Search results for "Fermi Gamma-ray Space Telescope"

showing 10 items of 108 documents

Observation of theβ-Delayedγ-Proton Decay ofZn56and its Impact on the Gamow-Teller Strength Evaluation

2014

We report the observation of a very exotic decay mode at the proton drip line, the $\ensuremath{\beta}$-delayed $\ensuremath{\gamma}$-proton decay, clearly seen in the $\ensuremath{\beta}$ decay of the ${T}_{z}=\ensuremath{-}2$ nucleus $^{56}\mathrm{Zn}$. Three $\ensuremath{\gamma}$-proton sequences have been observed after the $\ensuremath{\beta}$ decay. Here this decay mode, already observed in the $sd$ shell, is seen for the first time in the $fp$ shell. Both $\ensuremath{\gamma}$ and proton decays have been taken into account in the estimation of the Fermi and Gamow-Teller strengths. Evidence for fragmentation of the Fermi strength due to strong isospin mixing is found.

Nuclear physicsPhysicsProton decayIsospinDouble beta decayNuclear TheoryGeneral Physics and AstronomyHigh Energy Physics::ExperimentNuclear ExperimentNuclear theoryBeta decayFermi Gamma-ray Space TelescopePhysical Review Letters
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Inclusive quasielastic neutrino reactions inC12andO16at intermediate energies

1993

Inclusive quasielastic neutrino (antineutrino) reactions on [sup 12]C and [sup 16]O at intermediate energies (50[lt][ital E][lt]400 MeV) are studied to investigate the effects of the nuclear medium on the total cross section and the energy spectrum of the outgoing leptons. The calculations are done in the local density approximation and various nuclear effects like Pauli blocking, Fermi motion, and strong-interaction renormalizations due to the presence of nucleons are taken into account. The corrections due to Coulomb effects are included which have been hitherto neglected in inclusive reactions. The results presented here are applicable to the inclusive reactions with neutrino beams plann…

Nuclear reactionPhysicsNuclear and High Energy PhysicsParticle physicsNuclear TheoryNuclear physicssymbols.namesakePauli exclusion principlesymbolsCoulombHigh Energy Physics::ExperimentNeutrinoNuclear ExperimentNucleonNeutrino oscillationFermi Gamma-ray Space TelescopeLeptonPhysical Review C
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Pion induced pion production on deuterium: A Quasifree process

1992

Abstract A detailed experimental analysis of the π+d → π+π−pp in-plane coincidence data first presented by Rui et al. is compared to an expanded version of the Oset and Vicente-Vacas model for pion-induced pion production on a free nucleon. This extended model averages over Fermi motion to describe the assumed quasifree nature of the process occurring on the deuteron and includes nine additional diagrams to account for the N ∗ → N (ππ) p-wave reaction channels. Experimental effects such as pion energy loss in the target and in the detectors, pion decay and muon detection are investigated and incorporated into the comparison of experimental data and theory. Inclusion of Fermi motion was foun…

Nuclear reactionPhysicsfew body reactionNuclear and High Energy PhysicsParticle physicsMuonNuclear Theorypion productionCoincidenceNuclear physicsPionDeuteriumpion production; few body reactionVertex (curve)Nuclear ExperimentNucleonFermi Gamma-ray Space Telescope
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THE RELATION BETWEEN AGN GAMMA-RAY EMISSION AND PARSEC-SCALE RADIO JETS

2009

We have compared the radio emission from a sample of parsec-scale AGN jets as measured by the VLBA at 15 GHz, with their associated gamma-ray properties that are reported in the Fermi LAT 3-month bright source list. We find in our radio-selected sample that the gamma-ray photon flux correlates well with the quasi-simultaneously measured compact radio flux density. The LAT-detected jets in our radio-selected complete sample generally have higher compact radio flux densities, and their parsec-scale cores are brighter (i.e., have higher brightness temperature) than the jets in the LAT non-detected objects. This suggests that the jets of bright gamma-ray AGN have preferentially higher Doppler-b…

PhotonActive galactic nucleusAstrophysics::High Energy Astrophysical PhenomenaFOS: Physical sciencesAstrophysics::Cosmology and Extragalactic AstrophysicsAstrophysics01 natural sciencesParseclaw.inventionTelescopelaw0103 physical sciences010303 astronomy & astrophysicsAstrophysics::Galaxy AstrophysicsHigh Energy Astrophysical Phenomena (astro-ph.HE)Physics010308 nuclear & particles physicsGamma rayAstronomy and AstrophysicsAstrophysics - Astrophysics of GalaxiesGalaxySpace and Planetary ScienceAstrophysics of Galaxies (astro-ph.GA)Brightness temperatureAstrophysics - High Energy Astrophysical PhenomenaFermi Gamma-ray Space TelescopeThe Astrophysical Journal
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Prolonged sub-luminous state of the new transitional pulsar candidate CXOU J110926.4-650224

2019

We report on a multi-wavelength study of the unclassified X-ray source CXOU J110926.4-650224 (J1109). We identified the optical counterpart as a blue star with a magnitude of $\sim$20.1 (3300-10500 $\require{mediawiki-texvc} \AA$). The optical emission was variable on timescales from hundreds to thousands of seconds. The spectrum showed prominent emission lines with variable profiles at different epochs. Simultaneous XMM-Newton and NuSTAR observations revealed a bimodal distribution of the X-ray count rates on timescales as short as tens of seconds, as well as sporadic flaring activity. The average broad-band (0.3-79 keV) spectrum was adequately described by an absorbed power law model with…

PhotonX-rays: BinarieAstrophysics::High Energy Astrophysical PhenomenaFluxFOS: Physical sciencesAstrophysicsMethods: Data analysiAstrophysics::Cosmology and Extragalactic Astrophysics7. Clean energy01 natural sciencesLuminosityAccretion accretion diskSettore FIS/05 - Astronomia E AstrofisicaPulsarMethods: Observational0103 physical sciencesEmission spectrum010303 astronomy & astrophysicsAstrophysics::Galaxy AstrophysicsPhysicsHigh Energy Astrophysical Phenomena (astro-ph.HE)010308 nuclear & particles physicsAstronomy and AstrophysicsStars: neutronX-rays: Individuals: CXOU J110926.4-650224Neutron star13. Climate actionSpace and Planetary ScienceMagnitude (astronomy)Astrophysics - High Energy Astrophysical PhenomenaFermi Gamma-ray Space Telescope
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Gamma-ray burst afterglow light curves from realistic density profiles

2011

The afterglow emission that follows gamma-ray bursts (GRBs) contains valuable information about the circumburst medium and, therefore, about the GRB progenitor. Theoretical studies of GRB blast waves, however, are often limited to simple density profiles for the external medium (mostly constant density and power-law R^{-k} ones). We argue that a large fraction of long-duration GRBs should take place in massive stellar clusters where the circumburst medium is much more complicated. As a case study, we simulate the propagation of a GRB blast wave in a medium shaped by the collision of the winds of O and Wolf-Rayet stars, the typical distance of which is d /sim 0.1 - 1 pc. Assuming a spherical…

Physics010308 nuclear & particles physicsAstrophysics::High Energy Astrophysical PhenomenaCompton scatteringAstronomyAstronomy and AstrophysicsAstrophysics::Cosmology and Extragalactic AstrophysicsAstrophysicsLight curve01 natural sciencesAfterglowlaw.inventionStarsSpace and Planetary Sciencelaw0103 physical sciencesAstrophysics::Solar and Stellar AstrophysicsGamma-ray burst010303 astronomy & astrophysicsAstrophysics::Galaxy AstrophysicsBlast waveFermi Gamma-ray Space TelescopeFlareMonthly Notices of the Royal Astronomical Society
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The $T_{z} = \pm 1 \to 0$ and $\pm 2 \to \pm 1$ Mirror Gamow--Teller Transitions in $pf$-shell Nuclei

2016

Gamow–Teller (GT) transitions are the most common weak-interaction processes in the Universe. They play important roles in various processes of nucleosynthesis, for example, in the rapid proton-capture process (rp-process). In the pf-shell region, the rp-process runs through neutron-deficient nuclei with Tz = −2, −1, and 0 mainly by means of GT and Fermi transitions, where Tz is the z component of isospin T defined by Tz = (N − Z)∕2. Under the assumption of isospin symmetry, mirror nuclei with reversed Z and N numbers, and thus with opposite signs of Tz, have the same structure. Therefore, symmetry is also expected for the GT transitions starting from and ending up in mirror nuclei. We have…

Physics010308 nuclear & particles physicsHadronShell (structure)General Physics and Astronomy01 natural sciencesSymmetry (physics)Nuclear physicsNucleosynthesisIsospin0103 physical sciencesMirror nuclei010306 general physicsFermi Gamma-ray Space TelescopeActa Physica Polonica B
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An algorithm for computing geometric relative velocities through Fermi and observational coordinates

2013

We present a numerical method for computing the \textit{Fermi} and \textit{observational coordinates} of a distant test particle with respect to an observer. We apply this method for computing some previously introduced concepts of relative velocity: \textit{kinematic}, \textit{Fermi}, \textit{spectroscopic} and \textit{astrometric} relative velocities. We also extend these concepts to non-convex normal neighborhoods and we make some convergence tests, studying some fundamental examples in Schwarzschild and Kerr spacetimes. Finally, we show an alternative method for computing the Fermi and astrometric relative velocities.

Physics83C10 83-08 65Z05Physics and Astronomy (miscellaneous)Numerical analysisMathematical analysisRelative velocityFOS: Physical sciencesKinematicsGeneral Relativity and Quantum Cosmology (gr-qc)Mathematical Physics (math-ph)Observer (physics)General Relativity and Quantum CosmologyConvergence testsTest particleSchwarzschild radiusMathematical PhysicsFermi Gamma-ray Space Telescope
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Influence of Electron-Electron Correlations and Lattice Effects on Positron-Electron Enhancement Factors

2010

We present an approach taking into account the effect of electron-electron (e-e) correlations on electron-positron (e-p) momentum density distributions. The approach bases on the modification of the Bethe-Goldstone (B-G) equation for the positron in the electron gas due to self-energy effects. The example calculations have been performed for selected parameters corresponding to simple metals. The calculated dependencies exhibit the increase of the e-p enhancement factors below Fermi momentum, like Kahana enhancements, and a decrease above the Fermi sphere, leading to a many-body “tail” in the e-p momentum density distributions. Moreover, the influence of lattice effects on enhancement facto…

PhysicsAnnihilationMechanical EngineeringElectronic structureElectronCondensed Matter PhysicsPositronMechanics of MaterialsLattice (order)General Materials ScienceAtomic physicsFermi gasPositron annihilationFermi Gamma-ray Space TelescopeMaterials Science Forum
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NH3 dynamics in Zn(NH3)4I2 and Zn(NH3)4Br2 investigated by incoherent quasielastic neutron scattering

1997

We report on studies of NH3 dynamics in Zn(NH3)4I2 and Zn(NH3)4Br2 by means of incoherent quasielastic neutron scattering in the temperature range from 150 to 300 K. Quasielastic experiments were carried out on the Fermi chopper time-of-flight spectrometer at NIST. The Lorentzian full-widths at half-maximum, ƒw, of the quasielastic line follow an Arrhenius law and increase from 0.39 [0.25] meV at 150 K to 1.33 [0.80] meV at 300 K. We find an activation energy Ea for the NH3 reorientations of 32(1) and 30(3) meV for Zn(NH3)4I2 and Zn(NH3)4Br2, respectively.

PhysicsArrhenius equationQuasielastic scatteringSpectrometerAnalytical chemistryActivation energyAtmospheric temperature rangeCondensed Matter PhysicsElectronic Optical and Magnetic MaterialsNuclear physicssymbols.namesakeQuasielastic neutron scatteringsymbolsElectrical and Electronic EngineeringFermi Gamma-ray Space TelescopeLine (formation)Physica B: Condensed Matter
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