Search results for "nuclear reaction"

showing 10 items of 449 documents

Inclusive quasielastic charged-current neutrino-nucleus reactions

2004

The Quasi-Elastic (QE) contribution of the nuclear inclusive electron scattering model developed in Nucl. Phys. A627 (1997) 543 is extended to the study of electroweak Charged Current (CC) induced nuclear reactions, at intermediate energies of interest for future neutrino oscillation experiments. The model accounts for, among other nuclear effects, long range nuclear (RPA) correlations, Final State Interaction (FSI) and Coulomb corrections. Predictions for the inclusive muon capture in $^{12}$C and the reaction $^{12}$C $(\nu_\mu,\mu^-)X$ near threshold are also given. RPA correlations are shown to play a crucial role and their inclusion leads to one of the best existing simultaneous descri…

Nuclear reactionPhysicsNuclear and High Energy PhysicsParticle physicsNuclear TheoryElectroweak interactionNuclear TheoryFOS: Physical sciencesFísicaMuon captureNuclear Theory (nucl-th)Nuclear physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)CoulombHigh Energy Physics::ExperimentNeutrinoNeutrino oscillationNuclear ExperimentElectron scatteringCharged current
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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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Kinematical coincidence method in transfer reactions

2013

A new method to extract high resolution angular distributions from kinematical coincidence measurements in binary reactions is presented. Kinematic is used to extract the center of mass angular distribution from the measured energy spectrum of light particles. Results obtained in the case of 10Be+p-->9Be+d reaction measured with the CHIMERA detector are shown. An angular resolution of few degrees in the center of mass is obtained.

Nuclear reactionPhysicsNuclear and High Energy PhysicsPhotonBinary reactionKinematical coincidenceResolution (electron density)FOS: Physical sciencesParticle detectorSpectral lineCoincidenceAngular distribution; Kinematical coincidence; Radioactive beam; Binary reactionAngular distribution; Binary reaction; Kinematical coincidence; Radioactive beam; Instrumentation; Nuclear and High Energy PhysicsRadioactive beamAngular resolutionCenter of massNuclear Experiment (nucl-ex)Atomic physicsAngular distributionNuclear ExperimentInstrumentationNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Study of three-nucleon mechanisms in the photodisintegration of 3He

1997

Abstract The cross section of the 3He(γ,pp)n reaction has been measured for the first time over a wide photon energy and proton angular range (200 MeV ≤ Eγ ≤ 800 MeV; 20° ≤ ϑplab ≤ 160°) using the large acceptance detector DAPHNE at the tagged photon facility of the MAMI microtron in Mainz. The wide kinematical coverage of the measurement has allowed a detailed analysis of three-nucleon absorption mechanisms. A model developed by Laget explains the main characteristics of the data in the Δ resonance region.

Nuclear reactionPhysicsNuclear and High Energy PhysicsPhotonProtonNuclear TheoryPhotofissionPhoton energyNuclear physicsPhotodisintegrationPhysics::Accelerator PhysicsNuclear ExperimentNucleonMicrotronNuclear Physics A
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Measurement of the partial cross sectionsσTT,σLT, and(σT+ɛσL)of the1H(e,e′π+)nreaction in theΔ(1232)resonance

2011

We report precision {sup 1}H(e, e{sup '{pi}+})n measurements in the {Delta}(1232) resonance at Q{sup 2}=0.127(GeV/c){sup 2} obtained at the MIT-Bates out-of-plane scattering facility. These are the lowest, but nonzero, Q{sup 2} measurements in the {pi}{sup +} channel. The data offer tests of the theoretical calculations, particularly of the background amplitude contributions. The chiral effective field theory and Sato-Lee model calculations are not in agreement with this experiment.

Nuclear reactionPhysicsNuclear and High Energy PhysicsPionMesonHadronResonanceSigmaElementary particleAtomic physicsNucleonPhysical Review C
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αdecay studies of very neutron-deficient francium and radium isotopes

2005

Very neutron-deficient francium and radium isotopes have been produced in fusion evaporation reactions using $^{63}\mathrm{Cu}$ and $^{65}\mathrm{Cu}$ ions on $^{141}\mathrm{Pr}$ targets and $^{36}\mathrm{Ar}$ ions on $^{170}\mathrm{Yb}$ targets. The gas-filled recoil separator RITU was employed to collect the fusion products and to separate them from the scattered beam. The activities were implanted into a position-sensitive silicon detector after passing through a gas-counter system. The isotopes were identified using spatial and time correlations between the implants and decays. Two new \ensuremath{\alpha} decaying radium isotopes, $^{201}\mathrm{Ra}$ and $^{202}\mathrm{Ra}$, were identi…

Nuclear reactionPhysicsNuclear and High Energy PhysicsProton010308 nuclear & particles physicsHadronchemistry.chemical_element7. Clean energy01 natural sciencesFranciumNuclear physicschemistryDecay energy0103 physical sciencesPhysics::Atomic PhysicsAlpha decay010306 general physicsNucleonRadioactive decayPhysical Review C
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Mass measurements in the vicinity of the doubly magic waiting pointNi56

2010

Masses of $^{56,57}\mathrm{Fe}$, $^{53}\mathrm{Co}$${}^{m}$, $^{53,56}\mathrm{Co}$, $^{55,56,57}\mathrm{Ni}$, $^{57,58}\mathrm{Cu}$, and $^{59,60}\mathrm{Zn}$ have been determined with the JYFLTRAP Penning trap mass spectrometer at the Ion-Guide Isotope Separator On-Line facility with a precision of $\ensuremath{\delta}m/m\ensuremath{\leqslant}3\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}8}$. The ${Q}_{\mathrm{EC}}$ values for $^{53}\mathrm{Co}$, $^{55}\mathrm{Ni}$, $^{56}\mathrm{Ni}$, $^{57}\mathrm{Cu}$, $^{58}\mathrm{Cu}$, and $^{59}\mathrm{Zn}$ have been measured directly with a typical precision of better than $0.7 \mathrm{keV}$ and Coulomb displacement energies have been dete…

Nuclear reactionPhysicsNuclear and High Energy PhysicsProton010308 nuclear & particles physicsQ valueHadronElementary particle01 natural sciencesBaryon0103 physical sciencesAtomic physics010306 general physicsNucleonEnergy (signal processing)Physical Review C
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Proton-hole states in theN=30neutron-rich isotopeK49

2010

Excited states in the N=30 neutron-rich isotope {sup 49}K have been studied using multinucleon transfer reactions with thin targets and the PRISMA-CLARA spectrometer combined with thick-target {gamma}-coincidence data from Gammasphere. The d{sub 3/2} proton-hole state is located 92 keV above the s{sub 1/2} ground state, and the proton-particle f{sub 7/2} state is suggested at 2104 keV. Three other levels are established as involving the coupling to 2{sup +} of two neutrons above the N=28 shell. The measured or estimated lifetimes served to reinforce the interpretation of the observed level structure, which is found to be in satisfactory agreement with shell-model calculations.

Nuclear reactionPhysicsNuclear and High Energy PhysicsProtonAstrophysics::High Energy Astrophysical PhenomenaExcited stateGammasphereNeutronAtomic physicsNuclear ExperimentGround stateNucleonCoupling (probability)Physical Review C
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Quasielastic proton knockout from 16O.

1994

The spectral function of the $^{16}\mathrm{O}$(e,e'p${)}^{15}$N reaction has been measured in quasielastic parallel kinematics. Momentum distributions are extracted for transitions to several discrete states, with emphasis on the low-lying positive parity states of $^{15}\mathrm{N}$. Spectroscopic factors and bound state wave functions are deduced from a DWIA analysis employing five different optical potentials. Coupled channels effects are investigated for the first four states of $^{15}\mathrm{N}$ and are found to be minimal. The spectroscopic results of the 1/${2}^{\mathrm{\ensuremath{-}}}$ ground state and the first 3/${2}^{\mathrm{\ensuremath{-}}}$ excited state indicate a 28%\ifmmode\…

Nuclear reactionPhysicsNuclear and High Energy PhysicsProtonExcited stateBound stateHadronSum rule in quantum mechanicsAtomic physicsNucleonGround statePhysical review. C, Nuclear physics
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Five-valence-protonN=82isotone137Cs

1999

Yrast excitations in the N=82 isotone {sup 137}Cs have been identified for the first time in thick-target {gamma}-ray coincidence measurements for the system {sup 232}Th+{sup 136}Xe using the Gammasphere array. The {sup 137}Cs nuclei were produced in deep inelastic one-proton-transfer reactions. By-products of the main investigation were two well-developed rotational bands which were identified in heavy reaction partner products complementary to {sup 137}Cs and are tentatively assigned to the little studied nucleus {sup 231}Ac. There was no difficulty in placing the 11 observed {sup 137}Cs transitions in a yrast level scheme extending to an I{sup {pi}}=(31/2{sup {minus}}) level at 5494 keV.…

Nuclear reactionPhysicsNuclear and High Energy PhysicsProtonExcited stateIsotoneYrastHadronGammasphereAtomic physicsNucleonPhysical Review C
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