASA/MPE barium <span class="hlt">release</span> at 5 earth radii on September 21, 1971. At the time of the <span class="hlt">release</span>, the magnetosphere was in the late recovery phase of a principal magnetic storm, the provisional Dst value was -13 <span class="hlt">gammas</span>, and the local horizontal disturbance at Great Whale River was near zero. Riometer and other observations indicated low-level widespread precipitation of high-<span class="hlt">energy</span> electrons at Great Whale River before, during, and after the <span class="hlt">release</span>. Cloudy sky at this station prevented optical observation of aurora. No magnetic or ionospheric effects attributable to the barium <span class="hlt">release</span> were detected at Great Whale River.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19850027613','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19850027613"><span>Lateral distribution of high <span class="hlt">energy</span> hadrons and <span class="hlt">gamma</span> ray in air shower cores observed with emulsion chambers</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Matano, T.; Machida, M.; Kawasumi, N.; Tsushima, I.; Honda, K.; Hashimoto, K.; Navia, C. E.; Matinic, N.; Aquirre, C.</p> <p>1985-01-01</p> <p>A high <span class="hlt">energy</span> event of a bundle of electrons, <span class="hlt">gamma</span> rays and hadronic <span class="hlt">gamma</span> rays in an air shower core were observed. The bundles were detected with an emulsion chamber with thickness of 15 cm lead. This air shower is estimated to be initiated with a proton with <span class="hlt">energy</span> around 10 to the 17th power to 10 to the 18th power eV at an altitude of around 100 gmc/2. Lateral distributions of the electromagnetic component with <span class="hlt">energy</span> above 2 TeV and also the hadronic component of <span class="hlt">energy</span> above 6 TeV of this air shower core were determined. Particles in the bundle are produced with process of the development of the nuclear cascade, the primary <span class="hlt">energy</span> of each interaction in the cascade which produces these particles is unknown. To know the primary <span class="hlt">energy</span> dependence of transverse momentum, the average products of <span class="hlt">energy</span> and distance for various average <span class="hlt">energies</span> of secondary particles are studied.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010SPIE.7732E..22B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010SPIE.7732E..22B"><span>A fast scintillator Compton telescope for medium-<span class="hlt">energy</span> <span class="hlt">gamma</span>-ray astronomy</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bloser, Peter F.; Ryan, James M.; Legere, Jason S.; Julien, Manuel; Bancroft, Christopher M.; McConnell, Mark L.; Wallace, Mark; Kippen, R. Marc; Tornga, Shawn</p> <p>2010-07-01</p> <p>The field of medium-<span class="hlt">energy</span> <span class="hlt">gamma</span>-ray astronomy urgently needs a new mission to build on the success of the COMPTEL instrument on the Compton <span class="hlt">Gamma</span> Ray Observatory. This mission must achieve sensitivity significantly greater than that of COMPTEL in order to advance the science of relativistic particle accelerators, nuclear astrophysics, and diffuse backgrounds, and bridge the gap between current and future hard X-ray missions and the high-<span class="hlt">energy</span> Fermi mission. Such an increase in sensitivity can only come about via a dramatic decrease in the instrumental background. We are currently developing a concept for a low-background Compton telescope that employs modern scintillator technology to achieve this increase in sensitivity. Specifically, by employing LaBr3 scintillators for the calorimeter, one can take advantage of the unique speed and resolving power of this material to improve the instrument sensitivity while simultaneously enhancing its spectroscopic and imaging performance. Also, using deuterated organic scintillator in the scattering detector will reduce internal background from neutron capture. We present calibration results from a laboratory prototype of such an instrument, including time-of-flight, <span class="hlt">energy</span>, and angular resolution, and compare them to simulation results using a detailed Monte Carlo model. We also describe the balloon payload we have built for a test flight of the instrument in the fall of 2010.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/21301372-derivation-relation-steepening-tev-selected-blazar-gamma-ray-spectra-energy-redshift','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/21301372-derivation-relation-steepening-tev-selected-blazar-gamma-ray-spectra-energy-redshift"><span>DERIVATION OF A RELATION FOR THE STEEPENING OF TeV-SELECTED BLAZAR {<span class="hlt">gamma</span>}-RAY SPECTRA WITH <span class="hlt">ENERGY</span> AND REDSHIFT</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Stecker, Floyd William; Scully, Sean T.</p> <p>2010-02-01</p> <p>We derive a relation for the steepening of blazar {<span class="hlt">gamma</span>}-ray spectra between the multi-GeV Fermi <span class="hlt">energy</span> range and the TeV <span class="hlt">energy</span> range observed by atmospheric Cerenkov telescopes. The change in spectral index is produced by two effects: (1) an intrinsic steepening, independent of redshift, owing to the properties of emission and absorption in the source and (2) a redshift-dependent steepening produced by intergalactic pair production interactions of blazar {<span class="hlt">gamma</span>}-rays with low-<span class="hlt">energy</span> photons of the 'intergalactic background light' (IBL). Given this relation, with good enough data on the mean {<span class="hlt">gamma</span>}-ray spectral <span class="hlt">energy</span> distribution of TeV-selected BL Lac objects, the redshift evolutionmore » of the IBL can, in principle, be determined independently of stellar evolution models. We apply our relation to the results of new Fermi observations of TeV-selected blazars.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19930071236&hterms=Good+Reasons&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3DGood%2BReasons','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19930071236&hterms=Good+Reasons&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3DGood%2BReasons"><span>Observation of high-<span class="hlt">energy</span> <span class="hlt">gamma</span> rays from the quasi-stellar object CTA 102</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Nolan, P. L.; Bertsch, D. L.; Fichtel, C. E.; Hartman, R. C.; Hunter, S. D.; Kanbach, G.; Kniffen, D. A.; Lin, Y. C.; Mattox, J. R.; Mayer-Hasselwander, H. A.</p> <p>1993-01-01</p> <p>The quasar CTA 102 (QSO 2230 + 114) was observed four times in 1991-1992 by the EGRET high-<span class="hlt">energy</span> <span class="hlt">gamma</span>-ray telescope on the Compton GRO satellite. In the 1992 January 23-February 6 observation, emission was detected at the level (2.4 +/- 0.5) x 10 exp 7 photons/sq cm s (E is greater than 100 MeV). The other observations produced upper limits or detections with lower significance which are consistent with the same flux. The photon spectrum can be represented by a power law with a number index of 2.6 +/- 0.2, the softest so far observed by EGRET. The emitted <span class="hlt">gamma</span>-ray luminosity, if isotropic, is 5 x 10 exp 47 ergs/s (H(0) = 75 km/s Mpc , q(0) = 0.5), although there are good reasons to believe that the <span class="hlt">gamma</span> emission is strongly beamed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017APS..DPPNM9008D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017APS..DPPNM9008D"><span><span class="hlt">Gamma</span> beams generation with high intensity lasers for two photon Breit-Wheeler pair production</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>D'Humieres, Emmanuel; Ribeyre, Xavier; Jansen, Oliver; Esnault, Leo; Jequier, Sophie; Dubois, Jean-Luc; Hulin, Sebastien; Tikhonchuk, Vladimir; Arefiev, Alex; Toncian, Toma; Sentoku, Yasuhiko</p> <p>2017-10-01</p> <p>Linear Breit-Wheeler pair creation is the lowest threshold process in photon-photon interaction, controlling the <span class="hlt">energy</span> <span class="hlt">release</span> in <span class="hlt">Gamma</span> Ray Bursts and Active Galactic Nuclei, but it has never been directly observed in the laboratory. Using numerical simulations, we demonstrate the possibility to produce collimated <span class="hlt">gamma</span> beams with high <span class="hlt">energy</span> conversion efficiency using high intensity lasers and innovative targets. When two of these beams collide at particular angles, our analytical calculations demonstrate a beaming effect easing the detection of the pairs in the laboratory. This effect has been confirmed in photon collision simulations using a recently developed innovative algorithm. An alternative scheme using Bremsstrahlung radiation produced by next generation high repetition rate laser systems is also being explored and the results of first optimization campaigns in this regime will be presented.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20030105664','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20030105664"><span>A Concept for a High-<span class="hlt">Energy</span> <span class="hlt">Gamma</span>-ray Polarimeter</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Bloser, P. F.; Hunter, S. D.; Depaola, G. O.; Longo, F.</p> <p>2003-01-01</p> <p>We present a concept for an imaging <span class="hlt">gamma</span>-ray polarimeter operating from approx. 50 MeV to approx. 1 GeV. Such an instrument would be valuable for the study of high-<span class="hlt">energy</span> pulsars, active galactic nuclei, supernova remnants, and <span class="hlt">gamma</span>-ray bursts. The concept makes use of pixelized gas micro-well detectors, under development at Goddard Space Flight Center, to record the electron-positron tracks from pair-production events in a large gas volume. Pixelized micro-well detectors have the potential to form large-volume 3-D track imagers with approx. 100 micron (rms) position resolution at moderate cost. The combination of high spatial resolution and a continuous low-density gas medium permits many thousands of measurements per radiation length, allowing the particle tracks to be imaged accurately before multiple scattering masks their original directions. The polarization of the incoming radiation may then be determined from the azimuthal distribution of the electron-positron pairs. We have performed Geant4 simulations of these processes to estimate the polarization sensitivity as a function of instrument parameters and event selection criteria.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JInst..12P7001R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JInst..12P7001R"><span>Characterization of high density SiPM non-linearity and <span class="hlt">energy</span> resolution for prompt <span class="hlt">gamma</span> imaging applications</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Regazzoni, V.; Acerbi, F.; Cozzi, G.; Ferri, A.; Fiorini, C.; Paternoster, G.; Piemonte, C.; Rucatti, D.; Zappalà, G.; Zorzi, N.; Gola, A.</p> <p>2017-07-01</p> <p>Fondazione Bruno Kessler (FBK) (Trento, Italy) has recently introduced High Density (HD) and Ultra High-Density (UHD) SiPMs, featuring very small micro-cell pitch. The high cell density is a very important factor to improve the linearity of the SiPM in high-dynamic-range applications, such as the scintillation light readout in high-<span class="hlt">energy</span> <span class="hlt">gamma</span>-ray spectroscopy and in prompt <span class="hlt">gamma</span> imaging for proton therapy. The <span class="hlt">energy</span> resolution at high <span class="hlt">energies</span> is a trade-off between the excess noise factor caused by the non-linearity of the SiPM and the photon detection efficiency of the detector. To study these effects, we developed a new setup that simulates the LYSO light emission in response to <span class="hlt">gamma</span> photons up to 30 MeV, using a pulsed light source. We measured the non-linearity and <span class="hlt">energy</span> resolution vs. <span class="hlt">energy</span> of the FBK RGB-HD e RGB-UHD SiPM technologies. We considered five different cell sizes, ranging from 10 μm up to 25 μm. With the UHD technology we were able to observe a remarkable reduction of the SiPM non-linearity, less than 5% at 5 MeV with 10 μm cells, which should be compared to a non-linearity of 50% with 25 μm-cell HD-SiPMs. With the same setup, we also measured the different components of the <span class="hlt">energy</span> resolution (intrinsic, statistical, detector and electronic noise) vs. cell size, over-voltage and <span class="hlt">energy</span> and we separated the different sources of excess noise factor.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/674811','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/674811"><span>Laboratory laser acceleration and high <span class="hlt">energy</span> astrophysics: {<span class="hlt">gamma</span>}-ray bursts and cosmic rays</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Tajima, T.; Takahashi, Y.</p> <p>1998-08-20</p> <p>Recent experimental progress in laser acceleration of charged particles (electrons) and its associated processes has shown that intense electromagnetic pulses can promptly accelerate charged particles to high <span class="hlt">energies</span> and that their <span class="hlt">energy</span> spectrum is quite hard. On the other hand some of the high <span class="hlt">energy</span> astrophysical phenomena such as extremely high <span class="hlt">energy</span> cosmic rays and energetic components of {<span class="hlt">gamma</span>}-ray bursts cry for new physical mechanisms for promptly accelerating particles to high <span class="hlt">energies</span>. The authors suggest that the basic physics involved in laser acceleration experiments sheds light on some of the underlying mechanisms and their <span class="hlt">energy</span> spectral characteristics of the promptlymore » accelerated particles in these high <span class="hlt">energy</span> astrophysical phenomena.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19950036455&hterms=discovery+pulsar&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Ddiscovery%2Bpulsar','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19950036455&hterms=discovery+pulsar&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Ddiscovery%2Bpulsar"><span>EGRET upper limits to the high-<span class="hlt">energy</span> <span class="hlt">gamma</span>-ray emission from the millisecond pulsars in nearby globular clusters</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Michelson, P. F.; Bertsch, D. L.; Brazier, K.; Chiang, J.; Dingus, B. L.; Fichtel, C. E.; Fierro, J.; Hartman, R. C.; Hunter, S. D.; Kanbach, G.</p> <p>1994-01-01</p> <p>We report upper limits to the high-<span class="hlt">energy</span> <span class="hlt">gamma</span>-ray emission from the millisecond pulsars (MSPs) in a number of globular clusters. The observations were done as part of an all-sky survey by the energetic <span class="hlt">Gamma</span> Ray Experiment Telescope (EGRET) on the Compton <span class="hlt">Gamma</span> Ray Observatory (CGRO) during Phase I of the CGRO mission (1991 June to 1992 November). Several theoretical models suggest that MSPs may be sources of high-<span class="hlt">energy</span> <span class="hlt">gamma</span> radiation emitted either as primary radiation from the pulsar magnetosphere or as secondary radiation generated by conversion into photons of a substantial part of the relativistic e(+/-) pair wind expected to flow from the pulsar. To date, no high-<span class="hlt">energy</span> emission has been detected from an individual MSP. However, a large number of MSPs are expected in globular cluster cores where the formation rate of accreting binary systems is high. Model predictions of the total number of pulsars range in the hundreds for some clusters. These expectations have been reinforced by recent discoveries of a substantial number of radio MSPs in several clusters; for example, 11 have been found in 47 Tucanae (Manchester et al.). The EGRET observations have been used to obtain upper limits for the efficiency eta of conversion of MSP spin-down power into hard <span class="hlt">gamma</span> rays. The upper limits are also compared with the <span class="hlt">gamma</span>-ray fluxes predicted from theoretical models of pulsar wind emission (Tavani). The EGRET limits put significant constraints on either the emission models or the number of pulsars in the globular clusters.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20110014211','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20110014211"><span>Highlights of GeV <span class="hlt">Gamma</span>-Ray Astronomy</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Thompson, David J.</p> <p>2010-01-01</p> <p>Because high-<span class="hlt">energy</span> <span class="hlt">gamma</span> rays are primarily produced by high-<span class="hlt">energy</span> particle interactions, the <span class="hlt">gamma</span>-ray survey of the sky by the Fermi <span class="hlt">Gamma</span>-ray Space Telescope offers a view of sites of cosmic ray production and interactions. <span class="hlt">Gamma</span>-ray bursts, pulsars, pulsar wind nebulae, binary sources, and Active Galactic Nuclei are all phenomena that reveal particle acceleration through their <span class="hlt">gamma</span>-ray emission. Diffuse Galactic <span class="hlt">gamma</span> radiation, Solar System <span class="hlt">gamma</span>-ray sources, and energetic radiation from supernova remnants are likely tracers of high-<span class="hlt">energy</span> particle interactions with matter and photon fields. This paper will present a broad overview of the constantly changing sky seen with the Large Area Telescope (LAT) on the Fermi spacecraft.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20020050368&hterms=sources+energy&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dsources%2Benergy','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20020050368&hterms=sources+energy&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dsources%2Benergy"><span>The BATSE Earth Occultation Catalog of Low <span class="hlt">Energy</span> <span class="hlt">Gamma</span> Ray Sources</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Harmon, B. A.; Wilson-Hodge, C. A.; Fishman, G. J.; Paciesas, W. S.; Zhang, S. N.; Finger, M. H.; Connaughton, V.; Koshut, T. M.; Henze, W.; McCollough, M. L.; <a style="text-decoration: none; " href="javascript:void(0); " onClick="displayelement('author_20020050368'); toggleEditAbsImage('author_20020050368_show'); toggleEditAbsImage('author_20020050368_hide'); "> <img style="display:inline; width:12px; height:12px; " src="images/arrow-up.gif" width="12" height="12" border="0" alt="hide" id="author_20020050368_show"> <img style="width:12px; height:12px; display:none; " src="images/arrow-down.gif" width="12" height="12" border="0" alt="hide" id="author_20020050368_hide"></p> <p>2002-01-01</p> <p>The Burst and Transient Source Experiment (BATSE), aboard the Compton <span class="hlt">Gamma</span> Ray Observatory (CGRO), provided a record of the hard X-ray/low <span class="hlt">energy</span> <span class="hlt">gamma</span> ray sky between April 1991 and June 2000. During that time, a catalog of known sources was derived from existing catalogs such as HEAO A-4 (Levine et al. 1984), as well as new transient sources discovered with BATSE and other X-ray monitors operating in the CGRO era. The Earth Occultation Technique (Harmon et al. 2001, astro-ph/0109069) was used to monitor a combination of these sources, mostly galactic, totaling to about 175 objects. The catalog will present the global properties of these sources and their probability of detection (greater than 10 mCrab, 20-100 keV) with BATSE. Systematic errors due to unknown sources or background components are included. Cursory analyses to search for new transients (35-80 mCrab in the 20-100 keV band) and super-orbital periods in known binary sources are also presented. Whole mission light curves and associated data production/analysis tools are being delivered to the High <span class="hlt">Energy</span> Astrophysics Science Archive Research Center (HEASARC) for public use.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20040082144','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20040082144"><span><span class="hlt">Gamma</span> Ray Pulsars: Multiwavelength Observations</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Thompson, David J.</p> <p>2004-01-01</p> <p>High-<span class="hlt">energy</span> <span class="hlt">gamma</span> rays are a valuable tool for studying particle acceleration and radiation in the magnetospheres of energetic pulsars. The seven or more pulsars seen by instruments on the Compton <span class="hlt">Gamma</span> Ray Observatory (CGRO) show that: the light curves usually have double-peak structures (suggesting a broad cone of emission); <span class="hlt">gamma</span> rays are frequently the dominant component of the radiated power; and all the spectra show evidence of a high-<span class="hlt">energy</span> turnover. For all the known <span class="hlt">gamma</span>-ray pulsars, multiwavelength observations and theoretical models based on such observations offer the prospect of gaining a broad understanding of these rotating neutron stars. The <span class="hlt">Gamma</span>-ray Large Area Space Telescope (GLAST), now in planning for a launch in 2006, will provide a major advance in sensitivity, <span class="hlt">energy</span> range, and sky coverage.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017ASPC..510..289P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017ASPC..510..289P"><span>Flare <span class="hlt">Energy</span> <span class="hlt">Release</span>: Internal Conflict, Contradiction with High Resolution Observations, Possible Solutions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pustilnik, L.</p> <p>2017-06-01</p> <p>All accepted paradigm of solar and stellar flares <span class="hlt">energy</span> <span class="hlt">release</span> based on 2 whales: 1. Source of <span class="hlt">energy</span> is free <span class="hlt">energy</span> of non-potential force free magnetic field in atmosphere above active region; 2. Process of ultrafast dissipation of magnetic fields is Reconnection in Thin Turbulent Current Sheet (RTTCS). Progress in observational techniques in last years provided ultra-high spatial resolution and in physics of turbulent plasma showed that real situation is much more complicated and standard approach is in contradiction both with observations and with problem of RTTCS stability. We present critical analysis of classic models of pre-flare <span class="hlt">energy</span> accumulation and its dissipation during flare <span class="hlt">energy</span> <span class="hlt">release</span> from pioneer works Giovanelli (1939, 1947) up to topological reconnection. We show that all accepted description of global force-free fields as source of future flare cannot be agreed with discovered in last years fine and ultra-fine current-magnetic structure included numerouse arcs-threads with diameters up to 100 km with constant sequence from photosphere to corona. This magnetic skeleton of thin current magnetic threads with strong interaction between them is main source of reserved magnetic <span class="hlt">energy</span> insolar atmosphere. Its dynamics will be controlled by percolation of magnetic stresses through network of current-magnetic threads with transition to flare state caused by critical value of global current. We show that thin turbulent current sheet is absolutely unstable configuration both caused by splitting to numerous linear currents by dissipative modes like to tearing, and as sequence of suppress of plasma turbulence caused by anomalous heating of turbulent plasma. In result of these factors primary RTTCS will be disrupted in numerous turbulent and normal plasma domains like to resistors network. Current propagation through this network will have percolation character with all accompanied properties of percolated systems: self-organization with formation power</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19870045631&hterms=Andromeda&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3DAndromeda','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19870045631&hterms=Andromeda&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3DAndromeda"><span>The Andromeda galaxy in <span class="hlt">gamma</span>-rays</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Oezel, M. E.; Berkhuijsen, E. M.</p> <p>1987-01-01</p> <p>Implications of high-<span class="hlt">energy</span> <span class="hlt">gamma</span>-ray observations of the Andromeda galaxy with the next generation of satellites <span class="hlt">Gamma</span>-1 and GRO are discussed in the context of the origin of cosmic rays and <span class="hlt">gamma</span>-ray processes. The present estimate of the total <span class="hlt">gamma</span>-ray flux of this galaxy at <span class="hlt">energies</span> above 100 MeV is a factor of about three less than previous estimates.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19770035709&hterms=Magnetic+energy&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3DMagnetic%2Benergy','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19770035709&hterms=Magnetic+energy&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3DMagnetic%2Benergy"><span><span class="hlt">Energy</span> <span class="hlt">released</span> by the interaction of coronal magnetic fields</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Sheeley, N. R., Jr.</p> <p>1976-01-01</p> <p>Comparisons between coronal spectroheliograms and photospheric magnetograms are presented to support the idea that as coronal magnetic fields interact, a process of field-line reconnection usually takes place as a natural way of preventing magnetic stresses from building up in the lower corona. This suggests that the <span class="hlt">energy</span> which would have been stored in stressed fields is continuously <span class="hlt">released</span> as kinetic <span class="hlt">energy</span> of material being driven aside to make way for the reconnecting fields. However, this kinetic <span class="hlt">energy</span> is negligible compared with the thermal <span class="hlt">energy</span> of the coronal plasma. Therefore, it appears that these slow adjustments of coronal magnetic fields cannot account for even the normal heating of the corona, much less the energetic events associated with solar flares.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li class="active"><span>14</span></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_14 --> <div id="page_15" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li class="active"><span>15</span></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="281"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19860062113&hterms=Quark&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3DQuark','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19860062113&hterms=Quark&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3DQuark"><span>Workshop on Cosmic Ray and High <span class="hlt">Energy</span> <span class="hlt">Gamma</span> Ray Experiments for the Space Station Era, Louisiana State University, Baton Rouge, October 17-20, 1984, Proceedings</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Jones, W. V. (Editor); Wefel, J. P. (Editor)</p> <p>1985-01-01</p> <p>The potential of the Space Station as a platform for cosmic-ray and high-<span class="hlt">energy</span> <span class="hlt">gamma</span>-ray astronomy is discussed in reviews, reports, and specific proposals. Topics examined include antiparticles and electrons, science facilities and new technology, high-<span class="hlt">energy</span> nuclear interactions, nuclear composition and <span class="hlt">energy</span> spectra, Space Shuttle experiments, Space Station facilities and detectors, high-<span class="hlt">energy</span> <span class="hlt">gamma</span> rays, and <span class="hlt">gamma</span>-ray facilities and techniques. Consideration is given to universal-baryon-symmetry testing on the scale of galactic clusters, particle studies in a high-inclination orbit, balloon-borne emulsion-chamber results on ultrarelativistic nucleus-nucleus interactions, ionization states of low-<span class="hlt">energy</span> cosmic rays, a large <span class="hlt">gamma</span>-ray telescope for point-source studies above 1 GeV, and the possible existence of stable quark matter.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19910057868&hterms=nolan&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3Dnolan','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19910057868&hterms=nolan&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3Dnolan"><span>The estimation of background production by cosmic rays in high-<span class="hlt">energy</span> <span class="hlt">gamma</span> ray telescopes</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Edwards, H. L.; Nolan, P. L.; Lin, Y. C.; Koch, D. G.; Bertsch, D. L.; Fichtel, C. E.; Hartman, R. C.; Hunter, S. D.; Kniffen, D. A.; Hughes, E. B.</p> <p>1991-01-01</p> <p>A calculational method of estimating instrumental background in high-<span class="hlt">energy</span> <span class="hlt">gamma</span>-ray telescopes, using the hadronic Monte Carlo code FLUKA87, is presented. The method is applied to the SAS-2 and EGRET telescope designs and is also used to explore the level of background to be expected for alternative configurations of the proposed GRITS telescope, which adapts the external fuel tank of a Space Shuttle as a <span class="hlt">gamma</span>-ray telescope with a very large collecting area. The background produced in proton-beam tests of EGRET is much less than the predicted level. This discrepancy appears to be due to the FLUKA87 inability to transport evaporation nucleons. It is predicted that the background in EGRET will be no more than 4-10 percent of the extragalactic diffuse <span class="hlt">gamma</span> radiation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19810004448','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19810004448"><span>Future prospects for <span class="hlt">gamma</span>-ray</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Fichtel, C.</p> <p>1980-01-01</p> <p>Astrophysical phenomena discussed are: the very energetic and nuclear processes associated with compact objects; astrophysical nucleo-synthesis; solar particle acceleration; the chemical composition of the planets and other bodies of the solar system; the structure of our galaxy; the origin and dynamic pressure effects of the cosmic rays; the high <span class="hlt">energy</span> particles and energetic processes in other galaxies, especially active ones; and the degree of matter antimater symmetry of the universe. The <span class="hlt">gamma</span> ray results of <span class="hlt">GAMMA</span>-I, the <span class="hlt">gamma</span> ray observatory, the <span class="hlt">gamma</span> ray burst network, solar polar, and very high <span class="hlt">energy</span> <span class="hlt">gamma</span> ray telescopes on the ground provide justification for more sophisticated telescopes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=1917440','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=1917440"><span>Development of tolerance to the effects of vigabatrin (<span class="hlt">gamma</span>-vinyl-GABA) on GABA <span class="hlt">release</span> from rat cerebral cortex, spinal cord and retina.</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Neal, M. J.; Shah, M. A.</p> <p>1990-01-01</p> <p>1. The effects of acute and chronic vigabatrin (<span class="hlt">gamma</span>-vinyl-GABA) (GVG) administration on <span class="hlt">gamma</span>-aminobutyric acid (GABA) levels and <span class="hlt">release</span> in rat cortical slices, spinal cord slices and retinas were studied. 2. GVG (250 mgkg-1 i.p.) administered to rats 18 h before death (acute administration) produced an almost 3 fold increase in GABA levels of the cortex and spinal cord and a 6 fold increase in retinal GABA. The levels of glutamate, aspartate, glycine and taurine were unaffected. 3. When GVG (250 mgkg-1 i.p.) was administered daily for 17 days (chronic administration) a similar (almost 3 fold) increase in cortical GABA occurred but the increases in spinal and retinal GABA were reduced by approximately 40%. 4. Acute administration of GVG strikingly increased the potassium-evoked <span class="hlt">release</span> (KCl 50 mM) of GABA from all three tissues. This enhanced evoked <span class="hlt">release</span> was reduced by about 50% in tissues taken from rats that had been chronically treated with GVG. 5. Acute administration of GVG reduced GABA-transaminase (GABA-T) activity by approximately 80% in cortex and cord and by 98% in the retina. Following the chronic administration of GVG, there was a trend for GABA-T activities to recover (significant only in cortex). Acute administration of GVG had no effect on glutamic acid decarboxylase (GAD) activity in cortex or spinal cord. However, chronic treatment resulted in significant decreases in GAD activity in both the cortex and cord (35% and 50% reduction respectively).(ABSTRACT TRUNCATED AT 250 WORDS) PMID:2379037</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19990028425','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19990028425"><span>Intergalactic Extinction of High <span class="hlt">Energy</span> <span class="hlt">Gamma</span>-Rays</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Stecker, F. W.</p> <p>1998-01-01</p> <p>We discuss the determination of the intergalactic pair-production absorption coefficient as derived by Stecker and De Jager by making use of a new empirically based calculation of the spectral <span class="hlt">energy</span> distribution of the intergalactic infrared radiation field as given by Malkan and Stecker. We show that the results of the Malkan and Stecker calculation agree well with recent data on the infrared background. We then show that Whipple observations of the flaring <span class="hlt">gamma</span>-ray spectrum of Mrk 421 hint at extragalactic absorption and that the HEGRA observations of the flaring spectrum of Mrk 501 appear to strongly indicate extragalactic absorption. We also discuss the determination of the y-ray opacity at higher redshifts, following the treatment of Salamon and Stecker. We give a predicted spectrum, with absorption included for PKS 2155-304. This XBL lies at a redshift of 0.12, the highest redshift source yet observed at an <span class="hlt">energy</span> above 0.3 TeV. This source should have its spectrum steepened by approx. 1 in its spectral index between approx. 0.3 and approx. 3 TeV and should show an absorption cutoff above approx. 6 TeV.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JAP...123i5703E','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JAP...123i5703E"><span><span class="hlt">Gamma</span> non-ionizing <span class="hlt">energy</span> loss: Comparison with the damage factor in silicon devices</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>El Allam, E.; Inguimbert, C.; Meulenberg, A.; Jorio, A.; Zorkani, I.</p> <p>2018-03-01</p> <p>The concept of non-ionizing <span class="hlt">energy</span> loss (NIEL) has been demonstrated to be a successful approach to describe the displacement damage effects in silicon materials and devices. However, some discrepancies exist in the literature between experimental damage factors and theoretical NIELs. 60Co <span class="hlt">gamma</span> rays having a low NIEL are an interesting particle source that can be used to validate the NIEL scaling approach. This paper presents different 60Co <span class="hlt">gamma</span> ray NIEL values for silicon targets. They are compared with the radiation-induced increase in the thermal generation rate of carriers per unit fluence. The differences between the different models, including one using molecular dynamics, are discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/22745740','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/22745740"><span>Blast shock wave mitigation using the hydraulic <span class="hlt">energy</span> redirection and <span class="hlt">release</span> technology.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Chen, Yun; Huang, Wei; Constantini, Shlomi</p> <p>2012-01-01</p> <p>A hydraulic <span class="hlt">energy</span> redirection and <span class="hlt">release</span> technology has been developed for mitigating the effects of blast shock waves on protected objects. The technology employs a liquid-filled plastic tubing as a blast overpressure transformer to transfer kinetic <span class="hlt">energy</span> of blast shock waves into hydraulic <span class="hlt">energy</span> in the plastic tubings. The hydraulic <span class="hlt">energy</span> is redirected through the plastic tubings to the openings at the lower ends, and then is quickly <span class="hlt">released</span> with the liquid flowing out through the openings. The samples of the specifically designed body armor in which the liquid-filled plastic tubings were installed vertically as the outer layer of the body armor were tested. The blast test results demonstrated that blast overpressure behind the body armor samples was remarkably reduced by 97% in 0.2 msec after the liquid flowed out of its appropriate volume through the openings. The results also suggested that a volumetric liquid surge might be created when kinetic <span class="hlt">energy</span> of blast shock wave was transferred into hydraulic <span class="hlt">energy</span> to cause a rapid physical movement or displacement of the liquid. The volumetric liquid surge has a strong destructive power, and can cause a noncontact, remote injury in humans (such as blast-induced traumatic brain injury and post-traumatic stress disorder) if it is created in cardiovascular system. The hydraulic <span class="hlt">energy</span> redirection and <span class="hlt">release</span> technology can successfully mitigate blast shock waves from the outer surface of the body armor. It should be further explored as an innovative approach to effectively protect against blast threats to civilian and military personnel.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3379975','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3379975"><span>Blast Shock Wave Mitigation Using the Hydraulic <span class="hlt">Energy</span> Redirection and <span class="hlt">Release</span> Technology</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Chen, Yun; Huang, Wei; Constantini, Shlomi</p> <p>2012-01-01</p> <p>A hydraulic <span class="hlt">energy</span> redirection and <span class="hlt">release</span> technology has been developed for mitigating the effects of blast shock waves on protected objects. The technology employs a liquid-filled plastic tubing as a blast overpressure transformer to transfer kinetic <span class="hlt">energy</span> of blast shock waves into hydraulic <span class="hlt">energy</span> in the plastic tubings. The hydraulic <span class="hlt">energy</span> is redirected through the plastic tubings to the openings at the lower ends, and then is quickly <span class="hlt">released</span> with the liquid flowing out through the openings. The samples of the specifically designed body armor in which the liquid-filled plastic tubings were installed vertically as the outer layer of the body armor were tested. The blast test results demonstrated that blast overpressure behind the body armor samples was remarkably reduced by 97% in 0.2 msec after the liquid flowed out of its appropriate volume through the openings. The results also suggested that a volumetric liquid surge might be created when kinetic <span class="hlt">energy</span> of blast shock wave was transferred into hydraulic <span class="hlt">energy</span> to cause a rapid physical movement or displacement of the liquid. The volumetric liquid surge has a strong destructive power, and can cause a noncontact, remote injury in humans (such as blast-induced traumatic brain injury and post-traumatic stress disorder) if it is created in cardiovascular system. The hydraulic <span class="hlt">energy</span> redirection and <span class="hlt">release</span> technology can successfully mitigate blast shock waves from the outer surface of the body armor. It should be further explored as an innovative approach to effectively protect against blast threats to civilian and military personnel. PMID:22745740</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017APS..MARH16003I','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017APS..MARH16003I"><span>Unleashing elastic <span class="hlt">energy</span>: dynamics of <span class="hlt">energy</span> <span class="hlt">release</span> in rubber bands and impulsive biological systems</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ilton, Mark; Cox, Suzanne; Egelmeers, Thijs; Patek, S. N.; Crosby, Alfred J.</p> <p></p> <p>Impulsive biological systems - which include mantis shrimp, trap-jaw ants, and venus fly traps - can reach high speeds by using elastic elements to store and rapidly <span class="hlt">release</span> <span class="hlt">energy</span>. The material behavior and shape changes critical to achieving rapid <span class="hlt">energy</span> <span class="hlt">release</span> in these systems are largely unknown due to limitations of materials testing instruments operating at high speed and large displacement. In this work, we perform fundamental, proof-of-concept measurements on the tensile retraction of elastomers. Using high speed imaging, the kinematics of retraction are measured for elastomers with varying mechanical properties and geometry. Based on the kinematics, the rate of <span class="hlt">energy</span> dissipation in the material is determined as a function of strain and strain-rate, along with a scaling relation which describes the dependence of maximum velocity on material properties. Understanding this scaling relation along with the material failure limits of the elastomer allows the prediction of material properties required for optimal performance. We demonstrate this concept experimentally by optimizing for maximum velocity in our synthetic model system, and achieve retraction velocities that exceed those in biological impulsive systems. This model system provides a foundation for future work connecting continuum performance to molecular architecture in impulsive systems.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19870011944','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19870011944"><span>Convergence of strain <span class="hlt">energy</span> <span class="hlt">release</span> rate components for edge-delaminated composite laminates</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Raju, I. S.; Crews, J. H., Jr.; Aminpour, M. A.</p> <p>1987-01-01</p> <p>Strain <span class="hlt">energy</span> <span class="hlt">release</span> rates for edge delaminated composite laminates were obtained using quasi 3 dimensional finite element analysis. The problem of edge delamination at the -35/90 interfaces of an 8-ply composite laminate subjected to uniform axial strain was studied. The individual components of the strain <span class="hlt">energy</span> <span class="hlt">release</span> rates did not show convergence as the delamination tip elements were made smaller. In contrast, the total strain <span class="hlt">energy</span> <span class="hlt">release</span> rate converged and remained unchanged as the delamination tip elements were made smaller and agreed with that calculated using a classical laminated plate theory. The studies of the near field solutions for a delamination at an interface between two dissimilar isotropic or orthotropic plates showed that the imaginary part of the singularity is the cause of the nonconvergent behavior of the individual components. To evaluate the accuracy of the results, an 8-ply laminate with the delamination modeled in a thin resin layer, that exists between the -35 and 90 plies, was analyzed. Because the delamination exists in a homogeneous isotropic material, the oscillatory component of the singularity vanishes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/9000670','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/9000670"><span>Role of polymorphic Fc receptor Fc <span class="hlt">gamma</span>RIIa in cytokine <span class="hlt">release</span> and adverse effects of murine IgG1 anti-CD3/T cell receptor antibody (WT31).</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Tax, W J; Tamboer, W P; Jacobs, C W; Frenken, L A; Koene, R A</p> <p>1997-01-15</p> <p>Anti-CD3 monoclonal antibody (mAb) OKT3 is immunosuppressive, but causes severe adverse effects during the first administration ("first-dose reaction"). These adverse effects are presumably caused by cytokine <span class="hlt">release</span> that results from T-cell activation. In vitro, T-cell activation by anti-CD3 mAb requires interaction with monocyte Fc receptors. The Fc receptor for murine IgG1, Fc <span class="hlt">gamma</span>RIIa, is polymorphic. In some individuals, murine IgG1 anti-CD3 mAb causes T-cell proliferation and cytokine <span class="hlt">release</span> in vitro (high responders [HR]), whereas in individuals with the low-responder (LR) phenotype it does not. We have now investigated the role of this Fc <span class="hlt">gamma</span>RIIa polymorphism in the <span class="hlt">release</span> of cytokines in vivo and the occurrence of adverse effects after the administration of WT31, a murine IgG1 anti-CD3/T cell receptor mAb. WT31 caused an increase of plasma tumor necrosis factor-alpha in all four HR patients and none of the five LR patients. In all HR patients except one, plasma <span class="hlt">gamma</span>-interferon and interleukin 6 also increased, and a first-dose response was observed, whereas no cytokine <span class="hlt">release</span> or adverse effects occurred in any of the LR patients. WT31 caused lymphopenia in all HR and none of the LR patients. FACS analysis demonstrated that in HR patients, after the initial disappearance of CD3+ cells from peripheral blood, modulation of CD3 occurred, whereas in LR patients a high degree of coating of the lymphocytes was observed. Surprisingly, WT31 also induced a marked granulocytopenia, as well as a decrease of thrombocytes, in three of the four HR patients (and in none of the LR patients). These data provide direct clinical evidence that Fc receptor interaction determines the <span class="hlt">release</span> of cytokines and the occurrence of adverse effects after administration of anti-CD3/T cell receptor mAb. Furthermore, these data suggest that tumor necrosis factor-alpha by itself is not sufficient to induce the first-dose reaction.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018NIMPA.893..109C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018NIMPA.893..109C"><span>A <span class="hlt">gamma</span> beam profile imager for ELI-NP <span class="hlt">Gamma</span> Beam System</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Cardarelli, P.; Paternò, G.; Di Domenico, G.; Consoli, E.; Marziani, M.; Andreotti, M.; Evangelisti, F.; Squerzanti, S.; Gambaccini, M.; Albergo, S.; Cappello, G.; Tricomi, A.; Veltri, M.; Adriani, O.; Borgheresi, R.; Graziani, G.; Passaleva, G.; Serban, A.; Starodubtsev, O.; Variola, A.; Palumbo, L.</p> <p>2018-06-01</p> <p>The <span class="hlt">Gamma</span> Beam System of ELI-Nuclear Physics is a high brilliance monochromatic <span class="hlt">gamma</span> source based on the inverse Compton interaction between an intense high power laser and a bright electron beam with tunable <span class="hlt">energy</span>. The source, currently being assembled in Magurele (Romania), is designed to provide a beam with tunable average <span class="hlt">energy</span> ranging from 0.2 to 19.5 MeV, rms <span class="hlt">energy</span> bandwidth down to 0.5% and flux of about 108 photons/s. The system includes a set of detectors for the diagnostic and complete characterization of the <span class="hlt">gamma</span> beam. To evaluate the spatial distribution of the beam a <span class="hlt">gamma</span> beam profile imager is required. For this purpose, a detector based on a scintillator target coupled to a CCD camera was designed and a prototype was tested at INFN-Ferrara laboratories. A set of analytical calculations and Monte Carlo simulations were carried out to optimize the imager design and evaluate the performance expected with ELI-NP <span class="hlt">gamma</span> beam. In this work the design of the imager is described in detail, as well as the simulation tools used and the results obtained. The simulation parameters were tuned and cross-checked with the experimental measurements carried out on the assembled prototype using the beam from an x-ray tube.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AIPC.1792b0003B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AIPC.1792b0003B"><span>High <span class="hlt">energy</span> neutrinos and <span class="hlt">gamma</span>-ray emission from supernovae in compact star clusters</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bykov, A. M.; Ellison, D. C.; Gladilin, P. E.; Osipov, S. M.</p> <p>2017-01-01</p> <p>Compact clusters of young massive stars are observed in the Milky Way and in starburst galaxies. The compact clusters with multiple powerful winds of young massive stars and supernova shocks are favorable sites for high-<span class="hlt">energy</span> particle acceleration. We argue that expanding young supernova (SN) shells in compact stellar clusters can be very efficient PeV CR accelerators. At a stage when a supernova shock is colliding with collective fast winds from massive stars in a compact cluster the Fermi mechanism allows particle acceleration to <span class="hlt">energies</span> well above the standard limits of diffusive shock acceleration in an isolated SNR. The <span class="hlt">energy</span> spectrum of protons in such an accelerator is a hard power-law with a broad spectral upturn above TeV before a break at multi-PeV <span class="hlt">energies</span>, providing a large <span class="hlt">energy</span> flux in the high-<span class="hlt">energy</span> end of the spectrum. The acceleration stage in the colliding shock flow lasts for a few hundred years after the supernova explosion producing high-<span class="hlt">energy</span> CRs that escape the accelerator and diffuse through the ambient matter producing γ-rays and neutrinos in inelastic nuclear collisions. In starburst galaxies a sizeable fraction of core collapse supernovae is expected to occur in compact star clusters and therefore their high <span class="hlt">energy</span> <span class="hlt">gamma</span>-ray and neutrino spectra in the PeV <span class="hlt">energy</span> regime may differ strongly from that of our Galaxy. To test the model with individual sources we briefly discuss the recent H.E.S.S. detections of <span class="hlt">gamma</span>-rays from two potential candidate sources, Westerlund 1 and HESS J1806-204 in the Milky Way. We argue that this model of compact star clusters, with typical parameters, could produce a neutrino flux sufficient to explain a fraction of the recently detected IceCube South Pole Observatory neutrinos.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017NuPhA.964...55N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017NuPhA.964...55N"><span>Updated level scheme of 172Yb from 171Yb(nth, γ) reaction studied via <span class="hlt">gamma-gamma</span> coincidence spectrometer</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Nguyen, Ngoc Anh; Nguyen, Xuan Hai; Pham, Dinh Khang; Nguyen, Quang Hung; Ho, Huu Thang</p> <p>2017-08-01</p> <p>This paper provides the updated information on the level scheme of 172Yb nucleus studied via 171Yb(nth, γ) reaction using the <span class="hlt">gamma-gamma</span> coincidence spectrometer at Dalat Nuclear Research Institute (Viet Nam). The latter is used because of its advantages in achieving the low Compton background as well as in identifying the correlated <span class="hlt">gamma</span> transitions. We have detected in total the <span class="hlt">energies</span> and intensities of 128 two-step <span class="hlt">gamma</span> cascades corresponding to 79 primary transitions. By comparing the measured data with those extracted from the ENSDF library, 61 primary <span class="hlt">gamma</span> transitions and corresponding <span class="hlt">energy</span> levels together with 20 secondary <span class="hlt">gamma</span> transitions are found to be the same as the ENSDF data. Beside that, 18 additional primary <span class="hlt">gamma</span> transitions and corresponding <span class="hlt">energy</span> levels plus 108 secondary ones are not found to currently exist in this library and they are therefore considered as the new data.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20130013643','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20130013643"><span>Status of the <span class="hlt">GAMMA</span>-400 Project</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Galper, A. M.; Adriani, O.; Aptekar, R. L.; Arkhangelskaja, I. V.; Arkhangelskiy, A. I.; Boezio, M.; Bonvicini, V.; Boyarchuk, K. A.; Gusakov, Yu. V.; Farber, M. O.; <a style="text-decoration: none; " href="javascript:void(0); " onClick="displayelement('author_20130013643'); toggleEditAbsImage('author_20130013643_show'); toggleEditAbsImage('author_20130013643_hide'); "> <img style="display:inline; width:12px; height:12px; " src="images/arrow-up.gif" width="12" height="12" border="0" alt="hide" id="author_20130013643_show"> <img style="width:12px; height:12px; display:none; " src="images/arrow-down.gif" width="12" height="12" border="0" alt="hide" id="author_20130013643_hide"></p> <p>2013-01-01</p> <p>The preliminary design of the new space <span class="hlt">gamma</span>-ray telescope <span class="hlt">GAMMA</span>-400 for the <span class="hlt">energy</span> range 100 MeV-3 TeV is presented. The angular resolution of the instrument, 1-2 deg at E(<span class="hlt">gamma</span>) approximately 100 MeV and approximately 0.01 at E(<span class="hlt">gamma</span>) greater than 100 GeV, its <span class="hlt">energy</span> resolution is approximately 1% at E(<span class="hlt">gamma</span>) greater than 100 GeV, and the proton rejection factor is approximately 10(exp 6) are optimized to address a broad range of science topics, such as search for signatures of dark matter, studies of Galactic and extragalactic <span class="hlt">gamma</span>-ray sources, Galactic and extragalactic diffuse emission, <span class="hlt">gamma</span>-ray bursts, as well as high-precision measurements of spectra of cosmic-ray electrons, positrons, and nuclei.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/19034939','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/19034939"><span>Environmentally friendly <span class="hlt">gamma</span>-MnO2 hexagon-based nanoarchitectures: structural understanding and their <span class="hlt">energy</span>-saving applications.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Wu, Changzheng; Xie, Wei; Zhang, Miao; Bai, Liangfei; Yang, Jinlong; Xie, Yi</p> <p>2009-01-01</p> <p>Although about 200,000 metric tons of <span class="hlt">gamma</span>-MnO(2) are used annually worldwide for industrial applications, the <span class="hlt">gamma</span>-MnO(2) structure is still known to possess a highly ambiguous crystal lattice. To better understand the <span class="hlt">gamma</span>-MnO(2) atomic structure, hexagon-based nanoarchitectures were successfully synthesized and used to elucidate its internal structure for the present work. The structural analysis results, obtained from the hexagon-based nanoarchitectures, clearly show the coexistence of akhtenskite (epsilon-MnO(2)), pyrolusite (beta-MnO(2)), and ramsdellite in the so-called <span class="hlt">gamma</span>-MnO(2) phase and verified the heterogeneous phase assembly of the <span class="hlt">gamma</span>-MnO(2) state, which violates the well-known "De Wolff" model and derivative models, but partially accords with Heuer's results. Furthermore, heterogeneous <span class="hlt">gamma</span>-MnO(2) assembly was found to be a metastable structure under hydrothermal conditions, and the individual components of the heterogeneous <span class="hlt">gamma</span>-MnO(2) system have structural similarities and a high lattice matches with pyrolusite (beta-MnO(2)). The as-obtained <span class="hlt">gamma</span>-MnO(2) nanoarchitectures are nontoxic and environmentally friendly, and the application of such nanoarchitectures as support matrices successfully mitigates the common problems for phase-change materials of inorganic salts, such as phase separation and supercooling-effects, thereby showing prospect in <span class="hlt">energy</span>-saving applications in future "smart-house" systems.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/20861408-limits-high-energy-gamma-neutrino-fluxes-from-sgr-giant-flare-december-amanda-ii-detector','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/20861408-limits-high-energy-gamma-neutrino-fluxes-from-sgr-giant-flare-december-amanda-ii-detector"><span>Limits on the High-<span class="hlt">Energy</span> <span class="hlt">Gamma</span> and Neutrino Fluxes from the SGR 1806-20 Giant Flare of 27 December 2004 with the AMANDA-II Detector</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Achterberg, A.; Duvoort, M. R.; Heise, J.</p> <p>2006-12-01</p> <p>On 27 December 2004, a giant {<span class="hlt">gamma</span>} flare from the Soft <span class="hlt">Gamma</span>-Ray Repeater 1806-20 saturated many satellite <span class="hlt">gamma</span>-ray detectors, being the brightest transient event ever observed in the Galaxy. AMANDA-II was used to search for down-going muons indicative of high-<span class="hlt">energy</span> <span class="hlt">gammas</span> and/or neutrinos from this object. The data revealed no significant signal, so upper limits (at 90% C.L.) on the normalization constant were set: 0.05(0.5) TeV{sup -1} m{sup -2} s{sup -1} for {<span class="hlt">gamma</span>}=-1.47 (-2) in the <span class="hlt">gamma</span> flux and 0.4(6.1) TeV{sup -1} m{sup -2} s{sup -1} for {<span class="hlt">gamma</span>}=-1.47 (-2) in the high-<span class="hlt">energy</span> neutrino flux.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20120015940','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20120015940"><span>The Impact of Electromagnetic Cascades of Very-high <span class="hlt">Energy</span> <span class="hlt">Gamma</span> Rays on the Extragalactic <span class="hlt">Gamma</span>-ray Background</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Venters, Tonia</p> <p>2012-01-01</p> <p>As very high <span class="hlt">energy</span> (VHE) photons propagate through the extragalactic background light (EBL), they interact with the soft photons of the EBL and initiate electromagnetic cascades of photons and electrons. The collective intensity of a cosmological population emitting at VHEs (such as blazars) will be attenuated at the highest <span class="hlt">energies</span> through interactions with the EBL and enhanced at lower <span class="hlt">energies</span> by the resulting cascade. As such, depending on the space density and spectra of the sources and the model of the EBL, cascade radiation can provide a significant contribution to the extragalactic <span class="hlt">gamma</span>-ray background (EGB). Through deflections of the charged particles of the cascade, an intergalactic magnetic field (IGMF) may leave an imprint on the anisotropy properties of the EGB. The impact of a strong IGMF is to isotropize lower <span class="hlt">energy</span> cascade photons, inducing a modulation in the anisotropy <span class="hlt">energy</span> spectrum of the EGB. We discuss the implications of cascade radiation for the origins of the EGB and the nature of the IGMF, as well as insight that will be provided by data from the Fermi Large Area Telescope in the upcoming years.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017A%26A...602A..98A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017A%26A...602A..98A"><span>Very-high-<span class="hlt">energy</span> <span class="hlt">gamma</span>-ray observations of the Type Ia Supernova SN 2014J with the MAGIC telescopes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ahnen, M. L.; Ansoldi, S.; Antonelli, L. A.; Antoranz, P.; Arcaro, C.; Babic, A.; Banerjee, B.; Bangale, P.; Barres de Almeida, U.; Barrio, J. A.; Becerra González, J.; Bednarek, W.; Bernardini, E.; Berti, A.; Biasuzzi, B.; Biland, A.; Blanch, O.; Bonnefoy, S.; Bonnoli, G.; Borracci, F.; Bretz, T.; Carosi, R.; Carosi, A.; Chatterjee, A.; Colin, P.; Colombo, E.; Contreras, J. L.; Cortina, J.; Covino, S.; Cumani, P.; Da Vela, P.; Dazzi, F.; De Angelis, A.; De Lotto, B.; de Oña Wilhelmi, E.; Di Pierro, F.; Doert, M.; Domínguez, A.; Dominis Prester, D.; Dorner, D.; Doro, M.; Einecke, S.; Eisenacher Glawion, D.; Elsaesser, D.; Engelkemeier, M.; Fallah Ramazani, V.; Fernández-Barral, A.; Fidalgo, D.; Fonseca, M. V.; Font, L.; Frantzen, K.; Fruck, C.; Galindo, D.; García López, R. J.; Garczarczyk, M.; Garrido Terrats, D.; Gaug, M.; Giammaria, P.; Godinović, N.; Gora, D.; Guberman, D.; Hadasch, D.; Hahn, A.; Hayashida, M.; Herrera, J.; Hose, J.; Hrupec, D.; Hughes, G.; Idec, W.; Kodani, K.; Konno, Y.; Kubo, H.; Kushida, J.; La Barbera, A.; Lelas, D.; Lindfors, E.; Lombardi, S.; Longo, F.; López, M.; López-Coto, R.; Majumdar, P.; Makariev, M.; Mallot, K.; Maneva, G.; Manganaro, M.; Mannheim, K.; Maraschi, L.; Marcote, B.; Mariotti, M.; Martínez, M.; Mazin, D.; Menzel, U.; Miranda, J. M.; Mirzoyan, R.; Moralejo, A.; Moretti, E.; Nakajima, D.; Neustroev, V.; Niedzwiecki, A.; Nievas Rosillo, M.; Nilsson, K.; Nishijima, K.; Noda, K.; Nogués, L.; Paiano, S.; Palacio, J.; Palatiello, M.; Paneque, D.; Paoletti, R.; Paredes, J. M.; Paredes-Fortuny, X.; Pedaletti, G.; Peresano, M.; Perri, L.; Persic, M.; Poutanen, J.; Prada Moroni, P. G.; Prandini, E.; Puljak, I.; Garcia, J. R.; Reichardt, I.; Rhode, W.; Ribó, M.; Rico, J.; Saito, T.; Satalecka, K.; Schroeder, S.; Schweizer, T.; Sillanpää, A.; Sitarek, J.; Snidaric, I.; Sobczynska, D.; Stamerra, A.; Strzys, M.; Surić, T.; Takalo, L.; Tavecchio, F.; Temnikov, P.; Terzić, T.; Tescaro, D.; Teshima, M.; Torres, D. F.; Toyama, T.; Treves, A.; Vanzo, G.; Vazquez Acosta, M.; Vovk, I.; Ward, J. E.; Will, M.; Wu, M. H.; Zanin, R.</p> <p>2017-06-01</p> <p>Context. In this work we present data from observations with the MAGIC telescopes of SN 2014J detected on January 21 2014, the closest Type Ia supernova since Imaging Air Cherenkov Telescopes started to operate. Aims: We aim to probe the possibility of very-high-<span class="hlt">energy</span> (VHE; E ≥ 100 GeV) <span class="hlt">gamma</span> rays produced in the early stages of Type Ia supernova explosions. Methods: We performed follow-up observations after this supernova (SN) explosion for five days, between January 27 and February 2 2014. We searched for <span class="hlt">gamma</span>-ray signals in the <span class="hlt">energy</span> range between 100 GeV and several TeV from the location of SN 2014J using data from a total of 5.5 h of observations. Prospects for observing <span class="hlt">gamma</span> rays of hadronic origin from SN 2014J in the near future are also being addressed. Results: No significant excess was detected from the direction of SN 2014J. Upper limits at 95% confidence level on the integral flux, assuming a power-law spectrum, dF/dE ∝ E- Γ, with a spectral index of Γ = 2.6, for <span class="hlt">energies</span> higher than 300 GeV and 700 GeV, are established at 1.3 × 10-12 and 4.1 × 10-13 photons cm-2 s-1, respectively. Conclusions: For the first time, upper limits on the VHE emission of a Type Ia supernova are established. The <span class="hlt">energy</span> fraction isotropically emitted into TeV <span class="hlt">gamma</span> rays during the first 10 days after the supernova explosion for <span class="hlt">energies</span> greater than 300 GeV is limited to 10-6 of the total available <span class="hlt">energy</span> budget ( 1051 erg). Within the assumed theoretical scenario, the MAGIC upper limits on the VHE emission suggest that SN 2014J will not be detectable in the future by any current or planned generation of Imaging Atmospheric Cherenkov Telescopes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19920054201&hterms=thomas+jenkins&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dthomas%2Bjenkins','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19920054201&hterms=thomas+jenkins&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dthomas%2Bjenkins"><span>Evaluation of the cosmic-ray induced background in coded aperture high <span class="hlt">energy</span> <span class="hlt">gamma</span>-ray telescopes</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Owens, Alan; Barbier, Loius M.; Frye, Glenn M.; Jenkins, Thomas L.</p> <p>1991-01-01</p> <p>While the application of coded-aperture techniques to high-<span class="hlt">energy</span> <span class="hlt">gamma</span>-ray astronomy offers potential arc-second angular resolution, concerns were raised about the level of secondary radiation produced in a thick high-z mask. A series of Monte-Carlo calculations are conducted to evaluate and quantify the cosmic-ray induced neutral particle background produced in a coded-aperture mask. It is shown that this component may be neglected, being at least a factor of 50 lower in intensity than the cosmic diffuse <span class="hlt">gamma</span>-rays.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li class="active"><span>15</span></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_15 --> <div id="page_16" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li class="active"><span>16</span></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="301"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1356715-constraining-high-energy-emission-from-gamma-ray-bursts-fermi','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1356715-constraining-high-energy-emission-from-gamma-ray-bursts-fermi"><span>Constraining the high-<span class="hlt">energy</span> emission from <span class="hlt">gamma</span>-ray bursts with Fermi</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Ackermann, M.; Ajello, M.; Baldini, L.; ...</p> <p>2012-07-17</p> <p>Here, we examine 288 <span class="hlt">gamma</span>-ray bursts (GRBs) detected by the Fermi <span class="hlt">Gamma</span>-ray Space Telescope's <span class="hlt">Gamma</span>-ray Burst Monitor (GBM) that fell within the field of view of Fermi's Large Area Telescope (LAT) during the first 2.5 years of observations, which showed no evidence for emission above 100 MeV. We report the photon flux upper limits in the 0.1-10 GeV range during the prompt emission phase as well as for fixed 30 s and 100 s integrations starting from the trigger time for each burst. We also compare these limits with the fluxes that would be expected from extrapolations of spectral fitsmore » presented in the first GBM spectral catalog and infer that roughly half of the GBM-detected bursts either require spectral breaks between the GBM and LAT <span class="hlt">energy</span> bands or have intrinsically steeper spectra above the peak of the νF ν spectra (E pk). In order to distinguish between these two scenarios, we perform joint GBM and LAT spectral fits to the 30 brightest GBM-detected bursts and find that a majority of these bursts are indeed softer above E pk than would be inferred from fitting the GBM data alone. Approximately 20% of this spectroscopic subsample show statistically significant evidence for a cutoff in their high-<span class="hlt">energy</span> spectra, which if assumed to be due to γγ attenuation, places limits on the maximum Lorentz factor associated with the relativistic outflow producing this emission. Furthermore, all of these latter bursts have maximum Lorentz factor estimates that are well below the minimum Lorentz factors calculated for LAT-detected GRBs, revealing a wide distribution in the bulk Lorentz factor of GRB outflows and indicating that LAT-detected bursts may represent the high end of this distribution.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012ApJ...754..121F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012ApJ...754..121F"><span>Constraining the High-<span class="hlt">energy</span> Emission from <span class="hlt">Gamma</span>-Ray Bursts with Fermi</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Fermi Large Area Telescope Team; Ackermann, M.; Ajello, M.; Baldini, L.; Barbiellini, G.; Baring, M. G.; Bechtol, K.; Bellazzini, R.; Blandford, R. D.; Bloom, E. D.; Bonamente, E.; Borgland, A. W.; Bottacini, E.; Bouvier, A.; Brigida, M.; Buehler, R.; Buson, S.; Caliandro, G. A.; Cameron, R. A.; Cecchi, C.; Charles, E.; Chekhtman, A.; Chiang, J.; Ciprini, S.; Claus, R.; Cohen-Tanugi, J.; Cutini, S.; D'Ammando, F.; de Palma, F.; Dermer, C. D.; Silva, E. do Couto e.; Drell, P. S.; Drlica-Wagner, A.; Favuzzi, C.; Fukazawa, Y.; Fusco, P.; Gargano, F.; Gasparrini, D.; Gehrels, N.; Germani, S.; Giglietto, N.; Giordano, F.; Giroletti, M.; Glanzman, T.; Granot, J.; Grenier, I. A.; Grove, J. E.; Hadasch, D.; Hanabata, Y.; Harding, A. K.; Hays, E.; Horan, D.; Jóhannesson, G.; Kataoka, J.; Knödlseder, J.; Kocevski, D.; Kuss, M.; Lande, J.; Longo, F.; Loparco, F.; Lovellette, M. N.; Lubrano, P.; Mazziotta, M. N.; McEnery, J.; McGlynn, S.; Michelson, P. F.; Mitthumsiri, W.; Monzani, M. E.; Moretti, E.; Morselli, A.; Moskalenko, I. V.; Murgia, S.; Naumann-Godo, M.; Norris, J. P.; Nuss, E.; Nymark, T.; Ohsugi, T.; Okumura, A.; Omodei, N.; Orlando, E.; Panetta, J. H.; Parent, D.; Pelassa, V.; Pesce-Rollins, M.; Piron, F.; Pivato, G.; Racusin, J. L.; Rainò, S.; Rando, R.; Razzaque, S.; Reimer, A.; Reimer, O.; Ritz, S.; Ryde, F.; Sgrò, C.; Siskind, E. J.; Sonbas, E.; Spandre, G.; Spinelli, P.; Stamatikos, M.; Stawarz, Łukasz; Suson, D. J.; Takahashi, H.; Tanaka, T.; Thayer, J. G.; Thayer, J. B.; Tibaldo, L.; Tinivella, M.; Tosti, G.; Uehara, T.; Vandenbroucke, J.; Vasileiou, V.; Vianello, G.; Vitale, V.; Waite, A. P.; Fermi Gamma-ray Burst Monitor Team; Connaughton, V.; Briggs, M. S.; Guirec, S.; Goldstein, A.; Burgess, J. M.; Bhat, P. N.; Bissaldi, E.; Camero-Arranz, A.; Fishman, J.; Fitzpatrick, G.; Foley, S.; Gruber, D.; Jenke, P.; Kippen, R. M.; Kouveliotou, C.; McBreen, S.; Meegan, C.; Paciesas, W. S.; Preece, R.; Rau, A.; Tierney, D.; van der Horst, A. J.; von Kienlin, A.; Wilson-Hodge, C.; Xiong, S.</p> <p>2012-08-01</p> <p>We examine 288 <span class="hlt">gamma</span>-ray bursts (GRBs) detected by the Fermi <span class="hlt">Gamma</span>-ray Space Telescope's <span class="hlt">Gamma</span>-ray Burst Monitor (GBM) that fell within the field of view of Fermi's Large Area Telescope (LAT) during the first 2.5 years of observations, which showed no evidence for emission above 100 MeV. We report the photon flux upper limits in the 0.1-10 GeV range during the prompt emission phase as well as for fixed 30 s and 100 s integrations starting from the trigger time for each burst. We compare these limits with the fluxes that would be expected from extrapolations of spectral fits presented in the first GBM spectral catalog and infer that roughly half of the GBM-detected bursts either require spectral breaks between the GBM and LAT <span class="hlt">energy</span> bands or have intrinsically steeper spectra above the peak of the νF ν spectra (E pk). In order to distinguish between these two scenarios, we perform joint GBM and LAT spectral fits to the 30 brightest GBM-detected bursts and find that a majority of these bursts are indeed softer above E pk than would be inferred from fitting the GBM data alone. Approximately 20% of this spectroscopic subsample show statistically significant evidence for a cutoff in their high-<span class="hlt">energy</span> spectra, which if assumed to be due to γγ attenuation, places limits on the maximum Lorentz factor associated with the relativistic outflow producing this emission. All of these latter bursts have maximum Lorentz factor estimates that are well below the minimum Lorentz factors calculated for LAT-detected GRBs, revealing a wide distribution in the bulk Lorentz factor of GRB outflows and indicating that LAT-detected bursts may represent the high end of this distribution.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/FR-2013-09-16/pdf/2013-22554.pdf','FEDREG'); return false;" href="https://www.gpo.gov/fdsys/pkg/FR-2013-09-16/pdf/2013-22554.pdf"><span>78 FR 56977 - Axcess International, Inc., <span class="hlt">Gamma</span> Pharmaceuticals, Inc., Innovex, Inc, Knight <span class="hlt">Energy</span> Corp...</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collection.action?collectionCode=FR">Federal Register 2010, 2011, 2012, 2013, 2014</a></p> <p></p> <p>2013-09-16</p> <p>... SECURITIES AND EXCHANGE COMMISSION [File No. 500-1] Axcess International, Inc., <span class="hlt">Gamma</span> Pharmaceuticals, Inc., Innovex, Inc, Knight <span class="hlt">Energy</span> Corp., Komodo, Inc., Uphonia, Inc., and Wilson Brothers USA, Inc., Order of Suspension of Trading September 12, 2013. It appears to the Securities and Exchange...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19740006352','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19740006352"><span><span class="hlt">Gamma</span>-ray astrophysics</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Stecker, F. W. (Editor); Trombka, J. I. (Editor)</p> <p>1973-01-01</p> <p>Conference papers on <span class="hlt">gamma</span> ray astrophysics are summarized. Data cover the <span class="hlt">energy</span> region from about 0.3 MeV to a few hundred GeV and theoretical models of production mechanisms that give rise to both galactic and extragalactic <span class="hlt">gamma</span> rays.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20040074235&hterms=energy+solar&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Denergy%2Bsolar','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20040074235&hterms=energy+solar&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Denergy%2Bsolar"><span>Solar Flares Observed with the Ramaty High <span class="hlt">Energy</span> Solar Spectroscopic Imager (RHESSI)</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Holman, Gordon D.</p> <p>2004-01-01</p> <p>Solar flares are impressive examples of explosive <span class="hlt">energy</span> <span class="hlt">release</span> in unconfined, magnetized plasma. It is generally believed that the flare <span class="hlt">energy</span> is derived from the coronal magnetic field. However, we have not been able to establish the specific <span class="hlt">energy</span> <span class="hlt">release</span> mechanism(s) or the relative partitioning of the <span class="hlt">released</span> <span class="hlt">energy</span> between heating, particle acceleration (electrons and ions), and mass motions. NASA's RHESSI Mission was designed to study the acceleration and evolution of electrons and ions in flares by observing the X-ray and <span class="hlt">gamma</span>-ray emissions these energetic particles produce. This is accomplished through the combination of high-resolution spectroscopy and spectroscopic imaging, including the first images of flares in <span class="hlt">gamma</span> rays. RHESSI has observed over 12,000 solar flares since its launch on February 5, 2002. I will demonstrate how we use the RHESSI spectra to deduce physical properties of accelerated electrons and hot plasma in flares. Using images to estimate volumes, w e typically find that the total <span class="hlt">energy</span> in accelerated electrons is comparable to that in the thermal plasma. I will also present flare observations that provide strong support for the presence of magnetic reconnection in a large-scale, vertical current sheet in the solar corona. RHESSI observations such as these are allowing us to probe more deeply into the physics of solar flares.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1352006','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1352006"><span>Measurements of the $$\\mathrm{ pp \\to W \\<span class="hlt">gamma\\gamma</span> }$$ and $$\\mathrm{ pp \\to Z \\<span class="hlt">gamma\\gamma</span> }$$ cross sections and limits on anomalous quartic gauge couplings at $$\\sqrt{s} =$$ 8 TeV</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Sirunyan, A. M.; Tumasyan, A.; Adam, W.</p> <p></p> <p>Here, measurements are presented ofmore » $$ \\mathrm{ W \\<span class="hlt">gamma\\gamma</span> } $$ and $$ \\mathrm{ Z \\<span class="hlt">gamma\\gamma</span> } $$ production in proton-proton collisions. Fiducial cross sections are reported based on a data sample corresponding to an integrated luminosity of 19.4 fb$$^{-1}$$ collected with the CMS detector at a center-of-mass <span class="hlt">energy</span> of 8 TeV. Signal is identified through the $$\\mathrm{ W } \\to \\ell\</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1352006-measurements-mathrm-pp-gamma-gamma-mathrm-pp-gamma-gamma-cross-sections-limits-anomalous-quartic-gauge-couplings-sqrt-tev','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1352006-measurements-mathrm-pp-gamma-gamma-mathrm-pp-gamma-gamma-cross-sections-limits-anomalous-quartic-gauge-couplings-sqrt-tev"><span>Measurements of the $$\\mathrm{ pp \\to W \\<span class="hlt">gamma\\gamma</span> }$$ and $$\\mathrm{ pp \\to Z \\<span class="hlt">gamma\\gamma</span> }$$ cross sections and limits on anomalous quartic gauge couplings at $$\\sqrt{s} =$$ 8 TeV</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Sirunyan, A. M.; Tumasyan, A.; Adam, W.; ...</p> <p>2017-10-11</p> <p>Here, measurements are presented ofmore » $$ \\mathrm{ W \\<span class="hlt">gamma\\gamma</span> } $$ and $$ \\mathrm{ Z \\<span class="hlt">gamma\\gamma</span> } $$ production in proton-proton collisions. Fiducial cross sections are reported based on a data sample corresponding to an integrated luminosity of 19.4 fb$$^{-1}$$ collected with the CMS detector at a center-of-mass <span class="hlt">energy</span> of 8 TeV. Signal is identified through the $$\\mathrm{ W } \\to \\ell\</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009EGUGA..11.2323R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009EGUGA..11.2323R"><span>Influence of LOD variations on seismic <span class="hlt">energy</span> <span class="hlt">release</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Riguzzi, F.; Krumm, F.; Wang, K.; Kiszely, M.; Varga, P.</p> <p>2009-04-01</p> <p>Tidal friction causes significant time variations of geodynamical parameters, among them geometrical flattening. The axial despinning of the Earth due to tidal friction through the change of flattening generates incremental meridional and azimuthal stresses. The stress pattern in an incompressible elastic upper mantle and crust is symmetric to the equator and has its inflection points at the critical latitude close to ±45°. Consequently the distribution of seismic <span class="hlt">energy</span> <span class="hlt">released</span> by strong, shallow focus earthquakes should have also sharp maxima at this latitude. To investigate the influence of length of day (LOD) variations on earthquake activity an earthquake catalogue of strongest seismic events (M>7.0) was completed for the period 1900-2007. It is shown with the use of this catalogue that for the studied time-interval the catalogue is complete and consists of the seismic events responsible for more than 90% of <span class="hlt">released</span> seismic <span class="hlt">energy</span>. Study of the catalogue for earthquakes M>7.0 shows that the seismic <span class="hlt">energy</span> discharged by the strongest seismic events has significant maxima at ±45°, what renders probably that the seismic activity of our planet is influenced by an external component, i.e. by the tidal friction, which acts through the variation of the hydrostatic figure of the Earth caused by it. Distribution along the latitude of earthquake numbers and <span class="hlt">energies</span> was investigated also for the case of global linear tectonic structures, such as mid ocean ridges and subduction zones. It can be shown that the number of the shallow focus shocks has a repartition along the latitude similar to the distribution of the linear tectonic structures. This means that the position of foci of seismic events is mainly controlled by the tectonic activity.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018AAS...23135549C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018AAS...23135549C"><span>Exploring the particle nature of dark matter with the All-sky Medium <span class="hlt">Energy</span> <span class="hlt">Gamma</span>-ray Observatory (AMEGO)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Caputo, Regina; Meyer, Manuel; Sánchez-Conde, Miguel; AMEGO</p> <p>2018-01-01</p> <p>The era of precision cosmology has revealed that ~80% of the matter in the universe is dark matter. Two leading candidates, motivated by both particle and astrophysics, are Weakly Interacting Massive Particles (WIMPs) and Weakly Interacting Sub-eV Particles (WISPs) like axions and axionlike particles. Both WIMPs and WISPs have distinct <span class="hlt">gamma</span>-ray signatures. Data from the Fermi Large Area Telescope (Fermi-LAT) continues to be an integral part of the search for these dark matter signatures spanning the 50 MeV to >300 GeV <span class="hlt">energy</span> range in a variety of astrophysical targets. Thus far, there are no conclusive detections; however, there is an intriguing excess of <span class="hlt">gamma</span> rays associated with Galactic center (GCE) that could be explained with WIMP annihilation. The angular resolution of the LAT at lower <span class="hlt">energies</span> makes source selection challenging and the true nature of the detected signal remains unknown. WISP searches using, e.g. supernova explosions, spectra of blazars, or strongly magnetized environments, would also greatly benefit from increased angular and <span class="hlt">energy</span> resolution, as well as from polarization measurements. To address these, we are developing AMEGO, the All-sky Medium <span class="hlt">Energy</span> <span class="hlt">Gamma</span>-ray Observatory. This instrument has a projected <span class="hlt">energy</span> and angular resolution that will increase sensitivity by a factor of 20-50 over previous instruments. This will allow us to explore new areas of dark matter parameter space and provide unprecedented access to its particle nature.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20170003550&hterms=energy&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3Denergy','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20170003550&hterms=energy&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3Denergy"><span>Fermi-Lat Observations of High-<span class="hlt">Energy</span> <span class="hlt">Gamma</span>-Ray Emission Toward the Galactic Center</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Ajello, M.; Albert, A.; Atwood, W.B.; Barbiellini, G.; Bastieri, D.; Bechtol, K.; Bellazzini, R.; Bissaldi, E.; Blandford, R. D.; Brandt, T. J.; <a style="text-decoration: none; " href="javascript:void(0); " onClick="displayelement('author_20170003550'); toggleEditAbsImage('author_20170003550_show'); toggleEditAbsImage('author_20170003550_hide'); "> <img style="display:inline; width:12px; height:12px; " src="images/arrow-up.gif" width="12" height="12" border="0" alt="hide" id="author_20170003550_show"> <img style="width:12px; height:12px; display:none; " src="images/arrow-down.gif" width="12" height="12" border="0" alt="hide" id="author_20170003550_hide"></p> <p>2016-01-01</p> <p>The Fermi Large Area Telescope (LAT) has provided the most detailed view to date of the emission toward the Galactic center (GC) in high-<span class="hlt">energy</span> <span class="hlt">gamma</span>-rays. This paper describes the analysis of data taken during the first 62 months of the mission in the <span class="hlt">energy</span> range 1-100 GeV from a 15 degrees x 15 degrees region about the direction of the GC. Specialized interstellar emission models (IEMs) are constructed to enable the separation of the <span class="hlt">gamma</span>-ray emissions produced by cosmic ray particles interacting with the interstellar gas and radiation fields in the Milky Way into that from the inner 1 kpc surrounding the GC, and that from the rest of the Galaxy. A catalog of point sources for the 15 degrees x 15 degrees region is self-consistently constructed using these IEMs: the First Fermi-LAT Inner Galaxy Point SourceCatalog (1FIG). The spatial locations, fluxes, and spectral properties of the 1FIG sources are presented, and compared with <span class="hlt">gamma</span>-ray point sources over the same region taken from existing catalogs. After subtracting the interstellar emission and point-source contributions a residual is found. If templates that peak toward the GC areused to model the positive residual the agreement with the data improves, but none of the additional templates tried account for all of its spatial structure. The spectrum of the positive residual modeled with these templates has a strong dependence on the choice of IEM.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/19694638','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/19694638"><span>Effects of peritoneal fluid from endometriosis patients on interferon-<span class="hlt">gamma</span>-induced protein-10 (CXCL10) and interleukin-8 (CXCL8) <span class="hlt">released</span> by neutrophils and CD4+ T cells.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Kim, Ji-Yeon; Lee, Dong-Hyung; Joo, Jong-Kil; Jin, Jun-O; Wang, Ji-Won; Hong, Young-Seoub; Kwak, Jong-Young; Lee, Kyu-Sup</p> <p>2009-09-01</p> <p>Intraperitoneal immuno-inflammatory changes may be associated with the pathogenesis of endometriosis. We evaluated the effects of peritoneal fluid obtained from patients with endometriosis (ePF) on the <span class="hlt">release</span> of interferon-<span class="hlt">gamma</span>-induced protein-10 (IP-10/CXCL10) and interleukin-8 (IL-8/CXCL8) by neutrophils, CD4(+) T cells, and monocytes. Neutrophils, CD4(+) T cells, and monocytes were cultured with ePF and the chemokine levels in the supernatants were then measured using enzyme-linked immunosorbent assay. The addition of ePF to cultures of CD4(+) T cells led to a significant increase in the <span class="hlt">release</span> of IP-10 when compared with control PF without endometriosis (cPF). There was a positive correlation between the levels of IL-8 and IP-10 in ePF (R = 0.89, P = 0.041), but not between the levels of IP-10 and IL-8 <span class="hlt">released</span> by neutrophils, CD4(+) T cells, and monocytes. The levels of IP-10 in ePF were positively correlated with the <span class="hlt">release</span> of IP-10 by ePF-treated neutrophils (R = 0.89, P < 0.001), CD4(+) T cells (R = 0.93, P < 0.001), and monocytes (R = 0.70, P = 0.01). Moreover, the addition of ePF significantly enhanced the interferon-<span class="hlt">gamma</span>-induced <span class="hlt">release</span> of IP-10 by nuetrophils and CD4(+) T cells. These findings suggest that neutrophils and T cells <span class="hlt">release</span> differential levels of IP-10 and IL-8 in response to stimulation with ePF, and that these cells are a major source of IP-10 in the PF of endometriosis patients.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19930000879','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19930000879"><span><span class="hlt">Gamma</span> ray astrophysics to the year 2000. Report of the NASA <span class="hlt">Gamma</span> Ray Program Working Group</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p></p> <p>1988-01-01</p> <p>Important developments in <span class="hlt">gamma</span>-ray astrophysics up to <span class="hlt">energies</span> of 100 GeV during the last decade are reviewed. Also, the report seeks to define the major current scientific goals of the field and proposes a vigorous program to pursue them, extending to the year 2000. The goals of <span class="hlt">gamma</span>-ray astronomy include the study of <span class="hlt">gamma</span> rays which provide the most direct means of studying many important problems in high <span class="hlt">energy</span> astrophysics including explosive nucleosynthesis, accelerated particle interactions and sources, and high-<span class="hlt">energy</span> processes around compact objects. The current research program in <span class="hlt">gamma</span>-ray astronomy in the U.S. including the space program, balloon program and foreign programs in <span class="hlt">gamma</span>-ray astronomy is described. The high priority recommendations for future study include an Explorer-class high resolution <span class="hlt">gamma</span>-ray spectroscopy mission and a Get Away Special cannister (GAS-can) or Scout class multiwavelength experiment for the study of <span class="hlt">gamma</span>-ray bursts. Continuing programs include an extended <span class="hlt">Gamma</span> Ray Observatory mission, continuation of the vigorous program of balloon observations of the nearby Supernova 1987A, augmentation of the balloon program to provide for new instruments and rapid scientific results, and continuation of support for theoretical research. Long term recommendations include new space missions using advanced detectors to better study <span class="hlt">gamma</span>-ray sources, the development of these detectors, continued study for the assembly of large detectors in space, collaboration with the <span class="hlt">gamma</span>-ray astronomy missions initiated by other countries, and consideration of the Space Station attached payloads for <span class="hlt">gamma</span>-ray experiments.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMSH51E2616D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMSH51E2616D"><span>High-<span class="hlt">Energy</span> Solar Energetic Particles & Long Duration <span class="hlt">Gamma</span>-Ray Flares — Is there a Connection?</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>de Nolfo, G. A.; Boezio, M.; Bruno, A.; Christian, E. R.; Martucci, M.; Mergè, M.; Mocchiutti, E.; Munini, R.; Ricci, M.; Ryan, J. M.; Share, G. H.; Stochaj, S.</p> <p>2016-12-01</p> <p>Little is known about the origin of the high-<span class="hlt">energy</span> and sustained emission from Long Duration <span class="hlt">Gamma</span>-Ray Flares (LDGRFs), identified with Compton <span class="hlt">Gamma</span>-Ray Observatory (CGRO), the Solar Maximum Mission (SMM), and now Fermi. Though Fermi/LAT has identified dozens of flares with LDGRF emission, the nature of this emission has been a challenge to explain both due to the extreme <span class="hlt">energies</span> and long durations. The highest <span class="hlt">energy</span> emission has generally been attributed to pion production from the interaction of high-<span class="hlt">energy</span> protons with the ambient matter, suggesting that particle acceleration occurs over large volumes extending high in the corona, either from stochastic acceleration within large coronal loops or from back precipitation from CME-driven shocks. It is possible to test these models by making direct comparisons between the accelerated ion population at the flare derived from the observations of Fermi/LAT with PAMELA measurements of solar energetic particles in the <span class="hlt">energy</span> range corresponding to the pion-related emission observed with Fermi. For nine SEP events, we compare the two populations (SEPs in space and the interacting population at the Sun) and discuss the implications in terms of the contending theories for LDGF emission. On behalf of the PAMELA Collaboration</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/17411203','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/17411203"><span><span class="hlt">Gamma</span>-ray detection efficiency of the microchannel plate installed as an ion detector in the low <span class="hlt">energy</span> particle instrument onboard the GEOTAIL satellite.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Tanaka, Y T; Yoshikawa, I; Yoshioka, K; Terasawa, T; Saito, Y; Mukai, T</p> <p>2007-03-01</p> <p>A microchannel plate (MCP) assembly has been used as an ion detector in the low <span class="hlt">energy</span> particle (LEP) instrument onboard the magnetospheric satellite GEOTAIL. Recently the MCP assembly has detected <span class="hlt">gamma</span> rays emitted from an astronomical object and has been shown to provide unique information of <span class="hlt">gamma</span> rays if they are intense enough. However, the detection efficiency for <span class="hlt">gamma</span> rays was not measured before launch, and therefore we could not analyze the LEP data quantitatively. In this article, we report the <span class="hlt">gamma</span>-ray detection efficiency of the MCP assembly. The measured efficiencies are 1.29%+/-0.71% and 0.21%+/-0.14% for normal incidence 60 and 662 keV <span class="hlt">gamma</span> rays, respectively. The incident angle dependence is also presented. Our calibration is crucial to study high <span class="hlt">energy</span> astrophysical phenomena by using the LEP.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19910020966','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19910020966"><span>Residual thermal and moisture influences on the strain <span class="hlt">energy</span> <span class="hlt">release</span> rate analysis of local delaminations from matrix cracks</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Obrien, T. K.</p> <p>1991-01-01</p> <p>An analysis utilizing laminated plate theory is developed to calculate the strain <span class="hlt">energy</span> <span class="hlt">release</span> rate associated with local delaminations originating at off-axis, single ply, matrix cracks in laminates subjected to uniaxial loads. The analysis includes the contribution of residual thermal and moisture stresses to the strain <span class="hlt">energy</span> <span class="hlt">released</span>. Examples are calculated for the strain <span class="hlt">energy</span> <span class="hlt">release</span> rate associated with local delaminations originating at 90 degrees and angle-ply (non-90 degrees) matrix ply cracks in glass epoxy and graphite epoxy laminates. The solution developed may be used to assess the relative contribution of mechanical, residual thermal, and moisture stresses on the strain <span class="hlt">energy</span> <span class="hlt">release</span> rate for local delamination for a variety of layups and materials.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016JInst..1111009I','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016JInst..1111009I"><span>Very high-<span class="hlt">energy</span> <span class="hlt">gamma</span>-ray follow-up program using neutrino triggers from IceCube</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>IceCube Collaboration; Aartsen, M. G.; Abraham, K.; Ackermann, M.; Adams, J.; Aguilar, J. A.; Ahlers, M.; Ahrens, M.; Altmann, D.; Andeen, K.; Anderson, T.; Ansseau, I.; Anton, G.; Archinger, M.; Argüelles, C.; Auffenberg, J.; Axani, S.; Bai, X.; Barwick, S. W.; Baum, V.; Bay, R.; Beatty, J. J.; Becker Tjus, J.; Becker, K.-H.; BenZvi, S.; Berley, D.; Bernardini, E.; Bernhard, A.; Besson, D. Z.; Binder, G.; Bindig, D.; Bissok, M.; Blaufuss, E.; Blot, S.; Bohm, C.; Börner, M.; Bos, F.; Bose, D.; Böser, S.; Botner, O.; Braun, J.; Brayeur, L.; Bretz, H.-P.; Bron, S.; Burgman, A.; Carver, T.; Casier, M.; Cheung, E.; Chirkin, D.; Christov, A.; Clark, K.; Classen, L.; Coenders, S.; Collin, G. H.; Conrad, J. M.; Cowen, D. F.; Cross, R.; Day, M.; de André, J. P. A. M.; De Clercq, C.; del Pino Rosendo, E.; Dembinski, H.; De Ridder, S.; Desiati, P.; de Vries, K. D.; de Wasseige, G.; de With, M.; DeYoung, T.; Díaz-Vélez, J. C.; di Lorenzo, V.; Dujmovic, H.; Dumm, J. P.; Dunkman, M.; Eberhardt, B.; Ehrhardt, T.; Eichmann, B.; Eller, P.; Euler, S.; Evenson, P. A.; Fahey, S.; Fazely, A. R.; Feintzeig, J.; Felde, J.; Filimonov, K.; Finley, C.; Flis, S.; Fösig, C.-C.; Franckowiak, A.; Franke, R.; Friedman, E.; Fuchs, T.; Gaisser, T. K.; Gallagher, J.; Gerhardt, L.; Ghorbani, K.; Giang, W.; Gladstone, L.; Glauch, T.; Glüsenkamp, T.; Goldschmidt, A.; Golup, G.; Gonzalez, J. G.; Grant, D.; Griffith, Z.; Haack, C.; Haj Ismail, A.; Hallgren, A.; Halzen, F.; Hansen, E.; Hansmann, T.; Hanson, K.; Hebecker, D.; Heereman, D.; Helbing, K.; Hellauer, R.; Hickford, S.; Hignight, J.; Hill, G. C.; Hoffman, K. D.; Hoffmann, R.; Holzapfel, K.; Hoshina, K.; Huang, F.; Huber, M.; Hultqvist, K.; In, S.; Ishihara, A.; Jacobi, E.; Japaridze, G. S.; Jeong, M.; Jero, K.; Jones, B. J. P.; Jurkovic, M.; Kappes, A.; Karg, T.; Karle, A.; Katz, U.; Kauer, M.; Keivani, A.; Kelley, J. L.; Kheirandish, A.; Kim, M.; Kintscher, T.; Kiryluk, J.; Kittler, T.; Klein, S. R.; Kohnen, G.; Koirala, R.; Kolanoski, H.; Konietz, R.; Köpke, L.; Kopper, C.; Kopper, S.; Koskinen, D. J.; Kowalski, M.; Krings, K.; Kroll, M.; Krückl, G.; Krüger, C.; Kunnen, J.; Kunwar, S.; Kurahashi, N.; Kuwabara, T.; Labare, M.; Lanfranchi, J. L.; Larson, M. J.; Lauber, F.; Lennarz, D.; Lesiak-Bzdak, M.; Leuermann, M.; Lu, L.; Lünemann, J.; Madsen, J.; Maggi, G.; Mahn, K. B. M.; Mancina, S.; Mandelartz, M.; Maruyama, R.; Mase, K.; Maunu, R.; McNally, F.; Meagher, K.; Medici, M.; Meier, M.; Meli, A.; Menne, T.; Merino, G.; Meures, T.; Miarecki, S.; Mohrmann, L.; Montaruli, T.; Moulai, M.; Nahnhauer, R.; Naumann, U.; Neer, G.; Niederhausen, H.; Nowicki, S. C.; Nygren, D. R.; Obertacke Pollmann, A.; Olivas, A.; O'Murchadha, A.; Palczewski, T.; Pandya, H.; Pankova, D. V.; Peiffer, P.; Penek, Ö.; Pepper, J. A.; Pérez de los Heros, C.; Pieloth, D.; Pinat, E.; Price, P. B.; Przybylski, G. T.; Quinnan, M.; Raab, C.; Rädel, L.; Rameez, M.; Rawlins, K.; Reimann, R.; Relethford, B.; Relich, M.; Resconi, E.; Rhode, W.; Richman, M.; Riedel, B.; Robertson, S.; Rongen, M.; Rott, C.; Ruhe, T.; Ryckbosch, D.; Rysewyk, D.; Sabbatini, L.; Sanchez Herrera, S. E.; Sandrock, A.; Sandroos, J.; Sarkar, S.; Satalecka, K.; Schlunder, P.; Schmidt, T.; Schoenen, S.; Schöneberg, S.; Schumacher, L.; Seckel, D.; Seunarine, S.; Soldin, D.; Song, M.; Spiczak, G. M.; Spiering, C.; Stanev, T.; Stasik, A.; Stettner, J.; Steuer, A.; Stezelberger, T.; Stokstad, R. G.; Stößl, A.; Ström, R.; Strotjohann, N. L.; Sullivan, G. W.; Sutherland, M.; Taavola, H.; Taboada, I.; Tatar, J.; Tenholt, F.; Ter-Antonyan, S.; Terliuk, A.; Tešić, G.; Tilav, S.; Toale, P. A.; Tobin, M. N.; Toscano, S.; Tosi, D.; Tselengidou, M.; Turcati, A.; Unger, E.; Usner, M.; Vandenbroucke, J.; van Eijndhoven, N.; Vanheule, S.; van Rossem, M.; van Santen, J.; Veenkamp, J.; Vehring, M.; Voge, M.; Vogel, E.; Vraeghe, M.; Walck, C.; Wallace, A.; Wallraff, M.; Wandkowsky, N.; Weaver, Ch.; Weiss, M. J.; Wendt, C.; Westerhoff, S.; Whelan, B. J.; Wickmann, S.; Wiebe, K.; Wiebusch, C. H.; Wille, L.; Williams, D. R.; Wills, L.; Wolf, M.; Wood, T. R.; Woolsey, E.; Woschnagg, K.; Xu, D. L.; Xu, X. W.; Xu, Y.; Yanez, J. P.; Yodh, G.; Yoshida, S.; Zoll, M.; MAGIC Collaboration; Ahnen, M. L.; Ansoldi, S.; Antonelli, L. A.; Antoranz, P.; Babic, A.; Banerjee, B.; Bangale, P.; Barres de Almeida, U.; Barrio, J. A.; Becerra González, J.; Bednarek, W.; Bernardini, E.; Berti, A.; Biasuzzi, B.; Biland, A.; Blanch, O.; Bonnefoy, S.; Bonnoli, G.; Borracci, F.; Bretz, T.; Buson, S.; Carosi, A.; Chatterjee, A.; Clavero, R.; Colin, P.; Colombo, E.; Contreras, J. L.; Cortina, J.; Covino, S.; Da Vela, P.; Dazzi, F.; De Angelis, A.; De Lotto, B.; de Oña Wilhelmi, E.; Di Pierro, F.; Doert, M.; Domínguez, A.; Dominis Prester, D.; Dorner, D.; Doro, M.; Einecke, S.; Eisenacher Glawion, D.; Elsaesser, D.; Engelkemeier, M.; Fallah Ramazani, V.; Fernández-Barral, A.; Fidalgo, D.; Fonseca, M. V.; Font, L.; Frantzen, K.; Fruck, C.; Galindo, D.; García López, R. J.; Garczarczyk, M.; Garrido Terrats, D.; Gaug, M.; Giammaria, P.; Godinović, N.; González Muñoz, A.; Góra, D.; Guberman, D.; Hadasch, D.; Hahn, A.; Hanabata, Y.; Hayashida, M.; Herrera, J.; Hose, J.; Hrupec, D.; Hughes, G.; Idec, W.; Kodani, K.; Konno, Y.; Kubo, H.; Kushida, J.; La Barbera, A.; Lelas, D.; Lindfors, E.; Lombardi, S.; Longo, F.; López, M.; López-Coto, R.; Majumdar, P.; Makariev, M.; Mallot, K.; Maneva, G.; Manganaro, M.; Mannheim, K.; Maraschi, L.; Marcote, B.; Mariotti, M.; Martínez, M.; Mazin, D.; Menzel, U.; Miranda, J. M.; Mirzoyan, R.; Moralejo, A.; Moretti, E.; Nakajima, D.; Neustroev, V.; Niedzwiecki, A.; Nievas Rosillo, M.; Nilsson, K.; Nishijima, K.; Noda, K.; Nogués, L.; Overkemping, A.; Paiano, S.; Palacio, J.; Palatiello, M.; Paneque, D.; Paoletti, R.; Paredes, J. M.; Paredes-Fortuny, X.; Pedaletti, G.; Peresano, M.; Perri, L.; Persic, M.; Poutanen, J.; Prada Moroni, P. G.; Prandini, E.; Puljak, I.; Reichardt, I.; Rhode, W.; Ribó, M.; Rico, J.; Rodriguez Garcia, J.; Saito, T.; Satalecka, K.; Schroeder, S.; Schultz, C.; Schweizer, T.; Sillanpää, A.; Sitarek, J.; Snidaric, I.; Sobczynska, D.; Stamerra, A.; Steinbring, T.; Strzys, M.; Surić, T.; Takalo, L.; Tavecchio, F.; Temnikov, P.; Terzić, T.; Tescaro, D.; Teshima, M.; Thaele, J.; Torres, D. F.; Toyama, T.; Treves, A.; Vanzo, G.; Verguilov, V.; Vovk, I.; Ward, J. E.; Will, M.; Wu, M. H.; Zanin, .; VERITAS Collaboration; Abeysekara, A. U.; Archambault, S.; Archer, A.; Benbow, W.; Bird, R.; Bourbeau, E.; Buchovecky, M.; Bugaev, V.; Byrum, K.; Cardenzana, J. V.; Cerruti, M.; Ciupik, L.; Connolly, M. P.; Cui, W.; Dickinson, H. J.; Dumm, J.; Eisch, J. D.; Errando, M.; Falcone, A.; Feng, Q.; Finley, J. P.; Fleischhack, H.; Flinders, A.; Fortson, L.; Furniss, A.; Gillanders, G. H.; Griffin, S.; Hütten, J. Grube M.; Håkansson, N.; Hervet, O.; Holder, J.; Humensky, T. B.; Johnson, C. A.; Kaaret, P.; Kar, P.; Kelley-Hoskins, N.; Kertzman, M.; Kieda, D.; Krause, M.; Krennrich, F.; Kumar, S.; Lang, M. J.; Maier, G.; McArthur, S.; McCann, A.; Moriarty, P.; Mukherjee, R.; Nguyen, T.; Nieto, D.; O'Brien, S.; Ong, R. A.; Otte, A. N.; Park, N.; Pohl, M.; Popkow, A.; Pueschel, E.; Quinn, J.; Ragan, K.; Reynolds, P. T.; Richards, G. T.; Roache, E.; Rulten, C.; Sadeh, I.; Santander, M.; Sembroski, G. H.; Shahinyan, K.; Staszak, D.; Telezhinsky, I.; Tucci, J. V.; Tyler, J.; Wakely, S. P.; Weinstein, A.; Wilcox, P.; Wilhelm, A.; Williams, D. A.; Zitzer, B.</p> <p>2016-11-01</p> <p>We describe and report the status of a neutrino-triggered program in IceCube that generates real-time alerts for <span class="hlt">gamma</span>-ray follow-up observations by atmospheric-Cherenkov telescopes (MAGIC and VERITAS). While IceCube is capable of monitoring the whole sky continuously, high-<span class="hlt">energy</span> <span class="hlt">gamma</span>-ray telescopes have restricted fields of view and in general are unlikely to be observing a potential neutrino-flaring source at the time such neutrinos are recorded. The use of neutrino-triggered alerts thus aims at increasing the availability of simultaneous multi-messenger data during potential neutrino flaring activity, which can increase the discovery potential and constrain the phenomenological interpretation of the high-<span class="hlt">energy</span> emission of selected source classes (e.g. blazars). The requirements of a fast and stable online analysis of potential neutrino signals and its operation are presented, along with first results of the program operating between 14 March 2012 and 31 December 2015.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20080043893&hterms=astronomy&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26Nf%3DPublication-Date%257CBTWN%2B20080101%2B20101231%26N%3D0%26No%3D20%26Ntt%3Dastronomy','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20080043893&hterms=astronomy&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26Nf%3DPublication-Date%257CBTWN%2B20080101%2B20101231%26N%3D0%26No%3D20%26Ntt%3Dastronomy"><span>GLAST and Ground-Based <span class="hlt">Gamma</span>-Ray Astronomy</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>McEnery, Julie</p> <p>2008-01-01</p> <p>The launch of the <span class="hlt">Gamma</span>-ray Large Area Space Telescope together with the advent of a new generation of ground-based <span class="hlt">gamma</span>-ray detectors such as VERITAS, HESS, MAGIC and CANGAROO, will usher in a new era of high-<span class="hlt">energy</span> <span class="hlt">gamma</span>-ray astrophysics. GLAST and the ground based <span class="hlt">gamma</span>-ray observatories will provide highly complementary capabilities for spectral, temporal and spatial studies of high <span class="hlt">energy</span> <span class="hlt">gamma</span>-ray sources. Joint observations will cover a huge <span class="hlt">energy</span> range, from 20 MeV to over 20 TeV. The LAT will survey the entire sky every three hours, allowing it both to perform uniform, long-term monitoring of variable sources and to detect flaring sources promptly. Both functions complement the high-sensitivity pointed observations provided by ground-based detectors. Finally, the large field of view of GLAST will allow a study of <span class="hlt">gamma</span>-ray emission on large angular scales and identify interesting regions of the sky for deeper studies at higher <span class="hlt">energies</span>. In this poster, we will discuss the science returns that might result from joint GLAST/ground-based <span class="hlt">gamma</span>-ray observations and illustrate them with detailed source simulations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/2416762','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/2416762"><span>Wetting characteristics and blood clotting on surfaces of copoly(<span class="hlt">gamma</span>-Benzyl-L-glutamate, <span class="hlt">gamma</span>-hydroxyethyl-L-glutamine).</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Yano, E; Komai, T; Kawasaki, T; Kaifu, K; Atsuta, T; Kubo, Y; Fujiwara, Y</p> <p>1985-09-01</p> <p>The film surface of poly(<span class="hlt">gamma</span>-benzyl-L-glutamate) (PBLG) was modified with 2-aminoethanol to enhance its hydrophilicity. Controlling the reaction conditions of PBLG and 2-aminoethanol, various types of copoly(<span class="hlt">gamma</span>-benzyl-L-glutamate, <span class="hlt">gamma</span>-hydroxyethyl-L-glutamine) film surfaces were obtained. Surface free <span class="hlt">energy</span> (<span class="hlt">gamma</span> sv), the dispersive component of <span class="hlt">gamma</span> sv (<span class="hlt">gamma</span> dsv), the nondispersive component of <span class="hlt">gamma</span> sv (<span class="hlt">gamma</span> psv), and the interfacial free <span class="hlt">energy</span> of polymer surface with water (<span class="hlt">gamma</span> sw), which were obtained by using the contact angle measurement and calculation method proposed by Andrade et al., were changed remarkably by the aminolysis. The <span class="hlt">gamma</span> sv value increased after 2 h of aminolysis from 48.2 (PBLG) to 65.3 dyn/cm and gradually increased to around 70 dyn/cm after 12 h reaction. (<span class="hlt">gamma</span> dsv) and (<span class="hlt">gamma</span> psv) changed from 31.0 and 17.2 dyn/cm (PBLG) to 26.5 and 44.3 dyn/cm, respectively. These parameters of the material surfaces, modified over 12 h reaction, were found to be similar to those of the surfaces of canine aorta, vein, and human fibrin membrane. Blood clotting times on these polymer surfaces were comparatively longer than on siliconized glass surfaces.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19790053291&hterms=Ankara&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3DAnkara','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19790053291&hterms=Ankara&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3DAnkara"><span>Comparison of high <span class="hlt">energy</span> <span class="hlt">gamma</span> rays from absolute value of b greater than 30 deg with the galactic neutral hydrogen distribution</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Ozel, M. E.; Ogelman, H.; Tumer, T.; Fichtel, C. E.; Hartman, R. C.; Kniffen, D. A.; Thompson, F. J.</p> <p>1978-01-01</p> <p>High-<span class="hlt">energy</span> <span class="hlt">gamma</span>-ray (<span class="hlt">energy</span> above 35 MeV) data from the SAS 2 satellite have been used to compare the intensity distribution of <span class="hlt">gamma</span> rays with that of neutral hydrogen (H I) density along the line of sight, at high galactic latitudes (absolute values greater than 30 deg). A model has been constructed for the case where the observed <span class="hlt">gamma</span>-ray intensity has been assumed to be the sum of a galactic component proportional to the H I distribution plus an isotropic extragalactic emission. A chi-squared test of the model parameters indicates that about 30% of the total high-latitude emission may originate within the Galaxy.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017A%26A...597A.115H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017A%26A...597A.115H"><span>First limits on the very-high <span class="hlt">energy</span> <span class="hlt">gamma</span>-ray afterglow emission of a fast radio burst. H.E.S.S. observations of FRB 150418</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>H.E.S.S. Collaboration; Abdalla, H.; Abramowski, A.; Aharonian, F.; Ait Benkhali, F.; Akhperjanian, A. G.; Andersson, T.; Angüner, E. O.; Arakawa, M.; Arrieta, M.; Aubert, P.; Backes, M.; Balzer, A.; Barnard, M.; Becherini, Y.; Becker Tjus, J.; Berge, D.; Bernhard, S.; Bernlöhr, K.; Blackwell, R.; Böttcher, M.; Boisson, C.; Bolmont, J.; Bordas, P.; Bregeon, J.; Brun, F.; Brun, P.; Bryan, M.; Büchele, M.; Bulik, T.; Capasso, M.; Carr, J.; Casanova, S.; Cerruti, M.; Chakraborty, N.; Chalme-Calvet, R.; Chaves, R. C. G.; Chen, A.; Chevalier, J.; Chrétien, M.; Coffaro, M.; Colafrancesco, S.; Cologna, G.; Condon, B.; Conrad, J.; Cui, Y.; Davids, I. D.; Decock, J.; Degrange, B.; Deil, C.; Devin, J.; Dewilt, P.; Dirson, L.; Djannati-Ataï, A.; Domainko, W.; Donath, A.; Drury, L. O.'c.; Dutson, K.; Dyks, J.; Edwards, T.; Egberts, K.; Eger, P.; Ernenwein, J.-P.; Eschbach, S.; Farnier, C.; Fegan, S.; Fernandes, M. V.; Fiasson, A.; Fontaine, G.; Förster, A.; Funk, S.; Füßling, M.; Gabici, S.; Gajdus, M.; Gallant, Y. A.; Garrigoux, T.; Giavitto, G.; Giebels, B.; Glicenstein, J. F.; Gottschall, D.; Goyal, A.; Grondin, M.-H.; Hahn, J.; Haupt, M.; Hawkes, J.; Heinzelmann, G.; Henri, G.; Hermann, G.; Hervet, O.; Hinton, J. A.; Hofmann, W.; Hoischen, C.; Holler, M.; Horns, D.; Ivascenko, A.; Iwasaki, H.; Jacholkowska, A.; Jamrozy, M.; Janiak, M.; Jankowsky, D.; Jankowsky, F.; Jingo, M.; Jogler, T.; Jouvin, L.; Jung-Richardt, I.; Kastendieck, M. A.; Katarzyński, K.; Katsuragawa, M.; Katz, U.; Kerszberg, D.; Khangulyan, D.; Khélifi, B.; Kieffer, M.; King, J.; Klepser, S.; Klochkov, D.; Kluźniak, W.; Kolitzus, D.; Komin, Nu.; Kosack, K.; Krakau, S.; Kraus, M.; Krüger, P. P.; Laffon, H.; Lamanna, G.; Lau, J.; Lees, J.-P.; Lefaucheur, J.; Lefranc, V.; Lemière, A.; Lemoine-Goumard, M.; Lenain, J.-P.; Leser, E.; Lohse, T.; Lorentz, M.; Liu, R.; López-Coto, R.; Lypova, I.; Marandon, V.; Marcowith, A.; Mariaud, C.; Marx, R.; Maurin, G.; Maxted, N.; Mayer, M.; Meintjes, P. J.; Meyer, M.; Mitchell, A. M. W.; Moderski, R.; Mohamed, M.; Mohrmann, L.; Morå, K.; Moulin, E.; Murach, T.; Nakashima, S.; de Naurois, M.; Niederwanger, F.; Niemiec, J.; Oakes, L.; O'Brien, P.; Odaka, H.; Öttl, S.; Ohm, S.; Ostrowski, M.; Oya, I.; Padovani, M.; Panter, M.; Parsons, R. D.; Pekeur, N. W.; Pelletier, G.; Perennes, C.; Petrucci, P.-O.; Peyaud, B.; Piel, Q.; Pita, S.; Poon, H.; Prokhorov, D.; Prokoph, H.; Pühlhofer, G.; Punch, M.; Quirrenbach, A.; Raab, S.; Reimer, A.; Reimer, O.; Renaud, M.; de Los Reyes, R.; Richter, S.; Rieger, F.; Romoli, C.; Rowell, G.; Rudak, B.; Rulten, C. B.; Sahakian, V.; Saito, S.; Salek, D.; Sanchez, D. A.; Santangelo, A.; Sasaki, M.; Schlickeiser, R.; Schüssler, F.; Schulz, A.; Schwanke, U.; Schwemmer, S.; Seglar-Arroyo, M.; Settimo, M.; Seyffert, A. S.; Shafi, N.; Shilon, I.; Simoni, R.; Sol, H.; Spanier, F.; Spengler, G.; Spies, F.; Stawarz, Ł.; Steenkamp, R.; Stegmann, C.; Stycz, K.; Sushch, I.; Takahashi, T.; Tavernet, J.-P.; Tavernier, T.; Taylor, A. M.; Terrier, R.; Tibaldo, L.; Tiziani, D.; Tluczykont, M.; Trichard, C.; Tsuji, N.; Tuffs, R.; Uchiyama, Y.; van der Walt, D. J.; van Eldik, C.; van Rensburg, C.; van Soelen, B.; Vasileiadis, G.; Veh, J.; Venter, C.; Viana, A.; Vincent, P.; Vink, J.; Voisin, F.; Völk, H. J.; Vuillaume, T.; Wadiasingh, Z.; Wagner, S. J.; Wagner, P.; Wagner, R. M.; White, R.; Wierzcholska, A.; Willmann, P.; Wörnlein, A.; Wouters, D.; Yang, R.; Zabalza, V.; Zaborov, D.; Zacharias, M.; Zanin, R.; Zdziarski, A. A.; Zech, A.; Zefi, F.; Ziegler, A.; Żywucka, N.; Superb Collaboration; Jankowski, F.; Keane, E. F.; Petroff, E.</p> <p>2017-01-01</p> <p>Aims: Following the detection of the fast radio burst FRB150418 by the SUPERB project at the Parkes radio telescope, we aim to search for very-high <span class="hlt">energy</span> <span class="hlt">gamma</span>-ray afterglow emission. Methods: Follow-up observations in the very-high <span class="hlt">energy</span> <span class="hlt">gamma</span>-ray domain were obtained with the H.E.S.S. imaging atmospheric Cherenkov telescope system within 14.5 h of the radio burst. Results: The obtained 1.4 h of <span class="hlt">gamma</span>-ray observations are presented and discussed. At the 99% C.L. we obtained an integral upper limit on the <span class="hlt">gamma</span>-ray flux of Φγ(E > 350 GeV) < 1.33 × 10-8 m-2 s-1. Differential flux upper limits as function of the photon <span class="hlt">energy</span> were derived and used to constrain the intrinsic high-<span class="hlt">energy</span> afterglow emission of FRB 150418. Conclusions: No hints for high-<span class="hlt">energy</span> afterglow emission of FRB 150418 were found. Taking absorption on the extragalactic background light into account and assuming a distance of z = 0.492 based on radio and optical counterpart studies and consistent with the FRB dispersion, we constrain the <span class="hlt">gamma</span>-ray luminosity at 1 TeV to L < 5.1 × 1047 erg/s at 99% C.L.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li class="active"><span>16</span></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_16 --> <div id="page_17" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li class="active"><span>17</span></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="321"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19970022951','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19970022951"><span>Timing the Geminga Pulsar with High-<span class="hlt">Energy</span> <span class="hlt">Gamma</span>-Rays</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Halpern, Jules P.</p> <p>1997-01-01</p> <p>This is a continuing program to extend and refine the ephemeris of the Geminga pulsar with annual observations for the remaining lifetime of EGRET. The data show that every revolution of Geminga is accounted for during the EGRET epoch, and that a coherent timing solution linking the phase between EGRET, COS-B, amd SAS-2, observations has now been achieved. The accuracy of the <span class="hlt">gamma</span>-ray timing is such that the proper motion of the pulsar can now be detected, consistent with the optical determination. The measured braking index over the 24.2 yr baseline is 17 +/- 1. Further observation is required to ascertain whether this very large braking index truly represents the <span class="hlt">energy</span> loss mechanism, perhaps related to the theory in which Geminga is near its <span class="hlt">gamma</span>-ray death line, or whether it is a manifestation of timing noise. Statistically significant timing residuals are detected in the EGRET data; they depart from the cubic ephemeris at a level of 23 milliperiods. The residuals appear to have a sinusoidal modulation with a period of about 5.1 yr. This could simply be a manifestation of timing noise, or it could be consistent with a planet of mass 1.7/sin i solar mass orbiting Geminga at a radius of 3.3/sin i AU.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19900009566','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19900009566"><span>Low-<span class="hlt">energy</span> <span class="hlt">gamma</span> ray attenuation characteristics of aviation fuels</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Singh, Jag J.; Shen, Chih-Ping; Sprinkle, Danny R.</p> <p>1990-01-01</p> <p>Am241 (59.5 keV) <span class="hlt">gamma</span> ray attenuation characteristics were investigated in 270 aviation fuel (Jet A and Jet A-1) samples from 76 airports around the world as a part of world wide study to measure the variability of aviation fuel properties as a function of season and geographical origin. All measurements were made at room temperature which varied from 20 to 27 C. Fuel densities (rho) were measured concurrently with their linear attenuation coefficients (mu), thus providing a measure of mass attenuation coefficient (mu/rho) for the test samples. In 43 fuel samples, rho and mu values were measured at more than one room temperature, thus providing mu/rho values for them at several temperatures. The results were found to be independent of the temperature at which mu and rho values were measured. It is noted that whereas the individual mu and rho values vary considerably from airport to airport as well as season to season, the mu/rho values for all samples are constant at 0.1843 + or - 0.0013 cu cm/gm. This constancy of mu/rho value for aviation fuels is significant since a nuclear fuel quantity gauging system based on low <span class="hlt">energy</span> <span class="hlt">gamma</span> ray attenuation will be viable throughout the world.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19820046843&hterms=palestine&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Dpalestine','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19820046843&hterms=palestine&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Dpalestine"><span>Cross correlation analysis of medium <span class="hlt">energy</span> <span class="hlt">gamma</span> rays for the Northern Hemisphere</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Long, J.; Zanrosso, E.; Zych, A. D.; White, R. S.</p> <p>1982-01-01</p> <p>In the cross correlation method the observed <span class="hlt">gamma</span> rays are compared with the expected telescope response for a discrete celestial source. The background consists of the atmospheric flux with its maximum near the horizon, the cosmic diffuse flux, and neutron induced <span class="hlt">gamma</span> rays in the telescope. In sharp contrast to the background, a celestial source produces an asymmetric azimuthal response which varies predictably in time as the source moves through the telescope's aperture. This contrast serves as the basis of the cross correlation technique. Continuous data of 47.5 hr were obtained during a balloon flight from Palestine, TX from 0930 UT on September 30, 1978 to 2300 UT on October 1, 1978. The Crab Nebula-Anticenter region was observed on two consecutive days. A number of other medium <span class="hlt">energy</span> source candidates also crossed the field-of-view. The obtained results are discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19760022032&hterms=Ankara&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3DAnkara','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19760022032&hterms=Ankara&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3DAnkara"><span><span class="hlt">Gamma</span> ray pulsars</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Oegelman, H.; Ayasli, S.; Hacinliyan, A.</p> <p>1976-01-01</p> <p>Recent data from the high <span class="hlt">energy</span> <span class="hlt">gamma</span> ray experiment have revealed the existence of four pulsars emitting photons above 35 MeV. An attempt is made to explain the <span class="hlt">gamma</span> ray emission from these pulsars in terms of an electron-photon cascade that develops in the magnetosphere of the pulsar. Although there is very little material above the surface of the pulsar, the very intense magnetic fields correspond to many radiation lengths which cause electrons to emit photons via magnetic bremsstrahlung and these photons to pair produce. The cascade develops until the mean photon <span class="hlt">energy</span> drops below the pair production threshold which happens to be in the <span class="hlt">gamma</span> ray range; at this stage the photons break out from the source.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/865965','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/865965"><span>Method of achieving the controlled <span class="hlt">release</span> of thermonuclear <span class="hlt">energy</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Brueckner, Keith A.</p> <p>1986-01-01</p> <p>A method of achieving the controlled <span class="hlt">release</span> of thermonuclear <span class="hlt">energy</span> by illuminating a minute, solid density, hollow shell of a mixture of material such as deuterium and tritium with a high intensity, uniformly converging laser wave to effect an extremely rapid build-up of <span class="hlt">energy</span> in inwardly traveling shock waves to implode the shell creating thermonuclear conditions causing a reaction of deuterons and tritons and a resultant high <span class="hlt">energy</span> thermonuclear burn. Utilizing the resulting <span class="hlt">energy</span> as a thermal source and to breed tritium or plutonium. The invention also contemplates a laser source wherein the flux level is increased with time to reduce the initial shock heating of fuel and provide maximum compression after implosion; and, in addition, computations and an equation are provided to enable the selection of a design having a high degree of stability and a dependable fusion performance by establishing a proper relationship between the laser <span class="hlt">energy</span> input and the size and character of the selected material for the fusion capsule.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20060056392','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20060056392"><span>Influence of Finite Element Software on <span class="hlt">Energy</span> <span class="hlt">Release</span> Rates Computed Using the Virtual Crack Closure Technique</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Krueger, Ronald; Goetze, Dirk; Ransom, Jonathon (Technical Monitor)</p> <p>2006-01-01</p> <p>Strain <span class="hlt">energy</span> <span class="hlt">release</span> rates were computed along straight delamination fronts of Double Cantilever Beam, End-Notched Flexure and Single Leg Bending specimens using the Virtual Crack Closure Technique (VCCT). Th e results were based on finite element analyses using ABAQUS# and ANSYS# and were calculated from the finite element results using the same post-processing routine to assure a consistent procedure. Mixed-mode strain <span class="hlt">energy</span> <span class="hlt">release</span> rates obtained from post-processing finite elem ent results were in good agreement for all element types used and all specimens modeled. Compared to previous studies, the models made of s olid twenty-node hexahedral elements and solid eight-node incompatible mode elements yielded excellent results. For both codes, models made of standard brick elements and elements with reduced integration did not correctly capture the distribution of the <span class="hlt">energy</span> <span class="hlt">release</span> rate acr oss the width of the specimens for the models chosen. The results suggested that element types with similar formulation yield matching results independent of the finite element software used. For comparison, m ixed-mode strain <span class="hlt">energy</span> <span class="hlt">release</span> rates were also calculated within ABAQUS#/Standard using the VCCT for ABAQUS# add on. For all specimens mod eled, mixed-mode strain <span class="hlt">energy</span> <span class="hlt">release</span> rates obtained from ABAQUS# finite element results using post-processing were almost identical to re sults calculated using the VCCT for ABAQUS# add on.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22654374-high-energy-neutrino-emission-from-short-gamma-ray-bursts-prospects-coincident-detection-gravitational-waves','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22654374-high-energy-neutrino-emission-from-short-gamma-ray-bursts-prospects-coincident-detection-gravitational-waves"><span>High-<span class="hlt">energy</span> Neutrino Emission from Short <span class="hlt">Gamma</span>-Ray Bursts: Prospects for Coincident Detection with Gravitational Waves</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Kimura, Shigeo S.; Murase, Kohta; Mészáros, Peter</p> <p></p> <p>We investigate current and future prospects for coincident detection of high-<span class="hlt">energy</span> neutrinos and gravitational waves (GWs). Short <span class="hlt">gamma</span>-ray bursts (SGRBs) are believed to originate from mergers of compact star binaries involving neutron stars. We estimate high-<span class="hlt">energy</span> neutrino fluences from prompt emission, extended emission (EE), X-ray flares, and plateau emission, and we show that neutrino signals associated with the EE are the most promising. Assuming that the cosmic-ray loading factor is ∼10 and the Lorentz factor distribution is lognormal, we calculate the probability of neutrino detection from EE by current and future neutrino detectors, and we find that the quasi-simultaneous detectionmore » of high-<span class="hlt">energy</span> neutrinos, <span class="hlt">gamma</span>-rays, and GWs is possible with future instruments or even with current instruments for nearby SGRBs having EE. We also discuss stacking analyses that will also be useful with future experiments such as IceCube-Gen2.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=GL-2002-001158&hterms=titanic&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dtitanic','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=GL-2002-001158&hterms=titanic&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dtitanic"><span>HUBBLE STAYS ON TRAIL OF FADING <span class="hlt">GAMMA</span>-RAY BURST FIREBALL</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p></p> <p>2002-01-01</p> <p>A Hubble Space Telescope image of the fading fireball from one of the universe's most mysterious phenomena, a <span class="hlt">gamma</span>-ray burst. Though the visible component has faded to 1/500th its brightness (27.7 magnitude) from the time it was first discovered by ground- based telescopes last March (the actual <span class="hlt">gamma</span>-ray burst took place on February 28), Hubble continues to clearly see the fireball and discriminated a surrounding nebulosity (at 25th magnitude) which is considered a host galaxy. The continued visibility of the burst, and the rate of its fading, support theories that the light from a <span class="hlt">gamma</span>-ray burst is an expanding relativistic (moving near the speed of light) fireball, possibly produced by the collision of two dense objects, such as an orbiting pair of neutron stars. If the burst happened nearby, within our own galaxy, the resulting fireball should have had only enough <span class="hlt">energy</span> to propel it into space for a month. The fact that this fireball is still visible after six months means the explosion was truly titanic and, to match the observed brightness, must have happened at the vast distances of galaxies. The <span class="hlt">energy</span> <span class="hlt">released</span> in a burst, which can last from a fraction of a second to a few hundred seconds, is equal to all of the Sun's <span class="hlt">energy</span> generated over its 10 billion year lifetime. The false-color image was taken Sept. 5, 1997 with the Space Telescope Imaging Spectrograph. Credit: Andrew Fruchter (STScI), Elena Pian (ITSRE-CNR), and NASA</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/19574351','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/19574351"><span>Radio imaging of the very-high-<span class="hlt">energy</span> <span class="hlt">gamma</span>-ray emission region in the central engine of a radio galaxy.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Acciari, V A; Aliu, E; Arlen, T; Bautista, M; Beilicke, M; Benbow, W; Bradbury, S M; Buckley, J H; Bugaev, V; Butt, Y; Byrum, K; Cannon, A; Celik, O; Cesarini, A; Chow, Y C; Ciupik, L; Cogan, P; Cui, W; Dickherber, R; Fegan, S J; Finley, J P; Fortin, P; Fortson, L; Furniss, A; Gall, D; Gillanders, G H; Grube, J; Guenette, R; Gyuk, G; Hanna, D; Holder, J; Horan, D; Hui, C M; Humensky, T B; Imran, A; Kaaret, P; Karlsson, N; Kieda, D; Kildea, J; Konopelko, A; Krawczynski, H; Krennrich, F; Lang, M J; LeBohec, S; Maier, G; McCann, A; McCutcheon, M; Millis, J; Moriarty, P; Ong, R A; Otte, A N; Pandel, D; Perkins, J S; Petry, D; Pohl, M; Quinn, J; Ragan, K; Reyes, L C; Reynolds, P T; Roache, E; Roache, E; Rose, H J; Schroedter, M; Sembroski, G H; Smith, A W; Swordy, S P; Theiling, M; Toner, J A; Varlotta, A; Vincent, S; Wakely, S P; Ward, J E; Weekes, T C; Weinstein, A; Williams, D A; Wissel, S; Wood, M; Walker, R C; Davies, F; Hardee, P E; Junor, W; Ly, C; Aharonian, F; Akhperjanian, A G; Anton, G; Barres de Almeida, U; Bazer-Bachi, A R; Becherini, Y; Behera, B; Bernlöhr, K; Bochow, A; Boisson, C; Bolmont, J; Borrel, V; Brucker, J; Brun, F; Brun, P; Bühler, R; Bulik, T; Büsching, I; Boutelier, T; Chadwick, P M; Charbonnier, A; Chaves, R C G; Cheesebrough, A; Chounet, L-M; Clapson, A C; Coignet, G; Dalton, M; Daniel, M K; Davids, I D; Degrange, B; Deil, C; Dickinson, H J; Djannati-Ataï, A; Domainko, W; Drury, L O'C; Dubois, F; Dubus, G; Dyks, J; Dyrda, M; Egberts, K; Emmanoulopoulos, D; Espigat, P; Farnier, C; Feinstein, F; Fiasson, A; Förster, A; Fontaine, G; Füssling, M; Gabici, S; Gallant, Y A; Gérard, L; Gerbig, D; Giebels, B; Glicenstein, J F; Glück, B; Goret, P; Göhring, D; Hauser, D; Hauser, M; Heinz, S; Heinzelmann, G; Henri, G; Hermann, G; Hinton, J A; Hoffmann, A; Hofmann, W; Holleran, M; Hoppe, S; Horns, D; Jacholkowska, A; de Jager, O C; Jahn, C; Jung, I; Katarzyński, K; Katz, U; Kaufmann, S; Kendziorra, E; Kerschhaggl, M; Khangulyan, D; Khélifi, B; Keogh, D; Kluźniak, W; Kneiske, T; Komin, Nu; Kosack, K; Lamanna, G; Lenain, J-P; Lohse, T; Marandon, V; Martin, J M; Martineau-Huynh, O; Marcowith, A; Maurin, D; McComb, T J L; Medina, M C; Moderski, R; Moulin, E; Naumann-Godo, M; de Naurois, M; Nedbal, D; Nekrassov, D; Nicholas, B; Niemiec, J; Nolan, S J; Ohm, S; Olive, J-F; de Oña Wilhelmi, E; Orford, K J; Ostrowski, M; Panter, M; Paz Arribas, M; Pedaletti, G; Pelletier, G; Petrucci, P-O; Pita, S; Pühlhofer, G; Punch, M; Quirrenbach, A; Raubenheimer, B C; Raue, M; Rayner, S M; Renaud, M; Rieger, F; Ripken, J; Rob, L; Rosier-Lees, S; Rowell, G; Rudak, B; Rulten, C B; Ruppel, J; Sahakian, V; Santangelo, A; Schlickeiser, R; Schöck, F M; Schröder, R; Schwanke, U; Schwarzburg, S; Schwemmer, S; Shalchi, A; Sikora, M; Skilton, J L; Sol, H; Spangler, D; Stawarz, Ł; Steenkamp, R; Stegmann, C; Stinzing, F; Superina, G; Szostek, A; Tam, P H; Tavernet, J-P; Terrier, R; Tibolla, O; Tluczykont, M; van Eldik, C; Vasileiadis, G; Venter, C; Venter, L; Vialle, J P; Vincent, P; Vivier, M; Völk, H J; Volpe, F; Wagner, S J; Ward, M; Zdziarski, A A; Zech, A; Anderhub, H; Antonelli, L A; Antoranz, P; Backes, M; Baixeras, C; Balestra, S; Barrio, J A; Bastieri, D; Becerra González, J; Becker, J K; Bednarek, W; Berger, K; Bernardini, E; Biland, A; Bock, R K; Bonnoli, G; Bordas, P; Borla Tridon, D; Bosch-Ramon, V; Bose, D; Braun, I; Bretz, T; Britvitch, I; Camara, M; Carmona, E; Commichau, S; Contreras, J L; Cortina, J; Costado, M T; Covino, S; Curtef, V; Dazzi, F; De Angelis, A; De Cea del Pozo, E; Delgado Mendez, C; De los Reyes, R; De Lotto, B; De Maria, M; De Sabata, F; Dominguez, A; Dorner, D; Doro, M; Elsaesser, D; Errando, M; Ferenc, D; Fernández, E; Firpo, R; Fonseca, M V; Font, L; Galante, N; García López, R J; Garczarczyk, M; Gaug, M; Goebel, F; Hadasch, D; Hayashida, M; Herrero, A; Hildebrand, D; Höhne-Mönch, D; Hose, J; Hsu, C C; Jogler, T; Kranich, D; La Barbera, A; Laille, A; Leonardo, E; Lindfors, E; Lombardi, S; Longo, F; López, M; Lorenz, E; Majumdar, P; Maneva, G; Mankuzhiyil, N; Mannheim, K; Maraschi, L; Mariotti, M; Martínez, M; Mazin, D; Meucci, M; Miranda, J M; Mirzoyan, R; Miyamoto, H; Moldón, J; Moles, M; Moralejo, A; Nieto, D; Nilsson, K; Ninkovic, J; Oya, I; Paoletti, R; Paredes, J M; Pasanen, M; Pascoli, D; Pauss, F; Pegna, R G; Perez-Torres, M A; Persic, M; Peruzzo, L; Prada, F; Prandini, E; Puchades, N; Reichardt, I; Rhode, W; Ribó, M; Rico, J; Rissi, M; Robert, A; Rügamer, S; Saggion, A; Saito, T Y; Salvati, M; Sanchez-Conde, M; Satalecka, K; Scalzotto, V; Scapin, V; Schweizer, T; Shayduk, M; Shore, S N; Sidro, N; Sierpowska-Bartosik, A; Sillanpää, A; Sitarek, J; Sobczynska, D; Spanier, F; Stamerra, A; Stark, L S; Takalo, L; Tavecchio, F; Temnikov, P; Tescaro, D; Teshima, M; Torres, D F; Turini, N; Vankov, H; Wagner, R M; Zabalza, V; Zandanel, F; Zanin, R; Zapatero, J</p> <p>2009-07-24</p> <p>The accretion of matter onto a massive black hole is believed to feed the relativistic plasma jets found in many active galactic nuclei (AGN). Although some AGN accelerate particles to <span class="hlt">energies</span> exceeding 10(12) electron volts and are bright sources of very-high-<span class="hlt">energy</span> (VHE) <span class="hlt">gamma</span>-ray emission, it is not yet known where the VHE emission originates. Here we report on radio and VHE observations of the radio galaxy Messier 87, revealing a period of extremely strong VHE <span class="hlt">gamma</span>-ray flares accompanied by a strong increase of the radio flux from its nucleus. These results imply that charged particles are accelerated to very high <span class="hlt">energies</span> in the immediate vicinity of the black hole.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22667210-search-very-high-energy-gamma-rays-from-missing-link-binary-pulsar-j1023+0038-veritas','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22667210-search-very-high-energy-gamma-rays-from-missing-link-binary-pulsar-j1023+0038-veritas"><span>A SEARCH FOR VERY HIGH <span class="hlt">ENERGY</span> <span class="hlt">GAMMA</span> RAYS FROM THE MISSING LINK BINARY PULSAR J1023+0038 WITH VERITAS</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Aliu, E.; Archambault, S.; Archer, A.</p> <p>2016-11-10</p> <p>The binary millisecond radio pulsar PSR J1023+0038 exhibits many characteristics similar to the <span class="hlt">gamma</span>-ray binary system PSR B1259–63/LS 2883, making it an ideal candidate for the study of high-<span class="hlt">energy</span> nonthermal emission. It has been the subject of multiwavelength campaigns following the disappearance of the pulsed radio emission in 2013 June, which revealed the appearance of an accretion disk around the neutron star. We present the results of very high <span class="hlt">energy</span> (VHE) <span class="hlt">gamma</span>-ray observations carried out by the Very Energetic Radiation Imaging Telescope Array System before and after this change of state. Searches for steady and pulsed emission of both datamore » sets yield no significant <span class="hlt">gamma</span>-ray signal above 100 GeV, and upper limits are given for both a steady and pulsed <span class="hlt">gamma</span>-ray flux. These upper limits are used to constrain the magnetic field strength in the shock region of the PSR J1023+0038 system. Assuming that VHE <span class="hlt">gamma</span> rays are produced via an inverse Compton mechanism in the shock region, we constrain the shock magnetic field to be greater than ∼2 G before the disappearance of the radio pulsar and greater than ∼10 G afterward.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010AIPC.1250...39S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010AIPC.1250...39S"><span>Experimental Determination of the HPGe Spectrometer Efficiency Calibration Curves for Various Sample Geometry for <span class="hlt">Gamma</span> <span class="hlt">Energy</span> from 50 keV to 2000 keV</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Saat, Ahmad; Hamzah, Zaini; Yusop, Mohammad Fariz; Zainal, Muhd Amiruddin</p> <p>2010-07-01</p> <p>Detection efficiency of a <span class="hlt">gamma</span>-ray spectrometry system is dependent upon among others, <span class="hlt">energy</span>, sample and detector geometry, volume and density of the samples. In the present study the efficiency calibration curves of newly acquired (August 2008) HPGe <span class="hlt">gamma</span>-ray spectrometry system was carried out for four sample container geometries, namely Marinelli beaker, disc, cylindrical beaker and vial, normally used for activity determination of <span class="hlt">gamma</span>-ray from environmental samples. Calibration standards were prepared by using known amount of analytical grade uranium trioxide ore, homogenized in plain flour into the respective containers. The ore produces <span class="hlt">gamma</span>-rays of <span class="hlt">energy</span> ranging from 53 keV to 1001 keV. Analytical grade potassium chloride were prepared to determine detection efficiency of 1460 keV <span class="hlt">gamma</span>-ray emitted by potassium isotope K-40. Plots of detection efficiency against <span class="hlt">gamma</span>-ray <span class="hlt">energy</span> for the four sample geometries were found to fit smoothly to a general form of ɛ = AΕa+BΕb, where ɛ is efficiency, Ε is <span class="hlt">energy</span> in keV, A, B, a and b are constants that are dependent on the sample geometries. All calibration curves showed the presence of a "knee" at about 180 keV. Comparison between the four geometries showed that the efficiency of Marinelli beaker is higher than cylindrical beaker and vial, while cylindrical disk showed the lowest.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016NIMPA.819..139P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016NIMPA.819..139P"><span>Use of borated polyethylene to improve low <span class="hlt">energy</span> response of a prompt <span class="hlt">gamma</span> based neutron dosimeter</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Priyada, P.; Ashwini, U.; Sarkar, P. K.</p> <p>2016-05-01</p> <p>The feasibility of using a combined sample of borated polyethylene and normal polyethylene to estimate neutron ambient dose equivalent from measured prompt <span class="hlt">gamma</span> emissions is investigated theoretically to demonstrate improvements in low <span class="hlt">energy</span> neutron dose response compared to only polyethylene. Monte Carlo simulations have been carried out using the FLUKA code to calculate the response of boron, hydrogen and carbon prompt <span class="hlt">gamma</span> emissions to mono energetic neutrons. The weighted least square method is employed to arrive at the best linear combination of these responses that approximates the ICRP fluence to dose conversion coefficients well in the <span class="hlt">energy</span> range of 10-8 MeV to 14 MeV. The configuration of the combined system is optimized through FLUKA simulations. The proposed method is validated theoretically with five different workplace neutron spectra with satisfactory outcome.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20010073288&hterms=energy+solar&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Denergy%2Bsolar','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20010073288&hterms=energy+solar&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Denergy%2Bsolar"><span>Solar Flares and the High <span class="hlt">Energy</span> Solar Spectroscopic Imager (HESSI)</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Holman, Gordon D.; Fisher, Richard R. (Technical Monitor)</p> <p>2001-01-01</p> <p>Solar flares are the biggest explosions in the solar system. They are important both for understanding explosive events in the Universe and for their impact on human technology and communications. The satellite-based HESSI is designed to study the explosive <span class="hlt">release</span> of <span class="hlt">energy</span> and the acceleration of electrons, protons, and other charged particles to high <span class="hlt">energies</span> in solar flares. HESSI produces "color" movies of the Sun in high-<span class="hlt">energy</span> X rays and <span class="hlt">gamma</span> rays radiated by these energetic particles. HESSI's X-ray and <span class="hlt">gamma</span>-ray images of flares are obtained using techniques similar to those used in radio interferometry. Ground-based radio observations of the Sun provide an important complement to the HESSI observations of solar flares. I will describe the HESSI Project and the high-<span class="hlt">energy</span> aspects of solar flares, and how these relate to radio astronomy techniques and observations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013NIMPA.720...83M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013NIMPA.720...83M"><span>Terrestrial <span class="hlt">gamma</span>-ray flashes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Marisaldi, Martino; Fuschino, Fabio; Labanti, Claudio; Tavani, Marco; Argan, Andrea; Del Monte, Ettore; Longo, Francesco; Barbiellini, Guido; Giuliani, Andrea; Trois, Alessio; Bulgarelli, Andrea; Gianotti, Fulvio; Trifoglio, Massimo</p> <p>2013-08-01</p> <p>Lightning and thunderstorm systems in general have been recently recognized as powerful particle accelerators, capable of producing electrons, positrons, <span class="hlt">gamma</span>-rays and neutrons with <span class="hlt">energies</span> as high as several tens of MeV. In fact, these natural systems turn out to be the highest <span class="hlt">energy</span> and most efficient natural particle accelerators on Earth. Terrestrial <span class="hlt">Gamma</span>-ray Flashes (TGFs) are millisecond long, very intense bursts of <span class="hlt">gamma</span>-rays and are one of the most intriguing manifestation of these natural accelerators. Only three currently operative missions are capable of detecting TGFs from space: the RHESSI, Fermi and AGILE satellites. In this paper we review the characteristics of TGFs, including <span class="hlt">energy</span> spectrum, timing structure, beam geometry and correlation with lightning, and the basic principles of the associated production models. Then we focus on the recent AGILE discoveries concerning the high <span class="hlt">energy</span> extension of the TGF spectrum up to 100 MeV, which is difficult to reconcile with current theoretical models.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015NIMPA.782...47C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015NIMPA.782...47C"><span>The neutron-<span class="hlt">gamma</span> Feynman variance to mean approach: <span class="hlt">Gamma</span> detection and total neutron-<span class="hlt">gamma</span> detection (theory and practice)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chernikova, Dina; Axell, Kåre; Avdic, Senada; Pázsit, Imre; Nordlund, Anders; Allard, Stefan</p> <p>2015-05-01</p> <p>Two versions of the neutron-<span class="hlt">gamma</span> variance to mean (Feynman-alpha method or Feynman-Y function) formula for either <span class="hlt">gamma</span> detection only or total neutron-<span class="hlt">gamma</span> detection, respectively, are derived and compared in this paper. The new formulas have particular importance for detectors of either <span class="hlt">gamma</span> photons or detectors sensitive to both neutron and <span class="hlt">gamma</span> radiation. If applied to a plastic or liquid scintillation detector, the total neutron-<span class="hlt">gamma</span> detection Feynman-Y expression corresponds to a situation where no discrimination is made between neutrons and <span class="hlt">gamma</span> particles. The <span class="hlt">gamma</span> variance to mean formulas are useful when a detector of only <span class="hlt">gamma</span> radiation is used or when working with a combined neutron-<span class="hlt">gamma</span> detector at high count rates. The theoretical derivation is based on the Chapman-Kolmogorov equation with the inclusion of general reactions and corresponding intensities for neutrons and <span class="hlt">gammas</span>, but with the inclusion of prompt reactions only. A one <span class="hlt">energy</span> group approximation is considered. The comparison of the two different theories is made by using reaction intensities obtained in MCNPX simulations with a simplified geometry for two scintillation detectors and a 252Cf-source. In addition, the variance to mean ratios, neutron, <span class="hlt">gamma</span> and total neutron-<span class="hlt">gamma</span> are evaluated experimentally for a weak 252Cf neutron-<span class="hlt">gamma</span> source, a 137Cs random <span class="hlt">gamma</span> source and a 22Na correlated <span class="hlt">gamma</span> source. Due to the focus being on the possibility of using neutron-<span class="hlt">gamma</span> variance to mean theories for both reactor and safeguards applications, we limited the present study to the general analytical expressions for Feynman-alpha formulas.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19780024088','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19780024088"><span>Solar <span class="hlt">Gamma</span> Rays Above 8 MeV</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Crannell, C. J.; Crannell, H.; Ramaty, R.</p> <p>1978-01-01</p> <p>Processes which lead to the production of <span class="hlt">gamma</span> rays with <span class="hlt">energy</span> greater than 8 MeV in solar flares are reviewed and evaluated. Excited states produced by inelastic scattering, charge exchange, and spallation reactions in the abundant nuclear species are considered in order to identify nuclear lines which may contribute to the <span class="hlt">Gamma</span> ray spectrum of solar flares. The flux of 15.11 MeV <span class="hlt">Gamma</span> rays relative to the flux of 4.44 MeV <span class="hlt">Gamma</span> rays from the de-excitation of the corresponding states in C12 is calculated for a number of assumed distributions of exciting particles. This flux ratio is a sensitive diagnostic of accelerated particle spectra. Other high <span class="hlt">energy</span> nuclear levels are not so isolated as the 15.11 MeV state and are not expected to be so strong. The spectrum of <span class="hlt">Gamma</span> rays from the decay of Pi dey is sensitive to the <span class="hlt">energy</span> distribution of particles accelerated to <span class="hlt">energies</span> greater than 100 MeV.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016A%26A...595A..98A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016A%26A...595A..98A"><span>Detection of very high <span class="hlt">energy</span> <span class="hlt">gamma</span>-ray emission from the gravitationally lensed blazar QSO B0218+357 with the MAGIC telescopes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ahnen, M. L.; Ansoldi, S.; Antonelli, L. A.; Antoranz, P.; Arcaro, C.; Babic, A.; Banerjee, B.; Bangale, P.; Barres de Almeida, U.; Barrio, J. A.; Becerra González, J.; Bednarek, W.; Bernardini, E.; Berti, A.; Biasuzzi, B.; Biland, A.; Blanch, O.; Bonnefoy, S.; Bonnoli, G.; Borracci, F.; Bretz, T.; Buson, S.; Carosi, A.; Chatterjee, A.; Clavero, R.; Colin, P.; Colombo, E.; Contreras, J. L.; Cortina, J.; Covino, S.; Da Vela, P.; Dazzi, F.; De Angelis, A.; De Lotto, B.; de Oña Wilhelmi, E.; Di Pierro, F.; Doert, M.; Domínguez, A.; Dominis Prester, D.; Dorner, D.; Doro, M.; Einecke, S.; Eisenacher Glawion, D.; Elsaesser, D.; Engelkemeier, M.; Fallah Ramazani, V.; Fernández-Barral, A.; Fidalgo, D.; Fonseca, M. V.; Font, L.; Frantzen, K.; Fruck, C.; Galindo, D.; García López, R. J.; Garczarczyk, M.; Garrido Terrats, D.; Gaug, M.; Giammaria, P.; Godinović, N.; Gora, D.; Guberman, D.; Hadasch, D.; Hahn, A.; Hayashida, M.; Herrera, J.; Hose, J.; Hrupec, D.; Hughes, G.; Idec, W.; Kodani, K.; Konno, Y.; Kubo, H.; Kushida, J.; La Barbera, A.; Lelas, D.; Lindfors, E.; Lombardi, S.; Longo, F.; López, M.; López-Coto, R.; Majumdar, P.; Makariev, M.; Mallot, K.; Maneva, G.; Manganaro, M.; Mannheim, K.; Maraschi, L.; Marcote, B.; Mariotti, M.; Martínez, M.; Mazin, D.; Menzel, U.; Miranda, J. M.; Mirzoyan, R.; Moralejo, A.; Moretti, E.; Nakajima, D.; Neustroev, V.; Niedzwiecki, A.; Nievas Rosillo, M.; Nilsson, K.; Nishijima, K.; Noda, K.; Nogués, L.; Paiano, S.; Palacio, J.; Palatiello, M.; Paneque, D.; Paoletti, R.; Paredes, J. M.; Paredes-Fortuny, X.; Pedaletti, G.; Peresano, M.; Perri, L.; Persic, M.; Poutanen, J.; Prada Moroni, P. G.; Prandini, E.; Puljak, I.; Garcia, J. R.; Reichardt, I.; Rhode, W.; Ribó, M.; Rico, J.; Saito, T.; Satalecka, K.; Schroeder, S.; Schweizer, T.; Shore, S. N.; Sillanpää, A.; Sitarek, J.; Snidaric, I.; Sobczynska, D.; Stamerra, A.; Strzys, M.; Surić, T.; Takalo, L.; Tavecchio, F.; Temnikov, P.; Terzić, T.; Tescaro, D.; Teshima, M.; Torres, D. F.; Toyama, T.; Treves, A.; Vanzo, G.; Verguilov, V.; Vovk, I.; Ward, J. E.; Will, M.; Wu, M. H.; Zanin, R.; Desiante, R.</p> <p>2016-11-01</p> <p>Context. QSO B0218+357 is a gravitationally lensed blazar located at a redshift of 0.944. The gravitational lensing splits the emitted radiation into two components that are spatially indistinguishable by <span class="hlt">gamma</span>-ray instruments, but separated by a 10-12 day delay. In July 2014, QSO B0218+357 experienced a violent flare observed by the Fermi-LAT and followed by the MAGIC telescopes. Aims: The spectral <span class="hlt">energy</span> distribution of QSO B0218+357 can give information on the energetics of z 1 very high <span class="hlt">energy</span> <span class="hlt">gamma</span>-ray sources. Moreover the <span class="hlt">gamma</span>-ray emission can also be used as a probe of the extragalactic background light at z 1. Methods: MAGIC performed observations of QSO B0218+357 during the expected arrival time of the delayed component of the emission. The MAGIC and Fermi-LAT observations were accompanied by quasi-simultaneous optical data from the KVA telescope and X-ray observations by Swift-XRT. We construct a multiwavelength spectral <span class="hlt">energy</span> distribution of QSO B0218+357 and use it to model the source. The GeV and sub-TeV data obtained by Fermi-LAT and MAGIC are used to set constraints on the extragalactic background light. Results: Very high <span class="hlt">energy</span> <span class="hlt">gamma</span>-ray emission was detected from the direction of QSO B0218+357 by the MAGIC telescopes during the expected time of arrival of the trailing component of the flare, making it the farthest very high <span class="hlt">energy</span> <span class="hlt">gamma</span>-ray source detected to date. The observed emission spans the <span class="hlt">energy</span> range from 65 to 175 GeV. The combined MAGIC and Fermi-LAT spectral <span class="hlt">energy</span> distribution of QSO B0218+357 is consistent with current extragalactic background light models. The broadband emission can be modeled in the framework of a two-zone external Compton scenario, where the GeV emission comes from an emission region in the jet, located outside the broad line region.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1355716','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1355716"><span>Detection of very high <span class="hlt">energy</span> <span class="hlt">gamma</span>-ray emission from the gravitationally lensed blazar QSO B0218+357 with the MAGIC telescopes</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Ahnen, M. L.; Ansoldi, S.; Antonelli, L. A.</p> <p></p> <p>QSO B0218+357 is a gravitationally lensed blazar located at a redshift of 0.944. The gravitational lensing splits the emitted radiation into two components that are spatially indistinguishable by <span class="hlt">gamma</span>-ray instruments, but separated by a 10–12 day delay. In July 2014, QSO B0218+357 experienced a violent flare observed by the Fermi-LAT and followed by the MAGIC telescopes. The spectral <span class="hlt">energy</span> distribution of QSO B0218+357 can give information on the energetics of z ~ 1 very high <span class="hlt">energy</span> <span class="hlt">gamma</span>-ray sources. Furthermore, the <span class="hlt">gamma</span>-ray emission can also be used as a probe of the extragalactic background light at z ~ 1. MAGIC performedmore » observations of QSO B0218+357 during the expected arrival time of the delayed component of the emission. The MAGIC and Fermi-LAT observations were accompanied by quasi-simultaneous optical data from the KVA telescope and X-ray observations by Swift-XRT. We construct a multiwavelength spectral <span class="hlt">energy</span> distribution of QSO B0218+357 and use it to model the source. The GeV and sub-TeV data obtained by Fermi-LAT and MAGIC are used to set constraints on the extragalactic background light. We detected very high <span class="hlt">energy</span> <span class="hlt">gamma</span>-ray emission from the direction of QSO B0218+357 by the MAGIC telescopes during the expected time of arrival of the trailing component of the flare, making it the farthest very high <span class="hlt">energy</span> <span class="hlt">gamma</span>-ray source detected to date. We also observed emission spans the <span class="hlt">energy</span> range from 65 to 175 GeV. The combined MAGIC and Fermi-LAT spectral <span class="hlt">energy</span> distribution of QSO B0218+357 is consistent with current extragalactic background light models. The broadband emission can be modeled in the framework of a two-zone external Compton scenario, where the GeV emission comes from an emission region in the jet, located outside the broad line region.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1355716-detection-very-high-energy-gamma-ray-emission-from-gravitationally-lensed-blazar-qso-b0218+357-magic-telescopes','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1355716-detection-very-high-energy-gamma-ray-emission-from-gravitationally-lensed-blazar-qso-b0218+357-magic-telescopes"><span>Detection of very high <span class="hlt">energy</span> <span class="hlt">gamma</span>-ray emission from the gravitationally lensed blazar QSO B0218+357 with the MAGIC telescopes</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Ahnen, M. L.; Ansoldi, S.; Antonelli, L. A.; ...</p> <p>2016-11-04</p> <p>QSO B0218+357 is a gravitationally lensed blazar located at a redshift of 0.944. The gravitational lensing splits the emitted radiation into two components that are spatially indistinguishable by <span class="hlt">gamma</span>-ray instruments, but separated by a 10–12 day delay. In July 2014, QSO B0218+357 experienced a violent flare observed by the Fermi-LAT and followed by the MAGIC telescopes. The spectral <span class="hlt">energy</span> distribution of QSO B0218+357 can give information on the energetics of z ~ 1 very high <span class="hlt">energy</span> <span class="hlt">gamma</span>-ray sources. Furthermore, the <span class="hlt">gamma</span>-ray emission can also be used as a probe of the extragalactic background light at z ~ 1. MAGIC performedmore » observations of QSO B0218+357 during the expected arrival time of the delayed component of the emission. The MAGIC and Fermi-LAT observations were accompanied by quasi-simultaneous optical data from the KVA telescope and X-ray observations by Swift-XRT. We construct a multiwavelength spectral <span class="hlt">energy</span> distribution of QSO B0218+357 and use it to model the source. The GeV and sub-TeV data obtained by Fermi-LAT and MAGIC are used to set constraints on the extragalactic background light. We detected very high <span class="hlt">energy</span> <span class="hlt">gamma</span>-ray emission from the direction of QSO B0218+357 by the MAGIC telescopes during the expected time of arrival of the trailing component of the flare, making it the farthest very high <span class="hlt">energy</span> <span class="hlt">gamma</span>-ray source detected to date. We also observed emission spans the <span class="hlt">energy</span> range from 65 to 175 GeV. The combined MAGIC and Fermi-LAT spectral <span class="hlt">energy</span> distribution of QSO B0218+357 is consistent with current extragalactic background light models. The broadband emission can be modeled in the framework of a two-zone external Compton scenario, where the GeV emission comes from an emission region in the jet, located outside the broad line region.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018ApJ...859L..11J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018ApJ...859L..11J"><span>Low-<span class="hlt">energy</span> Electrons in <span class="hlt">Gamma</span>-Ray Burst Afterglow Models</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jóhannesson, Guđlaugur; Björnsson, Gunnlaugur</p> <p>2018-05-01</p> <p>Observations of <span class="hlt">gamma</span>-ray burst (GRB) afterglows have long provided the most detailed information about the origin of this spectacular phenomenon. The model that is most commonly used to extract physical properties of the event from the observations is the relativistic fireball model, where ejected material moving at relativistic speeds creates a shock wave when it interacts with the surrounding medium. Electrons are accelerated in the shock wave, generating the observed synchrotron emission through interactions with the magnetic field in the downstream medium. It is usually assumed that the accelerated electrons follow a simple power-law distribution in <span class="hlt">energy</span> between specific <span class="hlt">energy</span> boundaries, and that no electron exists outside these boundaries. This Letter explores the consequences of adding a low-<span class="hlt">energy</span> power-law segment to the electron distribution with <span class="hlt">energy</span> that contributes insignificantly to the total <span class="hlt">energy</span> budget of the distribution. The low-<span class="hlt">energy</span> electrons have a significant impact on the radio emission, providing synchrotron absorption and emission at these long wavelengths. Shorter wavelengths are affected through the normalization of the distribution. The new model is used to analyze the light curves of GRB 990510, and the resulting parameters are compared to a model without the extra electrons. The quality of the fit and the best-fit parameters are significantly affected by the additional model component. The new component is in one case found to strongly affect the X-ray light curves, showing how changes to the model at radio frequencies can affect light curves at other frequencies through changes in best-fit model parameters.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li class="active"><span>17</span></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_17 --> <div id="page_18" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li class="active"><span>18</span></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="341"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008HEAD...10.3605W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008HEAD...10.3605W"><span>The <span class="hlt">Gamma</span>-Ray Imager GRI</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wunderer, Cornelia B.; GRI Collaboration</p> <p>2008-03-01</p> <p>Observations of the <span class="hlt">gamma</span>-ray sky reveal the most powerful sources and the most violent events in the Universe. While at lower wavebands the observed emission is generally dominated by thermal processes, the <span class="hlt">gamma</span>-ray sky provides us with a view on the non-thermal Universe. Here particles are accelerated to extreme relativistic <span class="hlt">energies</span> by mechanisms which are still poorly understood, and nuclear reactions are synthesizing the basic constituents of our world. Cosmic accelerators and cosmic explosions are major science themes that are addressed in the <span class="hlt">gamma</span>-ray regime. ESA's INTEGRAL observatory currently provides the astronomical community with a unique tool to investigate the sky up to MeV <span class="hlt">energies</span> and hundreds of sources, new classes of objects, extraordinary views of antimatter annihilation in our Galaxy, and fingerprints of recent nucleosynthesis processes have been discovered. NASA's GLAST mission will similarly take the next step in surveying the high-<span class="hlt">energy</span> ( GeV) sky, and NuSTAR will pioneer focusing observations at hard X-ray <span class="hlt">energies</span> (to 80 keV). There will be clearly a growing need to perform deeper, more focused investigations of <span class="hlt">gamma</span>-ray sources in the 100-keV to MeV regime. Recent technological advances in the domain of <span class="hlt">gamma</span>-ray focusing using Laue diffraction and multilayer-coated mirror techniques have paved the way towards a <span class="hlt">gamma</span>-ray mission, providing major improvements compared to past missions regarding sensitivity and angular resolution. Such a future <span class="hlt">Gamma</span>-Ray Imager will allow the study of particle acceleration processes and explosion physics in unprecedented detail, providing essential clues on the innermost nature of the most violent and most energetic processes in the Universe.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26410785','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26410785"><span>Highly fluorescent carbon dots for visible sensing of doxorubicin <span class="hlt">release</span> based on efficient nanosurface <span class="hlt">energy</span> transfer.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Wang, Beibei; Wang, Shujun; Wang, Yanfang; Lv, Yan; Wu, Hao; Ma, Xiaojun; Tan, Mingqian</p> <p>2016-01-01</p> <p>To prepare fluorescent carbon dots for loading cationic anticancer drug through donor-quenched nanosurface <span class="hlt">energy</span> transfer in visible sensing of drug <span class="hlt">release</span>. Highly fluorescent carbon dots (CDs) were prepared by a facile hydrothermal approach from citric acid and o-phenylenediamine. The obtained CDs showed a high quantum yield of 46 % and exhibited good cytocompatibility even at 1 mg/ml. The cationic anticancer drug doxorubicin (DOX) can be loaded onto the negatively charged CDs through electrostatic interactions. Additionally, the fluorescent CDs feature reversible donor-quenched mode nanosurface <span class="hlt">energy</span> transfer. When loading the <span class="hlt">energy</span> receptor DOX, the donor CDs' fluorescence was switched "off", while it turned "on" again after DOX <span class="hlt">release</span> from the surface through endocytic uptake. Most DOX molecules were <span class="hlt">released</span> from the CDs after 6 h incubation and entered cell nuclear region after 8 h, suggesting the drug delivery system may have potential for visible sensing in drug <span class="hlt">release</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/20360067','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/20360067"><span>Fermi <span class="hlt">gamma</span>-ray imaging of a radio galaxy.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Abdo, A A; Ackermann, M; Ajello, M; Atwood, W B; Baldini, L; Ballet, J; Barbiellini, G; Bastieri, D; Baughman, B M; Bechtol, K; Bellazzini, R; Berenji, B; Blandford, R D; Bloom, E D; Bonamente, E; Borgland, A W; Bregeon, J; Brez, A; Brigida, M; Bruel, P; Burnett, T H; Buson, S; Caliandro, G A; Cameron, R A; Caraveo, P A; Casandjian, J M; Cavazzuti, E; Cecchi, C; Celik, O; Chekhtman, A; Cheung, C C; Chiang, J; Ciprini, S; Claus, R; Cohen-Tanugi, J; Colafrancesco, S; Cominsky, L R; Conrad, J; Costamante, L; Cutini, S; Davis, D S; Dermer, C D; de Angelis, A; de Palma, F; Digel, S W; do Couto e Silva, E; Drell, P S; Dubois, R; Dumora, D; Farnier, C; Favuzzi, C; Fegan, S J; Finke, J; Focke, W B; Fortin, P; Fukazawa, Y; Funk, S; Fusco, P; Gargano, F; Gasparrini, D; Gehrels, N; Georganopoulos, M; Germani, S; Giebels, B; Giglietto, N; Giordano, F; Giroletti, M; Glanzman, T; Godfrey, G; Grenier, I A; Grove, J E; Guillemot, L; Guiriec, S; Hanabata, Y; Harding, A K; Hayashida, M; Hays, E; Hughes, R E; Jackson, M S; Jóhannesson, G; Johnson, A S; Johnson, T J; Johnson, W N; Kamae, T; Katagiri, H; Kataoka, J; Kawai, N; Kerr, M; Knödlseder, J; Kocian, M L; Kuss, M; Lande, J; Latronico, L; Lemoine-Goumard, M; Longo, F; Loparco, F; Lott, B; Lovellette, M N; Lubrano, P; Madejski, G M; Makeev, A; Mazziotta, M N; McConville, W; McEnery, J E; Meurer, C; Michelson, P F; Mitthumsiri, W; Mizuno, T; Moiseev, A A; Monte, C; Monzani, M E; Morselli, A; Moskalenko, I V; Murgia, S; Nolan, P L; Norris, J P; Nuss, E; Ohsugi, T; Omodei, N; Orlando, E; Ormes, J F; Paneque, D; Parent, D; Pelassa, V; Pepe, M; Pesce-Rollins, M; Piron, F; Porter, T A; Rainò, S; Rando, R; Razzano, M; Razzaque, S; Reimer, A; Reimer, O; Reposeur, T; Ritz, S; Rochester, L S; Rodriguez, A Y; Romani, R W; Roth, M; Ryde, F; Sadrozinski, H F-W; Sambruna, R; Sanchez, D; Sander, A; Saz Parkinson, P M; Scargle, J D; Sgrò, C; Siskind, E J; Smith, D A; Smith, P D; Spandre, G; Spinelli, P; Starck, J-L; Stawarz, Ł; Strickman, M S; Suson, D J; Tajima, H; Takahashi, H; Takahashi, T; Tanaka, T; Thayer, J B; Thayer, J G; Thompson, D J; Tibaldo, L; Torres, D F; Tosti, G; Tramacere, A; Uchiyama, Y; Usher, T L; Vasileiou, V; Vilchez, N; Vitale, V; Waite, A P; Wallace, E; Wang, P; Winer, B L; Wood, K S; Ylinen, T; Ziegler, M; Hardcastle, M J; Kazanas, D</p> <p>2010-05-07</p> <p>The Fermi <span class="hlt">Gamma</span>-ray Space Telescope has detected the <span class="hlt">gamma</span>-ray glow emanating from the giant radio lobes of the radio galaxy Centaurus A. The resolved <span class="hlt">gamma</span>-ray image shows the lobes clearly separated from the central active source. In contrast to all other active galaxies detected so far in high-<span class="hlt">energy</span> <span class="hlt">gamma</span>-rays, the lobe flux constitutes a considerable portion (greater than one-half) of the total source emission. The <span class="hlt">gamma</span>-ray emission from the lobes is interpreted as inverse Compton-scattered relic radiation from the cosmic microwave background, with additional contribution at higher <span class="hlt">energies</span> from the infrared-to-optical extragalactic background light. These measurements provide <span class="hlt">gamma</span>-ray constraints on the magnetic field and particle <span class="hlt">energy</span> content in radio galaxy lobes, as well as a promising method to probe the cosmic relic photon fields.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/18167121','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/18167121"><span>Lactobacillus GG has in vitro effects on enhanced interleukin-10 and interferon-<span class="hlt">gamma</span> <span class="hlt">release</span> of mononuclear cells but no in vivo effects in supplemented mothers and their neonates.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Kopp, M V; Goldstein, M; Dietschek, A; Sofke, J; Heinzmann, A; Urbanek, R</p> <p>2008-04-01</p> <p>The value of probiotics for primary prevention is controversial. Moreover, only little is known about the underlying immunological mechanisms of action. Therefore, we assessed the proliferative response and cytokine <span class="hlt">release</span> in cultures of isolated mononuclear cells from pregnant women and their neonates supplemented with Lactobacillus GG (LGG) or placebo. In a double-blind, placebo-controlled prospective trial, pregnant women with at least one first-degree relative or a partner with an atopic disease were randomly assigned to receive either the probiotic LGG (ATCC 53103; 5 x 10(9) colony-forming units LGG twice daily) or placebo 4-6 weeks before expected delivery, followed by a post-natal period of 6 months. Cord blood mononuclear cells (CBMC) and peripheral blood mononuclear cells (PBMC) of the corresponding mother were isolated from cord blood and peripheral blood (n=68). The proliferative response of CBMC and PBMC was expressed as the stimulation index (SI), which was calculated according to the ratio between the mean counts per minute (c.p.m.) values measured in the wells with stimulated cells and the mean c.p.m. values measured in the wells with unstimulated cells. Additionally, the cytokines IFN-<span class="hlt">gamma</span>, IL-10 and IL-13 in the cell culture supernatants were measured using the ELISA technique. No difference was observed between the LGG-supplemented group and the placebo group in terms of the proliferative capacity of maternal or neonatal cord blood cells in response to IL-2, beta-lactoglobulin or LGG. In vitro stimulation with LGG resulted in significantly enhanced <span class="hlt">release</span> of IL-10 and IFN-<span class="hlt">gamma</span>, compared with cytokine <span class="hlt">release</span> in unstimulated controls. However, this phenomenon was observed in supernatants of maternal and neonatal MC in both groups, independent of prior supplementation with LGG. LGG has in vitro effects on enhanced IL-10 and IFN-<span class="hlt">gamma</span> <span class="hlt">release</span> of mononuclear cells. However, supplementation with LGG during pregnancy did not alter the proliferative</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/15858565','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/15858565"><span>An exceptionally bright flare from SGR 1806-20 and the origins of short-duration <span class="hlt">gamma</span>-ray bursts.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Hurley, K; Boggs, S E; Smith, D M; Duncan, R C; Lin, R; Zoglauer, A; Krucker, S; Hurford, G; Hudson, H; Wigger, C; Hajdas, W; Thompson, C; Mitrofanov, I; Sanin, A; Boynton, W; Fellows, C; von Kienlin, A; Lichti, G; Rau, A; Cline, T</p> <p>2005-04-28</p> <p>Soft-<span class="hlt">gamma</span>-ray repeaters (SGRs) are galactic X-ray stars that emit numerous short-duration (about 0.1 s) bursts of hard X-rays during sporadic active periods. They are thought to be magnetars: strongly magnetized neutron stars with emissions powered by the dissipation of magnetic <span class="hlt">energy</span>. Here we report the detection of a long (380 s) giant flare from SGR 1806-20, which was much more luminous than any previous transient event observed in our Galaxy. (In the first 0.2 s, the flare <span class="hlt">released</span> as much <span class="hlt">energy</span> as the Sun radiates in a quarter of a million years.) Its power can be explained by a catastrophic instability involving global crust failure and magnetic reconnection on a magnetar, with possible large-scale untwisting of magnetic field lines outside the star. From a great distance this event would appear to be a short-duration, hard-spectrum cosmic <span class="hlt">gamma</span>-ray burst. At least a significant fraction of the mysterious short-duration <span class="hlt">gamma</span>-ray bursts may therefore come from extragalactic magnetars.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018ApJS..234....3G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018ApJS..234....3G"><span>Low-<span class="hlt">energy</span> Spectra of <span class="hlt">Gamma</span>-Ray Bursts from Cooling Electrons</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Geng, Jin-Jun; Huang, Yong-Feng; Wu, Xue-Feng; Zhang, Bing; Zong, Hong-Shi</p> <p>2018-01-01</p> <p>The low-<span class="hlt">energy</span> spectra of <span class="hlt">gamma</span>-ray bursts’ (GRBs) prompt emission are closely related to the <span class="hlt">energy</span> distribution of electrons, which is further regulated by their cooling processes. We develop a numerical code to calculate the evolution of the electron distribution with given initial parameters, in which three cooling processes (i.e., adiabatic, synchrotron, and inverse Compton cooling) and the effect of a decaying magnetic field are coherently considered. A sequence of results is presented by exploring the plausible parameter space for both the fireball and the Poynting flux–dominated regime. Different cooling patterns for the electrons can be identified, and they are featured by a specific dominant cooling mechanism. Our results show that the hardening of the low-<span class="hlt">energy</span> spectra can be attributed to the dominance of synchrotron self-Compton cooling within the internal shock model or to decaying synchrotron cooling within the Poynting flux–dominated jet scenario. These two mechanisms can be distinguished by observing the hard low-<span class="hlt">energy</span> spectra of isolated short pulses in some GRBs. The dominance of adiabatic cooling can also lead to hard low-<span class="hlt">energy</span> spectra when the ejecta is moving at an extreme relativistic speed. The information from the time-resolved low-<span class="hlt">energy</span> spectra can help to probe the physical characteristics of the GRB ejecta via our numerical results.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19910071981&hterms=nolan&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3Dnolan','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19910071981&hterms=nolan&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3Dnolan"><span>Lunar occultations for <span class="hlt">gamma</span>-ray source measurements</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Koch, David G.; Hughes, E. B.; Nolan, Patrick L.</p> <p>1990-01-01</p> <p>The unambiguous association of discrete <span class="hlt">gamma</span>-ray sources with objects radiating at other wavelengths, the separation of discrete sources from the extended emission within the Galaxy, the mapping of <span class="hlt">gamma</span>-ray emission from nearby galaxies and the measurement of structure within a discrete source cannot presently be accomplished at <span class="hlt">gamma</span>-ray <span class="hlt">energies</span>. In the past, the detection processes used in high-<span class="hlt">energy</span> <span class="hlt">gamma</span>-ray astronomy have not allowed for good angular resolution. This problem can be overcome by placing <span class="hlt">gamma</span>-ray detectors on the moon and using the horizon as an occulting edge to achieve arcsec resolution. For purposes of discussion, this concept is examined for <span class="hlt">gamma</span> rays above 100 MeV for which pair production dominates the detection process and locally-generated nuclear <span class="hlt">gamma</span> rays do not contribute to the background.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19860022013','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19860022013"><span><span class="hlt">Gamma</span>-ray line astrophysics</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Lingenfelter, R. E.; Ramaty, R.</p> <p>1986-01-01</p> <p>Recent observations of <span class="hlt">gamma</span>-ray line emission from solar flares, <span class="hlt">gamma</span>-ray bursts, the galactic center, the interstellar medium and the jets of SS433 are reviewed. The implications of these observations on high <span class="hlt">energy</span> processes in these sources are discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1426668','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1426668"><span>The Dark <span class="hlt">Energy</span> Survey Data <span class="hlt">Release</span> 1</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Abbott, T.M.C.; et al.</p> <p></p> <p>We describe the first public data <span class="hlt">release</span> of the Dark <span class="hlt">Energy</span> Survey, DES DR1, consisting of reduced single epoch images, coadded images, coadded source catalogs, and associated products and services assembled over the first three years of DES science operations. DES DR1 is based on optical/near-infrared imaging from 345 distinct nights (August 2013 to February 2016) by the Dark <span class="hlt">Energy</span> Camera mounted on the 4-m Blanco telescope at Cerro Tololo Inter-American Observatory in Chile. We <span class="hlt">release</span> data from the DES wide-area survey covering ~5,000 sq. deg. of the southern Galactic cap in five broad photometric bands, grizY. DES DR1 hasmore » a median delivered point-spread function of g = 1.12, r = 0.96, i = 0.88, z = 0.84, and Y = 0.90 arcsec FWHM, a photometric precision of < 1% in all bands, and an astrometric precision of 151 mas. The median coadded catalog depth for a 1.95" diameter aperture at S/N = 10 is g = 24.33, r = 24.08, i = 23.44, z = 22.69, and Y = 21.44 mag. DES DR1 includes nearly 400M distinct astronomical objects detected in ~10,000 coadd tiles of size 0.534 sq. deg. produced from ~39,000 individual exposures. Benchmark galaxy and stellar samples contain ~310M and ~ 80M objects, respectively, following a basic object quality selection. These data are accessible through a range of interfaces, including query web clients, image cutout servers, jupyter notebooks, and an interactive coadd image visualization tool. DES DR1 constitutes the largest photometric data set to date at the achieved depth and photometric precision.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EPJC...77...20A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EPJC...77...20A"><span>Stacked search for time shifted high <span class="hlt">energy</span> neutrinos from <span class="hlt">gamma</span> ray bursts with the Antares neutrino telescope</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Adrián-Martínez, S.; Albert, A.; André, M.; Anghinolfi, M.; Anton, G.; Ardid, M.; Aubert, J.-J.; Baret, B.; Barrios-Marti, J.; Basa, S.; Bertin, V.; Biagi, S.; Bormuth, R.; Bouwhuis, M. C.; Bruijn, R.; Brunner, J.; Busto, J.; Capone, A.; Caramete, L.; Carr, J.; Chiarusi, T.; Circella, M.; Coniglione, R.; Costantini, H.; Coyle, P.; Creusot, A.; Dekeyser, I.; Deschamps, A.; De Bonis, G.; Distefano, C.; Donzaud, C.; Dornic, D.; Drouhin, D.; Dumas, A.; Eberl, T.; Elsässer, D.; Enzenhöfer, A.; Fehn, K.; Felis, I.; Fermani, P.; Folger, F.; Fusco, L. A.; Galatà, S.; Gay, P.; Geißelsöder, S.; Geyer, K.; Giordano, V.; Gleixner, A.; Gracia-Ruiz, R.; Graf, K.; Hallmann, S.; van Haren, H.; Heijboer, A. J.; Hello, Y.; Hernández-Rey, J. J.; Hößl, J.; Hofestädt, J.; Hugon, C.; James, C. W.; de Jong, M.; Kadler, M.; Kalekin, O.; Katz, U.; Kießling, D.; Kooijman, P.; Kouchner, A.; Kreter, M.; Kreykenbohm, I.; Kulikovskiy, V.; Lahmann, R.; Lefèvre, D.; Leonora, E.; Loucatos, S.; Marcelin, M.; Margiotta, A.; Marinelli, A.; Martínez-Mora, J. A.; Mathieu, A.; Michael, T.; Migliozzi, P.; Moussa, A.; Müller, C.; Nezri, E.; Păvălaş, G. E.; Pellegrino, C.; Perrina, C.; Piattelli, P.; Popa, V.; Pradier, T.; Racca, C.; Riccobene, G.; Richter, R.; Roensch, K.; Saldaña, M.; Samtleben, D. F. E.; Sánchez-Losa, A.; Sanguineti, M.; Sapienza, P.; Schmid, J.; Schnabel, J.; Schüssler, F.; Seitz, T.; Sieger, C.; Spurio, M.; Steijger, J. J. M.; Stolarczyk, Th.; Taiuti, M.; Tamburini, C.; Trovato, A.; Tselengidou, M.; Tönnis, C.; Vallage, B.; Vallée, C.; Van Elewyck, V.; Visser, E.; Vivolo, D.; Wagner, S.; Wilms, J.; Zornoza, J. D.; Zúñiga, J.</p> <p>2017-01-01</p> <p>A search for high-<span class="hlt">energy</span> neutrino emission correlated with <span class="hlt">gamma</span>-ray bursts outside the electromagnetic prompt-emission time window is presented. Using a stacking approach of the time delays between reported <span class="hlt">gamma</span>-ray burst alerts and spatially coincident muon-neutrino signatures, data from the Antares neutrino telescope recorded between 2007 and 2012 are analysed. One year of public data from the IceCube detector between 2008 and 2009 have been also investigated. The respective timing profiles are scanned for statistically significant accumulations within 40 days of the <span class="hlt">Gamma</span> Ray Burst, as expected from Lorentz Invariance Violation effects and some astrophysical models. No significant excess over the expected accidental coincidence rate could be found in either of the two data sets. The average strength of the neutrino signal is found to be fainter than one detectable neutrino signal per hundred <span class="hlt">gamma</span>-ray bursts in the Antares data at 90% confidence level.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/491616','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/491616"><span>Thermal-neutron capture <span class="hlt">gamma</span>-rays. Volume 1</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Tuli, J.K.</p> <p>1997-05-01</p> <p>The <span class="hlt">energy</span> and photon intensity of <span class="hlt">gamma</span> rays as seen in thermal-neutron capture are presented in ascending order of <span class="hlt">gamma</span> <span class="hlt">energy</span>. All those <span class="hlt">gamma</span>-rays with intensity of {ge} 2% of the strongest transition are included. The two strongest transitions seen for the target nuclide are indicated in each case. Where the target nuclide mass number is indicated as nat the natural target was used. The <span class="hlt">gamma</span> <span class="hlt">energies</span> given are in keV. The <span class="hlt">gamma</span> intensities given are relative to 100 for the strongest transition. All data for A > 44 are taken from Evaluated Nuclear Structure Data File (4/97), a computermore » file of evaluated nuclear structure data maintained by the National Nuclear Data Center, Brookhaven National Laboratory, on behalf of the Nuclear Structure and Decay and Decay Data network, coordinated by the International Atomic <span class="hlt">Energy</span> Agency, Vienna. These data are published in Nuclear Data Sheets, Academic Press, San Diego, CA. The data for A {le} 44 is taken from ``Prompt <span class="hlt">Gamma</span> Rays from Thermal-Neutron Capture,`` M.A. Lone, R.A. Leavitt, D.A. Harrison, Atomic Data and Nuclear Data Tables 26, 511 (1981).« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22011802-detection-gamma-ray-binary-ls-+61-degree-sign-low-flux-state-very-high-energy-gamma-rays-magic-telescopes','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22011802-detection-gamma-ray-binary-ls-+61-degree-sign-low-flux-state-very-high-energy-gamma-rays-magic-telescopes"><span>DETECTION OF THE {<span class="hlt">gamma</span>}-RAY BINARY LS I +61 Degree-Sign 303 IN A LOW-FLUX STATE AT VERY HIGH <span class="hlt">ENERGY</span> {<span class="hlt">gamma</span>}-RAYS WITH THE MAGIC TELESCOPES IN 2009</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Aleksic, J.; Blanch, O.; Alvarez, E. A.</p> <p>2012-02-10</p> <p>We present very high <span class="hlt">energy</span> (E > 100 GeV) {<span class="hlt">gamma</span>}-ray observations of the {<span class="hlt">gamma</span>}-ray binary system LS I +61 Degree-Sign 303 obtained with the MAGIC stereo system between 2009 October and 2010 January. We detect a 6.3{sigma} {<span class="hlt">gamma</span>}-ray signal above 400 GeV in the combined data set. The integral flux above an <span class="hlt">energy</span> of 300 GeV is F(E > 300 GeV) = (1.4 {+-} 0.3{sub stat} {+-} 0.4{sub syst}) Multiplication-Sign 10{sup -12} cm{sup -2} s{sup -1}, which corresponds to about 1.3% of the Crab Nebula flux in the same <span class="hlt">energy</span> range. The orbit-averaged flux of LS I +61 Degree-Sign 303more » in the orbital phase interval 0.6-0.7, where a maximum of the TeV flux is expected, is lower by almost an order of magnitude compared to our previous measurements between 2005 September and 2008 January. This provides evidence for a new low-flux state in LS I +61 Degree-Sign 303. We find that the change to the low-flux state cannot be solely explained by an increase of photon-photon absorption around the compact star.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013JPhCS.451a2014M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013JPhCS.451a2014M"><span>Dynamic <span class="hlt">energy</span> <span class="hlt">release</span> rate in couple-stress elasticity</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Morini, L.; Piccolroaz, A.; Mishuris, G.</p> <p>2013-07-01</p> <p>This paper is concerned with <span class="hlt">energy</span> <span class="hlt">release</span> rate for dynamic steady state crack problems in elastic materials with microstructures. A Mode III semi-infinite crack subject to loading applied on the crack surfaces is considered. The micropolar behaviour of the material is described by the theory of couple-stress elasticity developed by Koiter. A general expression for the dynamic J-integral including both traslational and micro-rotational inertial contributions is derived, and the conservation of this integral on a path surrounding the crack tip is demonstrated.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22156659-gamma-rays-from-centaurus','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22156659-gamma-rays-from-centaurus"><span><span class="hlt">Gamma</span> rays from Centaurus A</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Gupta, Nayantara, E-mail: nayan@phy.iitb.ac.in</p> <p>2008-06-15</p> <p>Centaurus A, the cosmic ray accelerator a few Mpc away from us, is possibly one of the nearest sources of extremely high <span class="hlt">energy</span> cosmic rays. We investigate whether the <span class="hlt">gamma</span> ray data currently available from Centaurus A in the GeV-TeV <span class="hlt">energy</span> band can be explained with only proton-proton interactions. We show that for a single power law proton spectrum, mechanisms of {<span class="hlt">gamma</span>}-ray production other than proton-proton interactions are needed inside this radio-galaxy to explain the <span class="hlt">gamma</span> ray flux observed by EGRET, upper limits from HESS/CANGAROO-III and the correlated extremely energetic cosmic ray events observed by the Pierre Auger experiment. Inmore » future, with better {<span class="hlt">gamma</span>}-ray data, and simultaneous observation with {<span class="hlt">gamma</span>}-ray and cosmic ray detectors, it will be possible to carry out such studies on different sources in more detail.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018APh....99...34A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018APh....99...34A"><span>Design and expected performance of a novel hybrid detector for very-high-<span class="hlt">energy</span> <span class="hlt">gamma</span>-ray astrophysics</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Assis, P.; Barres de Almeida, U.; Blanco, A.; Conceição, R.; D'Ettorre Piazzoli, B.; De Angelis, A.; Doro, M.; Fonte, P.; Lopes, L.; Matthiae, G.; Pimenta, M.; Shellard, R.; Tomé, B.</p> <p>2018-05-01</p> <p>Current detectors for Very-High-<span class="hlt">Energy</span> γ-ray astrophysics are either pointing instruments with a small field of view (Cherenkov telescopes), or large field-of-view instruments with relatively large <span class="hlt">energy</span> thresholds (extensive air shower detectors). In this article, we propose a new hybrid extensive air shower detector sensitive in an <span class="hlt">energy</span> region starting from about 100 GeV. The detector combines a small water-Cherenkov detector, able to provide a calorimetric measurement of shower particles at ground, with resistive plate chambers which contribute significantly to the accurate shower geometry reconstruction. A full simulation of this detector concept shows that it is able to reach better sensitivity than any previous <span class="hlt">gamma</span>-ray wide field-of-view experiment in the sub-TeV <span class="hlt">energy</span> region. It is expected to detect with a 5σ significance a source fainter than the Crab Nebula in one year at 100 GeV and, above 1 TeV a source as faint as 10% of it. As such, this instrument is suited to detect transient phenomena making it a very powerful tool to trigger observations of variable sources and to detect transients coupled to gravitational waves and <span class="hlt">gamma</span>-ray bursts.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010PhPl...17a2109B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010PhPl...17a2109B"><span><span class="hlt">Energy</span> <span class="hlt">release</span> and transfer in guide field reconnection</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Birn, J.; Hesse, M.</p> <p>2010-01-01</p> <p>Properties of <span class="hlt">energy</span> <span class="hlt">release</span> and transfer by magnetic reconnection in the presence of a guide field are investigated on the basis of 2.5-dimensional magnetohydrodynamic (MHD) and particle-in-cell (PIC) simulations. Two initial configurations are considered: a plane current sheet with a uniform guide field of 80% of the reconnecting magnetic field component and a force-free current sheet in which the magnetic field strength is constant but the field direction rotates by 180° through the current sheet. The onset of reconnection is stimulated by localized, temporally limited compression. Both MHD and PIC simulations consistently show that the outgoing <span class="hlt">energy</span> fluxes are dominated by (redirected) Poynting flux and enthalpy flux, whereas bulk kinetic <span class="hlt">energy</span> flux and heat flux (in the PIC simulation) are small. The Poynting flux is mainly associated with the magnetic <span class="hlt">energy</span> of the guide field which is carried from inflow to outflow without much alteration. The conversion of annihilated magnetic <span class="hlt">energy</span> to enthalpy flux (that is, thermal <span class="hlt">energy</span>) stems mainly from the fact that the outflow occurs into a closed field region governed by approximate force balance between Lorentz and pressure gradient forces. Therefore, the <span class="hlt">energy</span> converted from magnetic to kinetic <span class="hlt">energy</span> by Lorentz force acceleration becomes immediately transferred to thermal <span class="hlt">energy</span> by the work done by the pressure gradient force. Strong similarities between late stages of MHD and PIC simulations result from the fact that conservation of mass and entropy content and footpoint displacement of magnetic flux tubes, imposed in MHD, are also approximately satisfied in the PIC simulations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2003EAEJA.....9933F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2003EAEJA.....9933F"><span>Carbon dioxide degassing and thermal <span class="hlt">energy</span> <span class="hlt">release</span> at Vesuvio (Italy)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Frondini, F.; Chiodini, G.; Caliro, S.; Cardellini, C.; Granieri, D.</p> <p>2003-04-01</p> <p>At Vesuvio, basing on the data of the CO2 flux surveys carried out in April and May 2000, are discharged about 130 t d-1 of CO2 through soil diffuse degassing. In the crater area the distribution of the soil temperatures show a general correspondence between the CO2 flux anomalies and the high temperatures, suggesting that the heating of the soil is mainly due to the condensation of the rising volcanic-hydrothermal fluids. Considering that the original H2O/CO2 ratio of hydrothermal fluids is recorded by fumarolic effluents, the steam associated to the CO2 output has been computed and amount to is 475 t d-1. The <span class="hlt">energy</span> produced by the steam condensation and cooling of the liquid phase is 1.26 1012 J d-1 (14.6 MW). The amounts of gas and <span class="hlt">energy</span> <span class="hlt">released</span> by Vesuvio are comparable to those <span class="hlt">released</span> by other volcanic degassing areas of the world and their estimates, through periodical CO2 flux surveys, can constitute a powerful tool to monitor the activity of the volcano.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018AAS...23144023P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018AAS...23144023P"><span>Examining the nature of very-high-<span class="hlt">energy</span> <span class="hlt">gamma</span>-ray emission from the AGN PKS 1222+216 and 3C 279</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Price, Sharleen; Brill, Ari; Mukherjee, Reshmi; VERITAS</p> <p>2018-01-01</p> <p>Blazars are a type of active galactic nuclei (AGN) that emit jets of ionized matter which move towards the Earth at relativistic speeds. In this research we carried out a study of two objects, 3C 279 and PKS 1222+216, which belong to the subset of blazars known as FSRQs (flat spectrum radio quasars), the most powerful TeV-detected sources at <span class="hlt">gamma</span>-ray <span class="hlt">energies</span> with bolometric luminosities exceeding 1048 erg/s. The high-<span class="hlt">energy</span> emission of quasars peaks in the MeV-GeV band, making these sources very rarely detectable in the TeV <span class="hlt">energy</span> range. In fact, only six FSRQs have ever been detected in this range by very-high-<span class="hlt">energy</span> <span class="hlt">gamma</span>-ray telescopes. We will present results from observing campaigns on 3C 279 in 2014 and 2016, when the object was detected in high flux states by Fermi-LAT. Observations include simultaneous coverage with the Fermi-LAT satellite and the VERITAS ground-based array spanning four decades in <span class="hlt">energy</span> from 100 MeV to 1 TeV. We will also report VERITAS observations of PKS 1222+216 between 2008 and 2017. The detection/non-detection of TeV emission during flaring episodes at MeV <span class="hlt">energies</span> will further contribute to our understanding of particle acceleration and <span class="hlt">gamma</span>-ray emission mechanisms in blazar jets.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20000017959','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20000017959"><span>COMPTEL Studies of <span class="hlt">Gamma</span>-Ray Bursts at MeV <span class="hlt">Energies</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>McConnell, Mark L.</p> <p>1999-01-01</p> <p>The purpose of this program was to analyse and interpret <span class="hlt">gamma</span>-ray burst (GRB) data using both telescope mode data and single detector burst mode data from COMPTEL. Collectively, these data span the <span class="hlt">energy</span> range from 300 keV up to 30 MeV. The initial goal of our proposal was to perform a standard analysis for each significant GRB event seen by COMPTEL. This includes GRBs that are registered by the telescope mode data as well as GRBs that are registered only in the burst mode data. (The latter category includes both GRBs that he outside of the FoV as well as GRBs within the FoV that are too weak to be seen in the telescope mode.) A second goal of our proposal was to define a set of data products (including deconvolved photon spectra) that, for each detected GRB event, would be made available via the COMPTEL GRB Web Page. The third goal of our program was to perform more detailed studies of selected GRB events. This represented a continuation of past GRB studies by the COMPTEL team. In general, we have met with only limited success in achieving these goals, in part due to the limited resources provided and our philosophy of utilizing local high school students to participate in this effort. Using local high school student support, however, we expect that considerable progress will be made in our efforts to catalog the COMPTEL <span class="hlt">gamma</span>-ray burst data between now and the end of the current academic year. In addition, observations with COMPTEL contributed to an analysis of GRB 990123, the first <span class="hlt">gamma</span>-ray burst with simultaneous optical observations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20030002464&hterms=sources+energy&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dsources%2Benergy','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20030002464&hterms=sources+energy&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dsources%2Benergy"><span>The BATSE Earth Occultation Catalog of Low <span class="hlt">Energy</span> <span class="hlt">Gamma</span> Ray Sources</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Harmon, B. A.; WilsonHodge, C. A.; Fishman, G. J.; Paciesas, W.</p> <p>2002-01-01</p> <p>The Burst and Transient Source Experiment (BATSE), aboard the Compton <span class="hlt">Gamma</span> Ray Observatory (CGRO), provided a record of the hard X-ray/low <span class="hlt">energy</span> <span class="hlt">gamma</span> ray sky between April 1991 and June 2000. During that time, a catalog of known sources was derived from existing catalogs such as HEAO A-4, as well as new transient sources discovered with BATSE and other X-ray monitors operating in the CGRO era. The Earth Occultation Technique was used to monitor a combination of these sources, mostly galactic, totaling to about 175 objects. The catalog will present the global properties of these sources and their probability of detection (> 10 mCrab, 20-100 keV) with BATSE. Systematic errors due to unknown sources or background components are included. Cursory analyses to search for new transients (35-80 mCrab in the 20-100 keV band) and super-orbital periods in known binary sources are also presented. Whole mission light curves and associated data production/analysis tools are being delivered to the HEASARC for public use.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li class="active"><span>18</span></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_18 --> <div id="page_19" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li class="active"><span>19</span></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="361"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/897937','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/897937"><span>Kinetic Modeling of Slow <span class="hlt">Energy</span> <span class="hlt">Release</span> in Non-Ideal Carbon Rich Explosives</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Vitello, P; Fried, L; Glaesemann, K</p> <p>2006-06-20</p> <p>We present here the first self-consistent kinetic based model for long time-scale <span class="hlt">energy</span> <span class="hlt">release</span> in detonation waves in the non-ideal explosive LX-17. Non-ideal, insensitive carbon rich explosives, such as those based on TATB, are believed to have significant late-time slow <span class="hlt">release</span> in <span class="hlt">energy</span>. One proposed source of this <span class="hlt">energy</span> is diffusion-limited growth of carbon clusters. In this paper we consider the late-time <span class="hlt">energy</span> <span class="hlt">release</span> problem in detonation waves using the thermochemical code CHEETAH linked to a multidimensional ALE hydrodynamics model. The linked CHEETAH-ALE model dimensional treats slowly reacting chemical species using kinetic rate laws, with chemical equilibrium assumed for speciesmore » coupled via fast time-scale reactions. In the model presented here we include separate rate equations for the transformation of the un-reacted explosive to product gases and for the growth of a small particulate form of condensed graphite to a large particulate form. The small particulate graphite is assumed to be in chemical equilibrium with the gaseous species allowing for coupling between the instantaneous thermodynamic state and the production of graphite clusters. For the explosive burn rate a pressure dependent rate law was used. Low pressure freezing of the gas species mass fractions was also included to account for regions where the kinetic coupling rates become longer than the hydrodynamic time-scales. The model rate parameters were calibrated using cylinder and rate-stick experimental data. Excellent long time agreement and size effect results were achieved.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22663057-ultra-high-energy-cosmic-rays-resultant-gamma-rays','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22663057-ultra-high-energy-cosmic-rays-resultant-gamma-rays"><span>ON ULTRA-HIGH-<span class="hlt">ENERGY</span> COSMIC RAYS AND THEIR RESULTANT <span class="hlt">GAMMA</span>-RAYS</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Gavish, Eyal; Eichler, David</p> <p>2016-05-01</p> <p>The Fermi Large Area Telescope collaboration has recently reported on 50 months of measurements of the isotropic extragalactic <span class="hlt">gamma</span>-ray background (EGRB) spectrum between 100 MeV and 820 GeV. Ultra-high-<span class="hlt">energy</span> cosmic ray (UHECR) protons interact with the cosmic microwave background photons and produce cascade photons of <span class="hlt">energies</span> 10 MeV–1 TeV that contribute to the EGRB flux. We examine seven possible evolution models for UHECRs and find that UHECR sources that evolve as the star formation rate (SFR), medium low luminosity active galactic nuclei type-1 ( L = 10{sup 43.5} erg s{sup −1} in the [0.5–2] KeV band), and BL Lacertae objectsmore » (BL Lacs) are the most acceptable given the constraints imposed by the observed EGRB. Other possibilities produce too much secondary γ -radiation. In all cases, the decaying dark matter (DM) contribution improves the fit at high <span class="hlt">energy</span>, but the contribution of still unresolved blazars, which would leave the smallest role for decaying DM, may yet provide an alternative improvement. The possibility that the entire EGRB can be fitted with resolvable but not-yet-resolved blazars, as recently claimed by Ajello et al., would leave little room in the EGRB to accommodate γ -rays from extragalactic UHECR production, even for many source evolution rates that would otherwise be acceptable. We find that under the assumption of UHECRs being mostly protons, there is not enough room for producing extragalactic UHECRs with active galactic nucleus, <span class="hlt">gamma</span>-ray burst, or even SFR source evolution. Sources that evolve as BL Lacs, on the other hand, would produce much less secondary γ -radiation and would remain a viable source of UHECRs, provided that they dominate.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20040012958','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20040012958"><span>Future Facilities for <span class="hlt">Gamma</span>-Ray Pulsar Studies</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Thompson, D. J.</p> <p>2003-01-01</p> <p>Pulsars seen at <span class="hlt">gamma</span>-ray <span class="hlt">energies</span> offer insight into particle acceleration to very high <span class="hlt">energies</span>, along with information about the geometry and interaction processes in the magnetospheres of these rotating neutron stars. During the next decade, a number of new <span class="hlt">gamma</span>-ray facilities will become available for pulsar studies. This brief review describes the motivation for <span class="hlt">gamma</span>-ray pulsar studies, the opportunities for such studies, and some specific discussion of the capabilities of the <span class="hlt">Gamma</span>-ray Large Area Space Telescope (GLAST) Large Area Telescope (LAT) for pulsar measurements.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1996ApJ...461L..37B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1996ApJ...461L..37B"><span>Electron Acceleration and Efficiency in Nonthermal <span class="hlt">Gamma</span>-Ray Sources</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bykov, A. M.; Meszaros, P.</p> <p>1996-04-01</p> <p>In energetic nonthermal sources such as <span class="hlt">gamma</span>-ray bursts, active galactic nuclei, or galactic jets, etc., one expects both relativistic and transrelativistic shocks accompanied by violent motions of moderately relativistic plasma. We present general considerations indicating that these sites are electron and positron accelerators leading to a modified power-law spectrum. The electron (or e+/-) <span class="hlt">energy</span> index is very hard, ~ <span class="hlt">gamma</span> -1 or flatter, up to a comoving frame break <span class="hlt">energy</span> <span class="hlt">gamma</span> *, and becomes steeper above that. In the example of <span class="hlt">gamma</span>-ray bursts, the Lorentz factor reaches <span class="hlt">gamma</span> * ~ 103 for e+/- accelerated by the internal shock ensemble on subhydrodynamical timescales. For pairs accelerated on hydrodynamical timescales in the external shocks, similar hard spectra are obtained, and the break Lorentz factor can be as high as <span class="hlt">gamma</span> * <~ 105. Radiation from the nonthermal electrons produces photon spectra with shapes and characteristic <span class="hlt">energies</span> in qualitative agreement with observed generic <span class="hlt">gamma</span>-ray burst and blazar spectra. The scenario described here provides a plausible way to solve one of the crucial problems of nonthermal high-<span class="hlt">energy</span> sources, namely, the efficient transfer of <span class="hlt">energy</span> from the proton flow to an appropriate nonthermal lepton component.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22661301-observable-signatures-energy-release-braided-coronal-loops','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22661301-observable-signatures-energy-release-braided-coronal-loops"><span>Observable Signatures of <span class="hlt">Energy</span> <span class="hlt">Release</span> in Braided Coronal Loops</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Pontin, D. I.; Janvier, M.; Tiwari, S. K.</p> <p></p> <p>We examine the turbulent relaxation of solar coronal loops containing non-trivial field line braiding. Such field line tangling in the corona has long been postulated in the context of coronal heating models. We focus on the observational signatures of <span class="hlt">energy</span> <span class="hlt">release</span> in such braided magnetic structures using MHD simulations and forward modeling tools. The aim is to answer the following question: if <span class="hlt">energy</span> <span class="hlt">release</span> occurs in a coronal loop containing braided magnetic flux, should we expect a clearly observable signature in emissions? We demonstrate that the presence of braided magnetic field lines does not guarantee a braided appearance to themore » observed intensities. Observed intensities may—but need not necessarily—reveal the underlying braided nature of the magnetic field, depending on the degree and pattern of the field line tangling within the loop. However, in all cases considered, the evolution of the braided loop is accompanied by localized heating regions as the loop relaxes. Factors that may influence the observational signatures are discussed. Recent high-resolution observations from Hi-C have claimed the first direct evidence of braided magnetic fields in the corona. Here we show that both the Hi-C data and some of our simulations give the appearance of braiding at a range of scales.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20110002783','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20110002783"><span>Terrestrial <span class="hlt">Gamma</span>-Ray Flashes (TGFs)</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Fishman, Gerald J.</p> <p>2010-01-01</p> <p>This slide presentation reviews the observation of Terrestrial <span class="hlt">Gamma</span> Ray Flashes (TGFs) by <span class="hlt">Gamma</span>-Ray Telescopes. These were: (1) BATSE /Compton Observatory, (2) Solar Spectroscopic Imager, (3) AGILE <span class="hlt">Gamma</span>-ray Telescope, and (4) <span class="hlt">Gamma</span>-ray Burst Monitor (GBM) on the Fermi <span class="hlt">Gamma</span>-ray Space Telescope. It contains charts which display the counts over time, a map or the TGFs observed by the Reuven Ramaty High <span class="hlt">Energy</span> Solar Spectroscopic Imager (RHESSI). and a map showing the latitude and longitude of 85 of the TGFs observed by the Fermi GBM.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/21499220-constraining-factor-sup-gamma-sup-astrophysical-energies','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/21499220-constraining-factor-sup-gamma-sup-astrophysical-energies"><span>Constraining the S factor of {sup 15}N(p,{<span class="hlt">gamma</span>}){sup 16}O at astrophysical <span class="hlt">energies</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>LeBlanc, P. J.; Goerres, J.; Beard, M.</p> <p>2010-11-15</p> <p>The {sup 15}N(p,{<span class="hlt">gamma</span>}){sup 16}O reaction represents a breakout reaction linking the first and second cycles of the CNO cycles redistributing the carbon and nitrogen abundances into the oxygen range. The reaction is dominated by two broad resonances, at E{sub p}=338 and 1028 keV, and a direct capture contribution to the ground state of {sup 16}O. Interference effects between these contributions both in the low-<span class="hlt">energy</span> region (E{sub p}<338 keV) and between the two resonances (338<E{sub p}<1028 keV) can dramatically affect the extrapolation to <span class="hlt">energies</span> of astrophysical interest. To facilitate a reliable extrapolation, the {sup 15}N(p,{<span class="hlt">gamma</span>}){sup 16}O reaction has been remeasured coveringmore » the <span class="hlt">energy</span> range from E{sub p}=1800 keV down to 130 keV. The results have been analyzed in the framework of a multilevel R-matrix theory and an S(0) value of 39.6 keV b has been found.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010ChPhL..27c8104L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010ChPhL..27c8104L"><span>Using <span class="hlt">Gamma</span>-Radiation for Drug <span class="hlt">Releasing</span> from MWNT Vehicle</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Li, Jun; Sun, Hao; Dai, Yao-Dong</p> <p>2010-03-01</p> <p>A drug delivery system via multi-walled carbon nanotube (MWNT) vehicle was synthesized in aqueous solution. MWNTs were first noncovalently functionalized with chitosan oligomers (CS) with a molecule weight of 4000-6000, making MWNTs water-soluble, and then a cancer ancillary drug tea polyphenols (TP) was conjugated mainly via the hydrogen bond between CS and TP molecules, making MWNTs efficient vehicle for drug delivering. The <span class="hlt">release</span> of drug molecules can be realized by pH variation and γ-radiation, leading to new methods for controlling drug <span class="hlt">release</span> from carbon nanotubes carrier. Due to the high penetrability of γ-rays, γ-radiation shows up new opportunities in controlled drug <span class="hlt">release</span>, possibly facilitating the future cancer treatment in vivo.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22597129-gamma-ray-imager-diii-tokamak','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22597129-gamma-ray-imager-diii-tokamak"><span><span class="hlt">Gamma</span> ray imager on the DIII-D tokamak</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Pace, D. C., E-mail: pacedc@fusion.gat.com; Taussig, D.; Eidietis, N. W.</p> <p>2016-04-15</p> <p>A <span class="hlt">gamma</span> ray camera is built for the DIII-D tokamak [J. Luxon, Nucl. Fusion 42, 614 (2002)] that provides spatial localization and <span class="hlt">energy</span> resolution of <span class="hlt">gamma</span> flux by combining a lead pinhole camera with custom-built detectors and optimized viewing geometry. This diagnostic system is installed on the outer midplane of the tokamak such that its 123 collimated sightlines extend across the tokamak radius while also covering most of the vertical extent of the plasma volume. A set of 30 bismuth germanate detectors can be secured in any of the available sightlines, allowing for customizable coverage in experiments with runaway electronsmore » in the <span class="hlt">energy</span> range of 1–60 MeV. Commissioning of the <span class="hlt">gamma</span> ray imager includes the quantification of electromagnetic noise sources in the tokamak machine hall and a measurement of the <span class="hlt">energy</span> spectrum of background <span class="hlt">gamma</span> radiation. First measurements of <span class="hlt">gamma</span> rays coming from the plasma provide a suitable testbed for implementing pulse height analysis that provides the <span class="hlt">energy</span> of detected <span class="hlt">gamma</span> photons.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1371566-gamma-ray-imager-diii-tokamak','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1371566-gamma-ray-imager-diii-tokamak"><span><span class="hlt">Gamma</span> ray imager on the DIII-D tokamak</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Pace, D. C.; Cooper, C. M.; Taussig, D.; ...</p> <p>2016-04-13</p> <p>A <span class="hlt">gamma</span> ray camera is built for the DIII-D tokamak [J. Luxon, Nucl. Fusion 42, 614 (2002)] that provides spatial localization and <span class="hlt">energy</span> resolution of <span class="hlt">gamma</span> flux by combining a lead pinhole camera with custom-built detectors and optimized viewing geometry. This diagnostic system is installed on the outer midplane of the tokamak such that its 123 collimated sightlines extend across the tokamak radius while also covering most of the vertical extent of the plasma volume. A set of 30 bismuth germanate detectors can be secured in any of the available sightlines, allowing for customizable coverage in experiments with runaway electronsmore » in the <span class="hlt">energy</span> range of 1- 60 MeV. Commissioning of the <span class="hlt">gamma</span> ray imager includes the quantification of electromagnetic noise sources in the tokamak machine hall and a measurement of the <span class="hlt">energy</span> spectrum of background <span class="hlt">gamma</span> radiation. In conclusion, first measurements of <span class="hlt">gamma</span> rays coming from the plasma provide a suitable testbed for implementing pulse height analysis that provides the <span class="hlt">energy</span> of detected <span class="hlt">gamma</span> photons.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010JEnM...28....1T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010JEnM...28....1T"><span>Chemical <span class="hlt">Energy</span> <span class="hlt">Release</span> in Several Recently Discovered Detonation and Deflagration Flows</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tarver, Craig M.</p> <p>2010-10-01</p> <p>Several recent experiments on complex detonation and deflagration flows are analyzed in terms of the chemical <span class="hlt">energy</span> <span class="hlt">release</span> required to sustain these flows. The observed double cellular structures in detonating gaseous nitromethane-oxygen and NO2-fuel (H2, CH4, and C2H6) mixtures are explained by the amplification of two distinct pressure wave frequencies by two exothermic reactions, the faster reaction forming vibrationally excited NO* and the slower reaction forming highly vibrationally excited N2**. The establishment of a Chapman-Jouguet (C-J) deflagration behind a weak shock wave, the C-J detonation established after a head-on collision with a shock front, and the C-J detonation conditions established in reactive supersonic flows are quantitatively calculated using the chemical <span class="hlt">energy</span> <span class="hlt">release</span> of a H2 + Cl2 mixture. For these three reactive flows, these calculations illustrate that different fractions of the exothermic chemical <span class="hlt">energy</span> are used to sustain steady-state propagation. C-J detonation calculations on the various initial states using the CHEETAH chemical equilibrium code are shown to be in good agreement with experimental detonation velocity measurements for the head-on collision and supersonic flow detonations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2004SPIE.5488..977R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2004SPIE.5488..977R"><span>MEGA: the next generation Medium <span class="hlt">Energy</span> <span class="hlt">Gamma</span>-ray Telescope</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ryan, James M.; Andritschke, Robert; Bloser, Peter F.; Cravens, James P.; Cherry, Michael L.; Di Cocco, Guido; Guzik, T. G.; Hartmann, Dieter H.; Hunter, Stanley H.; Kanbach, Gottfried; Kippen, R. M.; Kurfess, James; Macri, John R.; McConnell, Mark L.; Miller, Richard S.; Paciesas, William S.; Phlips, Bernard; Reglero, Victor; Stacy, J. G.; Strickman, Mark; Vestrand, W. Thomas; Wefel, John P.; Wulf, Eric; Zoglauer, Andreas; Zych, Allen D.</p> <p>2004-10-01</p> <p>The MEGA mission would enable a sensitive all-sky survey of the medium-<span class="hlt">energy</span> ?-ray sky (0.3-50 MeV). This mission will bridge the huge sensitivity gap between the COMPTEL and OSSE experiments on the Compton <span class="hlt">Gamma</span> Ray Observatory, the SPI and IBIS instruments on INTEGRAL and the visionary ACT mission. It will, among other things, serve to compile a much larger catalog of sources in this <span class="hlt">energy</span> range, perform far deeper searches for supernovae, better measure the galactic continuum emission as well as identify the components of the cosmic diffuse emission. The large field of view will allow MEGA to continuously monitor the sky for transient and variable sources. It will accomplish these goals with a stack of Si-strip detector (SSD) planes surrounded by a dense high-Z calorimeter. At lower photon <span class="hlt">energies</span> (below ~30 MeV), the design is sensitive to Compton interactions, with the SSD system serving as a scattering medium that also detects and measures the Compton recoil <span class="hlt">energy</span> deposit. If the <span class="hlt">energy</span> of the recoil electron is sufficiently high (> 2 MeV), the track of the recoil electron can also be defined. At higher photon <span class="hlt">energies</span> (above ~10 MeV), the design is sensitive to pair production events, with the SSD system measuring the tracks of the electron and positron. We will discuss the various types of event signatures in detail and describe the advantages of this design over previous Compton telescope designs. Effective area, sensitivity and resolving power estimates are also presented along with simulations of expected scientific results and beam calibration results from the prototype instrument.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25695613','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25695613"><span>Elimination of scattered <span class="hlt">gamma</span> rays from injection sites using upper offset <span class="hlt">energy</span> windows in sentinel lymph node scintigraphy.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Yoneyama, Hiroto; Tsushima, Hiroyuki; Onoguchi, Masahisa; Konishi, Takahiro; Nakajima, Kenichi; Kinuya, Seigo</p> <p>2015-05-01</p> <p>The identification of sentinel lymph nodes (SLNs) near injection sites is difficult because of scattered <span class="hlt">gamma</span> rays. The purpose of this study was to investigate the optimal <span class="hlt">energy</span> windows for elimination of scattered <span class="hlt">gamma</span> rays in order to improve the detection of SLNs. The clinical study group consisted of 56 female patients with breast cancer. While the <span class="hlt">energy</span> was centred at 140 keV with a 20% window for Tc-99m, this <span class="hlt">energy</span> window was divided into five subwindows with every 4% in planar imaging. Regions of interest were placed on SLNs and the background, and contrast was calculated using a standard equation. The confidence levels of interpretations were evaluated using a five-grade scale. The contrast provided by 145.6 keV±2% was the best, followed by 140 keV±2%, 151.2 keV±2%, 134.4 keV±2% and 128.8 keV±2% in that order. When 128.8 keV±2% and 134.4 keV±2% were eliminated from 140 keV±10% (145.6 keV±6%), the contrast of SLNs improved significantly. The confidence levels of interpretation and detection rate provided by the planar images with 140 keV±10% were 4.74±0.58 and 94.8%, respectively, and those provided by 145.6 keV±6% were 4.94±0.20 and 100%. Because lower <span class="hlt">energy</span> windows contain many scattered <span class="hlt">gamma</span> rays, upper offset <span class="hlt">energy</span> windows, which exclude lower <span class="hlt">energy</span> windows, improve the image contrast of SLNs near injection sites.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19930054261&hterms=solar+energy&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dsolar%2Benergy','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19930054261&hterms=solar+energy&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dsolar%2Benergy"><span>Numerical modeling of the <span class="hlt">energy</span> storage and <span class="hlt">release</span> in solar flares</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Wu, S. T.; Weng, F. S.</p> <p>1993-01-01</p> <p>This paper reports on investigation of the photospheric magnetic field-line footpoint motion (usually referred to as shear motion) and magnetic flux emerging from below the surface in relation to <span class="hlt">energy</span> storage in a solar flare. These causality relationships are demonstrated by using numerical magnetohydrodynamic simulations. From these results, one may conclude that the <span class="hlt">energy</span> stored in solar flares is in the form of currents. The dynamic process through which these currents reach a critical value is discussed as well as how these currents lead to <span class="hlt">energy</span> <span class="hlt">release</span>, such as the explosive events of solar flares.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19830014615','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19830014615"><span>The <span class="hlt">energy</span> <span class="hlt">release</span> in earthquakes, and subduction zone seismicity and stress in slabs. Ph.D. Thesis</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Vassiliou, M. S.</p> <p>1983-01-01</p> <p><span class="hlt">Energy</span> <span class="hlt">release</span> in earthquakes is discussed. Dynamic <span class="hlt">energy</span> from source time function, a simplified procedure for modeling deep focus events, static <span class="hlt">energy</span> estimates, near source <span class="hlt">energy</span> studies, and <span class="hlt">energy</span> and magnitude are addressed. Subduction zone seismicity and stress in slabs are also discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2000AIPC..510..551E','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2000AIPC..510..551E"><span>High-<span class="hlt">energy</span> solar flare observations at the Y2K maximum</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Emslie, A. Gordon</p> <p>2000-04-01</p> <p>Solar flares afford an opportunity to observe processes associated with the acceleration and propagation of high-<span class="hlt">energy</span> particles at a level of detail not accessible in any other astrophysical source. I will review some key results from previous high-<span class="hlt">energy</span> solar flare observations, including those from the Compton <span class="hlt">Gamma</span>-Ray Observatory, and the problems that they pose for our understanding of <span class="hlt">energy</span> <span class="hlt">release</span> and particle acceleration processes in the astrophysical environment. I will then discuss a program of high-<span class="hlt">energy</span> observations to be carried out during the upcoming 2000-2001 solar maximum that is aimed at addressing and resolving these issues. A key element in this observational program is the High <span class="hlt">Energy</span> Solar Spectroscopic Imager (HESSI) spacecraft, which will provide imaging spectroscopic observations with spatial, temporal, and <span class="hlt">energy</span> resolutions commensurate with the physical processes believed to be operating, and will in addition provide the first true <span class="hlt">gamma</span>-ray spectroscopy of an astrophysical source. .</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20150023327','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20150023327"><span>Fermi: The <span class="hlt">Gamma</span>-Ray Large Area Telescope</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>McEnery, Julie</p> <p>2015-01-01</p> <p>Following its launch in June 2008, high-<span class="hlt">energy</span> <span class="hlt">gamma</span>-ray observations by the Fermi <span class="hlt">Gamma</span>-ray Space Telescope have unveiled over 1000 new sources and opened an important and previously unexplored window on a wide variety of phenomena. These have included the discovery of an population of pulsars pulsing only in <span class="hlt">gamma</span> rays; the detection of photons up to 10s of GeV from <span class="hlt">gamma</span>-ray bursts, enhancing our understanding of the astrophysics of these powerful explosions; the detection of hundreds of active galaxies; a measurement of the high <span class="hlt">energy</span> cosmic-ray electron spectrum which may imply the presence of nearby astrophysical particle accelerators; the determination of the diffuse <span class="hlt">gamma</span>-ray emission with unprecedented accuracy and the constraints on phenomena such as supersymmetric dark-matter annihilations and exotic relics from the Big Bang. Continuous monitoring of the high-<span class="hlt">energy</span> <span class="hlt">gamma</span>-ray sky has uncovered numerous outbursts from active galaxies and the discovery of transient sources in our galaxy. In this talk I will describe the current status of the Fermi observatory and review the science highlights from Fermi.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20160005415','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20160005415"><span>Fermi: The <span class="hlt">Gamma</span>-Ray Large Area Telescope</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>McEnery, Julie</p> <p>2014-01-01</p> <p>Following its launch in June 2008, high-<span class="hlt">energy</span> <span class="hlt">gamma</span>-ray observations by the Fermi <span class="hlt">Gamma</span>-ray Space Telescope have unveiled over 1000 new sources and opened an important and previously unexplored window on a wide variety of phenomena. These have included the discovery of an population of pulsars pulsing only in <span class="hlt">gamma</span> rays; the detection of photons up to 10 seconds of gigaelectronvolts from <span class="hlt">gamma</span>-ray bursts, enhancing our understanding of the astrophysics of these powerful explosions; the detection of hundreds of active galaxies; a measurement of the high <span class="hlt">energy</span> cosmic-ray electron spectrum which may imply the presence of nearby astrophysical particle accelerators; the determination of the diffuse <span class="hlt">gamma</span>-ray emission with unprecedented accuracy and the constraints on phenomena such as super-symmetric dark-matter annihilations and exotic relics from the Big Bang. Continuous monitoring of the high-<span class="hlt">energy</span> <span class="hlt">gamma</span>-ray sky has uncovered numerous outbursts from active galaxies and the discovery of transient sources in our galaxy. In this talk I will describe the current status of the Fermi observatory and review the science highlights from Fermi.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19780024028','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19780024028"><span><span class="hlt">Gamma</span> ray spectroscopy in astrophysics. [conferences</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Cline, T. L. (Editor); Ramaty, R. (Editor)</p> <p>1978-01-01</p> <p>Experimental and theoretical aspects of <span class="hlt">gamma</span> ray spectroscopy in high <span class="hlt">energy</span> astrophysics are discussed. Line spectra from solar, stellar, planetary, and cosmic <span class="hlt">gamma</span> rays are examined as well as HEAO investigations, the prospects of a <span class="hlt">gamma</span> ray observatory, and follow-on X-ray experiments in space.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19980193189','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19980193189"><span>Implications of <span class="hlt">Gamma</span>-Ray Transparency Constraints in Blazars: Minimum Distances and <span class="hlt">Gamma</span>-Ray Collimation</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Becker, Peter A.; Kafatos, Menas</p> <p>1995-01-01</p> <p>We develop a general expression for the <span class="hlt">gamma</span> - <span class="hlt">gamma</span> absorption coefficient, alpha(sub <span class="hlt">gamma(gamma</span>)) for <span class="hlt">gamma</span>-rays propagating in an arbitrary direction at an arbitrary point in space above an X-ray-emitting accretion disk. The X-ray intensity is assumed to vary as a power law in <span class="hlt">energy</span> and radius between the outer disk radius, R(sub 0), and the inner radius, R(sub ms) which is the radius of marginal stability for a Schwarzschild black hole. We use our result for alpha(sub <span class="hlt">gamma(gamma</span>)) to calculate the <span class="hlt">gamma</span> - <span class="hlt">gamma</span> optical depth, tau(sub <span class="hlt">gamma(gamma</span>)) for <span class="hlt">gamma</span> - rays created at height z and propagating at angle Phi relative to the disk axis, and we show that for Phi = 0 and z greater than or approx equal to R(sub 0), tau(sub <span class="hlt">gamma(gamma</span>)) proportional to Epsilon(sup alpha)z(sup -2(alpha) - 3), where alpha is the X-ray spectral index and Epsilon is the <span class="hlt">gamma</span> - ray <span class="hlt">energy</span>. As an application, we use our formalism to compute the minimum distance between the central black hole and the site of production of the <span class="hlt">gamma</span>-rays detected by EGRET during the 1991 June flare of 3C 279. In order to obtain an upper limit, we assume that all of the X-rays observed contemporaneously by Ginga were emitted by the disk. Our results suggest that the observed <span class="hlt">gamma</span> - rays may have originated within less than or approx equal to 45 GM/sq c from a black hole of mass greater than or approx equal to 10(exp 9) solar mass, perhaps in active plasma located above the central funnel of the accretion disk. This raises the possibility of establishing a direct connection between the production of the observed <span class="hlt">gamma</span> - rays and the accretion of material onto the black hole. We also consider the variation of the optical depth as a function of the angle of propagation Phi. Our results indicate that the "focusing" of the <span class="hlt">gamma</span> - rays along the disk axis due to pair production is strong enough to explain the observed degree of alignment in blazar sources. If the <span class="hlt">gamma</span> - rays are produced isotropically</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li class="active"><span>19</span></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_19 --> <div id="page_20" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li class="active"><span>20</span></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="381"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/467464-high-statistics-search-ultrahigh-energy-gamma-ray-emission-from-cygnus-hercules','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/467464-high-statistics-search-ultrahigh-energy-gamma-ray-emission-from-cygnus-hercules"><span>High statistics search for ultrahigh <span class="hlt">energy</span> {<span class="hlt">gamma</span>}-ray emission from Cygnus X-3 and Hercules X-1</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Borione, A.; Chantell, M.C.; Covault, C.E.</p> <p>1997-02-01</p> <p>We have carried out a high statistics (2{times}10{sup 9} events) search for ultrahigh <span class="hlt">energy</span> {<span class="hlt">gamma</span>}-ray emission from the x-ray binary sources Cygnus X-3 and Hercules X-1. Using data taken with the CASA-MIA detector over a five year period (1990{endash}1995), we find no evidence for steady emission from either source. The derived 90{percent} C.L. upper limit to the steady integral flux of {<span class="hlt">gamma</span>} rays from Cygnus X-3 is {Phi}(E{gt}115TeV){lt}6.3{times}10{sup {minus}15} photons cm{sup {minus}2}sec{sup {minus}1}, and from Hercules X-1 it is {Phi}(E{gt}115TeV){lt}8.5{times}10{sup {minus}15} photonscm{sup {minus}2}sec{sup {minus}1}. These limits are more than two orders of magnitude lower than earlier claimed detections and aremore » better than recent experiments operating in the same <span class="hlt">energy</span> range. We have also searched for transient emission on time periods of one day and 0.5 h and find no evidence for such emission from either source. The typical daily limit on the integral {<span class="hlt">gamma</span>}-ray flux from Cygnus X-3 or Hercules X-1 is {Phi}{sub daily}(E{gt}115TeV){lt}2.0{times}10{sup {minus}13} photons cm{sup {minus}2}sec{sup {minus}1}. For Cygnus X-3, we see no evidence for emission correlated with the 4.8 h x-ray periodicity or with the occurrence of large radio flares. Unless one postulates that these sources were very active earlier and are now dormant, the limits presented here put into question the earlier results, and highlight the difficulties that possible future experiments will have in detecting {<span class="hlt">gamma</span>}-ray signals at ultrahigh <span class="hlt">energies</span>. {copyright} {ital 1997} {ital The American Physical Society}« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20090016210&hterms=photon&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3Dphoton','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20090016210&hterms=photon&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3Dphoton"><span>Stellar Photon Archaeology with <span class="hlt">Gamma</span>-Rays</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Stecker, Floyd W.</p> <p>2009-01-01</p> <p>Ongoing deep surveys of galaxy luminosity distribution functions, spectral <span class="hlt">energy</span> distributions and backwards evolution models of star formation rates can be used to calculate the past history of intergalactic photon densities and, from them, the present and past optical depth of the Universe to <span class="hlt">gamma</span>-rays from pair production interactions with these photons. The <span class="hlt">energy</span>-redshift dependence of the optical depth of the Universe to <span class="hlt">gamma</span>-rays has become known as the Fazio-Stecker relation (Fazio & Stecker 1970). Stecker, Malkan & Scully have calculated the densities of intergalactic background light (IBL) photons of <span class="hlt">energies</span> from 0.03 eV to the Lyman limit at 13.6 eV and for 0$ < z < $6, using deep survey galaxy observations from Spitzer, Hubble and GALEX and have consequently predicted spectral absorption features for extragalactic <span class="hlt">gamma</span>-ray sources. This procedure can also be reversed. Determining the cutoff <span class="hlt">energies</span> of <span class="hlt">gamma</span>-ray sources with known redshifts using the recently launched Fermi <span class="hlt">gamma</span>-ray space telescope may enable a more precise determination of the IBL photon densities in the past, i.e., the "archaeo-IBL.", and therefore allow a better measure of the past history of the total star formation rate, including that from galaxies too faint to be observed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28121730','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28121730"><span>Radon <span class="hlt">Release</span> and Its Simulated Effect on Radiation Doses.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Orabi, Momen</p> <p>2017-03-01</p> <p>One of the main factors that affect the uncertainty in calculating the <span class="hlt">gamma</span>-radiation absorbed dose rate inside a room is the variation in the degree of secular equilibrium of the considered radioactive series. A component of this factor, considered in this paper, is the <span class="hlt">release</span> of radon (Rn) from building materials to the living space of the room. This <span class="hlt">release</span> takes place through different steps. These steps are represented and mathematically formulated. The diffusion of radon inside the material is described by Fick's second law. Some of the factors affecting the radon <span class="hlt">release</span> rate (e.g. covering walls, moisture, structure of the building materials, etc.) are discussed. This scheme is used to study the impact of radon <span class="hlt">release</span> on the <span class="hlt">gamma</span>-radiation absorbed dose rate inside a room. The investigation is carried out by exploiting the MCNP simulation software. Different building materials are considered with different radon <span class="hlt">release</span> rates. Special care is given to Rn due to its relatively higher half-life and higher indoor concentration than the other radon isotopes. The results of the presented model show that the radon <span class="hlt">release</span> is of a significant impact in some building materials.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19950048255&hterms=viewing+zone&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dviewing%2Bzone','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19950048255&hterms=viewing+zone&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dviewing%2Bzone"><span><span class="hlt">Gamma</span>-ray pulsars: Emission zones and viewing geometries</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Romani, Roger W.; Yadigaroglu, I.-A.</p> <p>1995-01-01</p> <p>There are now a half-dozen young pulsars detected in high-<span class="hlt">energy</span> photons by the Compton <span class="hlt">Gamma</span>-Ray Observatory (CGRO), showing a variety of emission efficiencies and pulse profiles. We present here a calculation of the pattern of high-<span class="hlt">energy</span> emission on the sky in a model which posits <span class="hlt">gamma</span>-ray production by charge-depleted gaps in the outer magnetosphere. This model accounts for the radio to <span class="hlt">gamma</span>-ray pulse offsets of the known pulsars, as well as the shape of the high-<span class="hlt">energy</span> pulse profiles. We also show that about one-third of emitting young radio pulsars will not be detected due to beaming effects, while approximately 2.5 times the number of radio-selected <span class="hlt">gamma</span>-ray pulsars will be viewed only high <span class="hlt">energies</span>. Finally we compute the polarization angle variation and find that the previously misunderstood optical polarization sweep of the Crab pulsar arises naturally in this picture. These results strongly support an outer magnetosphere location for the <span class="hlt">gamma</span>-ray emission.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/21578249-constraining-emissivity-ultrahigh-energy-cosmic-rays-distant-universe-diffuse-gamma-ray-emission','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/21578249-constraining-emissivity-ultrahigh-energy-cosmic-rays-distant-universe-diffuse-gamma-ray-emission"><span>CONSTRAINING THE EMISSIVITY OF ULTRAHIGH <span class="hlt">ENERGY</span> COSMIC RAYS IN THE DISTANT UNIVERSE WITH THE DIFFUSE <span class="hlt">GAMMA</span>-RAY EMISSION</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Wang Xiangyu; Liu Ruoyu; Aharonian, Felix</p> <p></p> <p>Ultrahigh cosmic rays (UHECRs) with <span class="hlt">energies</span> {approx}> 10{sup 19} eV emitted at cosmological distances will be attenuated by cosmic microwave and infrared background radiation through photohadronic processes. Lower <span class="hlt">energy</span> extragalactic cosmic rays ({approx}10{sup 18}-10{sup 19} eV) can only travel a linear distance smaller than {approx}Gpc in a Hubble time due to the diffusion if the extragalactic magnetic fields are as strong as nano-Gauss. These prevent us from directly observing most of the UHECRs in the universe, and thus the observed UHECR intensity reflects only the emissivity in the nearby universe within hundreds of Mpc. However, UHECRs in the distant universe,more » through interactions with the cosmic background photons, produce UHE electrons and <span class="hlt">gamma</span> rays that in turn initiate electromagnetic cascades on cosmic background photons. This secondary cascade radiation forms part of the extragalactic diffuse GeV-TeV <span class="hlt">gamma</span>-ray radiation and, unlike the original UHECRs, is observable. Motivated by new measurements of extragalactic diffuse <span class="hlt">gamma</span>-ray background radiation by Fermi/Large Area Telescope, we obtained upper limit placed on the UHECR emissivity in the distant universe by requiring that the cascade radiation they produce not exceed the observed levels. By comparison with the <span class="hlt">gamma</span>-ray emissivity of candidate UHECR sources (such as <span class="hlt">gamma</span>-ray bursts (GRBs) and active galactic nuclei) at high redshifts, we find that the obtained upper limit for a flat proton spectrum is {approx_equal} 10{sup 1.5} times larger than the <span class="hlt">gamma</span>-ray emissivity in GRBs and {approx_equal} 10 times smaller than the <span class="hlt">gamma</span>-ray emissivity in BL Lac objects. In the case of iron nuclei composition, the derived upper limit of UHECR emissivity is a factor of 3-5 times higher. Robust upper limit on the cosmogenic neutrino flux is further obtained, which is marginally reachable by the Icecube detector and the next-generation detector JEM-EUSO.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20070005048','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20070005048"><span>Future <span class="hlt">Gamma</span>-Ray Observations of Pulsars and their Environments</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Thompson, David J.</p> <p>2006-01-01</p> <p>Pulsars and pulsar wind nebulae seen at <span class="hlt">gamma</span>-ray <span class="hlt">energies</span> offer insight into particle acceleration to very high <span class="hlt">energies</span> under extreme conditions. Pulsed emission provides information about the geometry and interaction processes in the magnetospheres of these rotating neutron stars, while the pulsar wind nebulae yield information about high-<span class="hlt">energy</span> particles interacting with their surroundings. During the next decade, a number of new and expanded <span class="hlt">gamma</span>-ray facilities will become available for pulsar studies, including Astro-rivelatore <span class="hlt">Gamma</span> a Immagini LEggero (AGILE) and <span class="hlt">Gamma</span>-ray Large Area Space Telescope (GLAST) in space and a number of higher-<span class="hlt">energy</span> ground-based systems. This review describes the capabilities of such observatories to answer some of the open questions about the highest-<span class="hlt">energy</span> processes involving neutron stars.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20010021127','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20010021127"><span><span class="hlt">Gamma</span>-ray Pulsars: Models and Predictions</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Harding Alice K.; White, Nicholas E. (Technical Monitor)</p> <p>2000-01-01</p> <p>Pulsed emission from <span class="hlt">gamma</span>-ray pulsars originates inside the magnetosphere, from radiation by charged particles accelerated near the magnetic poles or in the outer gaps. In polar cap models, the high <span class="hlt">energy</span> spectrum is cut off by magnetic pair production above an <span class="hlt">energy</span> that is, dependent on the local magnetic field strength. While most young pulsars with surface fields in the range B = 10(exp 12) - 10(exp 13) G are expected to have high <span class="hlt">energy</span> cutoffs around several GeV, the <span class="hlt">gamma</span>-ray spectra of old pulsars having lower surface fields may extend to 50 GeV. Although the <span class="hlt">gamma</span>-ray emission of older pulsars is weaker, detecting pulsed emission at high <span class="hlt">energies</span> from nearby sources would be an important confirmation of polar cap models. Outer gap models predict more gradual high-<span class="hlt">energy</span> turnovers of the primary curvature emission around 10 GeV, but also predict an inverse Compton component extending to TeV <span class="hlt">energies</span>. Detection of pulsed TeV emission, which would not survive attenuation at the polar caps, is thus an important test of outer gap models. Next-generation <span class="hlt">gamma</span>-ray telescopes sensitive to GeV-TeV emission will provide critical tests of pulsar acceleration and emission mechanisms.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016cosp...41E..91A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016cosp...41E..91A"><span>The control and data acquisition structure for the <span class="hlt">GAMMA</span>-400 space <span class="hlt">gamma</span>-telescope</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Arkhangelskiy, Andrey</p> <p>2016-07-01</p> <p>The <span class="hlt">GAMMA</span>-400 space project is intended for precision investigation of the cosmic <span class="hlt">gamma</span>-emission in the <span class="hlt">energy</span> band from keV region up to several TeV, electrons and positrons fluxes from ˜~1~GeV up to ˜~10~TeV and high <span class="hlt">energy</span> cosmic-ray nuclei fluxes. A description of the control and data acquisition structure for <span class="hlt">gamma</span>-telescope involved in the <span class="hlt">GAMMA</span> 400 space project is given. The technical capabilities of all specialized equipment providing the functioning of the scientific instrumentation and satellite support systems are unified in a single structure. Control of the scientific instruments is maintained using one-time pulse radio commands and program commands transmitted via onboard control system and scientific data acquisition system. Up to 100~GByte of data per day can be transferred to the ground segment of the project. The correctness of the proposed and implemented structure, engineering solutions and electronic elemental base selection has been verified experimentally with the scientific complex prototype in the laboratory conditions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19910063361&hterms=physics+astrophysics&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dphysics%2Bastrophysics','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19910063361&hterms=physics+astrophysics&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dphysics%2Bastrophysics"><span>The goals of <span class="hlt">gamma</span>-ray spectroscopy in high <span class="hlt">energy</span> astrophysics</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Lingenfelter, Richard E.; Higdon, James C.; Leventhal, Marvin; Ramaty, Reuven; Woosley, Stanford E.</p> <p>1990-01-01</p> <p>The use of high resolution <span class="hlt">gamma</span>-ray spectroscopy in astrophysics is discussed with specific attention given to the application of the Nuclear Astrophysics Explorer (NAE). The <span class="hlt">gamma</span>-ray lines from nuclear transitions in radionucleic decay and positron annihilation permits the study of current sites, rates and models of nucleosynthesis, and galactic structure. Diffuse galactic emission is discussed, and the high-resolution observations of <span class="hlt">gamma</span>-ray lines from discrete sites are also described. Interstellar mixing and elemental abundances can also be inferred from high-resolution <span class="hlt">gamma</span>-ray spectroscopy of nucleosynthetic products. Compact objects can also be examined by means of <span class="hlt">gamma</span>-ray emissions, allowing better understanding of neutron stars and the accreting black hole near the galactic center. Solar physics can also be investigated by examining such features as solar-flare particle acceleration and atmospheric abundances.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/21067330-gamma-ray-astrophysics-agile','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/21067330-gamma-ray-astrophysics-agile"><span><span class="hlt">Gamma</span>-ray Astrophysics with AGILE</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Longo, Francesco; Tavani, M.; Barbiellini, G.</p> <p>2007-07-12</p> <p>AGILE will explore the <span class="hlt">gamma</span>-ray Universe with a very innovative instrument combining for the first time a <span class="hlt">gamma</span>-ray imager and a hard X-ray imager. AGILE will be operational in spring 2007 and it will provide crucial data for the study of Active Galactic Nuclei, <span class="hlt">Gamma</span>-Ray Bursts, unidentified <span class="hlt">gamma</span>-ray sources. Galactic compact objects, supernova remnants, TeV sources, and fundamental physics by microsecond timing. The AGILE instrument is designed to simultaneously detect and image photons in the 30 MeV - 50 GeV and 15 - 45 keV <span class="hlt">energy</span> bands with excellent imaging and timing capabilities, and a large field of view coveringmore » {approx} 1/5 of the entire sky at <span class="hlt">energies</span> above 30 MeV. A CsI calorimeter is capable of GRB triggering in the <span class="hlt">energy</span> band 0.3-50 MeV AGILE is now (March 2007) undergoing launcher integration and testing. The PLSV launch is planned in spring 2007. AGILE is then foreseen to be fully operational during the summer of 2007.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1154960','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1154960"><span>Explosive Products EOS: Adjustment for detonation speed and <span class="hlt">energy</span> <span class="hlt">release</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Menikoff, Ralph</p> <p>2014-09-05</p> <p>Propagating detonation waves exhibit a curvature effect in which the detonation speed decreases with increasing front curvature. The curvature effect is due to the width of the wave profile. Numerically, the wave profile depends on resolution. With coarse resolution, the wave width is too large and results in a curvature effect that is too large. Consequently, the detonation speed decreases as the cell size is increased. We propose a modification to the products equation of state (EOS) to compensate for the effect of numerical resolution; i.e., to increase the CJ pressure in order that a simulation propagates a detonation wavemore » with a speed that is on average correct. The EOS modification also adjusts the <span class="hlt">release</span> isentrope to correct the <span class="hlt">energy</span> <span class="hlt">release</span>.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/5248668','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/5248668"><span>Integral measurements of neutron and <span class="hlt">gamma</span>-ray leakage fluxes from the Little Boy replica</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Muckenthaler, F.J.</p> <p></p> <p>This report presents integral measurements of neutron and <span class="hlt">gamma</span>-ray leakage fluxes from a critical mockup of the Hiroshima bomb Little Boy at Los Alamos National Laobratory with detector systems developed by Oak Ridge National Laboratory. Bonner ball detectors were used to map the neutron fluxes in the horizontal midplane at various distances from the mockup and for selected polar angles, keeping the source-detector separation constant. <span class="hlt">Gamma</span>-ray <span class="hlt">energy</span> deposition measurements were made with thermoluminescent detectors at several locations on the iron shell of the source mockup. The measurements were performed as part of a larger progam to provide benchmark data formore » testing the methods used to calculate the radiation <span class="hlt">released</span> from the Little Boy bomb over Hiroshima. 3 references, 10 figures.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AIPC.1852d0004D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AIPC.1852d0004D"><span>About cosmic <span class="hlt">gamma</span> ray lines</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Diehl, Roland</p> <p>2017-06-01</p> <p><span class="hlt">Gamma</span> ray lines from cosmic sources convey the action of nuclear reactions in cosmic sites and their impacts on astrophysical objects. <span class="hlt">Gamma</span> rays at characteristic <span class="hlt">energies</span> result from nuclear transitions following radioactive decays or high-<span class="hlt">energy</span> collisions with excitation of nuclei. The <span class="hlt">gamma</span>-ray line from the annihilation of positrons at 511 keV falls into the same <span class="hlt">energy</span> window, although of different origin. We present here the concepts of cosmic <span class="hlt">gamma</span> ray spectrometry and the corresponding instruments and missions, followed by a discussion of recent results and the challenges and open issues for the future. Among the lessons learned are the diffuse radioactive afterglow of massive-star nucleosynthesis in 26Al and 60Fe <span class="hlt">gamma</span> rays, which is now being exploited towards the cycle of matter driven by massive stars and their supernovae; large interstellar cavities and superbubbles have been recognised to be of key importance here. Also, constraints on the complex processes making stars explode as either thermonuclear or core-collapse supernovae are being illuminated by <span class="hlt">gamma</span>-ray lines, in this case from shortlived radioactivities from 56Ni and 44Ti decays. In particular, the three-dimensionality and asphericities that have recently been recognised as important are enlightened in different ways through such <span class="hlt">gamma</span>-ray line spectroscopy. Finally, the distribution of positron annihilation <span class="hlt">gamma</span> ray emission with its puzzling bulge-dominated intensity disctribution is measured through spatially-resolved spectra, which indicate that annihilation conditions may differ in different parts of our Galaxy. But it is now understood that a variety of sources may feed positrons into the interstellar medium, and their characteristics largely get lost during slowing down and propagation of positrons before annihilation; a recent microquasar flare was caught as an opportunity to see positrons annihilate at a source.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19870029645&hterms=topic&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dtopic','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19870029645&hterms=topic&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dtopic"><span>Topics in <span class="hlt">gamma</span> ray astronomy</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Ramaty, R.; Lingenfelter, R. E.</p> <p>1986-01-01</p> <p>Observations of <span class="hlt">gamma</span> rays from solar flares, <span class="hlt">gamma</span> ray bursts, the Galactic center, galactic nucleosynthesis, SS433, and Cygnus X-3, and their effects on astrophysical problems are discussed. It is observed that <span class="hlt">gamma</span> ray spectra from solar flares are applicable to the study of particle acceleration and confinement and the determination of chemical abundances in the solar atmosphere. The <span class="hlt">gamma</span> ray lines from the compact galactic object SS433 are utilized to examine the acceleration of jets, and analysis of the <span class="hlt">gamma</span> ray lines of Cygnus X-3 reveal that particles can be accelerated in compact sources to ultrahigh <span class="hlt">energies</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19740032604&hterms=pulse-shape+discrimination&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dpulse-shape%2Bdiscrimination','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19740032604&hterms=pulse-shape+discrimination&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dpulse-shape%2Bdiscrimination"><span><span class="hlt">Energy</span> spectrum and flux of 3- to 20-Mev neutrons and 1- to 10-Mev <span class="hlt">gamma</span> rays in the atmosphere</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Klumpar, D. M.; Lockwood, J. A.; Saint Onge, R. N.; Friling, L. A.</p> <p>1973-01-01</p> <p>An experiment is described which was designed to measure the neutron and <span class="hlt">gamma</span> ray <span class="hlt">energy</span> spectrums and fluxes in the <span class="hlt">energy</span> intervals 3 to 20 MeV and 1 to 10 MeV, respectively. In addition, from the 3 to 20-MeV proton recoil spectrums it is possible to infer the shape of the neutron <span class="hlt">energy</span> spectrum from 20 to 50 MeV. The detecting system utilized a separate charged particle rejection scheme and a two-parameter display system for the output from the pulse shape discrimination which separated <span class="hlt">gamma</span> rays from neutrons (n). Two long-duration flights were made with this detector in 1970 at Palestine, Tex. (P sub c = 4.6 Gv) and at Ft. Churchill, Canada (P sub c = 0.3 Gv).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017ApJ...842...85A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017ApJ...842...85A"><span>Search for Very High-<span class="hlt">energy</span> <span class="hlt">Gamma</span> Rays from the Northern Fermi Bubble Region with HAWC</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Abeysekara, A. U.; Albert, A.; Alfaro, R.; Alvarez, C.; Álvarez, J. D.; Arceo, R.; Arteaga-Velázquez, J. C.; Ayala Solares, H. A.; Barber, A. S.; Bautista-Elivar, N.; Becerril, A.; Belmont-Moreno, E.; BenZvi, S. Y.; Berley, D.; Braun, J.; Brisbois, C.; Caballero-Mora, K. S.; Capistrán, T.; Carramiñana, A.; Casanova, S.; Castillo, M.; Cotti, U.; Cotzomi, J.; Coutiño de León, S.; De León, C.; De la Fuente, E.; Diaz Hernandez, R.; Dingus, B. L.; DuVernois, M. A.; Díaz-Vélez, J. C.; Ellsworth, R. W.; Engel, K.; Fick, B.; Fiorino, D. W.; Fleischhack, H.; Fraija, N.; García-González, J. A.; Garfias, F.; Gerhardt, M.; González Muñoz, A.; González, M. M.; Goodman, J. A.; Hampel-Arias, Z.; Harding, J. P.; Hernandez, S.; Hernandez-Almada, A.; Hinton, J.; Hona, B.; Hui, C. M.; Hüntemeyer, P.; Iriarte, A.; Jardin-Blicq, A.; Joshi, V.; Kaufmann, S.; Kieda, D.; Lara, A.; Lauer, R. J.; Lee, W. H.; Lennarz, D.; León Vargas, H.; Linnemann, J. T.; Longinotti, A. L.; Raya, G. Luis; Luna-García, R.; López-Coto, R.; Malone, K.; Marinelli, S. S.; Martinez, O.; Martinez-Castellanos, I.; Martínez-Castro, J.; Martínez-Huerta, H.; Matthews, J. A.; Miranda-Romagnoli, P.; Moreno, E.; Mostafá, M.; Nellen, L.; Newbold, M.; Nisa, M. U.; Noriega-Papaqui, R.; Pelayo, R.; Pretz, J.; Pérez-Pérez, E. G.; Ren, Z.; Rho, C. D.; Rivière, C.; Rosa-González, D.; Rosenberg, M.; Ruiz-Velasco, E.; Salazar, H.; Salesa Greus, F.; Sandoval, A.; Schneider, M.; Schoorlemmer, H.; Sinnis, G.; Smith, A. J.; Springer, R. W.; Surajbali, P.; Taboada, I.; Tibolla, O.; Tollefson, K.; Torres, I.; Ukwatta, T. N.; Vianello, G.; Weisgarber, T.; Westerhoff, S.; Wisher, I. G.; Wood, J.; Yapici, T.; Yodh, G. B.; Zepeda, A.; Zhou, H.</p> <p>2017-06-01</p> <p>We present a search for very high-<span class="hlt">energy</span> <span class="hlt">gamma</span>-ray emission from the Northern Fermi Bubble region using data collected with the High Altitude Water Cherenkov <span class="hlt">gamma</span>-ray observatory. The size of the data set is 290 days. No significant excess is observed in the Northern Fermi Bubble region, so upper limits above 1 TeV are calculated. The upper limits are between 3× {10}-7 {GeV} {{cm}}-2 {{{s}}}-1 {{sr}}-1 and 4× {10}-8 {GeV} {{cm}}-2 {{{s}}}-1 {{sr}}-1. The upper limits disfavor a proton injection spectrum that extends beyond 100 TeV without being suppressed. They also disfavor a hadronic injection spectrum derived from neutrino measurements.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/4891808','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/4891808"><span>New hemolysin (<span class="hlt">gamma</span>) produced by Escherichia coli.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Walton, J R; Smith, D H</p> <p>1969-04-01</p> <p>A new hemolysin (<span class="hlt">gamma</span>) of Escherichia coli, active in the absence of viable bacteria, has been recognized in mutants resistant to nalidixic acid. Nalidixic acid affects either the production or <span class="hlt">release</span> of the hemolysin.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1992JCoMa..26.2028R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1992JCoMa..26.2028R"><span>Method for computing <span class="hlt">energy</span> <span class="hlt">release</span> rate using the elastic work factor approach</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Rhee, K. Y.; Ernst, H. A.</p> <p>1992-01-01</p> <p>The elastic work factor eta(el) concept was applied to composite structures for the calculation of total <span class="hlt">energy</span> <span class="hlt">release</span> rate by using a single specimen. Cracked lap shear specimens with four different unidirectional fiber orientation were used to examine the dependence of eta(el) on the material properties. Also, three different thickness ratios (lap/strap) were used to determine how geometric conditions affect eta(el). The eta(el) values were calculated in two different ways: compliance method and crack closure method. The results show that the two methods produce comparable eta(el) values and, while eta(el) is affected significantly by geometric conditions, it is reasonably independent of material properties for the given geometry. The results also showed that the elastic work factor can be used to calculate total <span class="hlt">energy</span> <span class="hlt">release</span> rate using a single specimen.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2004xmm..pres...77.','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2004xmm..pres...77."><span>ESA's Integral solves thirty-year old <span class="hlt">gamma</span>-ray mystery</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p></p> <p></p> <p>-ray sources towards the direction of the Galactic centre. Lebrun's team includes Ubertini and seventeen other European scientists with long-standing experience in high-<span class="hlt">energy</span> astrophysics. Much to the team's surprise, almost half of these sources do not fall in any class of known <span class="hlt">gamma</span>-ray objects. They probably represent a new population of <span class="hlt">gamma</span>-ray emitters. The first clues about a new class of <span class="hlt">gamma</span>-ray objects came last October, when Integral discovered an intriguing <span class="hlt">gamma</span>-ray source, known as IGRJ16318-4848. The data from Integral and ESA's other high-<span class="hlt">energy</span> observatory XMM-Newton suggested that this object is a binary system, probably including a black hole or neutron star, embedded in a thick cocoon of cold gas and dust. When gas from the companion star is accelerated and swallowed by the black hole, <span class="hlt">energy</span> is <span class="hlt">released</span> at all wavelengths, mostly in the <span class="hlt">gamma</span> rays. However, Lebrun is cautious to draw premature conclusions about the sources detected in the Galactic centre. Other interpretations are also possible that do not involve black holes. For instance, these objects could be the remains of exploded stars that are being energised by rapidly rotating celestial 'powerhouses', known as pulsars. Observations with another Integral instrument (SPI, the Spectrometer on Integral) could provide Lebrun and his team with more information on the nature of these sources. SPI measures the <span class="hlt">energy</span> of incoming <span class="hlt">gamma</span> rays with extraordinary accuracy and allows scientist to gain a better understanding of the physical mechanisms that generate them. However, regardless of the precise nature of these <span class="hlt">gamma</span>-ray sources, Integral's observations have convincingly shown that the <span class="hlt">energy</span> output from these new objects accounts for almost ninety per cent of the soft <span class="hlt">gamma</span>-ray background coming from the centre of the Galaxy. This result raises the tantalising possibility that objects of this type hide everywhere in the Galaxy, not just in its centre. Again, Lebrun is cautious, saying, "It is</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016PhDT........58K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016PhDT........58K"><span>Topics in High-<span class="hlt">Energy</span> Astrophysics: X-ray Time Lags and <span class="hlt">Gamma</span>-ray Flares</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kroon, John J.</p> <p>2016-03-01</p> <p>The Universe is host to a wide variety of high-<span class="hlt">energy</span> processes that convert gravitational potential <span class="hlt">energy</span> or rest-mass <span class="hlt">energy</span> into non-thermal radiation such as bremsstrahlung and synchrotron. Prevailing models of X-ray emission from accreting Black Hole Binaries (BHBs) struggle to simultaneously fit the quiescent X-ray spectrum and the transients which result in the phenomenon known as X-ray time lags. And similarly, classical models of diffusive shock acceleration in pulsar wind nebulae fail to explain the extreme particle acceleration in very short timescales as is inferred from recent <span class="hlt">gamma</span>-ray flares from the Crab nebula. In this dissertation, I develop new exact analytic models to shed light on these intriguing processes. I take a fresh look at the formation of X-ray time lags in compact sources using a new mathematical approach in which I obtain the exact Green's function solution. The resulting Green's function allows one to explore a variety of injection scenarios, including both monochromatic and broadband (bremsstrahlung) seed photon injection. I obtain the exact solution for the dependence of the time lags on the Fourier frequency, for both homogeneous and inhomogeneous clouds. The model can successfully reproduce both the observed time lags and the quiescent X-ray spectrum using a single set of coronal parameters. I show that the implied coronal radii in the new model are significantly smaller than those obtained in the Monte Carlo simulations, hence greatly reducing the coronal heating problem. Recent bright <span class="hlt">gamma</span>-ray flares from the Crab nebula observed by AGILE and Fermi reaching GeV <span class="hlt">energies</span> and lasting several days challenge the contemporary model for particle acceleration in pulsar wind nebulae, specifically the diffusive shock acceleration model. Simulations indicate electron/positron pairs in the Crab nebula pulsar wind must be accelerated up to PeV <span class="hlt">energies</span> in the presence of ambient magnetic fields with strength B ~100 microG. No</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li class="active"><span>20</span></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_20 --> <div id="page_21" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li class="active"><span>21</span></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="401"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20140013397','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20140013397"><span><span class="hlt">Energy</span> <span class="hlt">Release</span> from Impacting Prominence Material Following the 2011 June 7 Eruption</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Gilbert, H. R.; Inglis, A. R.; Mays, M. L.; Ofman, L.; Thompson, B. J.; Young, C. A.</p> <p>2013-01-01</p> <p>Solar filaments exhibit a range of eruptive-like dynamic activity, ranging from the full or partial eruption of the filament mass and surrounding magnetic structure as a coronal mass ejection to a fully confined or failed eruption. On 2011 June 7, a dramatic partial eruption of a filament was observed by multiple instruments on board the Solar Dynamics Observatory (SDO) and Solar-Terrestrial Relations Observatory. One of the interesting aspects of this event is the response of the solar atmosphere as non-escaping material falls inward under the influence of gravity. The impact sites show clear evidence of brightening in the observed extreme ultraviolet wavelengths due to <span class="hlt">energy</span> <span class="hlt">release</span>. Two plausible physical mechanisms for explaining the brightening are considered: heating of the plasma due to the kinetic <span class="hlt">energy</span> of impacting material compressing the plasma, or reconnection between the magnetic field of low-lying loops and the field carried by the impacting material. By analyzing the emission of the brightenings in several SDO/Atmospheric Imaging Assembly wavelengths, and comparing the kinetic <span class="hlt">energy</span> of the impacting material (7.6 × 10(exp 26) - 5.8 × 10(exp 27) erg) to the radiative <span class="hlt">energy</span> (approx. 1.9 × 10(exp 25) - 2.5 × 10(exp 26) erg), we find the dominant mechanism of <span class="hlt">energy</span> <span class="hlt">release</span> involved in the observed brightening is plasma compression.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19850026444','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19850026444"><span>Ultrarelativistic electrons and solar flare <span class="hlt">gamma</span>-radiation</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Semukhin, P. E.; Kovaltsov, G. A.</p> <p>1985-01-01</p> <p>Ten solar flares with <span class="hlt">gamma</span> radiation in excess of 10 MeV were observed. Almost all took place within a heliolatitude greater than 60 deg, close to the solar limb, an indication of the essential anisotropy of high-<span class="hlt">energy</span> <span class="hlt">gamma</span> radiation. This high-<span class="hlt">energy</span> solar flare <span class="hlt">gamma</span> radiation can be explained by the specific features of the bremsstrahlung of ultrarelativistic electrons trapped within the magnetic arc of the solar atmosphere, even if the acceleration of the electrons is anisotropic.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19990115859&hterms=sources+energy&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dsources%2Benergy','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19990115859&hterms=sources+energy&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dsources%2Benergy"><span>Preview of the BATSE Earth Occultation Catalog of Low <span class="hlt">Energy</span> <span class="hlt">Gamma</span> Ray Sources</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Harmon, B. A.; Wilson, C. A.; Fishman, G. J.; McCollough, M. L.; Robinson, C. R.; Sahi, M.; Paciesas, W. S.; Zhang, S. N.</p> <p>1999-01-01</p> <p>The Burst and Transient Source Experiment (BATSE) aboard the Compton <span class="hlt">Gamma</span> Ray Observatory (CGRO) has been detecting and monitoring point sources in the high <span class="hlt">energy</span> sky since 1991. Although BATSE is best known for <span class="hlt">gamma</span> ray bursts, it also monitors the sky for longer-lived sources of radiation. Using the Earth occultation technique to extract flux information, a catalog is being prepared of about 150 sources potential emission in the large area detectors (20-1000 keV). The catalog will contain light curves, representative spectra, and parametric data for black hole and neutron star binaries, active galaxies, and super-nova remnants. In this preview, we present light curves for persistent and transient sources, and also show examples of what type of information can be obtained from the BATSE Earth occultation database. Options for making the data easily accessible as an "on line" WWW document are being explored.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20160005800&hterms=solar+two&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dsolar%2Btwo','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20160005800&hterms=solar+two&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dsolar%2Btwo"><span>High-<span class="hlt">Energy</span> <span class="hlt">Gamma</span>-Ray Emission From Solar Flares: Summary of Fermi LAT Detections and Analysis of Two M-Class Flares</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Ackermann, M.; Ajello, M.; Albert, A.; Allafort, A.; Baldini, L.; Barbiellini, G.; Bastieri, D.; Bechtol, K.; Bellazzini, R.; Bissaldi, E.; <a style="text-decoration: none; " href="javascript:void(0); " onClick="displayelement('author_20160005800'); toggleEditAbsImage('author_20160005800_show'); toggleEditAbsImage('author_20160005800_hide'); "> <img style="display:inline; width:12px; height:12px; " src="images/arrow-up.gif" width="12" height="12" border="0" alt="hide" id="author_20160005800_show"> <img style="width:12px; height:12px; display:none; " src="images/arrow-down.gif" width="12" height="12" border="0" alt="hide" id="author_20160005800_hide"></p> <p>2013-01-01</p> <p>We present the detections of 19 solar flares detected in high-<span class="hlt">energy</span> <span class="hlt">gamma</span> rays (above 100 MeV) with the Fermi Large Area Telescope (LAT) during its rst four years of operation. Interestingly, all ares are associated with fairly fast Coronal Mass Ejections (CMEs) and are not all powerful X-ray ares. We then describe the detailed temporal, spatial and spectral characteristics of the rst two long-lasting events: the 2011 March 7 are, a moderate (M3.7) impulsive are followed by slowly varying <span class="hlt">gamma</span>-ray emission over 13 hours, and the 2011 June 7 M2.5 are, which was followed by <span class="hlt">gamma</span>-ray emission lasting for 2 hours. We compare the Fermi-LAT data with X-ray and proton data measurements from GOES and RHESSI. We argue that a hadronic origin of the <span class="hlt">gamma</span> rays is more likely than a leptonic origin and nd that the <span class="hlt">energy</span> spectrum of the proton distribution softens after the 2011 March 7 are, favoring a scenario with continuous acceleration at the are site. This work suggests that proton acceleration in solar ares is more common than previously thought, occurring for even modest X-ray ares, and for longer durations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/536796','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/536796"><span>The low-temperature scintillation properties of bismuth germanate and its application to high-<span class="hlt">energy</span> <span class="hlt">gamma</span> radiation imaging devices.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Piltingsrud, H V</p> <p>1979-12-01</p> <p>Bismuth germanate is a scintillation material with very high z, and high density (7.13 g/cm3). It is a rugged, nonhygroscopic, crystalline material with room-temperature scintillation properties described by previous investigators as having a light yield approximately 8% of that of NaI(Tl), emission peak at approximately 480 nm, decay constant of 0.3 microsec, and <span class="hlt">energy</span> resolution congruent to 15% (FWHM) for Cs-137 <span class="hlt">gamma</span> radiations. These properties make it an excellent candidate for applications involving the detection of high-<span class="hlt">energy</span> <span class="hlt">gamma</span> photons and positron annihilation radiation, particularly when good spatial resolution is desired. At room temperature, however, the application of this material is somewhat limited by low light output and poor <span class="hlt">energy</span> resolution. This paper presents new data on the scintillation properties of bismuth germanate as a function of temperature from -- 196 degrees C to j0 degrees C. Low-temperature use of the material is shown to greatly improve its light yield and <span class="hlt">energy</span> resolution. The implications of this work to the design of imaging devices for high-<span class="hlt">energy</span> radiation in health physics and nuclear medicine are discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20040071148&hterms=sources+energy&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dsources%2Benergy','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20040071148&hterms=sources+energy&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dsources%2Benergy"><span>The BATSE Earth Occultation Catalog of Low <span class="hlt">Energy</span> <span class="hlt">Gamma</span>-Ray Sources</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Harmon, B. A.; Wilson-Hodge, C. A.; Fishman, G. J.; Paciesas, W. S.; Zhang, S. N.; Finger, M. H.; Connaughton, V.; Koshut, T. M.; Henze, W.; McCollough, M. L.</p> <p>2004-01-01</p> <p>The Burst and Transient Source Experiment (BATSE),aboard the COmptOn <span class="hlt">Gamma</span> Ray Observatory (CGRO), provided a record of the hard X-ray/low <span class="hlt">energy</span> <span class="hlt">gamma</span> ray sky between April 1991 and June 2000. During that time, a catalog of known sources was derived from existing catalogs such as HEAO A-4 (Levine et al. 19841, as well as new transient sources discovered with RATSE and other X-ray monitors operating in the CGRO era. The Earth Occultation Technique (Harmon et al. 2001, astro-ph/0109069) was used to monitor a combination of these sources, mostly galactic, totaling about 175 objects. The catalog will present the global properties of these sources and their probability of detection (>lO mCrab, 20-100 keV) with BATSE. Systematic errors due to unknown sources or background components are included. Cursory analyses to search for new transients (35-80 mCrab in the 20-100 keV band) and super-orbital periods in known binary sources are also presented. Whole mission light curves and associated data production/analysis tools are being delivered to the HEASARC for public use.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=MSFC-9134213&hterms=Internet+invisible&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3DInternet%2Binvisible','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=MSFC-9134213&hterms=Internet+invisible&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3DInternet%2Binvisible"><span>Compton <span class="hlt">Gamma</span>-Ray Observatory</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p></p> <p>1991-01-01</p> <p>This photograph shows the Compton <span class="hlt">Gamma</span>-Ray Observatory being <span class="hlt">released</span> from the Remote Manipulator System (RMS) arm aboard the Space Shuttle Atlantis during the STS-35 mission in April 1991. The GRO reentered the Earth's atmosphere and ended its successful mission in June 2000. For nearly 9 years, GRO's Burst and Transient Source Experiment (BATSE), designed and built by the Marshall Space Flight Center, kept an unblinking watch on the universe to alert scientist to the invisible, mysterious <span class="hlt">gamma</span>-ray bursts that had puzzled them for decades. By studying <span class="hlt">gamma</span>-rays from objects like black holes, pulsars, quasars, neutron stars, and other exotic objects, scientists could discover clues to the birth, evolution, and death of star, galaxies, and the universe. The <span class="hlt">gamma</span>-ray instrument was one of four major science instruments aboard the Compton. It consisted of eight detectors, or modules, located at each corner of the rectangular satellite to simultaneously scan the entire universe for bursts of <span class="hlt">gamma</span>-rays ranging in duration from fractions of a second to minutes. In January 1999, the instrument, via the Internet, cued a computer-controlled telescope at Las Alamos National Laboratory in Los Alamos, New Mexico, within 20 seconds of registering a burst. With this capability, the <span class="hlt">gamma</span>-ray experiment came to serve as a <span class="hlt">gamma</span>-ray burst alert for the Hubble Space Telescope, the Chandra X-Ray Observatory, and major gound-based observatories around the world. Thirty-seven universities, observatories, and NASA centers in 19 states, and 11 more institutions in Europe and Russia, participated in BATSE's science program.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018ATel11545....1M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018ATel11545....1M"><span>MAGIC detection of increased activity from FSRQ 3C 279 at very-high-<span class="hlt">energy</span> <span class="hlt">gamma</span> rays</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mirzoyan, Razmik</p> <p>2018-04-01</p> <p>The MAGIC telescopes observed an increase in the very-high-<span class="hlt">energy</span> (VHE; > 100 GeV) <span class="hlt">gamma</span>-ray flux from FSRQ 3C 279 at radio coordinates R.A.=194.04652737 deg and Dec= -5.78931242 deg, J2000.0 (Fey et al. 2004, AJ, 127, 3587).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20110008713','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20110008713"><span>Millisecond Pulsars at <span class="hlt">Gamma</span>-Ray <span class="hlt">Energies</span>: Fermi Detections and Implications</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Harding, Alice K.</p> <p>2011-01-01</p> <p>The Fermi <span class="hlt">Gamma</span>-Ray Space Telescope has revolutionized the study of pulsar physics with the discovery of new populations of radio quiet and millisecond <span class="hlt">gamma</span>-ray pulsars. The Fermi Large Area Telescope has so far discovered approx.20 new <span class="hlt">gamma</span>-ray millisecond pulsars (MSPs) by both folding at periods of known radio MSPs or by detecting them as <span class="hlt">gamma</span>-ray sources that are followed up by radio pulsar searches. The second method has resulted in a phenomenally successful synergy, with -30 new radio MSPs (to date) having been discovered at Fermi unidentified source locations and the <span class="hlt">gamma</span>-ray pulsations having then been detected in a number of these using the radio timing solutions. Many of the newly discovered MSPs may be suitable for addition to the collection of very stable MSPs used for gravitational wave detection. Detection of such a large number of MSPs was surprising, given that most have relatively low spin-down luminosity and surface field strength. I will discuss their properties and the implications for pulsar particle acceleration and emission, as well as their potential contribution to <span class="hlt">gamma</span>-ray backgrounds and Galactic cosmic rays.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014JInst...9C2031N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014JInst...9C2031N"><span>A novel Compton camera design featuring a rear-panel shield for substantial noise reduction in <span class="hlt">gamma</span>-ray images</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Nishiyama, T.; Kataoka, J.; Kishimoto, A.; Fujita, T.; Iwamoto, Y.; Taya, T.; Ohsuka, S.; Nakamura, S.; Hirayanagi, M.; Sakurai, N.; Adachi, S.; Uchiyama, T.</p> <p>2014-12-01</p> <p>After the Japanese nuclear disaster in 2011, large amounts of radioactive isotopes were <span class="hlt">released</span> and still remain a serious problem in Japan. Consequently, various <span class="hlt">gamma</span> cameras are being developed to help identify radiation hotspots and ensure effective decontamination operation. The Compton camera utilizes the kinematics of Compton scattering to contract images without using a mechanical collimator, and features a wide field of view. For instance, we have developed a novel Compton camera that features a small size (13 × 14 × 15 cm3) and light weight (1.9 kg), but which also achieves high sensitivity thanks to Ce:GAGG scintillators optically coupled wiith MPPC arrays. By definition, in such a Compton camera, <span class="hlt">gamma</span> rays are expected to scatter in the ``scatterer'' and then be fully absorbed in the ``absorber'' (in what is called a forward-scattered event). However, high <span class="hlt">energy</span> <span class="hlt">gamma</span> rays often interact with the detector in the opposite direction - initially scattered in the absorber and then absorbed in the scatterer - in what is called a ``back-scattered'' event. Any contamination of such back-scattered events is known to substantially degrade the quality of <span class="hlt">gamma</span>-ray images, but determining the order of <span class="hlt">gamma</span>-ray interaction based solely on <span class="hlt">energy</span> deposits in the scatterer and absorber is quite difficult. For this reason, we propose a novel yet simple Compton camera design that includes a rear-panel shield (a few mm thick) consisting of W or Pb located just behind the scatterer. Since the <span class="hlt">energy</span> of scattered <span class="hlt">gamma</span> rays in back-scattered events is much lower than that in forward-scattered events, we can effectively discriminate and reduce back-scattered events to improve the signal-to-noise ratio in the images. This paper presents our detailed optimization of the rear-panel shield using Geant4 simulation, and describes a demonstration test using our Compton camera.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/7344849-experimental-determination-energy-spectrum-atmospheric-gamma-rays-mev','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/7344849-experimental-determination-energy-spectrum-atmospheric-gamma-rays-mev"><span>Experimental determination of <span class="hlt">energy</span> spectrum of atmospheric <span class="hlt">gamma</span> rays. [0. 9 to 18. 0 MeV</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Martin, I.M.; Dutra, S.L.G.; Palmeira, R.A.R.</p> <p></p> <p>The <span class="hlt">energy</span> spectrum of atmospheric <span class="hlt">gamma</span> rays from 0.9 to 18.0 MeV was measured as a function of altitude in a series of two balloon flights from Sao Jose dos Campos, Sao Paulo, Brasil (12 GV cut-off rigidity). The detector used was a NaI(T1) crystal with a 1-cm-thick plastic scintillator anti-coincidence shield, connected to a 128-channel pulse height analyzer. Above 20 g/cm/sup 2/ the <span class="hlt">energy</span> spectrum could be fitted to a power law with exponent 1.0 + or - 0.1 independent of the altitude. From 20 to 760 g/cm/sup 2/ the spectrum was found to be somewhat steeper, with themore » exponential index being 1.3 + or - 0.1. At 3.5 g/cm/sup 2/ the <span class="hlt">gamma</span> ray flux was 0.30 photons/cm/sup 2/ -s at 1 MeV. These measurements are discussed and compared with calculated results. (auth)« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/18784718','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/18784718"><span>Broadband observations of the naked-eye <span class="hlt">gamma</span>-ray burst GRB 080319B.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Racusin, J L; Karpov, S V; Sokolowski, M; Granot, J; Wu, X F; Pal'shin, V; Covino, S; van der Horst, A J; Oates, S R; Schady, P; Smith, R J; Cummings, J; Starling, R L C; Piotrowski, L W; Zhang, B; Evans, P A; Holland, S T; Malek, K; Page, M T; Vetere, L; Margutti, R; Guidorzi, C; Kamble, A P; Curran, P A; Beardmore, A; Kouveliotou, C; Mankiewicz, L; Melandri, A; O'Brien, P T; Page, K L; Piran, T; Tanvir, N R; Wrochna, G; Aptekar, R L; Barthelmy, S; Bartolini, C; Beskin, G M; Bondar, S; Bremer, M; Campana, S; Castro-Tirado, A; Cucchiara, A; Cwiok, M; D'Avanzo, P; D'Elia, V; Valle, M Della; de Ugarte Postigo, A; Dominik, W; Falcone, A; Fiore, F; Fox, D B; Frederiks, D D; Fruchter, A S; Fugazza, D; Garrett, M A; Gehrels, N; Golenetskii, S; Gomboc, A; Gorosabel, J; Greco, G; Guarnieri, A; Immler, S; Jelinek, M; Kasprowicz, G; La Parola, V; Levan, A J; Mangano, V; Mazets, E P; Molinari, E; Moretti, A; Nawrocki, K; Oleynik, P P; Osborne, J P; Pagani, C; Pandey, S B; Paragi, Z; Perri, M; Piccioni, A; Ramirez-Ruiz, E; Roming, P W A; Steele, I A; Strom, R G; Testa, V; Tosti, G; Ulanov, M V; Wiersema, K; Wijers, R A M J; Winters, J M; Zarnecki, A F; Zerbi, F; Mészáros, P; Chincarini, G; Burrows, D N</p> <p>2008-09-11</p> <p>Long-duration <span class="hlt">gamma</span>-ray bursts (GRBs) <span class="hlt">release</span> copious amounts of <span class="hlt">energy</span> across the entire electromagnetic spectrum, and so provide a window into the process of black hole formation from the collapse of massive stars. Previous early optical observations of even the most exceptional GRBs (990123 and 030329) lacked both the temporal resolution to probe the optical flash in detail and the accuracy needed to trace the transition from the prompt emission within the outflow to external shocks caused by interaction with the progenitor environment. Here we report observations of the extraordinarily bright prompt optical and <span class="hlt">gamma</span>-ray emission of GRB 080319B that provide diagnostics within seconds of its formation, followed by broadband observations of the afterglow decay that continued for weeks. We show that the prompt emission stems from a single physical region, implying an extremely relativistic outflow that propagates within the narrow inner core of a two-component jet.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JLTP..tmp..156K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JLTP..tmp..156K"><span>Development of MMC <span class="hlt">Gamma</span> Detectors for Precise Characterization of Uranium Isotopes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kim, G. B.; Flynn, C. C.; Kempf, S.; Gastaldo, L.; Fleischmann, A.; Enss, C.; Friedrich, S.</p> <p>2018-06-01</p> <p>Precise nuclear data from radioactive decays are important for the accurate non-destructive assay of fissile materials in nuclear safeguards. We are developing high <span class="hlt">energy</span> resolution <span class="hlt">gamma</span> detectors based on metallic magnetic calorimeters (MMCs) to accurately measure <span class="hlt">gamma</span>-ray <span class="hlt">energies</span> and branching ratios of uranium isotopes. Our MMC <span class="hlt">gamma</span> detectors exhibit good linearity, reproducibility and a consistent response function for low <span class="hlt">energy</span> <span class="hlt">gamma</span>-rays. We illustrate the capabilities of MMCs to improve literature values of nuclear data with an analysis of <span class="hlt">gamma</span> spectra of U-233. In this context, we also improve the value of the <span class="hlt">energy</span> for the single <span class="hlt">gamma</span>-ray of the U-233 daughter Ra-225 by over an order of magnitude from 40.09 ± 0.05 to 40.0932 ± 0.0007 keV.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JPhCS.934a2022D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JPhCS.934a2022D"><span>The “Carpet-3” air shower array to search for diffuse <span class="hlt">gamma</span> rays with <span class="hlt">energy</span> Eγ>100TeV</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Dzhappuev, D. D.; I, V. B. Petkov V.; Kudzhaev, A. U.; Lidvansky, A. S.; Volchenko, V. I.; Volchenko, G. V.; Gorbacheva, E. A.; Dzaparova, I. M.; Klimenko, N. F.; Kurenya, A. N.; Mikhilova, O. I.; Khadzhiev, M. M.; Yanin, A. F.</p> <p>2017-12-01</p> <p>At present an experiment for measuring the flux of cosmic diffuse <span class="hlt">gamma</span> rays with <span class="hlt">energy</span> higher than 100 TeV (experiment “Carpet-3”) is being prepared at the Baksan Neutrino Observatory of the Institute for Nuclear Research, Russian Academy of Sciences. The preparation of the experiment implies considerable enlargement of the area of both muon detector and surface part of the shower array. At the moment the plastic scintillation counters with a total continuous area of 410 m2 are installed in the muon detector (MD) underground tunnels, and they are totally equipped with electronics. Adjusting of the counters and their electronic circuits is in progress. Six modules of shower detectors (out of twenty planned to be installed) have already been placed on the surface of the MD absorber. A new liquid scintillation detector is developed for modules of the ground -surface part of the array, whose characteristics are presented. It is shown that the “Carpet-3” air shower array will have the best sensitivity to the flux of primary <span class="hlt">gamma</span> rays with <span class="hlt">energies</span> in the range 100TeV - 1PeV, being quite competitive in <span class="hlt">gamma</span>-ray astronomy at such <span class="hlt">energies</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EPJWC.15307007T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EPJWC.15307007T"><span>Precise calculation of neutron-capture reactions contribution in <span class="hlt">energy</span> <span class="hlt">release</span> for different types of VVER-1000 fuel assemblies</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tikhomirov, Georgy; Bahdanovich, Rynat; Pham, Phu</p> <p>2017-09-01</p> <p>Precise calculation of <span class="hlt">energy</span> <span class="hlt">release</span> in a nuclear reactor is necessary to obtain the correct spatial power distribution and predict characteristics of burned nuclear fuel. In this work, previously developed method for calculation neutron-capture reactions - capture component - contribution in effective <span class="hlt">energy</span> <span class="hlt">release</span> in a fuel core of nuclear reactor is discussed. The method was improved and implemented to the different models of VVER-1000 reactor developed for MCU 5 and MCNP 4 computer codes. Different models of equivalent cell and fuel assembly in the beginning of fuel cycle were calculated. These models differ by the geometry, fuel enrichment and presence of burnable absorbers. It is shown, that capture component depends on fuel enrichment and presence of burnable absorbers. Its value varies for different types of hot fuel assemblies from 3.35% to 3.85% of effective <span class="hlt">energy</span> <span class="hlt">release</span>. Average capture component contribution in effective <span class="hlt">energy</span> <span class="hlt">release</span> for typical serial fresh fuel of VVER-1000 is 3.5%, which is 7 MeV/fission. The method will be used in future to estimate the dependency of capture <span class="hlt">energy</span> on fuel density, burn-up, etc.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19850048771&hterms=sonar&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3Dsonar','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19850048771&hterms=sonar&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3Dsonar"><span>Helios 1 energetic particle observations of the solar <span class="hlt">gamma</span>-ray/neutron flare events of 1982 June 3 and 1980 June 21</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Mcdonald, F. B.; Van Hollebeke, M. A. I.</p> <p>1985-01-01</p> <p>The characteristics of the energetic particles associated with the solar <span class="hlt">gamma</span>-ray/neutron flare events of June 3, 1982 and June 21, 1980 observed by the Goddard cosmic-ray experiment on Helios 1 (at heliocentric distances of 0.57 and 0.54 AU, respectively) differ in several important respects from typical sonar particle increases. In particular, the June 3, 1982 event has a proton <span class="hlt">energy</span> spectrum which fits a remarkable flat power law in kinetic <span class="hlt">energy</span> with a spectral index of 1.2, an electron/proton ratio of 1 at 4 MeV, and a small but well-defined precursor event that began some 3 hr before the impulsive flare increase. Similar energetic particle precursors were observed for the <span class="hlt">gamma</span>-ray associated 1980 June 21 and June 7 flare events. At <span class="hlt">energies</span> less than about 40 MeV, the particle onset time measured for the June 3, 1982 event is anomalous, suggesting that these lower <span class="hlt">energy</span> particles may have been <span class="hlt">released</span> at the sun about 1-2 minutes before the higher <span class="hlt">energy</span> particles.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28260825','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28260825"><span>Preliminary evaluation of a novel <span class="hlt">energy</span>-resolved photon-counting <span class="hlt">gamma</span> ray detector.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Meng, L-J; Tan, J W; Spartiotis, K; Schulman, T</p> <p>2009-06-11</p> <p>In this paper, we present the design and preliminary performance evaluation of a novel <span class="hlt">energy</span>-resolved photon-counting (ERPC) detector for <span class="hlt">gamma</span> ray imaging applications. The prototype ERPC detector has an active area of 4.4 cm × 4.4 cm, which is pixelated into 128 × 128 square pixels with a pitch size of 350 µm × 350µm. The current detector consists of multiple detector hybrids, each with a CdTe crystal of 1.1 cm × 2.2 cm × 1 mm, bump-bonded onto a custom-designed application-specific integrated circuit (ASIC). The ERPC ASIC has 2048 readout channels arranged in a 32 × 64 array. Each channel is equipped with pre- and shaping-amplifiers, a discriminator, peak/hold circuitry and an analog-to-digital converter (ADC) for digitizing the signal amplitude. In order to compensate for the pixel-to-pixel variation, two 8-bit digital-to-analog converters (DACs) are implemented into each channel for tuning the gain and offset. The ERPC detector is designed to offer a high spatial resolution, a wide dynamic range of 12-200 keV and a good <span class="hlt">energy</span> resolution of 3-4 keV. The hybrid detector configuration provides a flexible detection area that can be easily tailored for different imaging applications. The intrinsic performance of a prototype ERPC detector was evaluated with various <span class="hlt">gamma</span> ray sources, and the results are presented.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/12018745','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/12018745"><span>Calibration of TLD badges for photons of <span class="hlt">energy</span> above 6 MeV and dosimetric intricacies in high <span class="hlt">energy</span> <span class="hlt">gamma</span> ray fields encountered in nuclear power plants.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Pradhan, A S; Bakshi, A K</p> <p>2002-01-01</p> <p>CaSO4:Dy and LiF TLDs do not exhibit photon <span class="hlt">energy</span> dependence beyond +/-55% for photons in the <span class="hlt">energy</span> range from 1 MeV to about 7 MeV. However, when sandwiched between metal filters or used in TLD badge holders having metal filters, the response changes for irradiation from high <span class="hlt">energy</span> photons as compared to that from 60Co <span class="hlt">gamma</span> rays (generally used for reference calibrations). This effect is about the same for both the lower atomic number TLD (LiF) and higher atomic number TLD (CaSO4:Dy). For TLDs held on the surface of the phantom and irradiated in collimated photon beams, the response of TLDs without any filter or those under the open window of the TLD badge is considerably reduced due to insufficient build-up to high <span class="hlt">energy</span> photons, whereas for uncollimated radiation fields from power reactors, an over-response is observed. It is observed that the use of inappropriate encapsulation of dosemeters would cause a significant error not only in the estimation of doses due to penetrating radiations but also in the estimation of beta doses in the mixed fields of beta radiation, high <span class="hlt">energy</span> <span class="hlt">gamma</span> rays and high <span class="hlt">energy</span> electrons often encountered in the fields of pressurised heavy water reactors.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20170003313','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20170003313"><span>Measurement of the High-<span class="hlt">Energy</span> <span class="hlt">Gamma</span>-Ray Emission from the Moon with the Fermi Large Area Telescope</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Ackermann, M.; Ajello, M.; Albert, A.; Atwood, W. B.; Baldini, L.; Barbiellini, G.; Bastieri, D.; Bellazzini, R.; Bissaldi, E.; Blandford, R. D.; <a style="text-decoration: none; " href="javascript:void(0); " onClick="displayelement('author_20170003313'); toggleEditAbsImage('author_20170003313_show'); toggleEditAbsImage('author_20170003313_hide'); "> <img style="display:inline; width:12px; height:12px; " src="images/arrow-up.gif" width="12" height="12" border="0" alt="hide" id="author_20170003313_show"> <img style="width:12px; height:12px; display:none; " src="images/arrow-down.gif" width="12" height="12" border="0" alt="hide" id="author_20170003313_hide"></p> <p>2016-01-01</p> <p>We have measured the <span class="hlt">gamma</span>-ray emission spectrum of the Moon using the data collected by the Large Area Telescope onboard the Fermi satellite during its first seven years of operation, in the <span class="hlt">energy</span> range from 30 MeV up to a few GeV. We have also studied the time evolution of the flux, finding a correlation with the solar activity. We have developed a full Monte Carlo simulation describing the interactions of cosmic rays with the lunar surface. The results of the present analysis can be explained in the framework of this model, where the production of <span class="hlt">gamma</span> rays is due to the interactions of cosmic-ray proton and helium nuclei with the surface of the Moon. Finally, we have used our simulation to derive the cosmic-ray proton and helium spectra near Earth from the Moon <span class="hlt">gamma</span>-ray data.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1266677-physics-reflective-optics-soft-gamma-ray-photon-energy-range','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1266677-physics-reflective-optics-soft-gamma-ray-photon-energy-range"><span>Physics of reflective optics for the soft <span class="hlt">gamma</span>-ray photon <span class="hlt">energy</span> range</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Fernandez-Perea, Monica; Descalle, Marie -Anne; Soufli, Regina; ...</p> <p>2013-07-12</p> <p>Traditional multilayer reflective optics that have been used in the past for imaging at x-ray photon <span class="hlt">energies</span> as high as 200 keV are governed by classical wave phenomena. However, their behavior at higher <span class="hlt">energies</span> is unknown, because of the increasing effect of incoherent scattering and the disagreement between experimental and theoretical optical properties of materials in the hard x-ray and <span class="hlt">gamma</span>-ray regimes. Here, we demonstrate that multilayer reflective optics can operate efficiently and according to classical wave physics up to photon <span class="hlt">energies</span> of at least 384 keV. We also use particle transport simulations to quantitatively determine that incoherent scattering takesmore » place in the mirrors but it does not affect the performance at the Bragg angles of operation. Furthermore, our results open up new possibilities of reflective optical designs in a spectral range where only diffractive optics (crystals and lenses) and crystal monochromators have been available until now.« less</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li class="active"><span>21</span></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_21 --> <div id="page_22" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li class="active"><span>22</span></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="421"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20160005332','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20160005332"><span>Fermi: The <span class="hlt">Gamma</span>-Ray Large Area Space Telescope</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>McEnery, Julie</p> <p>2014-01-01</p> <p>Following its launch in June 2008, high-<span class="hlt">energy</span> <span class="hlt">gamma</span>-ray observations by the Fermi <span class="hlt">Gamma</span>-ray Space Telescope have unveiled over 1000 new sources and opened an important and previously unexplored window on a wide variety of phenomena. These have included the discovery of an population of pulsars pulsing only in <span class="hlt">gamma</span> rays; the detection of photons up to 10s of GeV from <span class="hlt">gamma</span>-ray bursts, enhancing our understanding of the astrophysics of these powerful explosions; the detection of hundreds of active galaxies; a measurement of the high <span class="hlt">energy</span> cosmic-ray electron spectrum which may imply the presence of nearby astrophysical particle accelerators; the determination of the diffuse <span class="hlt">gamma</span>-ray emission with unprecedented accuracy and the constraints on phenomena such as supersymmetric dark-matter annihilations and exotic relics from the Big Bang. Continuous monitoring of the high-<span class="hlt">energy</span> <span class="hlt">gamma</span>-ray sky has uncovered numerous outbursts from active galaxies and the discovery of transient sources in our galaxy. In this talk I will describe the current status of the Fermi observatory and review the science highlights from Fermi.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19900003152','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19900003152"><span>The solar <span class="hlt">gamma</span> ray and neutron capabilities of COMPTEL on the <span class="hlt">Gamma</span> Ray Observatory</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Ryan, James M.; Lockwood, John A.</p> <p>1989-01-01</p> <p>The imaging Compton telescope COMPTEL on the <span class="hlt">Gamma</span> Ray Observatory (GRO) has unusual spectroscopic capabilities for measuring solar <span class="hlt">gamma</span>-ray and neutron emission. The launch of the GRO is scheduled for June 1990 near the peak of the sunspot cycle. With a 30 to 40 percent probability for the Sun being in the COMPTEL field-of-view during the sunlit part of an orbit, a large number of flares will be observed above the 800 keV <span class="hlt">gamma</span>-ray threshold of the telescope. The telescope <span class="hlt">energy</span> range extends to 30 MeV with high time resolution burst spectra available from 0.1 to 10 MeV. Strong Compton tail suppression of instrumental <span class="hlt">gamma</span>-ray interactions will facilitate improved spectral analysis of solar flare emissions. In addition, the high signal to noise ratio for neutron detection and measurement will provide new neutron spectroscopic capabilities. Specifically, a flare similar to that of 3 June 1982 will provide spectroscopic data on greater than 1500 individual neutrons, enough to construct an unambiguous spectrum in the <span class="hlt">energy</span> range of 20 to 200 MeV. Details of the instrument and its response to solar <span class="hlt">gamma</span>-rays and neutrons will be presented.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/19883256','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/19883256"><span>Physicochemical properties and antioxidant activity of <span class="hlt">gamma</span>-oryzanol-loaded liposome formulations for topical use.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Viriyaroj, Amornrat; Ngawhirunpat, Tanasait; Sukma, Monrudee; Akkaramongkolporn, Prasert; Ruktanonchai, Uracha; Opanasopit, Praneet</p> <p>2009-01-01</p> <p>The objective of this study is to prepare the <span class="hlt">gamma</span>-oryzanol-loaded liposomes and investigate their physicochemical properties and antioxidant activity intended for cosmetic applications. Liposomes, Composing phosphatidylCholine (PC) and Cholesterol (Chol), CHAPS or sodium taurocholate (NaTC) were prepared by sonication method. <span class="hlt">Gamma</span>-oryzanol-loaded liposomes were prepared by using 3, 5 and 10% <span class="hlt">gamma</span>-oryzanol as an initial concentration. The formulation factors in a particular type and composition of lipid and initial drug loading on the physicochemical properties (i.e., particle size, zeta potential, entrapment efficiency, drug <span class="hlt">release</span>) and antioxidant activity were studied. The particle sizes of bare liposomes were in nanometer range. The <span class="hlt">gamma</span>-oryzanol-loaded liposomes in formulations of PC/CHAPS and PC/NaTC liposomes were smaller than PC/Chol liposomes. The incorporation efficiency of 10% <span class="hlt">gamma</span>-oryzanol-loaded PC/Chol liposomes was less than <span class="hlt">gamma</span>-oryzanol-loaded PC/CHAPS liposomes and PC/NaTC liposomes allowing higher in vitro <span class="hlt">release</span> rate due to higher free <span class="hlt">gamma</span>-oryzanol in buffer solution. The antioxidant activity of <span class="hlt">gamma</span>-oryzanol-loaded liposomes was not different from pure <span class="hlt">gamma</span>-oryzanol. Both <span class="hlt">gamma</span>-oryzanol-loaded PC/CHAPS liposomes and PC/NaTC liposomes were showed to enhance the antioxidant activity in NHF cells. <span class="hlt">gamma</span>-oryzanol-loaded PC/Chol liposomes demonstrated the lowest cytotoxicity in NHF cells. It was conceivably concluded that liposomes prepared in this study are suitable for <span class="hlt">gamma</span>-oryzanol incorporation without loss of antioxidant activity.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017NIMPA.866..164S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017NIMPA.866..164S"><span>PANDORA, a large volume low-<span class="hlt">energy</span> neutron detector with real-time neutron-<span class="hlt">gamma</span> discrimination</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Stuhl, L.; Sasano, M.; Yako, K.; Yasuda, J.; Baba, H.; Ota, S.; Uesaka, T.</p> <p>2017-09-01</p> <p>The PANDORA (Particle Analyzer Neutron Detector Of Real-time Acquisition) system, which was developed for use in inverse kinematics experiments with unstable isotope beams, is a neutron detector based on a plastic scintillator coupled to a digital readout. PANDORA can be used for any reaction study involving the emission of low <span class="hlt">energy</span> neutrons (100 keV-10 MeV) where background suppression and an increased signal-to-noise ratio are crucial. The digital readout system provides an opportunity for pulse shape discrimination (PSD) of the detected particles as well as intelligent triggering based on PSD. The figure of merit results of PANDORA are compared to the data in literature. Using PANDORA, 91 ± 1% of all detected neutrons can be separated, while 91 ± 1% of the detected <span class="hlt">gamma</span> rays can be excluded, reducing the <span class="hlt">gamma</span> ray background by one order of magnitude.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19780008042','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19780008042"><span>Diffuse <span class="hlt">gamma</span> radiation</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Fichtel, C. E.; Simpson, G. A.; Thompson, D. J.</p> <p>1977-01-01</p> <p>An examination of the intensity, <span class="hlt">energy</span> spectrum, and spatial distribution of the diffuse <span class="hlt">gamma</span>-radiation observed by SAS-2 satellite away from the galactic plane in the <span class="hlt">energy</span> range above 35 MeV has shown that it consists of two components. One component is generally correlated with galactic latitudes, the atomic hydrogen column density was deduced from 21 cm measurements, and the continuum radio emission, believed to be synchrotron emission. It has an <span class="hlt">energy</span> spectrum similar to that in the plane and joins smoothly to the intense radiation from the plane. It is therefore presumed to be of galactic origin. The other component is apparently isotropic, at least on a coarse scale, and has a steep <span class="hlt">energy</span> spectrum. No evidence is found for a cosmic ray halo surrounding the galaxy in the shape of a sphere or oblate spheroid with galactic dimensions. Constraints for a halo model with significantly larger dimensions are set on the basis of an upper limit to the <span class="hlt">gamma</span>-ray anisotropy.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22522197-energy-release-initiation-sunquake-class-flare','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22522197-energy-release-initiation-sunquake-class-flare"><span><span class="hlt">ENERGY</span> <span class="hlt">RELEASE</span> AND INITIATION OF A SUNQUAKE IN A C-CLASS FLARE</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Sharykin, I. N.; Kosovichev, A. G.; Zimovets, I. V.</p> <p></p> <p>We present an analysis of the C7.0 solar flare from 2013 February 17, revealing a strong helioseismic response (sunquake) caused by a compact impact observed with the Helioseismic and Magnetic Imager on board the Solar Dynamics Observatory (SDO) in the low atmosphere. This is the weakest known C-class flare generating a sunquake event. To investigate the possible mechanisms of this event and understand the role of accelerated charged particles and photospheric electric currents, we use data from three space observatories: RHESSI, SDO, and Geostationary Operational Environmental Satellite. We find that the photospheric flare impact does not spatially correspond to themore » strongest hard X-ray emission source, but both of these events are parts of the same <span class="hlt">energy</span> <span class="hlt">release</span>. Our analysis reveals a close association of the flare <span class="hlt">energy</span> <span class="hlt">release</span> with a rapid increase in the electric currents and suggests that the sunquake initiation is unlikely to be caused by the impact of high-<span class="hlt">energy</span> electrons, but may be associated with rapid current dissipation or a localized impulsive Lorentz force in the lower layers of the solar atmosphere.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010RaPC...79..286Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010RaPC...79..286Z"><span>Influence of <span class="hlt">gamma</span> radiation onto polymeric matrix with papain</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zulli, Gislaine; Lopes, Patrícia Santos; Velasco, Maria Valéria Robles; Alcântara, Mara Tânia Silva; Rogero, Sizue Ota; Lugao, Ademar Benévolo; Mathor, Monica Beatriz</p> <p>2010-03-01</p> <p>Papain is a proteolytic enzyme that has been widely used as debridement agent for scars and wound healing treatment. However, papain presents low stability, which limits its use to extemporaneous or short shelf-life formulations. The purpose of this study was to entrap papain into a polymeric matrix in order to obtain a drug delivery system that could be used as medical device. Since these systems must be sterile, <span class="hlt">gamma</span> radiation is an interesting option and presents advantages in relation to conventional agents: no radioactive residues are formed; the product can be sterilized inside the final packaging and has an excellent reliability. The normative reference for the establishment of the sterilizing dose determines 25 kGy as the inactivation dose for viable microorganisms. A silicone dispersion was selected to prepare membranes containing 2% (w/w) papain. Irradiated and non-irradiated membranes were simultaneously assessed in order to verify whether <span class="hlt">gamma</span> radiation interferes with the drug-<span class="hlt">releasing</span> profile. Results showed that irradiation does not affect significantly papain <span class="hlt">release</span> and its activity. Therefore papain shows radioresistance in the irradiation conditions applied. In conclusion, <span class="hlt">gamma</span> radiation can be easily used as sterilizing agent without affecting the papain <span class="hlt">release</span> profile and its activity onto the biocompatible device is studied.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19880033086&hterms=INF&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3DINF','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19880033086&hterms=INF&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3DINF"><span>Potential mechanisms of cytosolic calcium modulation in interferon-<span class="hlt">gamma</span> treated U937 cells</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Klein, Jon B.; Mcleish, Kenneth R.; Sonnenfeld, Gerald; Dean, William L.</p> <p>1987-01-01</p> <p>The ability of interferon-<span class="hlt">gamma</span> (IFN-<span class="hlt">gamma</span>) to alter cytoplasmic Ca(2+) content in the monocytelike cell line U937 was investigated, using a slow Ca-channel blocker, diltiazem. In addition, the Ca-ATPase and the Ca-uptake activities were measured in isolated U937 membranes, together with the effect of inositol trisphosphate (IP3) upon the Ca(2+) <span class="hlt">release</span> from Ca-loaded membranes. The addition of 50 U/ml INF-<span class="hlt">gamma</span> to U937 cultures was found to increase internal Ca(2+) by about 100 percent within 3 min. The increase was significantly reduced by incubation in Ca-free buffer or by the addition of diltiazem. A crude membrane preparation from U937 cells was found to contain significant amounts of Ca-ATPase activity and to sequester Ca(2+) to a level of 8 nmol/mg in 30 sec; the addition of IP3 induced <span class="hlt">release</span> of a portion of the sequestered Ca(2+) which was then resequestered. The results suggest that IFN-<span class="hlt">gamma</span> causes an increase of cytoplasmic Ca(2+), in part, by the IP3-induced <span class="hlt">release</span> from the internal storage sites and, in part, from the entry of extracellular Ca through slow channels.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19920012689','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19920012689"><span>Low <span class="hlt">energy</span> <span class="hlt">gamma</span> ray emission from the Cygnus OB2 association</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Chen, Wan; White, Richard L.</p> <p>1992-01-01</p> <p>According to our newly developed model of <span class="hlt">gamma</span>-ray emission from chaotic early-type stellar winds, we predict the combined <span class="hlt">gamma</span>-ray flux from the circumstellar winds of many very luminous early-type stars in the Cyg OB2 association can be detectable by the Energetic <span class="hlt">Gamma</span> Ray Experiment Telescope (EGRET) (and maybe also by OSSE) on CGRO. Due to different radiation mechanisms, the <span class="hlt">gamma</span>-ray spectrum from stellar winds can be quite different from that of CYG X-3; this spectral difference and the time-variation of Cyg X-3 flux will help to distinguish the <span class="hlt">gamma</span>-ray components from different sources in this small region, which is spatially unresolvable by CGRO.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28065630','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28065630"><span>Digital <span class="hlt">gamma-gamma</span> coincidence HPGe system for environmental analysis.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Marković, Nikola; Roos, Per; Nielsen, Sven Poul</p> <p>2017-08-01</p> <p>The performance of a new <span class="hlt">gamma-gamma</span> coincidence spectrometer system for environmental samples analysis at the Center for Nuclear Technologies of the Technical University of Denmark (DTU) is reported. Nutech Coincidence Low <span class="hlt">Energy</span> Germanium Sandwich (NUCLeGeS) system consists of two HPGe detectors in a surface laboratory with a digital acquisition system used to collect the data in time-stamped list mode with 10ns time resolution. The spectrometer is used in both anticoincidence and coincidence modes. Copyright © 2017 Elsevier Ltd. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018NaPho..12..319B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018NaPho..12..319B"><span>Giant collimated <span class="hlt">gamma</span>-ray flashes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Benedetti, Alberto; Tamburini, Matteo; Keitel, Christoph H.</p> <p>2018-06-01</p> <p>Bright sources of high-<span class="hlt">energy</span> electromagnetic radiation are widely employed in fundamental research, industry and medicine1,2. This motivated the construction of Compton-based facilities planned to yield bright <span class="hlt">gamma</span>-ray pulses with <span class="hlt">energies</span> up to3 20 MeV. Here, we demonstrate a novel mechanism based on the strongly amplified synchrotron emission that occurs when a sufficiently dense ultra-relativistic electron beam interacts with a millimetre-thickness conductor. For electron beam densities exceeding approximately 3 × 1019 cm-3, electromagnetic instabilities occur, and the ultra-relativistic electrons travel through self-generated electromagnetic fields as large as 107-108 gauss. This results in the production of a collimated <span class="hlt">gamma</span>-ray pulse with peak brilliance above 1025 photons s-1 mrad-2 mm-2 per 0.1% bandwidth, photon <span class="hlt">energies</span> ranging from 200 keV to gigaelectronvolts and up to 60% electron-to-photon <span class="hlt">energy</span> conversion efficiency. These findings pave the way to compact, high-repetition-rate (kilohertz) sources of short (≲30 fs), collimated (milliradian) and high-flux (>1012 photons s-1) <span class="hlt">gamma</span>-ray pulses.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19910063389&hterms=iodine&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3Diodine','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19910063389&hterms=iodine&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3Diodine"><span>Mercuric iodine room temperature <span class="hlt">gamma</span>-ray detectors</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Patt, Bradley E.; Markakis, Jeffrey M.; Gerrish, Vernon M.; Haymes, Robert C.; Trombka, Jacob I.</p> <p>1990-01-01</p> <p>high resolution mercuric iodide room temperature <span class="hlt">gamma</span>-ray detectors have excellent potential as an essential component of space instruments to be used for high <span class="hlt">energy</span> astrophysics. Mercuric iodide detectors are being developed both as photodetectors used in combination with scintillation crystals to detect <span class="hlt">gamma</span>-rays, and as direct <span class="hlt">gamma</span>-ray detectors. These detectors are highly radiation damage resistant. The list of applications includes <span class="hlt">gamma</span>-ray burst detection, <span class="hlt">gamma</span>-ray line astronomy, solar flare studies, and elemental analysis.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19980237961','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19980237961"><span><span class="hlt">Gamma</span> Radiation from PSR B1055-52</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Thompson, D. J.; Bailes, M.; Bertsch, D. L.; Cordes, J.; DAmico, N. D.; Esposito, J. A.; Finley, J.; Hartman, R. C.; Hermsen, W.; Kanbach, G.; <a style="text-decoration: none; " href="javascript:void(0); " onClick="displayelement('author_19980237961'); toggleEditAbsImage('author_19980237961_show'); toggleEditAbsImage('author_19980237961_hide'); "> <img style="display:inline; width:12px; height:12px; " src="images/arrow-up.gif" width="12" height="12" border="0" alt="hide" id="author_19980237961_show"> <img style="width:12px; height:12px; display:none; " src="images/arrow-down.gif" width="12" height="12" border="0" alt="hide" id="author_19980237961_hide"></p> <p>1998-01-01</p> <p>The telescopes on the Compton <span class="hlt">Gamma</span> Ray Observatory (CCRO) have observed PSR B1055-52 a number of times between 1991 and 1998. From these data, a more detailed picture of the <span class="hlt">gamma</span> radiation from this source has been developed, showing several characteristics which distinguish this pulsar: the light curve is complex; there is no detectable unpulsed emission; the <span class="hlt">energy</span> spectrum is flat, with no evidence of a sharp high-<span class="hlt">energy</span> cutoff up to greater than 4 GeV. Comparisons of the <span class="hlt">gamma</span>-ray data with observations at longer wavelengths show that no two of the known <span class="hlt">gamma</span>-ray pulsars have quite the same characteristics; this diversity makes interpretation in terms of theoretical models difficult.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19990042027','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19990042027"><span><span class="hlt">Gamma</span> Radiation from PSR B1055-52</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Thompson, D. J.; Bailes, M.; Bertsch, D. L.; Cordes, J.; DAmico, N.; Esposito, J. A.; Finley, J.; Hartman, R. C.; Hermsen, W.; Kanbach, G.; <a style="text-decoration: none; " href="javascript:void(0); " onClick="displayelement('author_19990042027'); toggleEditAbsImage('author_19990042027_show'); toggleEditAbsImage('author_19990042027_hide'); "> <img style="display:inline; width:12px; height:12px; " src="images/arrow-up.gif" width="12" height="12" border="0" alt="hide" id="author_19990042027_show"> <img style="width:12px; height:12px; display:none; " src="images/arrow-down.gif" width="12" height="12" border="0" alt="hide" id="author_19990042027_hide"></p> <p>1999-01-01</p> <p>The telescopes on the Compton <span class="hlt">Gamma</span> Ray Observatory (CGRO) have observed PSR B1055-52 a number of times between 1991 and 1998. From these data, a more detailed picture of the <span class="hlt">gamma</span> radiation from this source has been developed, showing several characteristics which distinguish this pulsar: the light curve is complex; there is no detectable unpulsed emission; the <span class="hlt">energy</span> spectrum is flat, with no evidence of a sharp high-<span class="hlt">energy</span> cutoff up to greater than 4 GeV. Comparisons of the <span class="hlt">gamma</span>-ray data with observations at longer wavelengths show that no two of the known <span class="hlt">gamma</span>-ray pulsars have quite the same characteristics; this diversity makes interpretation in terms of theoretical models difficult.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2005ApJ...621..181D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2005ApJ...621..181D"><span>Spectrum of Very High <span class="hlt">Energy</span> <span class="hlt">Gamma</span>-Rays from the blazar 1ES 1959+650 during Flaring Activity in 2002</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Daniel, M. K.; Badran, H. M.; Bond, I. H.; Boyle, P. J.; Bradbury, S. M.; Buckley, J. H.; Carter-Lewis, D. A.; Catanese, M.; Celik, O.; Cogan, P.; Cui, W.; D'Vali, M.; de la Calle Perez, I.; Duke, C.; Falcone, A.; Fegan, D. J.; Fegan, S. J.; Finley, J. P.; Fortson, L. F.; Gaidos, J. A.; Gammell, S.; Gibbs, K.; Gillanders, G. H.; Grube, J.; Hall, J.; Hall, T. A.; Hanna, D.; Hillas, A. M.; Holder, J.; Horan, D.; Humensky, T. B.; Jarvis, A.; Jordan, M.; Kenny, G. E.; Kertzman, M.; Kieda, D.; Kildea, J.; Knapp, J.; Kosack, K.; Krawczynski, H.; Krennrich, F.; Lang, M. J.; Le Bohec, S.; Linton, E.; Lloyd-Evans, J.; Milovanovic, A.; Moriarty, P.; Müller, D.; Nagai, T.; Nolan, S.; Ong, R. A.; Pallassini, R.; Petry, D.; Power-Mooney, B.; Quinn, J.; Quinn, M.; Ragan, K.; Rebillot, P.; Reynolds, P. T.; Rose, H. J.; Schroedter, M.; Sembroski, G. H.; Swordy, S. P.; Syson, A.; Vassiliev, V. V.; Wakely, S. P.; Walker, G.; Weekes, T. C.; Zweerink, J.</p> <p>2005-03-01</p> <p>The blazar 1ES 1959+650 was observed in a flaring state with the Whipple 10 m Imaging Atmospheric Cerenkov Telescope in 2002 May. A spectral analysis has been carried out on the data from that time period, and the resulting very high <span class="hlt">energy</span> <span class="hlt">gamma</span>-ray spectrum (E>=316 GeV) can be well fitted by a power law of differential spectral index α=2.78+/-0.12stat+/-0.21sys. On 2002 June 4, the source flared dramatically in the <span class="hlt">gamma</span>-ray range without any coincident increase in the X-ray emission, providing the first unambiguous example of an ``orphan'' <span class="hlt">gamma</span>-ray flare from a blazar. The <span class="hlt">gamma</span>-ray spectrum for these data can also be described by a simple power-law fit with α=2.82+/-0.15stat+/-0.30sys. There is no compelling evidence for spectral variability or for any cutoff to the spectrum.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20140017714','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20140017714"><span>A Pair Production Telescope for Medium-<span class="hlt">Energy</span> <span class="hlt">Gamma</span>-Ray Polarimetry</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Hunter, Stanley D.; Bloser, Peter F.; Depaola, Gerardo; Dion, Michael P.; DeNolfo, Georgia A.; Hanu, Andrei; Iparraguirre, Marcos; Legere, Jason; Longo, Francesco; McConnell, Mark L.; <a style="text-decoration: none; " href="javascript:void(0); " onClick="displayelement('author_20140017714'); toggleEditAbsImage('author_20140017714_show'); toggleEditAbsImage('author_20140017714_hide'); "> <img style="display:inline; width:12px; height:12px; " src="images/arrow-up.gif" width="12" height="12" border="0" alt="hide" id="author_20140017714_show"> <img style="width:12px; height:12px; display:none; " src="images/arrow-down.gif" width="12" height="12" border="0" alt="hide" id="author_20140017714_hide"></p> <p>2014-01-01</p> <p>We describe the science motivation and development of a pair production telescope for medium-<span class="hlt">energy</span> (approximately 5-200 Mega electron Volts) <span class="hlt">gamma</span>-ray polarimetry. Our instrument concept, the Advanced Energetic Pair Telescope (AdEPT), takes advantage of the Three-Dimensional Track Imager, a low-density gaseous time projection chamber, to achieve angular resolution within a factor of two of the pair production kinematics limit (approximately 0.6 deg at 70 Mega electron Volts), continuum sensitivity comparable with the Fermi-LAT front detector (is less than 3 x 10(exp -6) Mega electron Volts per square centimeter per second at 70 Mega electron Volts), and minimum detectable polarization less than 10% for a 10 milliCrab source in 10(exp 6) s.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1090844','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1090844"><span>Measuring the charged pion polarizability in the <span class="hlt">gamma</span> <span class="hlt">gamma</span> -> pi+pi- reaction</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Lawrence, David W.; Miskimen, Rory A.; Mushkarenkov, Alexander Nikolaevich</p> <p>2013-08-01</p> <p>Development has begun of a new experiment to measure the charged pion polarizabilitymore » $$\\alpha_{\\pi}-\\beta_{\\pi}$$. The charged pion polarizability ranks among the most important tests of low-<span class="hlt">energy</span> QCD presently unresolved by experiment. Analogous to precision measurements of $$\\pi^{\\circ}\\rightarrow\\<span class="hlt">gamma\\gamma</span>$$ that test the intrinsic odd-parity (anomalous) sector of QCD, the pion polarizability tests the intrinsic even-parity sector of QCD. The measurement will be performed using the $$\\<span class="hlt">gamma\\gamma</span>\\rightarrow\\pi^{+{}}\\pi^{-{}}$$ cross section accessed via the Primakoff mechanism on nuclear targets using the GlueX detector in Hall D at Jefferson Lab. The linearly polarized photon source in Hall-D will be utilized to separate the Primakoff cross-section from coherent $$\\rho^{\\circ}$$ production.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28536507','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28536507"><span>Dopamine Modulates Delta-<span class="hlt">Gamma</span> Phase-Amplitude Coupling in the Prefrontal Cortex of Behaving Rats.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Andino-Pavlovsky, Victoria; Souza, Annie C; Scheffer-Teixeira, Robson; Tort, Adriano B L; Etchenique, Roberto; Ribeiro, Sidarta</p> <p>2017-01-01</p> <p>Dopamine <span class="hlt">release</span> and phase-amplitude cross-frequency coupling (CFC) have independently been implicated in prefrontal cortex (PFC) functioning. To causally investigate whether dopamine <span class="hlt">release</span> affects phase-amplitude comodulation between different frequencies in local field potentials (LFP) recorded from the medial PFC (mPFC) of behaving rats, we used RuBiDopa, a light-sensitive caged compound that <span class="hlt">releases</span> the neurotransmitter dopamine when irradiated with visible light. LFP power did not change in any frequency band after the application of light-uncaged dopamine, but significantly strengthened phase-amplitude comodulation between delta and <span class="hlt">gamma</span> oscillations. Saline did not exert significant changes, while injections of dopamine and RuBiDopa produced a slow increase in comodulation for several minutes after the injection. The results show that dopamine <span class="hlt">release</span> in the medial PFC shifts phase-amplitude comodulation from theta-<span class="hlt">gamma</span> to delta-<span class="hlt">gamma</span>. Although being preliminary results due to the limitation of the low number of animals present in this study, our findings suggest that dopamine-mediated modification of the frequencies involved in comodulation could be a mechanism by which this neurotransmitter regulates functioning in mPFC.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015PhPro..74..246A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015PhPro..74..246A"><span><span class="hlt">Gamma</span>-telescopes Fermi/LAT and <span class="hlt">GAMMA</span>-400 Trigger Systems Event Recognizing Methods Comparison</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Arkhangelskaja, I. V.; Murchenko, A. E.; Chasovikov, E. N.; Arkhangelskiy, A. I.; Kheymits, M. D.</p> <p></p> <p>Usually instruments for high-<span class="hlt">energy</span> γ-quanta registration consists of converter (where γ-quanta produced pairs) and calorimeter for particles <span class="hlt">energy</span> measurements surrounded by anticoincidence shield used to events identification (whether incident particle was charged or neutral). The influence of pair formation by γ-quanta in shield and the backsplash (moved in the opposite direction particles created due high <span class="hlt">energy</span> γ-rays interact with calorimeter) should be taken into account. It leads to decrease both effective area and registration efficiency at E>10 GeV. In the presented article the event recognizing methods used in Fermi/LAT trigger system is considered in comparison with the ones applied in counting and triggers signals formation system of <span class="hlt">gamma</span>-telescope <span class="hlt">GAMMA</span>-400. The <span class="hlt">GAMMA</span>-400 (<span class="hlt">Gamma</span> Astronomical Multifunctional Modular Apparatus) will be the new high-apogee space γ-observatory. The <span class="hlt">GAMMA</span>-400 consist of converter-tracker based on silicon-strip coordinate detectors interleaved with tungsten foils, imaging calorimeter make of 2 layers of double (x, y) silicon strip coordinate detectors interleaved with planes of CsI(Tl) crystals and the electromagnetic calorimeter CC2 consists only of CsI(Tl) crystals. Several plastics detections systems used as anticoincidence shield, for particles <span class="hlt">energy</span> and moving direction estimations. The main differences of <span class="hlt">GAMMA</span>-400 constructions from Fermi/LAT one are using the time-of-flight system with base of 50 cm and double layer structure of plastic detectors provides more effective particles direction definition and backsplash rejection. Also two calorimeters in <span class="hlt">GAMMA</span>-400 composed the total absorbtion spectrometer with total thickness ∼ 25 X0 or ∼1.2 λ0 for vertical incident particles registration and 54 X0 or 2.5 λ0 for laterally incident ones (where λ0 is nuclear interaction length). It provides <span class="hlt">energy</span> resolution 1-2% for 10 GeV-3.0×103 GeV events while the Fermi/LAT <span class="hlt">energy</span> resolution does not reach such a</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.osti.gov/sciencecinema/biblio/987416','SCIGOVIMAGE-SCICINEMA'); return false;" href="http://www.osti.gov/sciencecinema/biblio/987416"><span>The Animated <span class="hlt">Gamma</span>-ray Sky Revealed by the Fermi <span class="hlt">Gamma</span>-ray Space Telescope</span></a></p> <p><a target="_blank" href="http://www.osti.gov/sciencecinema/">ScienceCinema</a></p> <p>Isabelle Grenier</p> <p>2018-04-17</p> <p>The Fermi <span class="hlt">Gamma</span>-ray Space Telescope has been observing the sky in <span class="hlt">gamma</span>-rays since August 2008.  In addition to breakthrough capabilities in <span class="hlt">energy</span> coverage (20 MeV-300 GeV) and angular resolution, the wide field of view of the Large Area Telescope enables observations of 20% of the sky at any instant, and of the whole sky every three hours. It has revealed a very animated sky with bright <span class="hlt">gamma</span>-ray bursts flashing and vanishing in minutes, powerful active galactic nuclei flaring over hours and days, many pulsars twinkling in the Milky Way, and X-ray binaries shimmering along their orbit. Most of these variable sources had not been seen by the Fermi predecessor, EGRET, and the wealth of new data already brings important clues to the origin of the high-<span class="hlt">energy</span> emission and particles powered by the compact objects. The telescope also brings crisp images of the bright <span class="hlt">gamma</span>-ray emission produced by cosmic-ray interactions in the interstellar medium, thus allowing to measure the cosmic nuclei and electron spectra across the Galaxy, to weigh interstellar clouds, in particular in the dark-gas phase. The telescope sensitivity at high <span class="hlt">energy</span> will soon provide useful constraints on dark-matter annihilations in a variety of environments. I will review the current results and future prospects of the Fermi mission.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li class="active"><span>22</span></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_22 --> <div id="page_23" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li class="active"><span>23</span></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li><a href="#" onclick='return showDiv("page_25");'>25</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="441"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1356467-impulsive-long-duration-high-energy-gamma-ray-emission-from-very-bright-march-solar-flares','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1356467-impulsive-long-duration-high-energy-gamma-ray-emission-from-very-bright-march-solar-flares"><span>Impulsive And Long Duration High-<span class="hlt">Energy</span> <span class="hlt">Gamma</span>-Ray Emission From The Very Bright 2012 March 7 Solar Flares</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Ajello, M.</p> <p>2014-06-10</p> <p>The Fermi Large Area Telescope (LAT) observed two bright X-class solar ares on 2012 March 7, and detected <span class="hlt">gamma</span>-rays up to 4 GeV. We detected <span class="hlt">gamma</span>-rays both during the impulsive and temporally-extended emission phases, with emission above 100 MeV lasting for approximately 20 hours. Accurate localization of the <span class="hlt">gamma</span>-ray production site(s) coincide with the solar active region from which X-ray emissions associated with these ares originated. Our analysis of the > 100 MeV <span class="hlt">gamma</span>-ray emission shows a relatively rapid monotonic decrease in flux during the first hour of the impulsive phase, and a much slower, almost monotonic decrease in fluxmore » for the next 20 hours. The spectra can be adequately described by a power law with a high <span class="hlt">energy</span> exponential cutoff, or as resulting from the decay of neutral pions produced by accelerated protons and ions with an isotropic power-law <span class="hlt">energy</span> distribution. The required proton spectrum has a number index 3, with minor variations during the impulsive phase, while during the temporally extended phase the spectrum softens monotonically, starting with index 4. The > 30 MeV proton flux and spectra observed near the Earth by the GOES satellites also show a monotonic flux decrease and spectral softening during the extended phase, but with a harder spectrum, with index 3. Based on the Fermi-LAT and GOES observations of the flux and spectral evolution of these bright ares, we explore the relative merits of prompt and continuous acceleration scenarios, hadronic and leptonic emission processes, and acceleration at the solar corona by the fast Coronal Mass Ejections (CME) as explanations for the observations. We conclude that the most likely scenario is continuous acceleration of protons in the solar corona which penetrate the lower solar atmosphere and produce pions that decay into <span class="hlt">gamma</span>-rays.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1356467','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1356467"><span>Impulsive And Long Duration High-<span class="hlt">Energy</span> <span class="hlt">Gamma</span>-Ray Emission From The Very Bright 2012 March 7 Solar Flares</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Ajello, M.</p> <p></p> <p>The Fermi Large Area Telescope (LAT) observed two bright X-class solar ares on 2012 March 7, and detected <span class="hlt">gamma</span>-rays up to 4 GeV. We detected <span class="hlt">gamma</span>-rays both during the impulsive and temporally-extended emission phases, with emission above 100 MeV lasting for approximately 20 hours. Accurate localization of the <span class="hlt">gamma</span>-ray production site(s) coincide with the solar active region from which X-ray emissions associated with these ares originated. Our analysis of the > 100 MeV <span class="hlt">gamma</span>-ray emission shows a relatively rapid monotonic decrease in flux during the first hour of the impulsive phase, and a much slower, almost monotonic decrease in fluxmore » for the next 20 hours. The spectra can be adequately described by a power law with a high <span class="hlt">energy</span> exponential cutoff, or as resulting from the decay of neutral pions produced by accelerated protons and ions with an isotropic power-law <span class="hlt">energy</span> distribution. The required proton spectrum has a number index 3, with minor variations during the impulsive phase, while during the temporally extended phase the spectrum softens monotonically, starting with index 4. The > 30 MeV proton flux and spectra observed near the Earth by the GOES satellites also show a monotonic flux decrease and spectral softening during the extended phase, but with a harder spectrum, with index 3. Based on the Fermi-LAT and GOES observations of the flux and spectral evolution of these bright ares, we explore the relative merits of prompt and continuous acceleration scenarios, hadronic and leptonic emission processes, and acceleration at the solar corona by the fast Coronal Mass Ejections (CME) as explanations for the observations. We conclude that the most likely scenario is continuous acceleration of protons in the solar corona which penetrate the lower solar atmosphere and produce pions that decay into <span class="hlt">gamma</span>-rays.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1246516-measurement-high-energy-gamma-ray-emission-from-moon-fermi-large-area-telescope','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1246516-measurement-high-energy-gamma-ray-emission-from-moon-fermi-large-area-telescope"><span>Measurement of the high-<span class="hlt">energy</span> <span class="hlt">gamma</span>-ray emission from the Moon with the Fermi Large Area Telescope</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Ackermann, M.; Ajello, M.; Albert, A.; ...</p> <p>2016-04-08</p> <p>We have measured the <span class="hlt">gamma</span>-ray emission spectrum of the Moon using the data collected by the Large Area Telescope onboard the Fermi satellite during its first seven years of operation, in the <span class="hlt">energy</span> range from 30 MeV up to a few GeV. We have also studied the time evolution of the flux, finding a correlation with the solar activity. We have developed a full Monte Carlo simulation describing the interactions of cosmic rays with the lunar surface. The results of the present analysis can be explained in the framework of this model, where the production of <span class="hlt">gamma</span> rays is duemore » to the interactions of cosmic-ray proton and helium nuclei with the surface of the Moon. Lastly, we have used our simulation to derive the cosmic-ray proton and helium spectra near Earth from the Moon <span class="hlt">gamma</span>-ray data.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/20434346','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/20434346"><span>Measurement of <span class="hlt">gamma</span>' precipitates in a nickel-based superalloy using <span class="hlt">energy</span>-filtered transmission electron microscopy coupled with automated segmenting techniques.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Tiley, J S; Viswanathan, G B; Shiveley, A; Tschopp, M; Srinivasan, R; Banerjee, R; Fraser, H L</p> <p>2010-08-01</p> <p>Precipitates of the ordered L1(2) <span class="hlt">gamma</span>' phase (dispersed in the face-centered cubic or FCC <span class="hlt">gamma</span> matrix) were imaged in Rene 88 DT, a commercial multicomponent Ni-based superalloy, using <span class="hlt">energy</span>-filtered transmission electron microscopy (EFTEM). Imaging was performed using the Cr, Co, Ni, Ti and Al elemental L-absorption edges in the <span class="hlt">energy</span> loss spectrum. Manual and automated segmentation procedures were utilized for identification of precipitate boundaries and measurement of precipitate sizes. The automated region growing technique for precipitate identification in images was determined to measure accurately precipitate diameters. In addition, the region growing technique provided a repeatable method for optimizing segmentation techniques for varying EFTEM conditions. (c) 2010 Elsevier Ltd. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19820059239&hterms=1073&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3D%2526%25231073','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19820059239&hterms=1073&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3D%2526%25231073"><span>Structure and creep rupture properties of directionally solidified eutectic <span class="hlt">gamma/gamma</span>-prime-alpha alloy</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Whittenberger, J. D.; Wirth, G.</p> <p>1982-01-01</p> <p>A simple ternary <span class="hlt">gamma/gamma</span>-prime-alpha alloy of nominal composition (wt-%) Ni-32Mo-6Al has been directionally solidified at 17 mm/h and tested in creep rupture at 1073, 1173, and 1273 K. A uniform microstructure consisting of square-shaped Mo fibers in a <span class="hlt">gamma</span> + <span class="hlt">gamma</span>-prime matrix was found despite some variation in the molybdenum and aluminum concentrations along the growth direction. Although the steady-state creep rate is well described by the normal stress temperature equation, the stress exponent (12) and the activation <span class="hlt">energy</span> (580 kJ/mol) are high. The rupture behavior is best characterized by the Larson-Miller parameter where the constant equals 20.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/6746788-effect-food-gastrointestinal-gi-transit-sustained-release-ibuprofen-tablets-evaluated-gamma-scintigraphy','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/6746788-effect-food-gastrointestinal-gi-transit-sustained-release-ibuprofen-tablets-evaluated-gamma-scintigraphy"><span>The effect of food on gastrointestinal (GI) transit of sustained-<span class="hlt">release</span> ibuprofen tablets as evaluated by <span class="hlt">gamma</span> scintigraphy</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Borin, M.T.; Khare, S.; Beihn, R.M.</p> <p>1990-03-01</p> <p>The GI transit of radiolabeled sustained-<span class="hlt">release</span> ibuprofen 800-mg tablets in eight healthy, fed volunteers was monitored using external <span class="hlt">gamma</span> scintigraphy. Ibuprofen serum concentrations were determined from blood samples drawn over 36 hr following dosing. Sustained-<span class="hlt">release</span> ibuprofen tablets containing 0.18% of 170Er2O3 (greater than 96% 170Er) in the bulk formulation were manufactured under pilot-scale conditions and were radiolabeled utilizing a neutron activation procedure which converted stable 170Er to radioactive 171Er (t1/2 = 7.5 hr). At the time of dosing, each tablet contained 50 mu Ci of 171Er. Dosage form position were reported at various time intervals. In five subjects the sustained-releasemore » tablet remained in the stomach and eroded slowly over 7-12 hr, resulting in gradual increases in small bowel radioactivity. In the remaining three subjects, the intact tablet was ejected from the stomach and a gastric residence time of approximately 4 hr was measured. This is in marked contrast to a previous study conducted in fasted volunteers in which gastric retention time ranged from 10 to 60 min. Differences in GI transit between fed and fasted volunteers had little effect on ibuprofen bioavailability. AUC and Tmax were unaltered and Cmax was increased by 24%, which is in agreement with results from a previous, crossover-design food effect study.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19880033400&hterms=attention+pictures&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dattention%2Bpictures','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19880033400&hterms=attention+pictures&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dattention%2Bpictures"><span>High-<span class="hlt">energy</span> particle production in solar flares (SEP, <span class="hlt">gamma</span>-ray and neutron emissions). [solar energetic particles</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Chupp, E. L.</p> <p>1987-01-01</p> <p>Electrons and ions, over a wide range of <span class="hlt">energies</span>, are produced in association with solar flares. Solar energetic particles (SEPs), observed in space and near earth, consist of electrons and ions that range in <span class="hlt">energy</span> from 10 keV to about 100 MeV and from 1 MeV to 20 GeV, respectively. SEPs are directly recorded by charged particle detectors, while X-ray, <span class="hlt">gamma</span>-ray, and neutron detectors indicate the properties of the accelerated particles (electrons and ions) which have interacted in the solar atmosphere. A major problem of solar physics is to understand the relationship between these two groups of charged particles; in particular whether they are accelerated by the same mechanism. The paper reviews the physics of <span class="hlt">gamma</span>-rays and neutron production in the solar atmosphere and the method by which properties of the primary charged particles produced in the solar flare can be deduced. Recent observations of energetic photons and neutrons in space and at the earth are used to present a current picture of the properties of impulsively flare accelerated electrons and ions. Some important properties discussed are time scale of production, composition, <span class="hlt">energy</span> spectra, accelerator geometry. Particular attention is given to energetic particle production in the large flare on June 3, 1982.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/17293313','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/17293313"><span>Introduction: recent developments in the study of <span class="hlt">gamma</span>-ray bursts.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Wells, Alan; Wijers, Ralph A M J; Rees, Martin J</p> <p>2007-05-15</p> <p><span class="hlt">Gamma</span>-ray bursts (GRBs) are immensely powerful explosions, originating at cosmological distances, whose outbursts persist for durations ranging from milliseconds to tens of seconds or more. In these brief moments, the explosions radiate more <span class="hlt">energy</span> than the Sun will <span class="hlt">release</span> in its entire 10Gyr lifetime. Current theories attribute these phenomena to the final collapse of a massive star, or the coalescence of a binary system induced by gravity wave emission. New results from Swift and related programmes offer fresh understanding of the physics of GRBs, and of the local environments and host galaxies of burst progenitors. Bursts found at very high red shifts are new tools for exploring the intergalactic medium, the first stars and the earliest stages of galaxy formation. This Royal Society Discussion Meeting has brought together leading figures in the field, together with young researchers and students, to discuss and review the latest results from NASA's Swift <span class="hlt">Gamma</span>-ray Burst Observatory and elsewhere, and to examine their impact on current understanding of the observed phenomena.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/16606256','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/16606256"><span>Dielectron widths of the <span class="hlt">Gamma</span>(1S,2S,3S) resonances.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Rosner, J L; Adam, N E; Alexander, J P; Berkelman, K; Cassel, D G; Duboscq, J E; Ecklund, K M; Ehrlich, R; Fields, L; Galik, R S; Gibbons, L; Gray, R; Gray, S W; Hartill, D L; Heltsley, B K; Hertz, D; Jones, C D; Kandaswamy, J; Kreinick, D L; Kuznetsov, V E; Mahlke-Krüger, H; Meyer, T O; Onyisi, P U E; Patterson, J R; Peterson, D; Phillips, E A; Pivarski, J; Riley, D; Ryd, A; Sadoff, A J; Schwarthoff, H; Shi, X; Stroiney, S; Sun, W M; Wilksen, T; Weinberger, M; Athar, S B; Avery, P; Breva-Newell, L; Patel, R; Potlia, V; Stoeck, H; Yelton, J; Rubin, P; Cawlfield, C; Eisenstein, B I; Karliner, I; Kim, D; Lowrey, N; Naik, P; Sedlack, C; Selen, M; White, E J; Wiss, J; Shepherd, M R; Besson, D; Pedlar, T K; Cronin-Hennessy, D; Gao, K Y; Gong, D T; Hietala, J; Kubota, Y; Klein, T; Lang, B W; Poling, R; Scott, A W; Smith, A; Dobbs, S; Metreveli, Z; Seth, K K; Tomaradze, A; Zweber, P; Ernst, J; Arms, K; Severini, H; Dytman, S A; Love, W; Mehrabyan, S; Savinov, V; Aquines, O; Li, Z; Lopez, A; Mendez, H; Ramirez, J; Huang, G S; Miller, D H; Pavlunin, V; Sanghi, B; Shipsey, I P J; Xin, B; Adams, G S; Anderson, M; Cummings, J P; Danko, I; Napolitano, J; He, Q; Insler, J; Muramatsu, H; Park, C S; Thorndike, E H; Coan, T E; Gao, Y S; Liu, F; Stroynowski, R; Artuso, M; Blusk, S; Butt, J; Li, J; Menaa, N; Mountain, R; Nisar, S; Randrianarivony, K; Redjimi, R; Sia, R; Skwarnicki, T; Stone, S; Wang, J C; Zhang, K; Csorna, S E; Bonvicini, G; Cinabro, D; Dubrovin, M; Lincoln, A; Asner, D M; Edwards, K W; Briere, R A; Chen, J; Ferguson, T; Tatishvili, G; Vogel, H; Watkins, M E</p> <p>2006-03-10</p> <p>We determine the dielectron widths of the <span class="hlt">Gamma</span>(1S), <span class="hlt">Gamma</span>(2S), and <span class="hlt">Gamma</span>(3S) resonances with better than 2% precision by integrating the cross section of e+e- --><span class="hlt">Gamma</span> over the e+e- center-of-mass <span class="hlt">energy</span>. Using e+e- <span class="hlt">energy</span> scans of the <span class="hlt">Gamma</span> resonances at the Cornell Electron Storage Ring and measuring <span class="hlt">Gamma</span> production with the CLEO detector, we find dielectron widths of 1.252+/-0.004(sigma(stat))+/-0.019(sigma(syst)) keV, 0.581+/-0.004+/-0.009 keV, and 0.413+/-0.004+/-0.006 keV for the <span class="hlt">Gamma</span>(1S), <span class="hlt">Gamma</span>(2S), and <span class="hlt">Gamma</span>(3S), respectively.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2004AAS...204.6315G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2004AAS...204.6315G"><span>Storage Rings in the Sky: <span class="hlt">Gamma</span> Ray Bursts and Galactic Gravitational Collapse Stored <span class="hlt">Energy</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Greyber, H. D.</p> <p>2004-05-01</p> <p>The recent discovery of almost 100% polarization of the prompt <span class="hlt">gamma</span> ray emission from GRB021206, (1), confirms my 44 year old ``Strong" Magnetic Field" model (SMF) for galactic dynamics. In SMF, Storage Ring particles were accelerated long ago during the original gravitational collapse of the pregalactic/prequasar plasma cloud that is permeated by an almost uniform primordial magnetic field (2,3) The enormous, intense, slender, relativistic, stable, completely coherent Storage Ring stores a very small fraction of the huge galactic gravitational collapse <span class="hlt">energy</span> in an almost radiationless state, unless disturbed. The concept of an Astrophysical Storage Ring was introduced by me in l961. At first it was to explain galactic structure, but soon it proved useful to explain active galactic nuclei (AGN) and the dynamics of quasar/AGN jets. AGN and galactic morphology, energetics and dynamics vary as the ratio of magnetic <span class="hlt">energy</span> to rotational <span class="hlt">energy</span> in the particular object. <span class="hlt">Gamma</span> ray bursts (GRB) are due simply to a ``rock". i.e. a white dwarf, ordinary star, neutron sstar, asteroid, planet, etc. falling rapidly through the Storage Ring and being almost instantly vaporized into a hot plasma fireball, causing an electromagnetic shower (2) Then the fireball speeds into the huge organized magnetic field surrounding the current ring, thus generating very highly polarized prompt <span class="hlt">gamma</span> ray emission (as seen in GRB021206) from the synchrotron radiation process. The timing fits the GRB observations nicely. For instance, a ``rock" racing at 1000 kilometers per second across a 20,000 km. path in the beam would produce a twenty second burst. Other times, a target might track across a short chord for a short burst. Space missions have shown that often typical currents in space plasmas are made up of slender filaments. Thus the puzzling less than one millisecond spikes observed in some GRB are simply describing the structure of that particular ring current at that particular time. 1</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2005MNRAS.360L..73N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2005MNRAS.360L..73N"><span>Outliers to the peak <span class="hlt">energy</span>-isotropic <span class="hlt">energy</span> relation in <span class="hlt">gamma</span>-ray bursts</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Nakar, Ehud; Piran, Tsvi</p> <p>2005-06-01</p> <p>The peak <span class="hlt">energy</span>-isotropic <span class="hlt">energy</span> (EpEi) relation is among the most intriguing recent discoveries concerning <span class="hlt">gamma</span>-ray bursts (GRBs). It can have numerous implications for our understanding of the emission mechanism of the bursts and for the application of GRBs to cosmological studies. However, this relation has been verified only for a small sample of bursts with measured redshifts. We propose here a test of whether a burst with an unknown redshift can potentially satisfy the EpEi relation. Applying this test to a large sample of BATSE bursts, we find that a significant fraction of those bursts cannot satisfy this relation. Our test is sensitive only to dim and hard bursts, and therefore this relation might still hold as an inequality (i.e. there are no intrinsically bright and soft bursts). We conclude that the observed relation seen in the sample of bursts with known redshift might be influenced by observational biases and the inability to locate and to localize well hard and weak bursts that have only a small number of photons. In particular, we point out that the threshold for detection, localization and redshift measurement is essentially higher than the threshold for detection alone. We predict that Swift will detect some hard and weak bursts that would be outliers to the EpEi relation. However, we cannot quantify this prediction. We stress the importance of understanding the detection-localization-redshift threshold for the coming Swift detections.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUSMSH23C..08K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUSMSH23C..08K"><span>Implications of the pion-decay <span class="hlt">gamma</span> emission and neutron observations with CORONAS-F/SONG</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kurt, V.; Yushkov, B.; Kudela, K.</p> <p>2013-05-01</p> <p>We analyzed the high-<span class="hlt">energy</span> <span class="hlt">gamma</span> and neutron emissions observed by the SONG instrument onboard the CORONAS-F satellite during August 25, 2001, October 28, 2003, November 4, 2003, and January 20, 2005 solar flares. These flares produced neutrons and/or protons recorded near Earth. The SONG response was consistent with detection of the pion-decay <span class="hlt">gamma</span> emission and neutrons in these events. We compared time profiles of various electromagnetic emissions and showed that the maximum of the pion-decay-emission coincided in time best of all with the soft X-ray derivative, dISXR/dt, maximum. We evaluated the <span class="hlt">energy</span> of accelerated ions and compared it with the <span class="hlt">energy</span> deposited by accelerated electrons. The ion <span class="hlt">energy</span> becomes comparable or even higher than the electron <span class="hlt">energy</span> from a certain step of flare development. So the time profile of dISXR/dt is a superposition of <span class="hlt">energy</span> deposited by both fractions of accelerated particles. This result allowed us to use a time profile of dISXR/dt as a real proxy of time behavior of the <span class="hlt">energy</span> <span class="hlt">release</span> at least during major flare analysis. In particular the time interval when the dISXR/dt value exceeds 0.9 of its maximum can be used as a unified reference point for the calculations of time delay between the high-<span class="hlt">energy</span> proton acceleration and GLE onset. Analysis of the total set of pion-decay emission observations shows that such temporal closeness of pion-decay emission maximum and the soft X-ray derivative maximum is typical but not obligatory.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20110015339','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20110015339"><span>Fermi <span class="hlt">Gamma</span>-Ray Space Telescope: Science Highlights for the First 8 Months</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Moiseev, Alexander</p> <p>2010-01-01</p> <p>The Fermi <span class="hlt">Gamma</span>-ray Space Telescope was launched on June 11, 2008 and since August 2008 has successfully been conducting routine science observations of high <span class="hlt">energy</span> phenomena in the <span class="hlt">gamma</span>-ray sky. A number of exciting discoveries have been made during its first year of operation, including blazar flares, high-<span class="hlt">energy</span> <span class="hlt">gamma</span>-ray bursts, and numerous new,<span class="hlt">gamma</span>-ray sources of different types, among them pulsars and Active Galactic Nuclei (AGN). fermi-LAT also performed accurate mea.<;urement of the diffuse <span class="hlt">gamma</span>-radiation which clarifies the Ge V excess reported by EGRET almost 10 years ago, high precision measurement of the high <span class="hlt">energy</span> electron spectrum, and other observations. An overview of the observatory status and recent results as of April 30, 2009, are presented. Key words: <span class="hlt">gamma</span>-ray astronomy, cosmic rays, <span class="hlt">gamma</span>-ray burst, pulsar, blazar. diffuse <span class="hlt">gamma</span>-radiation</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1399942','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1399942"><span>Vanderbilt University <span class="hlt">Gamma</span> Irradiation of Nano-modified Concrete (2017 Milestone Report)</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Deichert, Geoffrey G.; Linton, Kory D.; Terrani, Kurt A.</p> <p></p> <p>This document outlines the irradiation of concrete specimens in the <span class="hlt">Gamma</span> Irradiation Facility in the High Flux Isotope Reactor (HFIR) at Oak Ridge National Laboratory (ORNL). Two <span class="hlt">gamma</span> irradiation runs were performed in July of 2017 on 18 reference mortar bar specimens, 26 reference cement paste bar specimens, and 28 reference cement paste tab specimens to determine the dose and temperature response of the specimens in the <span class="hlt">gamma</span> irradiation environment. Specimens from the first two <span class="hlt">gamma</span> irradiations were surveyed and <span class="hlt">released</span> to Vanderbilt University. The temperature and dose information obtained informs the test parameters of the final two <span class="hlt">gamma</span> irradiationsmore » of nano-modified concrete planned for FY 2018.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/491617','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/491617"><span>Thermal-neutron capture <span class="hlt">gamma</span>-rays. Volume 2</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Tuli, J.K.</p> <p>1997-05-01</p> <p>The <span class="hlt">energy</span> and photon intensity of <span class="hlt">gamma</span> rays as seen in thermal-neutron capture are presented ordered by Z, A of target nuclei. All <span class="hlt">gamma</span>-rays with intensity of {ge}2% of the strongest transition are included. The strongest transition is indicated in each case. Where the target nuclide mass number is indicated as nat the natural target was used. The <span class="hlt">gamma</span> <span class="hlt">energies</span> given are in keV. The <span class="hlt">gamma</span> intensities given are relative to 100 for the strongest transition. All data for A > 44 are taken from Evaluated Nuclear Structure Data File (4/97), a computer file of evaluated nuclear structure data maintainedmore » by the National Nuclear Data Center, Brookhaven National Laboratory, on behalf of the Nuclear Structure and Decay and Decay Data network, coordinated by the International Atomic <span class="hlt">Energy</span> Agency, Vienna. These data are published in Nuclear Data Sheets, Academic Press, San Diego, CA. The data for A {le} 44 is taken from ``Prompt <span class="hlt">Gamma</span> Rays from Thermal-Neutron Capture,`` M.A. Lone, R.A. Leavitt, D.A. Harrison, Atomic Data and Nuclear Data Tables 26, 511 (1981).« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/8057825','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/8057825"><span>Bifactorial versus monofactorial molecular status of Staphylococcus aureus <span class="hlt">gamma</span>-toxin.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Guidi-Rontani, C; Fouque, F; Alouf, J E</p> <p>1994-01-01</p> <p>The extracellular Staphylococcus aureus <span class="hlt">gamma</span>-toxin (hemolysin) <span class="hlt">released</span> by the Smith 5R strain has been purified (M(r) 38 kDa, pl 9.55). We established that this cytolysin is a single polypeptide fully lytic on rabbit erythrocytes. In contrast, this toxin alone was unable to lyse other cells and was required to act jointly with an accessory 58 kDa protein <span class="hlt">released</span> by the same strain. This protein, named sensitizing protein (SP), was required in order to damage the cytoplasmic membranes of other red blood cells including human erythrocytes as well as that of other eukaryotic cells (Jurkat and Hep-2). The lytic process can be referred to as conditional synergistic or cooperative lysis. <span class="hlt">gamma</span>-toxin, and SP were also found able to disrupt phospholipid/cholesterol containing liposomes. We demonstrated that a minor membrane phospholipid, phosphatidylinositol, is crucial for <span class="hlt">gamma</span>-toxin binding to cells and/or channel formation through membrane lipid bilayer.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1174865','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/1174865"><span><span class="hlt">Gamma</span> watermarking</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Ishikawa, Muriel Y.; Wood, Lowell L.; Lougheed, Ronald W.; Moody, Kenton J.; Wang, Tzu-Fang</p> <p>2004-05-25</p> <p>A covert, <span class="hlt">gamma</span>-ray "signature" is used as a "watermark" for property identification. This new watermarking technology is based on a unique steganographic or "hidden writing" digital signature, implemented in tiny quantities of <span class="hlt">gamma</span>-ray-emitting radioisotopic material combinations, generally covertly emplaced on or within an object. This digital signature may be readily recovered at distant future times, by placing a sensitive, high <span class="hlt">energy</span>-resolution <span class="hlt">gamma</span>-ray detecting instrument reasonably precisely over the location of the watermark, which location may be known only to the object's owner; however, the signature is concealed from all ordinary detection means because its exceedingly low level of activity is obscured by the natural radiation background (including the <span class="hlt">gamma</span> radiation naturally emanating from the object itself, from cosmic radiation and material surroundings, from human bodies, etc.). The "watermark" is used in object-tagging for establishing object identity, history or ownership. It thus may serve as an aid to law enforcement officials in identifying stolen property and prosecuting theft thereof. Highly effective, potentially very low cost identification-on demand of items of most all types is thus made possible.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22531355-delayed-gamma-measurements-different-nuclear-research-reactors-bringing-out-importance-delayed-contribution-gamma-flux-calculations','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22531355-delayed-gamma-measurements-different-nuclear-research-reactors-bringing-out-importance-delayed-contribution-gamma-flux-calculations"><span>Delayed <span class="hlt">Gamma</span> Measurements in Different Nuclear Research Reactors Bringing Out the Importance of the Delayed Contribution in <span class="hlt">Gamma</span> Flux Calculations</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Fourmentel, D.; Radulovic, V.; Barbot, L.</p> <p></p> <p>Neutron and <span class="hlt">gamma</span> flux levels are key parameters in nuclear research reactors. In Material Testing Reactors, such as the future Jules Horowitz Reactor, under construction at the French Alternative <span class="hlt">Energies</span> and Atomic <span class="hlt">Energy</span> Commission (CEA Cadarache, France), the expected <span class="hlt">gamma</span> flux levels are very high (nuclear heating is of the order of 20 W/g at 100 MWth). As <span class="hlt">gamma</span> rays deposit their <span class="hlt">energy</span> in the reactor structures and structural materials it is important to take them into account when designing irradiation devices. There are only a few sensors which allow measurements of the nuclear heating ; a recent development atmore » the CEA Cadarache allows measurements of the <span class="hlt">gamma</span> flux using a miniature ionization chamber (MIC). The measured MIC response is often compared with calculation using modern Monte Carlo (MC) neutron and photon transport codes, such as TRIPOLI-4 and MCNP6. In these calculations only the production of prompt <span class="hlt">gamma</span> rays in the reactor is usually modelled thus neglecting the delayed <span class="hlt">gamma</span> rays. Hence calculations and measurements are usually in better accordance for the neutron flux than for the <span class="hlt">gamma</span> flux. In this paper we study the contribution of delayed <span class="hlt">gamma</span> rays to the total MIC signal in order to estimate the systematic error in <span class="hlt">gamma</span> flux MC calculations. In order to experimentally determine the delayed <span class="hlt">gamma</span> flux contributions to the MIC response, we performed <span class="hlt">gamma</span> flux measurements with CEA developed MIC at three different research reactors: the OSIRIS reactor (MTR - 70 MWth at CEA Saclay, France), the TRIGA MARK II reactor (TRIGA - 250 kWth at the Jozef Stefan Institute, Slovenia) and the MARIA reactor (MTR - 30 MWth at the National Center for Nuclear Research, Poland). In order to experimentally assess the delayed <span class="hlt">gamma</span> flux contribution to the total <span class="hlt">gamma</span> flux, several reactor shut down (scram) experiments were performed specifically for the purpose of the measurements. Results show that on average about 30 % of the MIC signal is</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMSH14B..05K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMSH14B..05K"><span>Triggers and Manifestations of Flare <span class="hlt">Energy</span> <span class="hlt">Release</span> in the Low Atmosphere</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kosovichev, A. G.; Sharykin, I. N.; Sadykov, V. M.; Vargas, S.; Zimovets, I. V.</p> <p>2016-12-01</p> <p>The main goal is to understand triggers and manifestations of the flare <span class="hlt">energy</span> <span class="hlt">release</span> in the lower layers of the solar atmosphere (the photosphere and chromosphere) using high-resolution optical observations and magnetic field measurements. As a case study we present results for an M-class flare. We analyze optical images, HMI Dopplergrams and vector magnetograms, and use Non-Linear Force-Free Field (NLFFF) extrapolation for reconstruction of the magnetic topology. The NLFFF modelling reveals interaction of oppositely directed magnetic flux-tubes in the Polarity Inversion Line (PIL). These two interacting magnetic flux tubes are observed as a compact sheared arcade along the PIL in the high-resolution broad-band continuum images from New Solar Telescope (NST). In the vicinity of the PIL, the NST H-alpha observations reveal formation of a thin three-ribbon structure corresponding to the small-scale photospheric magnetic arcade. Magnetic reconnection is triggered by two interacting magnetic flux tubes with forming current sheet extended along the PIL. Presented observational results evidence in favor of location of the primary <span class="hlt">energy</span> <span class="hlt">release</span> site in the dense chromosphere where plasma is partially ionized in the region of strong electric currents concentrated near the polarity inversion line.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19790006996','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19790006996"><span>Enclosure fire hazard analysis using relative <span class="hlt">energy</span> <span class="hlt">release</span> criteria. [burning rate and combustion control</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Coulbert, C. D.</p> <p>1978-01-01</p> <p>A method for predicting the probable course of fire development in an enclosure is presented. This fire modeling approach uses a graphic plot of five fire development constraints, the relative <span class="hlt">energy</span> <span class="hlt">release</span> criteria (RERC), to bound the heat <span class="hlt">release</span> rates in an enclosure as a function of time. The five RERC are flame spread rate, fuel surface area, ventilation, enclosure volume, and total fuel load. They may be calculated versus time based on the specified or empirical conditions describing the specific enclosure, the fuel type and load, and the ventilation. The calculation of these five criteria, using the common basis of <span class="hlt">energy</span> <span class="hlt">release</span> rates versus time, provides a unifying framework for the utilization of available experimental data from all phases of fire development. The plot of these criteria reveals the probable fire development envelope and indicates which fire constraint will be controlling during a criteria time period. Examples of RERC application to fire characterization and control and to hazard analysis are presented along with recommendations for the further development of the concept.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li class="active"><span>23</span></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li><a href="#" onclick='return showDiv("page_25");'>25</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_23 --> <div id="page_24" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li class="active"><span>24</span></li> <li><a href="#" onclick='return showDiv("page_25");'>25</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="461"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19730025046','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19730025046"><span>Celestial diffuse <span class="hlt">gamma</span> radiation above 30 MeV observed by SAS-2</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Fichtel, C. E.; Kniffen, D. A.; Hartman, R. C.</p> <p>1973-01-01</p> <p>The Small Astronomy Satellite (SAS)-2, launched on November 15, 1972, carried into orbit a 32-deck magnetic-core digitized spark chamber <span class="hlt">gamma</span> ray telescope to study celestial <span class="hlt">gamma</span> radiation in the <span class="hlt">energy</span> range above 30 MeV. In the study of several regions with b sub 2 15 deg, a finite, diffuse flux of <span class="hlt">gamma</span> rays with a steep <span class="hlt">energy</span> spectrum in the <span class="hlt">energy</span> region from 35 to 200 MeV is observed. Representing the <span class="hlt">energy</span> spectrum by a power law of the form dJ/dE = AE to - alpha power over this <span class="hlt">energy</span> range, alpha is found along with the integral flux above 100 MeV. Combining this result with existing low <span class="hlt">energy</span> <span class="hlt">gamma</span> ray data yields an <span class="hlt">energy</span> spectrum which is not a simple power law in <span class="hlt">energy</span>, as in the X-ray region, but which demonstrates first an increase and then a decrease in slope, consistent within uncertainties with that predicted by cosmological theories, including the continuous production of high <span class="hlt">energy</span> <span class="hlt">gamma</span> rays primarily from neutral pi mesons throughout the history of the universe.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015RaPC..110...87S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015RaPC..110...87S"><span><span class="hlt">Gamma</span>-ray <span class="hlt">energy</span> buildup factor calculations and shielding effects of some Jordanian building structures</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sharaf, J. M.; Saleh, H.</p> <p>2015-05-01</p> <p>The shielding properties of three different construction styles, and building materials, commonly used in Jordan, were evaluated using parameters such as attenuation coefficients, equivalent atomic number, penetration depth and <span class="hlt">energy</span> buildup factor. Geometric progression (GP) method was used to calculate <span class="hlt">gamma</span>-ray <span class="hlt">energy</span> buildup factors of limestone, concrete, bricks, cement plaster and air for the <span class="hlt">energy</span> range 0.05-3 MeV, and penetration depths up to 40 mfp. It has been observed that among the examined building materials, limestone offers highest value for equivalent atomic number and linear attenuation coefficient and the lowest values for penetration depth and <span class="hlt">energy</span> buildup factor. The obtained buildup factors were used as basic data to establish the total equivalent <span class="hlt">energy</span> buildup factors for three different multilayer construction styles using an iterative method. The three styles were then compared in terms of fractional transmission of photons at different incident photon <span class="hlt">energies</span>. It is concluded that, in case of any nuclear accident, large multistory buildings with five layers exterior walls, style A, could effectively attenuate radiation more than small dwellings of any construction style.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PhDT.......113D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PhDT.......113D"><span>Understanding the Relationships Between Architecture, Chemistry, and <span class="hlt">Energy</span> <span class="hlt">Release</span> of Energetic Nanocomposites</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>DeLisio, Jeffery Brandon</p> <p></p> <p>Energetic nanocomposites are a class of reactive material that incorporate nanosized materials or features in order to enhance reaction kinetics and <span class="hlt">energy</span> densities. Typically, these systems employ metal nanoparticles as the fuel source and have demonstrated reactivities orders of magnitude larger than more traditionally used micron-sized metal fuels. One drawback of using nanosized metals is that the nascent oxide shell comprises a significant weight percent as the particle size decreases. This shell also complicates the understanding of oxidation mechanisms of nanosized metal fuels. In this dissertation, I apply a two-fold approach to understanding the relationships between architecture, chemistry, and <span class="hlt">energy</span> <span class="hlt">release</span> of energetic nanocomposites by 1) investigating alternative metal fuels to develop a deeper understanding of the reaction mechanisms of energetic nanocomposites and 2) creating unique microstructures to tailor macroscopic properties allowing for customizability of energetic performance. In order to accurately study these systems, new analytical techniques capable of high heating rate analysis were developed. The oxidation mechanisms of tantalum nanoparticles was first probed using high heating rate TEM and Temperature-Jump Time-of-Flight Mass Spectrometry (T-Jump TOFMS) and shell crystallization was found to plan an important role in the mechanism. An air-sensitive sample holder was developed and employed to analyze the decomposition and oxidation of molecular aluminum compounds, which theoretically can achieve similar <span class="hlt">energy</span> <span class="hlt">release</span> rates to monomolecular explosives in addition to much higher <span class="hlt">energy</span> densities. In order to obtain simultaneous thermal and speciation data at high heating rates, a nanocalorimeter was integrated into the TOFMS system and measurements were performed on Al/CuO nanolaminates to probe the effect of bilayer thickness on <span class="hlt">energy</span> <span class="hlt">release</span>. An electrospray based approach to creating energetic nanocomposites with tunable</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20020020365&hterms=imprint&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3Dimprint','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20020020365&hterms=imprint&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3Dimprint"><span>BATSE Observations of <span class="hlt">Gamma</span>-Ray Burst Tails</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Connaughton, Valerie; Six, N. Frank (Technical Monitor)</p> <p>2001-01-01</p> <p>With the discovery of low-<span class="hlt">energy</span> radiation appearing to come from the site of <span class="hlt">gamma</span>-ray bursts in the hours to weeks after the initial burst of <span class="hlt">gamma</span> rays, it would appear that astronomers have seen a cosmological imprint made by the burster on its surroundings. I discuss in this paper the phenomenon of post-burst emission in BATSE (Burst and Transient Source Experiment) <span class="hlt">gamma</span>-ray bursts at <span class="hlt">energies</span> traditionally associated with prompt emission. By summing the background-subtracted signals from hundreds of bursts, I find that tails out to hundreds of seconds after the trigger may be a common feature of long events (duration greater than 2s), and perhaps of the shorter bursts at a lower and shorter-lived level. The tail component appears independent of both the duration (within the long GRB sample) and brightness of the prompt burst emission, and may be softer. Some individual bursts have visible tails at <span class="hlt">gamma</span>-ray <span class="hlt">energies</span> and the spectrum in at least a few cases is different from that of the prompt emission. Afterglow at lower <span class="hlt">energies</span> was detected for one of these bursts, GRB-991216, raising the possibility of afterglow observations over large <span class="hlt">energy</span> ranges using the next generation of GRB detectors in conjunction with sensitive space or ground-based telescopes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20020046688&hterms=imprint&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Dimprint','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20020046688&hterms=imprint&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Dimprint"><span>BATSE Observations of <span class="hlt">Gamma</span>-Ray Burst Tails</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Connaughton, Valerie</p> <p>2002-01-01</p> <p>With the observation of low-<span class="hlt">energy</span> radiation coming from the site of <span class="hlt">gamma</span>-ray bursts in the hours to weeks after the initial <span class="hlt">gamma</span> ray burst, it appears that astronomers have discovered a cosmological imprint made by the burster on its surroundings. This paper discusses the phenomenon of postburst emission in Burst and Transient Source Experiment (BATSE) <span class="hlt">gamma</span>-ray bursts at <span class="hlt">energies</span> usually associated with prompt emission. After summing up the background-subtracted signals from hundreds of bursts, it is found that tails out to hundreds of seconds after the trigger could be a common feature of events of a duration greater than 2 seconds, and perhaps of the shorter bursts at a lower and shorter-lived level. The tail component may be softer and seems independent of the duration (within the long-GRB sample) and brightness of the prompt burst emission. Some individual bursts have visible tails at <span class="hlt">gamma</span>-ray <span class="hlt">energies</span>, and the spectrum in a few cases differs from that of the prompt emission. For one of these bursts, GRB 991216, afterglow at lower <span class="hlt">energies</span> was detected, which raised the possibility of seeing afterglow observations over large <span class="hlt">energy</span> ranges using the next generation of GRB detectors in addition to sensitive space- or ground-based telescopes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20120013550&hterms=gbm&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Dgbm','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20120013550&hterms=gbm&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Dgbm"><span>Fermi <span class="hlt">Gamma</span>-Ray Space Telescope</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>McEnery, Julie E.; Michelson, Peter F.; Paclesas, William S.; Ritz, Steven</p> <p>2012-01-01</p> <p>The Fermi <span class="hlt">Gamma</span>-ray Space Telescope, launched in June 2008, is an observatory designed to survey the high-<span class="hlt">energy</span> <span class="hlt">gamma</span>-ray sky. The primary instrument, the Large Area Telescope (LAT), provides observations from 20 MeV to greater than 300 GeV. A second instrument, the <span class="hlt">Gamma</span>-ray Burst Monitor (GBM), provides observations of transients from less than 10 keV to 40 MeV. We describe the design and performance of the instruments and their subsystems, the spacecraft and the ground system.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20150008362','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20150008362"><span>Fermi: The <span class="hlt">Gamma</span>-Ray Large Area Telescope Mission Status</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>McEnery, Julie</p> <p>2014-01-01</p> <p>Following its launch in June 2008, high-<span class="hlt">energy</span> <span class="hlt">gamma</span>-ray observations by the Fermi <span class="hlt">Gamma</span>-ray Space Telescope have unveiled over 1000 new sources and opened an important and previously unexplored window on a wide variety of phenomena. These have included the discovery of an population of pulsars pulsing only in <span class="hlt">gamma</span> rays; the detection of photons up to 10s of GeV from <span class="hlt">gamma</span>-ray bursts, enhancing our understanding of the astrophysics of these powerful explosions; the detection of hundreds of active galaxies; a measurement of the high <span class="hlt">energy</span> cosmic-ray electron spectrum which may imply the presence of nearby astrophysical particle accelerators; the determination of the diffuse <span class="hlt">gamma</span>-ray emission with unprecedented accuracy and the constraints on phenomena such as supersymmetric dark-matter annihilations and exotic relics from the Big Bang. Continuous monitoring of the high-<span class="hlt">energy</span> <span class="hlt">gamma</span>-ray sky has uncovered numerous outbursts from active galaxies and the discovery of transient sources in our galaxy. In this talk I will describe the current status of the Fermi observatory and review the science highlights from Fermi.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1982NIMPR.193..391S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1982NIMPR.193..391S"><span>Inner-shell/subshell photoionization cross section measurements using a <span class="hlt">gamma</span> excited variable <span class="hlt">energy</span> X-ray source</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sood, B. S.; Allawadhi, K. L.; Arora, S. K.</p> <p>1982-02-01</p> <p>The method developed for the determination of K/L shell photoionization cross sections in various elements, 39 ≤ Z ≤ 92, in the characteristic X-ray <span class="hlt">energy</span> region using a <span class="hlt">gamma</span> excited variable <span class="hlt">energy</span> X-ray source has been used for the measurement of L III subshell photoionization cross sections in Pb, Th and U. The measurements are made at the K X-ray <span class="hlt">energies</span> of Rb, Nb and Mo, since these are able to excite selectively the L III subshells of Pb, Th and U, respectively. The results, when compared with theoretical calculations of Scofield, are found to agree within the uncertainties of determination.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/5674012-modulation-release-norepinephrine-gamma-aminobutyric-acid-morphine-frontal-cerebral-cortex-rat','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/5674012-modulation-release-norepinephrine-gamma-aminobutyric-acid-morphine-frontal-cerebral-cortex-rat"><span>Modulation of the <span class="hlt">release</span> of norepinephrine by <span class="hlt">gamma</span>-aminobutyric acid and morphine in the frontal cerebral cortex of the rat</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Peoples, R.W.</p> <p>1989-01-01</p> <p>Agents that enhance <span class="hlt">gamma</span>-aminobutyric acid, or GABA, neurotransmission modulate certain effects of opioids, such as analgesia. Opioid analgesia is mediated in part by norepinephrine in the forebrain. In this study, the interactions between morphine and GABAergic agents on <span class="hlt">release</span> of ({sup 3}H) norepinephrine from rat frontal cerebral cortical slices were examined. GABA, 5 {times} 10{sup {minus}5}-10{sup {minus}3} M, enhanced potassium stimulated ({sup 3}H) norepinephrine <span class="hlt">release</span> and reversed the inhibitory effect of morphine in a noncompetitive manner. GABA did not enhance <span class="hlt">release</span> of ({sup 3}H) norepinephrine stimulated by the calcium ionophore A23187. The effect of GABA was reduced by the GABA{submore » A} receptor antagonists bicuculline methiodide or picrotoxin, and by the selective inhibitor of GABA uptake SKF 89976A, but was blocked completely only when bicuculline methiodide and SKF 89976A were used in combination. The GABA{sub A} agonist muscimol, 10{sup {minus}4} M, mimicked the effect of GABA, but the GABA{sub B} agonist ({plus minus})baclofen, 10{sup {minus}4} M, did not affect the <span class="hlt">release</span> of ({sup 3}H) norepinephrine in the absence or the presence of morphine. Thus GABA appears to produce this effect by stimulating GABA uptake and GABA{sub A}, but not GABA{sub B}, receptors. In contrast to the results that would be predicted for an event involving GABA{sub A} receptors, however, the effect of GABA did not desensitize, and benzodiazepine agonists did not enhance the effect of GABA at any concentration tested between 10{sup {minus}8} and 10{sup {minus}4} M. Thus these receptors may constitute a subclass of GABA{sub A} receptors. These results support a role of GABA uptake and GABA{sub A} receptors in enhancing the <span class="hlt">release</span> of norepinephrine and modulating its inhibition by opioids in the frontal cortex of the rat.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19950017961','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19950017961"><span><span class="hlt">Gamma</span>-ray emission from globular clusters. Shock high <span class="hlt">energy</span> emission from the Be-Star/Pulsar System PSR 1259-63. Echoes in x-ray novae</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kaaret, Philip</p> <p>1995-01-01</p> <p>This grant covers work on the Compton phase 3 investigation, 'Shock High <span class="hlt">Energy</span> Emission from the Be- Star/Pulsar System PSR 1259-63' and cycle 4 investigations 'Diffuse <span class="hlt">Gamma</span>-Ray Emission at High Latitudes' and 'Echoes in X-Ray Novae'. Work under the investigation 'Diffuse <span class="hlt">Gamma</span>-Ray Emission at High Latitudes' has lead to the publication of a paper (attached), describing <span class="hlt">gamma</span>-ray emissivity variations in the northern galactic hemisphere. Using archival EGRET data, we have found a large irregular region of enhanced <span class="hlt">gamma</span>-ray emissivity at <span class="hlt">energies</span> greater 100 MeV. This is the first observation of local structure in the <span class="hlt">gamma</span>-ray emissivity. Work under the investigation 'Echoes in X-Ray Novae' is proceeding with analysis of data from OSSE from the transient source GRO J1655-40. The outburst of this source last fall triggered this Target of Opportunity investigation. Preliminary spectral analysis shows emission out to 600 keV and a pure power low spectrum with no evidence of an exponential cutoff. Work is complete on the analysis of BATSE data from the Be-Star/Pulsar Sustem PSR 1259-63.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20040050223&hterms=Mysteries&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3DMysteries','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20040050223&hterms=Mysteries&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3DMysteries"><span>The Mystery of <span class="hlt">Gamma</span>-Ray Bursts</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Fishman, Gerald J.</p> <p>2004-01-01</p> <p><span class="hlt">Gamma</span>-ray bursts remain one of the greatest mysteries in astrophysics. Observations of <span class="hlt">gamma</span>-ray bursts made by the BATSE experiment on the Compton <span class="hlt">Gamma</span>-Ray Observatory will be described. Most workers in the field now believe that they originate from cosmological distances. This view has been reinforced by observations this year of several optical afterglow counterparts to <span class="hlt">gamma</span>-ray bursts. A summary of these recent discoveries will be presented, along with their implications for models of the burst emission mechanism and the <span class="hlt">energy</span> source of the bursts.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19790053795&hterms=Ankara&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3DAnkara','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19790053795&hterms=Ankara&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3DAnkara"><span>Galactic plane <span class="hlt">gamma</span>-radiation</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Hartman, R. C.; Kniffen, D. A.; Thompson, D. J.; Fichtel, C. E.; Ogelman, H. B.; Tumer, T.; Ozel, M. E.</p> <p>1979-01-01</p> <p>Analysis of the SAS 2 data together with the COS B results shows that the distribution of galactic <span class="hlt">gamma</span>-radiation has several similarities to that of other large-scale tracers of galactic structure. The radiation is primarily confined to a thin disc which exhibits offsets from b = 0 degrees similar to warping at radio frequencies. The principal distinction of the <span class="hlt">gamma</span>-radiation is a stronger contrast in intensity between the region from 310 to 45 degrees in longitude and the regions away from the center that can be attributed to a variation in cosmic-ray density as a function of position in Galaxy. The diffuse galactic <span class="hlt">gamma</span>-ray <span class="hlt">energy</span> spectrum shows no significant variation in direction, and the spectrum seen along the plane is the same as that for the galactic component of the <span class="hlt">gamma</span>-radiation at high altitudes. The uniformity of the galactic <span class="hlt">gamma</span>-ray spectrum, the smooth decrease in intensity as a function of altitude, and the absence of any galactic <span class="hlt">gamma</span>-ray sources at high altitudes indicate a diffuse origin for bulk of the galactic <span class="hlt">gamma</span>-radiation rather than a collection of localized sources.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1985RpSpR...6...33A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1985RpSpR...6...33A"><span>Hard <span class="hlt">gamma</span> radiation background from coding collimator of <span class="hlt">gamma</span> telescope under space experiment conditions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Aleksandrov, A. P.; Berezovoy, A. N.; Galper, A. M.; Grachev, V. M.; Dmitrenko, V. V.; Kirillov-Ugryumov, V. G.; Lebedev, V. V.; Lyakhov, V. A.; Moiseyev, A. A.; Ulin, S. Y.</p> <p>1985-09-01</p> <p>Coding collimators are used to improve the angular resolution of <span class="hlt">gamma</span>-ray telescopes at <span class="hlt">energies</span> above 50 MeV. However, the interaction of cosmic rays with the collimation material can lead to the appearance of a <span class="hlt">gamma</span>-ray background flux which can have a deleterious effect on measurement efficiency. An experiment was performed on the Salyut-6-Soyuz spacecraft system with the Elena-F small-scale <span class="hlt">gamma</span>-ray telescope in order to measure the magnitude of this background. It is shown that, even at a zenith angle of approximately zero degrees (the angle at which the <span class="hlt">gamma</span>-ray observations are made), the coding collimator has only an insignificant effect on the background conditions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19850027528','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19850027528"><span>Development of observational and instrumental techniques in hard X-ray and medium <span class="hlt">energy</span> <span class="hlt">gamma</span>-ray astronomy</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Pelling, M.</p> <p>1985-01-01</p> <p>The technical activities, scientific results, related space hardware projects and personnel of the high <span class="hlt">energy</span> astrophysics program are reported. The development of observational and instrumental techniques in hard X-ray (0.001 to 100 keV) and medium <span class="hlt">energy</span> <span class="hlt">gamma</span>-ray (0.1 to 10 MeV) astronomy are examined. Many of these techniques were developed explicitly for use on high altitude balloons where most of the scientific results were obtained. The extensive observational activity using balloons are tabulated. Virtually every research activity will eventually result in a major space hardware development effort.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22663094-tev-gamma-ray-observations-galactic-center-ridge-veritas','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22663094-tev-gamma-ray-observations-galactic-center-ridge-veritas"><span>TEV <span class="hlt">GAMMA</span>-RAY OBSERVATIONS OF THE GALACTIC CENTER RIDGE BY VERITAS</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Archer, A.; Buckley, J. H.; Bugaev, V.</p> <p>2016-04-20</p> <p>The Galactic Center ridge has been observed extensively in the past by both GeV and TeV <span class="hlt">gamma</span>-ray instruments revealing a wealth of structure, including a diffuse component and the point sources G0.9+0.1 (a composite supernova remnant) and Sgr A* (believed to be associated with the supermassive black hole located at the center of our Galaxy). Previous very high <span class="hlt">energy</span> (VHE) <span class="hlt">gamma</span>-ray observations with the H.E.S.S. experiment have also detected an extended TeV <span class="hlt">gamma</span>-ray component along the Galactic plane in the >300 GeV <span class="hlt">gamma</span>-ray regime. Here we report on observations of the Galactic Center ridge from 2010 to 2014 by themore » VERITAS telescope array in the >2 TeV <span class="hlt">energy</span> range. From these observations we (1) provide improved measurements of the differential <span class="hlt">energy</span> spectrum for Sgr A* in the >2 TeV <span class="hlt">gamma</span>-ray regime, (2) provide a detection in the >2 TeV <span class="hlt">gamma</span>-ray emission from the composite SNR G0.9+0.1 and an improved determination of its multi-TeV <span class="hlt">gamma</span>-ray <span class="hlt">energy</span> spectrum, and (3) report on the detection of VER J1746-289, a localized enhancement of >2 TeV <span class="hlt">gamma</span>-ray emission along the Galactic plane.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/21596552-measurement-sup-gd-gamma-reaction-dance-gamma-calorimeter-array','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/21596552-measurement-sup-gd-gamma-reaction-dance-gamma-calorimeter-array"><span>Measurement of the {sup 157}Gd(n,{<span class="hlt">gamma</span>}) reaction with the DANCE {<span class="hlt">gamma</span>} calorimeter array</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Chyzh, A.; Dashdorj, D.; Lawrence Livermore National Laboratory, Livermore, California 94551</p> <p>2011-07-15</p> <p>The {sup 157}Gd(n,{<span class="hlt">gamma</span>}) reaction was measured with the DANCE {<span class="hlt">gamma</span>} calorimeter (consisting of 160 BaF{sub 2} scintillation detectors) at the Los Alamos Neutron Science Center. The multiplicity distributions of the {<span class="hlt">gamma</span>} decay were used to determine the resonance spins up to E{sub n}=300 eV. The {<span class="hlt">gamma</span>}-ray <span class="hlt">energy</span> spectra for different multiplicities were measured for the s-wave resonances. The shapes of these spectra were compared with simulations based on the use of the DICEBOX statistical model code. Simulations showed that the scissors mode is required not only for the ground-state transitions but also for transitions between excited states.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JInst..13P3005H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JInst..13P3005H"><span>Simulated and measured neutron/<span class="hlt">gamma</span> light output distribution for poly-energetic neutron/<span class="hlt">gamma</span> sources</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hosseini, S. A.; Zangian, M.; Aghabozorgi, S.</p> <p>2018-03-01</p> <p>In the present paper, the light output distribution due to poly-energetic neutron/<span class="hlt">gamma</span> (neutron or <span class="hlt">gamma</span>) source was calculated using the developed MCNPX-ESUT-PE (MCNPX-<span class="hlt">Energy</span> engineering of Sharif University of Technology-Poly Energetic version) computational code. The simulation of light output distribution includes the modeling of the particle transport, the calculation of scintillation photons induced by charged particles, simulation of the scintillation photon transport and considering the light resolution obtained from the experiment. The developed computational code is able to simulate the light output distribution due to any neutron/<span class="hlt">gamma</span> source. In the experimental step of the present study, the neutron-<span class="hlt">gamma</span> discrimination based on the light output distribution was performed using the zero crossing method. As a case study, 241Am-9Be source was considered and the simulated and measured neutron/<span class="hlt">gamma</span> light output distributions were compared. There is an acceptable agreement between the discriminated neutron/<span class="hlt">gamma</span> light output distributions obtained from the simulation and experiment.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20110013305','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20110013305"><span>Discoveries by the Fermi <span class="hlt">Gamma</span> Ray Space Telescope</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Gehrels, Neil</p> <p>2011-01-01</p> <p>Fermi is a large space <span class="hlt">gamma</span>-ray mission developed by NASA and the DOE with major contributions from France, Germany, Italy, Japan and Sweden. It was launched in June 2008 and has been performing flawlessly since then. The main instrument is the Large Area Telescope (LAT) operating in the 20 MeV to 300 GeV range and a smaller monitor instrument is the <span class="hlt">Gamma</span>-ray Burst Monitor (GBM) operating in the 8 keV to 40 MeV range. New findings are occurring every week. Some of the key discoveries are: 1) Discovery of many new <span class="hlt">gamma</span>-ray pulsars, including <span class="hlt">gamma</span>-ray only and millisecond pulsars. 2) Detection of high <span class="hlt">energy</span> <span class="hlt">gamma</span>-ray emission from globular clusters, most likely due to summed emission from msec pulsars. 3) Discovery of delayed and extended high <span class="hlt">energy</span> <span class="hlt">gamma</span>-ray emission from short and long <span class="hlt">gamma</span>-ray busts. 4) Detection of approximately 250 <span class="hlt">gamma</span>-ray bursts per year with the GBM instrument. 5) Most accurate measurement of the cosmic ray electron spectrum between 30 GeV and 1 TeV, showing some excess above the conventional diffusion model. The talk will present the new discoveries and their implications.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017MNRAS.472.3474A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017MNRAS.472.3474A"><span>Search for very high-<span class="hlt">energy</span> <span class="hlt">gamma</span>-ray emission from the microquasar Cygnus X-1 with the MAGIC telescopes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ahnen, M. L.; Ansoldi, S.; Antonelli, L. A.; Arcaro, C.; Babić, A.; Banerjee, B.; Bangale, P.; Barres de Almeida, U.; Barrio, J. A.; Becerra González, J.; Bednarek, W.; Bernardini, E.; Berti, A.; Bhattacharyya, W.; Biasuzzi, B.; Biland, A.; Blanch, O.; Bonnefoy, S.; Bonnoli, G.; Carosi, R.; Carosi, A.; Chatterjee, A.; Colin, P.; Colombo, E.; Contreras, J. L.; Cortina, J.; Covino, S.; Cumani, P.; da Vela, P.; Dazzi, F.; de Angelis, A.; de Lotto, B.; de Oña Wilhelmi, E.; di Pierro, F.; Doert, M.; Domínguez, A.; Dominis Prester, D.; Dorner, D.; Doro, M.; Einecke, S.; Eisenacher Glawion, D.; Elsaesser, D.; Engelkemeier, M.; Fallah Ramazani, V.; Fernández-Barral, A.; Fidalgo, D.; Fonseca, M. V.; Font, L.; Fruck, C.; Galindo, D.; García López, R. J.; Garczarczyk, M.; Gaug, M.; Giammaria, P.; Godinović, N.; Gora, D.; Guberman, D.; Hadasch, D.; Hahn, A.; Hassan, T.; Hayashida, M.; Herrera, J.; Hose, J.; Hrupec, D.; Ishio, K.; Konno, Y.; Kubo, H.; Kushida, J.; Kuveždić, D.; Lelas, D.; Lindfors, E.; Lombardi, S.; Longo, F.; López, M.; Maggio, C.; Majumdar, P.; Makariev, M.; Maneva, G.; Manganaro, M.; Mannheim, K.; Maraschi, L.; Mariotti, M.; Martínez, M.; Mazin, D.; Menzel, U.; Minev, M.; Mirzoyan, R.; Moralejo, A.; Moreno, V.; Moretti, E.; Neustroev, V.; Niedzwiecki, A.; Nievas Rosillo, M.; Nilsson, K.; Ninci, D.; Nishijima, K.; Noda, K.; Nogués, L.; Paiano, S.; Palacio, J.; Paneque, D.; Paoletti, R.; Paredes, J. M.; Paredes-Fortuny, X.; Pedaletti, G.; Peresano, M.; Perri, L.; Persic, M.; Prada Moroni, P. G.; Prandini, E.; Puljak, I.; Garcia, J. R.; Reichardt, I.; Rhode, W.; Ribó, M.; Rico, J.; Righi, C.; Saito, T.; Satalecka, K.; Schroeder, S.; Schweizer, T.; Sitarek, J.; Šnidarić, I.; Sobczynska, D.; Stamerra, A.; Strzys, M.; Surić, T.; Takalo, L.; Tavecchio, F.; Temnikov, P.; Terzić, T.; Tescaro, D.; Teshima, M.; Torres, D. F.; Torres-Albà, N.; Treves, A.; Vanzo, G.; Vazquez Acosta, M.; Vovk, I.; Ward, J. E.; Will, M.; Zarić, D.; MAGIC Collaboration; Bosch-Ramon, V.; Pooley, G. G.; Trushkin, S. A.; Zanin, R.</p> <p>2017-12-01</p> <p>The microquasar Cygnus X-1 displays the two typical soft and hard X-ray states of a black hole transient. During the latter, Cygnus X-1 shows a one-sided relativistic radio-jet. Recent detection of the system in the high <span class="hlt">energy</span> (HE; E ≳ 60 MeV) <span class="hlt">gamma</span>-ray range with Fermi-LAT associates this emission with the outflow. Former MAGIC observations revealed a hint of flaring activity in the very high-<span class="hlt">energy</span> (VHE; E ≳ 100 GeV) regime during this X-ray state. We analyse ∼97 h of Cygnus X-1 data taken with the MAGIC telescopes between July 2007 and October 2014. To shed light on the correlation between hard X-ray and VHE <span class="hlt">gamma</span> rays as previously suggested, we study each main X-ray state separately. We perform an orbital phase-folded analysis to look for variability in the VHE band. Additionally, to place this variability behaviour in a multiwavelength context, we compare our results with Fermi-LAT, AGILE, Swift-BAT, MAXI, RXTE-ASM, AMI and RATAN-600 data. We do not detect Cygnus X-1 in the VHE regime. We establish upper limits for each X-ray state, assuming a power-law distribution with photon index Γ = 3.2. For steady emission in the hard and soft X-ray states, we set integral upper limits at 95 per cent confidence level for <span class="hlt">energies</span> above 200 GeV at 2.6 × 10-12 photons cm-2 s-1 and 1.0 × 10-11 photons cm-2 s-1, respectively. We rule out steady VHE <span class="hlt">gamma</span>-ray emission above this <span class="hlt">energy</span> range, at the level of the MAGIC sensitivity, originating in the interaction between the relativistic jet and the surrounding medium, while the emission above this flux level produced inside the binary still remains a valid possibility.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017xru..conf...33A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017xru..conf...33A"><span>Measuring cosmological parameters with <span class="hlt">Gamma</span>-Ray Bursts: status and perspectives</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Amati, L.</p> <p>2017-10-01</p> <p>Given their huge isotropic-equivalent radiated <span class="hlt">energies</span>, up to more than 10^{54} erg <span class="hlt">released</span> in a few tens of seconds, and their redshift distribution extending up to more than z = 9, <span class="hlt">Gamma</span>-Ray Bursts (GRB) are in principle a powerful tool for measuring the geometry and expansion rate of the Universe. In the recent years, several attempts have been made to exploit the correlation between the photon <span class="hlt">energy</span> at which the nuFnu spectrum peaks ('peak <span class="hlt">energy</span>') and the radiated <span class="hlt">energy</span> (or luminosity) for 'standardizing' GRBs and use them as tools (complementary to other probes like SN Ia, BAO and the CMB) for the estimate of cosmological parameters. These studies show that already with the present data set GRBs can provide a signicant and independent confirmation of Ω_{M} ˜ 0.3 for a flat ΛCDM universe and that the measurements expected from present and next GRB experiments (e.g. Swift, Fermi/GBM, SVOM, CALET/GBM, UFFO) will allow us to substantially improve the constraints on Ω_{M} and Ω_{Λ}, and, in particular, to get unique clues on dark <span class="hlt">energy</span> properties and evolution.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li class="active"><span>24</span></li> <li><a href="#" onclick='return showDiv("page_25");'>25</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_24 --> <div id="page_25" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li class="active"><span>25</span></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="481"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5422429','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5422429"><span>Dopamine Modulates Delta-<span class="hlt">Gamma</span> Phase-Amplitude Coupling in the Prefrontal Cortex of Behaving Rats</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Andino-Pavlovsky, Victoria; Souza, Annie C.; Scheffer-Teixeira, Robson; Tort, Adriano B. L.; Etchenique, Roberto; Ribeiro, Sidarta</p> <p>2017-01-01</p> <p>Dopamine <span class="hlt">release</span> and phase-amplitude cross-frequency coupling (CFC) have independently been implicated in prefrontal cortex (PFC) functioning. To causally investigate whether dopamine <span class="hlt">release</span> affects phase-amplitude comodulation between different frequencies in local field potentials (LFP) recorded from the medial PFC (mPFC) of behaving rats, we used RuBiDopa, a light-sensitive caged compound that <span class="hlt">releases</span> the neurotransmitter dopamine when irradiated with visible light. LFP power did not change in any frequency band after the application of light-uncaged dopamine, but significantly strengthened phase-amplitude comodulation between delta and <span class="hlt">gamma</span> oscillations. Saline did not exert significant changes, while injections of dopamine and RuBiDopa produced a slow increase in comodulation for several minutes after the injection. The results show that dopamine <span class="hlt">release</span> in the medial PFC shifts phase-amplitude comodulation from theta-<span class="hlt">gamma</span> to delta-<span class="hlt">gamma</span>. Although being preliminary results due to the limitation of the low number of animals present in this study, our findings suggest that dopamine-mediated modification of the frequencies involved in comodulation could be a mechanism by which this neurotransmitter regulates functioning in mPFC. PMID:28536507</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008SPIE.7079E..17W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008SPIE.7079E..17W"><span>Strontium iodide scintillators for high <span class="hlt">energy</span> resolution <span class="hlt">gamma</span> ray spectroscopy</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wilson, Cody M.; van Loef, Edgar V.; Glodo, Jarek; Cherepy, Nerine; Hull, Giulia; Payne, Stephen; Choong, Woon-Seng; Moses, William; Shah, Kanai S.</p> <p>2008-08-01</p> <p>Recently SrI2, a scintillator patented by Hofstadter in 1968, has been rediscovered and shown to possess remarkable scintillation properties. The light output of SrI2:Eu2+ has been measured to be even higher than previously observed and exceeds 120,000 photons/MeV, making it one of the brightest scintillators in existence. The crystal also has excellent <span class="hlt">energy</span> resolution of less than 3% at 662 keV. The response is highly linear over a wide range of <span class="hlt">gamma</span> ray <span class="hlt">energies</span>. The emission of SrI2:Eu2+ and SrI2:Ce3+/Na+ is well-matched to both photomultiplier tubes and blue-enhanced silicon photodiodes. While SrI2:Eu2+ is relatively slow, SrI2:Ce3+/Na+ has a fast response. SrI2 crystals with many different dopant concentrations have been grown and characterized. In this presentation, crystal growth techniques as well as the effects of dopant concentration on the scintillation properties of SrI2, over the range 0.5% to 8% Eu2+ and 0.5% to 2% Ce3+/Na+, will be discussed in detail.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19860049989&hterms=gamma+ray+irradiation&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dgamma%2Bray%2Birradiation','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19860049989&hterms=gamma+ray+irradiation&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dgamma%2Bray%2Birradiation"><span>High <span class="hlt">energy</span> irradiations simulating cosmic-ray-induced planetary <span class="hlt">gamma</span> ray production. I - Fe target</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Metzger, A. E.; Parker, R. H.; Yellin, J.</p> <p>1986-01-01</p> <p>Two thick Fe targets were bombarded by a series of 6 GeV proton irradiations for the purpose of simulating the cosmic ray bombardment of planetary objects in space. <span class="hlt">Gamma</span> ray <span class="hlt">energy</span> spectra were obtained with a germanium solid state detector during the bombardment, and 46 of the <span class="hlt">gamma</span> ray lines were ascribed to the Fe targets. A comparison between observed and predicted values showed good agreement for Fe lines from neutron inelastic scattering and spallation reactions, and less satisfactory agreement for neutron capture reactions, the latter attributed to the difference in composition between the Fe target and the mean lunar abundance used in the modeling. Through an analysis of the irradiation results together with continuum data obtained in lunar orbit, it was found that 100 hours of measurement with a current instrument should generate a spectrum containing approximately 20 lines due to Fe alone, with a 2-sigma sensitivity for detection of about 0.2 percent.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20030061075','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20030061075"><span>A Search for Early High-<span class="hlt">Energy</span> Afterglows in BATSE <span class="hlt">Gamma</span>-Ray Bursts</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Giblin, Timothy W.</p> <p>2003-01-01</p> <p>The scope of this project was to perform a detailed search for the early high-<span class="hlt">energy</span> afterglow component of <span class="hlt">gamma</span>-ray bursts (GRBs) in the BATSE GRB data archive. GRBs are believed to be the product of shock waves generated in a relativistic outflow from the demise of extremely massive stars and/or binary neutron star mergers. The outflow undeniably encounters the ambient medium of the progenitor object and another shock wave is set up. A forward shock propagates into the medium and a reverse shock propagates through the ejecta. This "external" shock dissipates the kinetic <span class="hlt">energy</span> of the ejecta in the form of radiation via synchrotron losses and slows the outflow eventually to a non-relativistic state. Radiation from the forward external shock is therefore expected to be long-lived, lasting days, weeks, and even months. This radiation is referred to as the 'afterglow'.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19900013997','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19900013997"><span><span class="hlt">Gamma</span> ray bursts: Current status of observations and theory</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Meegan, Charles A.</p> <p>1990-01-01</p> <p><span class="hlt">Gamma</span>-ray bursts display a wide range of temporal and spectral characteristics, but typically last several seconds and emit most of their <span class="hlt">energy</span> in the low-<span class="hlt">energy</span> <span class="hlt">gamma</span>-ray region. The burst sources appear to be isotropically distributed on the sky. Several lines of evidence suggest magnetic neutron stars as sources for bursts. A variety of <span class="hlt">energy</span> sources and emission mechanisms were proposed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19900013210','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19900013210"><span><span class="hlt">Gamma</span> ray bursts: Current status of observations and theory</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Meegan, Charles A.</p> <p>1990-01-01</p> <p><span class="hlt">Gamma</span> ray bursts display a wide range of temporal and spectral characteristics, but typically last several seconds and emit most of their <span class="hlt">energy</span> in a low <span class="hlt">energy</span>, <span class="hlt">gamma</span> ray region. The burst sources appear to be isotropically distributed on the sky. Several lines of evidence suggest magnetic neutron stars as sources for bursts. A variety of <span class="hlt">energy</span> sources and emission mechanisms are proposed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1985RScI...56..975M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1985RScI...56..975M"><span>Fusion <span class="hlt">gamma</span> diagnostics</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Medley, S. S.; Cecil, F. E.; Cole, D.; Conway, M. A.; Wilkinson, F. J., III</p> <p>1985-05-01</p> <p>Nuclear reactions of interest in fusion research often possess a branch yielding prompt emission of <span class="hlt">gamma</span> radiation in excess of 15 MeV which can be exploited to provide a new fusion reaction diagnostic having applications similar to conventional neutron emission measurements. Conceptual aspects of fusion <span class="hlt">gamma</span> diagnostics are discussed with emphasis on application to the Tokamak Fusion Test Reactor (TFTR) during deuterium neutral beam heating of D-T and D-3He plasmas. Recent measurements of the D (T, γ)5He, D(3He, γ)5Li, and D(D, γ)4He branching ratios at low center-of-mass <span class="hlt">energy</span> (30-100 keV) and of the response of a large volume Ne226 detector for <span class="hlt">gamma</span> detection in high neutron backgrounds are presented. Using a well-shielded Ne226 detector during 20 MW-120 kV deuterium beam heating of a tritium plasma in TFTR, the D(T, γ)5He <span class="hlt">gamma</span> signal level is estimated to be 3.5×105 cps.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/4306692-operational-characteristics-armour-fission-gas-gamma-facility','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/4306692-operational-characteristics-armour-fission-gas-gamma-facility"><span>OPERATIONAL CHARACTERISTICS OF THE ARMOUR FISSION GAS <span class="hlt">GAMMA</span> FACILITY</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Terrell, C.W.; McElroy, W.N.</p> <p>1958-10-31</p> <p>As the reactor power level is changed frequently, the radiation levels in the <span class="hlt">gamma</span> facility fluctuate. Data are presented to show the power dependency of the <span class="hlt">gamma</span> dose rate and the manner of growth and decay. Additional data show the dependercy of the equilibrium <span class="hlt">gamma</span> activity on the foel temperature and total system pressure. The final phase of the work is directed toward determining an average <span class="hlt">gamma</span> <span class="hlt">energy</span> by attenuation measurements with various thicknesses of several materials. The neutrou flux associated with the gas phase activity is determined by foil measurement. From the measurements of dose rate and average gammamore » <span class="hlt">energy</span>, calculations to determine the number of curies of gas phase decay <span class="hlt">gamma</span> activity per watt of reactor power are presented. (auth)« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1994sao..reptS....W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1994sao..reptS....W"><span>Very high <span class="hlt">gamma</span> ray extension of GRO observations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Weekes, Trevor C.</p> <p>1994-12-01</p> <p>The membership, progress, and invited talks, publications, and proceedings made by the Whipple <span class="hlt">Gamma</span> Ray Collaboration is reported for june 1990 through May 1994. Progress was made in the following areas: the May 1994 Markarian Flare at Whipple and EGRET (Energetic <span class="hlt">Gamma</span> Ray Experiment Telescope) <span class="hlt">energies</span>; AGN's (Active Galactic Nuclei); bursts; supernova remnants; and simulations and <span class="hlt">energy</span> spectra.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://images.nasa.gov/#/details-GSFC_20171208_Archive_e000686.html','SCIGOVIMAGE-NASA'); return false;" href="https://images.nasa.gov/#/details-GSFC_20171208_Archive_e000686.html"><span><span class="hlt">Gamma</span>-Ray "Raindrops" from Flaring Blazar</span></a></p> <p><a target="_blank" href="https://images.nasa.gov/">NASA Image and Video Library</a></p> <p></p> <p>2017-12-08</p> <p>This visualization shows <span class="hlt">gamma</span> rays detected during 3C 279's big flare by the LAT instrument on NASA's Fermi satellite. <span class="hlt">Gamma</span> rays are represented as expanding circles reminiscent of raindrops on water. The flare is an abrupt shower of "rain" that trails off toward the end of the movie. Both the maximum size of the circle and its color represent the <span class="hlt">energy</span> of the <span class="hlt">gamma</span> ray, with white lowest and magenta highest. In a second version of the visualization, a background map shows how the LAT detects 3C 279 and other sources by accumulating high-<span class="hlt">energy</span> photons over time (brighter squares reflect higher numbers of <span class="hlt">gamma</span> rays). The movie starts on June 14 and ends June 17. The area shown is a region of the sky five degrees on a side and centered on the position of 3C 279. Read more: go.nasa.gov/1TqximF Credits: NASA/DOE/Fermi LAT Collaboration</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014HEAD...1410611E','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014HEAD...1410611E"><span>Bright <span class="hlt">gamma</span>-ray flares of the quasars 3C 279 and PKS 1222+216 observed at the highest <span class="hlt">energies</span> with Fermi-LAT and VERITAS</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Errando, Manel</p> <p>2014-08-01</p> <p>Flat spectrum radio quasars (FSRQs) are the most powerful sources continuously detected at <span class="hlt">gamma</span>-ray <span class="hlt">energies</span>, with luminosities exceeding 1048 erg s-1. The high-<span class="hlt">energy</span> emission of quasars peaks in the MeV-GeV band, and only a few episodic detections have been reported at very high <span class="hlt">energies</span> (VHE, E>100 GeV). We will present the first results from an observing campaign on the FSRQ 3C 279 in April 2014 during the brightest <span class="hlt">gamma</span>-ray outburst ever recorded for this object, with flux exceeding the historic 1991 flare seen by EGRET. Observations include simultaneous coverage with the Fermi-LAT satellite and the VERITAS ground-based array spanning four decades in <span class="hlt">energy</span> from 100 MeV to 1 TeV with unprecedented sensitivity. We will also report on the detection of persistent VHE emission from the quasar PKS 1222+216 over a week-long period in March 2014. These observations present strong challenges to current models of <span class="hlt">energy</span> dissipation in relativistic jets. The implications of the absence/presence of VHE emission in connection with flaring activity in the MeV-GeV regime will be discussed, especially concerning the role of ambient photon fields in the radiation mechanisms, and the size and location of the <span class="hlt">gamma</span>-ray emission region.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://images.nasa.gov/#/details-GSFC_20171208_Archive_e002215.html','SCIGOVIMAGE-NASA'); return false;" href="https://images.nasa.gov/#/details-GSFC_20171208_Archive_e002215.html"><span>Fermi Sees the <span class="hlt">Gamma</span> Ray Sky</span></a></p> <p><a target="_blank" href="https://images.nasa.gov/">NASA Image and Video Library</a></p> <p></p> <p>2009-10-30</p> <p>This view of the <span class="hlt">gamma</span>-ray sky constructed from one year of Fermi LAT observations is the best view of the extreme universe to date. The map shows the rate at which the LAT detects <span class="hlt">gamma</span> rays with <span class="hlt">energies</span> above 300 million electron volts -- about 120 million times the <span class="hlt">energy</span> of visible light -- from different sky directions. Brighter colors equal higher rates. Credit: NASA/DOE/Fermi LAT Collaboration Full story: www.nasa.gov/mission_pages/GLAST/news/first_year.html</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19770014043&hterms=Ankara&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3DAnkara','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19770014043&hterms=Ankara&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3DAnkara"><span><span class="hlt">Gamma</span> ray pulsars. [electron-photon cascades</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Oegelman, H.; Ayasli, S.; Hacinliyan, A.</p> <p>1977-01-01</p> <p>Data from the SAS-2 high-<span class="hlt">energy</span> <span class="hlt">gamma</span>-ray experiment reveal the existence of four pulsars emitting photons above 35 MeV. An attempt is made to explain the <span class="hlt">gamma</span>-ray emission from these pulsars in terms of an electron-photon cascade that develops in the magnetosphere of the pulsar. Although there is very little material above the surface of the pulsar, the very intense magnetic fields (10 to the 12th power gauss) correspond to many radiation lengths which cause electrons to emit photons by magnetic bremsstrahlung and which cause these photons to pair-produce. The cascade develops until the mean photon <span class="hlt">energy</span> drops below the pair-production threshold which is in the <span class="hlt">gamma</span>-ray range; at this stage, the photons break out from the source.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/21057315-agile-mission-gamma-ray-bursts','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/21057315-agile-mission-gamma-ray-bursts"><span>The AGILE Mission and <span class="hlt">Gamma</span>-Ray Bursts</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Longo, Francesco; INFN, section of Trieste; Tavani, M.</p> <p>2007-05-01</p> <p>The AGILE Mission will explore the <span class="hlt">gamma</span>-ray Universe with a very innovative instrument combining for the first time a <span class="hlt">gamma</span>-ray imager and a hard X-ray imager. AGILE will be operational at the beginning of 2007 and it will provide crucial data for the study of Active Galactic Nuclei, <span class="hlt">Gamma</span>-Ray Bursts, unidentified <span class="hlt">gamma</span>-ray sources, Galactic compact objects, supernova remnants, TeV sources, and fundamental physics by microsecond timing. The AGILE instrument is designed to simultaneously detect and image photons in the 30 MeV - 50 GeV and 15 - 45 keV <span class="hlt">energy</span> bands with excellent imaging and timing capabilities, and a largemore » field of view covering {approx} 1/5 of the entire sky at <span class="hlt">energies</span> above 30 MeV. A CsI calorimeter is capable of GRB triggering in the <span class="hlt">energy</span> band 0.3-50 MeV. The broadband detection of GRBs and the study of implications for particle acceleration and high <span class="hlt">energy</span> emission are primary goals of the mission. AGILE can image GRBs with 2-3 arcminute error boxes in the hard X-ray range, and provide broadband photon-by photon detection in the 15-45 keV, 03-50 MeV, and 30 MeV-30 GeV <span class="hlt">energy</span> ranges. Microsecond on-board photon tagging and a {approx} 100 microsecond <span class="hlt">gamma</span>-ray detection deadtime will be crucial for fast GRB timing. On-board calculated GRB coordinates and <span class="hlt">energy</span> fluxes will be quickly transmitted to the ground by an ORBCOMM transceiver. AGILE is now (January 2007) undergoing final satellite integration and testing. The PLS V launch is planned in spring 2007. AGILE is then foreseen to be fully operational during the summer of 2007.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19990021206','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19990021206"><span>Analysis of Data from the Energetic <span class="hlt">Gamma</span>-Ray Experiment Telescope (EGRET) on the Compton <span class="hlt">Gamma</span> Ray Observatory</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kniffen, Donald A.; Elliott, William W.</p> <p>1999-01-01</p> <p>The final report consists of summaries of work proposed, work accomplished, papers and presentations published and continuing work regarding the cooperative agreement. The work under the agreement is based on high <span class="hlt">energy</span> <span class="hlt">gamma</span> ray source data analysis collected from the Energetic <span class="hlt">Gamma</span>-Ray Experiment Telescope (EGRET).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/20078951','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/20078951"><span>[Coactivators in <span class="hlt">energy</span> metabolism: peroxisome proliferator-activated receptor-<span class="hlt">gamma</span> coactivator 1 family].</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Wang, Rui; Chang, Yong-sheng; Fang, Fu-de</p> <p>2009-12-01</p> <p>Peroxisome proliferator-activated receptor <span class="hlt">gamma</span> coactivator 1 (PGC1) family is highly expressed in tissues with high <span class="hlt">energy</span> metabolism. They coactivate transcription factors in regulating genes engaged in processes such as gluconeogenesis, adipose beta-oxydation, lipoprotein synthesis and secretion, mitochondrial biogenesis, and oxidative metabolism. Protein conformation studies demonstrated that they lack DNA binding domains and act as coactivators through physical interaction with transcription factors. PGC1 activity is regulated at transcription level or by multiple covalent chemical modifications such as phosphorylation, methylation and acetylation/deacetylation. Abnormal expression of PGC1 coactivators usually is closely correlated with diseases such as diabetes, obesity, hyperglycemia, hyperlipemia, and arterial and brain neuron necrosis diseases.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016nova.pres..914K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016nova.pres..914K"><span>Found: A Galaxy's Missing <span class="hlt">Gamma</span> Rays</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kohler, Susanna</p> <p>2016-04-01</p> <p>Recent reanalysis of data from the Fermi <span class="hlt">Gamma</span>-ray Space Telescope has resulted in the first detection of high-<span class="hlt">energy</span> <span class="hlt">gamma</span> rays emitted from a nearby galaxy. This discovery reveals more about how supernovae interact with their environments.Colliding Supernova RemnantAfter a stellar explosion, the supernovas ejecta expand, eventually encountering the ambient interstellar medium. According to models, this generates a strong shock, and a fraction of the kinetic <span class="hlt">energy</span> of the ejecta is transferred into cosmic rays high-<span class="hlt">energy</span> radiation composed primarily of protons and atomic nuclei. Much is still unknown about this process, however. One open question is: what fraction of the supernovas explosion power goes into accelerating these cosmic rays?In theory, one way to answer this is by looking for <span class="hlt">gamma</span> rays. In a starburst galaxy, the collision of the supernova-accelerated cosmic rays with the dense interstellar medium is predicted to produce high-<span class="hlt">energy</span> <span class="hlt">gamma</span> rays. That radiation should then escape the galaxy and be visible to us.Pass 8 to the RescueObservational tests of this model, however, have beenstumped by Arp 220. This nearby ultraluminous infrared galaxy is the product of a galaxy merger ~700 million years ago that fueled a frenzy of starbirth. Due to its dusty interior and extreme levels of star formation, Arp 220 has long been predicted to emit the <span class="hlt">gamma</span> rays produced by supernova-accelerated cosmic rays. But though weve looked, <span class="hlt">gamma</span>-ray emission has never been detected from this galaxy until now.In a recent study, a team of scientists led by Fang-Kun Peng (Nanjing University) reprocessed 7.5 years of Fermi observations using the new Pass 8 analysis software. The resulting increase in resolution revealed the first detection of GeV emission from Arp 220!Acceleration Efficiency<span class="hlt">Gamma</span>-ray luminosity vs. total infrared luminosity for LAT-detected star-forming galaxies and Seyferts. Arp 220s luminosities are consistent with the scaling relation. [Peng et al. 2016</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24738031','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24738031"><span>Tuberculin Skin Tests versus Interferon-<span class="hlt">Gamma</span> <span class="hlt">Release</span> Assays in Tuberculosis Screening among Immigrant Visa Applicants.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Chuke, Stella O; Yen, Nguyen Thi Ngoc; Laserson, Kayla F; Phuoc, Nguyen Huu; Trinh, Nguyen An; Nhung, Duong Thi Cam; Mai, Vo Thi Chi; Qui, An Dang; Hai, Hoang Hoa; Loan, Le Thien Huong; Jones, Warren G; Whitworth, William C; Shah, J Jina; Painter, John A; Mazurek, Gerald H; Maloney, Susan A</p> <p>2014-01-01</p> <p>Objective. Use of tuberculin skin tests (TSTs) and interferon <span class="hlt">gamma</span> <span class="hlt">release</span> assays (IGRAs) as part of tuberculosis (TB) screening among immigrants from high TB-burden countries has not been fully evaluated. Methods. Prevalence of Mycobacterium tuberculosis infection (MTBI) based on TST, or the QuantiFERON-TB Gold test (QFT-G), was determined among immigrant applicants in Vietnam bound for the United States (US); factors associated with test results and discordance were assessed; predictive values of TST and QFT-G for identifying chest radiographs (CXRs) consistent with TB were calculated. Results. Of 1,246 immigrant visa applicants studied, 57.9% were TST positive, 28.3% were QFT-G positive, and test agreement was 59.4%. Increasing age was associated with positive TST results, positive QFT-G results, TST-positive but QFT-G-negative discordance, and abnormal CXRs consistent with TB. Positive predictive values of TST and QFT-G for an abnormal CXR were 25.9% and 25.6%, respectively. Conclusion. The estimated prevalence of MTBI among US-bound visa applicants in Vietnam based on TST was twice that based on QFT-G, and 14 times higher than a TST-based estimate of MTBI prevalence reported for the general US population in 2000. QFT-G was not better than TST at predicting abnormal CXRs consistent with TB.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22167746-new-class-very-high-energy-gamma-ray-emitters-radio-dark-mini-shells-surrounding-active-galactic-nucleus-jets','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22167746-new-class-very-high-energy-gamma-ray-emitters-radio-dark-mini-shells-surrounding-active-galactic-nucleus-jets"><span>NEW CLASS OF VERY HIGH <span class="hlt">ENERGY</span> {<span class="hlt">gamma</span>}-RAY EMITTERS: RADIO-DARK MINI SHELLS SURROUNDING ACTIVE GALACTIC NUCLEUS JETS</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Kino, Motoki; Ito, Hirotaka; Kawakatu, Nozomu</p> <p></p> <p>We explore non-thermal emission from a shocked interstellar medium, which is identified as an expanding shell, driven by a relativistic jet in active galactic nuclei (AGNs). In this work, we particularly focus on parsec-scale size mini shells surrounding mini radio lobes. From the radio to X-ray band, the mini radio lobe emission dominates the faint emission from the mini shell. On the other hand, we find that inverse-Compton (IC) emission from the shell can overwhelm the associated lobe emission at the very high <span class="hlt">energy</span> (VHE; E > 100 GeV) {<span class="hlt">gamma</span>}-ray range, because <span class="hlt">energy</span> densities of synchrotron photons from the lobemore » and/or soft photons from the AGN nucleus are large and IC scattering works effectively. The predicted IC emission from nearby mini shells can be detected with the Cherenkov Telescope Array and they are potentially a new class of VHE {<span class="hlt">gamma</span>}-ray emitters.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1418916','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1418916"><span>Magnetic Microcalorimeter (MMC) <span class="hlt">Gamma</span> Detectors with Ultra-High <span class="hlt">Energy</span> Resolution</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Friedrich, Stephen</p> <p></p> <p>The goal of this LCP is to develop ultra-high resolution <span class="hlt">gamma</span> detectors based on magnetic microcalorimeters (MMCs) for accurate non-destructive analysis (NDA) of nuclear materials. For highest <span class="hlt">energy</span> resolution, we will introduce erbium-doped silver (Ag:Er) as a novel sensor material, and implement several geometry and design changes to improve the signal-to-noise ratio. The detector sensitivity will be increased by developing arrays of 32 Ag:Er pixels read out by 16 SQUID preamplifiers, and by developing a cryogenic Compton veto to reduce the spectral background. Since best MMC performance requires detector operation at ~10 mK, we will purchase a dilution refrigerator withmore » a base temperature <10 mK and adapt it for MMC operation. The detector performance will be tested with radioactive sources of interest to the safeguards community.« less</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li class="active"><span>25</span></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_25 --> <div class="footer-extlink text-muted" style="margin-bottom:1rem; text-align:center;">Some links on this page may take you to non-federal websites. Their policies may differ from this site.</div> </div><!-- container --> <footer><a id="backToTop" href="#top"> </a><nav><a id="backToTop" href="#top"> </a><ul class="links"><a id="backToTop" href="#top"> </a><li><a id="backToTop" href="#top"></a><a href="/sitemap.html">Site Map</a></li> <li><a href="/members/index.html">Members Only</a></li> <li><a href="/website-policies.html">Website Policies</a></li> <li><a href="https://doe.responsibledisclosure.com/hc/en-us" target="_blank">Vulnerability Disclosure Program</a></li> <li><a href="/contact.html">Contact Us</a></li> </ul> <div class="small">Science.gov is maintained by the U.S. Department of Energy's <a href="https://www.osti.gov/" target="_blank">Office of Scientific and Technical Information</a>, in partnership with <a href="https://www.cendi.gov/" target="_blank">CENDI</a>.</div> </nav> </footer> <script type="text/javascript"><!-- // var lastDiv = ""; function showDiv(divName) { // hide last div if (lastDiv) { document.getElementById(lastDiv).className = "hiddenDiv"; } //if value of the box is not nothing and an object with that name exists, then change the class if (divName && document.getElementById(divName)) { document.getElementById(divName).className = "visibleDiv"; lastDiv = divName; } } //--> </script> <script> /** * Function that tracks a click on an outbound link in Google Analytics. * This function takes a valid URL string as an argument, and uses that URL string * as the event label. */ var trackOutboundLink = function(url,collectionCode) { try { h = window.open(url); setTimeout(function() { ga('send', 'event', 'topic-page-click-through', collectionCode, url); }, 1000); } catch(err){} }; </script> <!-- Google Analytics --> <script> (function(i,s,o,g,r,a,m){i['GoogleAnalyticsObject']=r;i[r]=i[r]||function(){ (i[r].q=i[r].q||[]).push(arguments)},i[r].l=1*new Date();a=s.createElement(o), m=s.getElementsByTagName(o)[0];a.async=1;a.src=g;m.parentNode.insertBefore(a,m) })(window,document,'script','//www.google-analytics.com/analytics.js','ga'); ga('create', 'UA-1122789-34', 'auto'); ga('send', 'pageview'); </script> <!-- End Google Analytics --> <script> showDiv('page_1') </script> </body> </html>