Search results for "Telescope"

showing 10 items of 499 documents

Production of excited double hypernuclei via Fermi breakup of excited strange systems

2011

Precise spectroscopy of multi-strange hypernuclei provides a unique chance to explore the hyperon-hyperon interaction. In the present work we explore the production of excited states in double hypernuclei following the micro-canonical break-up of an initially excited double hypernucleus which is created by the absorption and conversion of a stopped $\Xi^{-}$ hyperon. Rather independent on the spectrum of possible excited states in the produced double hypernuclei the formation of excited states dominates in our model. For different initial target nuclei which absorb the $\Xi^-$, different double hypernuclei nuclei dominate. Thus the ability to assign the various observable $\gamma$-transitio…

PhysicsNuclear and High Energy Physics010308 nuclear & particles physicsNuclear TheoryHyperonFOS: Physical sciencesObservableHypernucleus01 natural sciencesSpectral lineNuclear physicsPionExcited state0103 physical sciencesNuclear Experiment (nucl-ex)Atomic physics010306 general physicsSpectroscopyNuclear ExperimentNuclear ExperimentFermi Gamma-ray Space Telescope
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Development and calibration of the tracking Compton/Pair telescope MEGA

2005

Abstract We describe the development and tests of the prototype for a new telescope for Medium Energy Gamma-ray Astronomy (MEGA) in the energy band 0.4–50 MeV. As a successor to COMPTEL and EGRET (at low energies), MEGA aims to improve the sensitivity for astronomical sources by at least an order of magnitude. It could thus fill the severe sensitivity gap between scheduled or operating hard-X-ray and high-energy gamma-ray missions and open the way for a future Advanced Compton Telescope. MEGA records and images γ-rays by completely tracking Compton and Pair creation events in a stack of double-sided Si-strip track detectors surrounded by a pixelated CsI calorimeter. A scaled down prototype …

PhysicsNuclear and High Energy PhysicsCalorimeter (particle physics)Physics::Instrumentation and Detectorsbusiness.industryAstrophysics::High Energy Astrophysical PhenomenaCompton telescopeAstrophysics::Instrumentation and Methods for AstrophysicsMega-Tracking (particle physics)law.inventionTelescopeOpticsStack (abstract data type)lawCalibrationSensitivity (control systems)businessInstrumentationNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Electromagnetic Production of the Hypertriton

1996

Kaon photoproduction on He3, gamma + He3 --> K+ + Hypertriton, is studied in the framework of the impulse approximation. Realistic He3 wave functions obtained as solutions of Faddeev equations with the Reid soft-core potential are used along with different Hypertriton wave functions. Results are compared for several elementary operator models, which can successfully describe the elementary kaon production off the proton up to a photon lab energy of k = 2.2 GeV. It is found that the corresponding cross sections are small, of the order of several nanobarns. It is also shown that the influence of Fermi motion is important, while the effect of different off-shell assumptions on the cross sec…

PhysicsNuclear and High Energy PhysicsFaddeev equationsPhotonNuclear TheoryNuclear TheoryFOS: Physical sciencesImpulse (physics)Nuclear physicsNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Physics::Atomic and Molecular ClustersWave functionNuclear ExperimentHypertritonFermi Gamma-ray Space Telescope
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Microscopic quasiparticle-phonon description of odd-mass127−133Xeisotopes and their β decay

1998

Quasiparticle-phonon equations of motion are solved starting from a microscopic realistic many-body Hamiltonian. In this microscopic quasiparticle-phonon model (MQPM) the relevant part of the three-quasiparticle Hilbert space may possibly be taken into account even in calculations using large single-particle bases. As an example, the MQPM is applied to the calculation of energy levels and Fermi and Gamow-Teller beta-decay transition amplitudes for transitions between odd-mass ${}^{127\ensuremath{-}133}\mathrm{Xe}$, ${}^{127\ensuremath{-}133}\mathrm{I}$, and ${}^{127\ensuremath{-}133}\mathrm{Cs}$ isotopes. Considering the fully microscopic nature of the MQPM, comparison of its results and da…

PhysicsNuclear and High Energy PhysicsIsotopePhononHilbert spaceEquations of motionsymbols.namesakeAmplitudeQuantum mechanicsQuasiparticlesymbolsCondensed Matter::Strongly Correlated ElectronsAtomic physicsHamiltonian (quantum mechanics)Fermi Gamma-ray Space TelescopePhysical Review C
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Peculiarities in fragment mass distribution in the 238U + 40Ar (243 MeV) reaction

2001

A pronounced fine structure (FS) in the form of distinct peaks was observed in neutron gated mass spectra from the decay of the 278110 composite system produced in the reaction 238U + 40Ar (243 MeV) at an initial excitation energy E * > 70 MeV. The FS peaks are located in the vicinity of mass numbers 70-80, 100, and 130, which correspond to those of magic nuclei (clusters). In the data there is also evidence for a new type of decay -- collinear cluster tripartition of an excited nucleus.

PhysicsNuclear and High Energy PhysicsMass distributionNuclear TheoryHadronCluster (physics)Mass spectrumNuclear fusionNeutronMAGIC (telescope)Atomic physicsNuclear ExperimentExcitationThe European Physical Journal A
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Theoretical study of incoherent phi photoproduction on a deuteron target

2012

We study the photoproduction of phi mesons in deuteron, paying attention to the modification of the cross section from bound protons to the free ones with the aim of comparing with recent results at LEPS. For this purpose we take into account Fermi motion in single scattering and rescattering of the phi to account for phi absorption on a second nucleon as well as the rescattering of the proton. We find that the contribution of the double scattering is much smaller than the typical cross section of gamma p to phi p in free space, which implies a very small screening of the phi production in deuteron. The contribution from the proton rescattering, on the other hand, is found to be not negligi…

PhysicsNuclear and High Energy PhysicsMesonProtonNuclear Theory010308 nuclear & particles physicsScatteringNuclear TheoryFísicaFOS: Physical sciences01 natural sciences7. Clean energyNuclear physicsMomentumNuclear Theory (nucl-th)Cross section (physics)Phase space0103 physical sciences010306 general physicsNucleonNuclear ExperimentFermi Gamma-ray Space Telescope
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Conservative upper limits on WIMP annihilation cross section from Fermi-LAT γ rays

2012

The spectrum of an isotropic extragalactic {\gamma}-ray background (EGB) has been measured by the Fermi-LAT telescope at high latitudes. Two new models for the EGB are derived from the subraction of unresolved point sources and extragalactic diffuse processes, which could explain from 30% to 70% of the Fermi-LAT EGB. Within the hypothesis that the two residual EGBs are entirely due to the annihilation of dark matter (DM) particles in the Galactic halo, we obtain stringent upper limits on their annihilation cross section. Severe bounds on a possible Sommerfeld enhancement of the annihilation cross section are set as well. Finally, we consider models for DM annihilation depending on the inver…

PhysicsNuclear and High Energy PhysicsParticle physicsAnnihilationdark matter theoryAstrophysics::High Energy Astrophysical PhenomenaDark matterGamma raysGamma rayAstrophysics::Cosmology and Extragalactic AstrophysicsAstrophysicsGalactic haloGamma rays; dark matter theoryPulsarWIMPHaloAstrophysics::Galaxy AstrophysicsFermi Gamma-ray Space Telescope
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Scalar isoscalar pion pairs in nuclei and theA(π,ππ)Xreaction

1999

The reaction A(pi,pi pi)X has been studied at low energies, paying particular attention to the interaction of the two final pions in the scalar isoscalar (I=J=0) channel. We have developed a microscopic model for the pion production, and then implemented the two pion final state interaction by using the results of a non-perturbative unitary coupled-channels method based in the standard chiral Lagrangians. The resulting model, describes well the reaction on the nucleon for all different isospin channels. Finally, we have considered the reaction in nuclei. Our calculation takes into account Fermi motion, Pauli blocking, pion absorption, and also the strong modification of the pi-pi interactio…

PhysicsNuclear and High Energy PhysicsParticle physicsIsoscalarNuclear TheoryScalar (mathematics)Nuclear physicssymbols.namesakePauli exclusion principlePionDeuteriumIsospinsymbolsNuclear ExperimentNucleonFermi Gamma-ray Space TelescopePhysical Review C
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Quasielastic neutrino (antineutrino) reactions in nuclei and the axial-vector form factor of the nucleon

1992

Abstract Quasielastic neutrino and antineutrino reactions in nuclei are studied to investigate the effect of the nuclear medium on the determination of axial dipole mass M A in nuclei. The calculations are done in the local density approximation and various nuclear effects like Pauli blocking, Fermi motion of nucleons and strong renormalization effects in the spin-isospin channel are taken into account. The nuclear effects are found to be quite large at low q 2 , but the data in this region are too meagre to influence the determination of M A . The experimental data on differential and total cross sections are found to be consistent with M A as determined from deuterium experiments and no c…

PhysicsNuclear and High Energy PhysicsParticle physicsNuclear TheoryForm factor (quantum field theory)Nuclear physicsDipolesymbols.namesakePauli exclusion principleDeuteriumsymbolsNeutrinoNuclear ExperimentNucleonPseudovectorFermi Gamma-ray Space TelescopeNuclear Physics A
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Mesonic and binding contributions to the EMC effect in a relativistic many-body approach

1996

We revise the conventional nuclear effects of Fermi motion, binding and pionic effects in deep inelastic lepton scattering using a relativistic formalism for an interacting Fermi sea and the local density approximation to translate results from nuclear matter to finite nuclei. In addition we also consider effects from rho-meson renormalization in the nucleus. The use of nucleon Green's functions in terms of their spectral functions offers a precise way to account for Fermi motion and binding. On the other hand the use of many body Feynman diagrams in a relativistic framework allows one to avoid using prescriptions given in the past to introduce relativistic corrections in a non relativistic…

PhysicsNuclear and High Energy PhysicsParticle physicsNuclear TheoryMesonHigh Energy Physics::PhenomenologyEMC effectNuclear TheoryFOS: Physical sciencesFísicaNuclear matterNuclear Theory (nucl-th)RenormalizationHigh Energy Physics - Phenomenologysymbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)symbolsFeynman diagramNucleonNuclear ExperimentFermi Gamma-ray Space TelescopeLepton
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