Search results for "Nucleon"

showing 10 items of 1041 documents

Reliable extraction of the dB(E1)/dE for 11Be from its breakup at 520 MeV/nucleon

2019

We analyze the breakup of the one-neutron halo nucleus 11Be measured at 520 MeV/nucleon at GSI on Pb and C targets within an eikonal description of the reaction including a proper treatment of special relativity. The Coulomb term of the projectile-target interaction is corrected at first order, while its nuclear part is described at the optical limit approximation. Good agreement with the data is obtained using a description of 11Be, which fits the breakup data of RIKEN. This solves the apparent discrepancy between the dB(E1)/dE estimations from GSI and RIKEN for this nucleus.

Nuclear and High Energy PhysicsRelativistic correctionNuclear TheoryNuclear TheoryFOS: Physical sciencesHalo nucleusSpecial relativityOne-neutron halo nucleidB(E1)/dENuclear breakup01 natural sciencesNuclear physicsNuclear Theory (nucl-th)Eikonal model0103 physical sciencesCoulombmedicineCoulomb breakup010306 general physicsNuclear ExperimentPhysics010308 nuclear & particles physicsEikonal equationBreakupPhysique atomique et nucléairelcsh:QC1-999medicine.anatomical_structureProper treatmentPhysics::Accelerator PhysicsNucleonNucleuslcsh:PhysicsPhysics Letters B
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A precision measurement of charm dimuon production in neutrino interactions from the NOMAD experiment

2013

We present our new measurement of the cross-section for charm dimuon production in neutrino iron interactions based upon the full statistics collected by the NOMAD experiment. After background subtraction we observe 15 344 charm dimuon events, providing the largest sample currently available. The analysis exploits the large inclusive charged current sample - about 9 x 10(6) events after all analysis cuts - and the high resolution NOMAD detector to constrain the total systematic uncertainty on the ratio of charm dimuon to inclusive Charged Current (CC) cross-sections to similar to 2%. We also perform a fit to the NOMAD data to extract the charm production parameters and the strange quark sea…

Nuclear and High Energy PhysicsStrange quarkParticle physicsCharm production; strange quark content of the nucleon; dimuon charm productionFOS: Physical sciencesCharm production ; Strange quark content of the nucleon ; Dimuon charm production ; Neutrino interactions01 natural sciencesCharm quarkHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Charm (quantum number)010306 general physicsCharged currentDimuon charm productionPhysicsQuantum chromodynamics010308 nuclear & particles physicsNeutrino interactionsFísicadimuon charm productionDeep inelastic scatteringstrange quark content of the nucleon3. Good healthCharm productionStrange quark content of the nucleonNeutrinoNucleonParticle Physics - Experiment
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Electron Ion Collider: The Next QCD Frontier: Understanding the glue that binds us all

2016

International audience; This White Paper presents the science case of an Electron-Ion Collider (EIC), focused on the structure and interactions of gluon-dominated matter, with the intent to articulate it to the broader nuclear science community. It was commissioned by the managements of Brookhaven National Laboratory (BNL) and Thomas Jefferson National Accelerator Facility (JLab) with the objective of presenting a summary of scientific opportunities and goals of the EIC as a follow-up to the 2007 NSAC Long Range plan. This document is a culmination of a community-wide effort in nuclear science following a series of workshops on EIC physics over the past decades and, in particular, the focus…

Nuclear and High Energy Physicsdesign [accelerator]nucl-th[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]parton: distribution functionnucleus: structure functionpolarized beamstructure function: spin[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]nucl-exstructure function [nucleon]Atomicproposed [colliding beams]design [detector]Particle and Plasma Physicsquantum chromodynamics[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]ddc:530Nuclearsaturation [gluon]colliding beams [electron nucleon]Hardware_REGISTER-TRANSFER-LEVELIMPLEMENTATIONdetector: designaccelerator: designhep-exnew physicsMolecularhep-phelectron nucleon: colliding beamsnucleon: structure functionstructure function [nucleus]Nuclear & Particles PhysicseRHICTheoryofComputation_MATHEMATICALLOGICANDFORMALLANGUAGESelectron nucleus: colliding beamscolliding beams: proposedTheoryofComputation_LOGICSANDMEANINGSOFPROGRAMS[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]gluon: saturationELICspin [structure function]Software_PROGRAMMINGLANGUAGEScolliding beams [electron nucleus]distribution function [parton]Hardware_LOGICDESIGNJefferson Lab
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Mirror energy differences above the 0f7/2 shell: First γ-ray spectroscopy of the Tz = −2 nucleus 56Zn

2021

5 pags., 4 figs.

Nuclear and High Energy Physicssinkki (metallit)QC1-999Nuclear Theory01 natural sciencesnucleon removalmirror nuclei0103 physical sciencesSubatomic Physicsmedicine010306 general physicsSpectroscopyradioactive ion beamsNuclear ExperimentNucleonsPhysics[PHYS]Physics [physics]isotoopitValence (chemistry)Isovector010308 nuclear & particles physicsYrastPhysicsFísicaSymmetry Breakingmedicine.anatomical_structureisospin symmetryshell-model calculationsExcited stateEnergy DifferenceAtomic physicsMultipole expansionydinfysiikkaNucleusBeam (structure)
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Advanced model for the prediction of the neutron-rich fission product yields

2013

The consistent models for the description of the independent fission product formation cross sections in the spontaneous fission and in the neutron and proton induced fission at the energies up to 100 MeV is developed. This model is a combination of new version of the two-component exciton model and a time-dependent statistical model for fusion-fission process with inclusion of dynamical effects for accurate calculations of nucleon composition and excitation energy of the fissioning nucleus at the scission point. For each member of the compound nucleus ensemble at the scission point, the primary fission fragment characteristics: kinetic and excitation energies and their yields are calculate…

Nuclear fission productCluster decayta114Proton010308 nuclear & particles physicsChemistryFissionPhysicsQC1-999Nuclear TheoryNuclear matter01 natural sciences7. Clean energyNuclear physics0103 physical sciencesPhysics::Atomic and Molecular ClustersNeutronAtomic physicsNuclear Experiment010306 general physicsNucleonSpontaneous fissionEPJ Web of Conferences
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Decay properties of exoticN≃28 S and Cl nuclei and theCa48/46Ca abundance ratio

1993

Beta-decay half-lives and \ensuremath{\beta}-delayed neutron-emission probabilities of the very neutron-rich nuclei $^{44}\mathrm{S}$ and $^{45--47}\mathrm{Cl}$ have been measured. These isotopes, which lie at or close to the N=28 magic shell, were produced in interactions of a 60 MeV/u $^{48}\mathrm{Ca}$ beam from GANIL (Grand Acc\'el\'erateur National d'Ions Lourds) with a $^{64}\mathrm{Ni}$ target, and were separated by the doubly achromatic spectrometer LISE (Ligne d'Ions Super Epluch\'es). Their decay was studied by a \ensuremath{\beta}-n time correlation measurement. The results are compared to recent model predictions and indicate a rapid weakening of the N=28 shell effect below $_{2…

Nuclear physicsBaryonPhysicsNuclear reactionNuclear and High Energy PhysicsHadronNuclear structureIsotopes of chlorineNeutronAtomic physicsNuclear ExperimentNucleonRadioactive decayPhysical Review C
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Local suppression of collectivity in theN=80isotones at theZ=58subshell closure

2013

) transition strengths [1] and thenumber of nucleons in the valence shell. The global behaviorof these quantities between the major shells as a function ofthe nucleon number is well understood in the frameworks ofboth collective and microscopic models. One could expect thatthese general trends in the collective properties between themajorshellsaremodulated bythesubshellstructure.However,it is usually thought that the pairing correlations with anenergy scale of about 2 MeV, smear out and dissolve thesubshell structure as long as the separation energies betweenthe subshells are only about a few hundred keV.The recently observed evolution of the isovectorquadrupole-collective valence-shell exc…

Nuclear physicsMass numberPhysicsNuclear and High Energy PhysicsPairingNuclear TheoryPhysics::Atomic and Molecular ClustersClosure (topology)NucleonValence electronPhysical Review C
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Inclusive Pion Double Charge Exchange on Light Nuclei above 0.5 GeV

1995

Inclusive double charge exchange (DCX) reaction A(π −, π +) X on 6Li and 16O was for the first time measured at incident kinetic energy T 0 = 1.1 GeV ( ≈ 5°) for outgoing particle momentum region where additional pion production is kinematically forbidden. The experiment was performed at secondary π − beam of the ITEP proton synchrotron using the 3m magnet spectrometer. The measured double differential cross section at 1.1 GeV together with our previous results at 0.6 and 0.75 GeV [1] and with the lower energy data [2] and [3] shows rather slow decrease with energy. This result is in contradiction with the fast fall of small angle DCX cross section calculated [4] in the standard mechanism o…

Nuclear physicsMomentumPhysicsRange (particle radiation)PionMesonProton SynchrotronHigh Energy Physics::ExperimentAtomic physicsNuclear ExperimentNucleonKinetic energyGlauber
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Role of statistical fluctuations in the emission ofδelectrons from dissipative heavy-ion collisions

1990

Energy spectra of {delta} electrons emitted in coincidence with deep-inelastic heavy-ion collisions are calculated within a Langevin Monte Carlo description using the surface-friction model. We investigate the effects that wipe out the originally expected oscillatory pattern of the spectra. Emphasis is placed on the role of statistical fluctuations in extracting interaction time distributions of deep-inelastic collisions from the measured {delta}-electron spectra. The calculations are compared to data for U+Au at 8.65 MeV/nucleon.

Nuclear physicsNuclear reactionPhysicsMonte Carlo methodGeneral Physics and AstronomyElementary particleElectronInelastic scatteringAtomic physicsStatistical fluctuationsNuclear ExperimentNucleonLeptonPhysical Review Letters
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Gamow-Teller Transitions and β-decay Half-life in Proton Rich pf-shell Nuclei

2010

In violent neutrino‐induced reactions at the core‐collapse stage of type II supernovae, Gamow‐Teller (GT) transitions starting from stable as well as unstable pf‐shell nuclei play important roles. In the β‐decay study of these unstable pf‐shell nuclei, half‐lives can be measured rather accurately. On the other hand, in high‐resolution (3He,t) charge‐exchange reactions at 0°, individual GT transitions up to high excitations can be studied. Assuming the isospin symmetry for the strengths of Tz = ±2→±1 analogous GT transitions, we present a “merged analysis” for the determination of GT transition strengths starting from proton‐rich Tz = −2 nuclei. We applied this analysis to the A = 52, T = 2 …

Nuclear physicsNuclear reactionPhysicsProtonIsospinNuclear TheoryHadronFermionAtomic physicsNuclear ExperimentNucleonIsotopes of heliumRadioactive decayAIP Conference Proceedings
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