Search results for "Nucleon"

showing 10 items of 1041 documents

Measurement of high energy resolution inelastic proton scattering at and close to zero degrees

2009

13 pages, 15 figures.-- Printed version published Jul 1, 2009.

Nuclear and High Energy PhysicsHigh energy resolutionM1 excitationForward scatterCyclotronMeasurement at 0 degreesTRANSITIONSInelastic scatteringDispersion matchingISOVECTORlaw.inventionSHELL NUCLEINuclear physicsNUCLEON-NUCLEON INTERACTIONlawBEAM LINEE1 Coulomb excitationFOCAL-PLANE POLARIMETERInstrumentationInelastic proton scatteringPolarization transfer coefficientsISOSCALARElastic scatteringPhysicsBackground subtractionPolarization transfer coefficientScatteringResolution (electron density)SPIN EXCITATIONSBeamlinePhysics::Accelerator PhysicsMeasurement at 0ºAtomic physicsSPECTROMETER GRAND RAIDENINTERMEDIATE ENERGIES
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Prompt D0, D+, and D*+ production in Pb–Pb collisions at √sNN = 5.02 TeV

2022

The production of prompt D0, D+, and D*+ mesons was measured at midrapidity (|y| < 0.5) in Pb–Pb collisions at the centre-of-mass energy per nucleon–nucleon pair √sNN = 5.02 TeV with the ALICE detector at the LHC. The D mesons were reconstructed via their hadronic decay channels and their production yields were measured in central (0–10%) and semicentral (30–50%) collisions. The measurement was performed up to a transverse momentum (pT) of 36 or 50 GeV/c depending on the D meson species and the centrality interval. For the first time in Pb–Pb collisions at the LHC, the yield of D0 mesons was measured down to pT = 0, which allowed a model-independent determination of the pT-integrated yield …

Nuclear and High Energy PhysicsLepton-Nucleon Scattering (experiments)High Energy Physics::PhenomenologyNuclear TheoryHigh Energy Physics::ExperimenthiukkasfysiikkaNuclear Experiment
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Pairing-quadrupole interplay in the neutron-deficient tin nuclei: First lifetime measurements of low-lying states in 106,108Sn

2020

The lifetimes of the low-lying excited states 2(+) and 4(+) have been directly measured in the neutron-deficient Sn-106,Sn-108 isotopes. the nuclei were populated via a deep-inelastic reaction and the lifetime measurement was performed employing a differential plunger device. the emitted gamma rays were detected by the AGATA array, while the reaction products were uniquely identified by the VAMOS++ magnetic spectrometer. Large-Scale Shell-Model calculations with realistic forces indicate that, independently of the pairing content of the interaction, the quadrupole force is dominant in the B(E2; 2(1)(+) -> 0(g.s)(+)) values and it describes well the experimental pattern for Sn104-114 ; the B…

Nuclear and High Energy PhysicsLight Snchemistry.chemical_elementFOS: Physical sciences[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]nucl-ex01 natural sciencesSubatomär fysikLifetime; Light Sn; Multi-nucleon transfer; Nuclear structure; Tracking array0103 physical sciencesSubatomic PhysicsNeutronTracking arrayNuclear Physics - ExperimentNuclear structureNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentPhysicsSpectrometerIsotopeLifetime ; Nuclear structure ; Multi-nucleon transfer ; Light Sn ; Tracking array010308 nuclear & particles physicsPhysicsMulti-nucleon transferlcsh:QC1-999chemistryPairingExcited stateQuadrupoleAGATAAtomic physicsTinlcsh:PhysicsLifetime
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Large-angle production of charged pions with 3-12.9 GeV/c incident protons on nuclear targets

2008

Measurements of the double-differential pi(+/-) production cross section in the momentum range 100 <= p <= 800 MeV/c and angle range 0.35 <= theta <= 2.15 rad in proton-beryllium, proton-carbon, proton-aluminium, proton-copper, proton-tin, proton-tantalum, and proton-lead collisions are presented. The data were taken with the large-acceptance HARP detector in the T9 beam line of the CERN PS. The pions were produced by proton beams in a momentum range from 3 to 12.9 GeV/c hitting a target with a thickness of 5% of a nuclear interaction length. Tracking and identification of the produced particles was performed by using a small-radius cylindrical Time Projection Chamber (TPC) placed inside a …

Nuclear and High Energy PhysicsMesonProtonPhysics::Instrumentation and DetectorsHadronNuclear TheoryFOS: Physical sciencesddc:500.27. Clean energy01 natural sciencesParticle detectorHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Nuclear interaction length010306 general physicsNuclear ExperimentPhysicsTime projection chamber010308 nuclear & particles physicsSettore FIS/01 - Fisica SperimentaleFísicaCharged particlePhysics::Accelerator PhysicsHigh Energy Physics::ExperimentAtomic physicsNucleonParticle Physics - Experiment
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Shell evolution of $N=40$ isotones towards $^{60}$Ca: First spectroscopy of $^{62}$Ti

2020

7 pags., 4 figs., 1 tab.

Nuclear and High Energy PhysicsNuclear TheoryNuclear TheoryAb initioFOS: Physical sciencesShell evolution[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]7. Clean energy01 natural sciencesShell evolution ; Radioactive beams ; Gamma-ray spectroscopyNuclear Theory (nucl-th)Gamma-ray spectroscopy; Radioactive beams; Shell evolution0103 physical sciencesddc:530Gamma-ray spectroscopyNuclear Experiment (nucl-ex)010306 general physicsSpectroscopyNuclear ExperimentNuclear ExperimentPhysics010308 nuclear & particles physicsIsland of inversionIsotonePhysicsStarke Wechselwirkung und exotische Kerne – Abteilung BlaumFísicalcsh:QC1-999Excited stateQuadrupoleAtomic physicsNucleonGround statelcsh:PhysicsRadioactive beams
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A first estimate of $\eta/s$ in Au+Au reactions at E$_{\rm lab}=1.23$ $A$GeV

2020

The HADES experiment at GSI has recently provided data on the flow coefficients $v_1,...,v_4$ for protons in Au+Au reactions at $E_{\rm lab} = 1.23$~$A$GeV (or $\sqrt{s_\mathrm{NN}}=2.4$ GeV). This data allows to estimate the shear viscosity over entropy ratio, $\eta/s$ at low energies via a coarse graining analysis of the UrQMD transport simulations of the flow harmonics in comparison to the experimental data. By this we can provide for the first time an estimate of $\eta/s\approx0.65\pm0.15$ (or $(8\pm2)\,(4\pi)^{-1}$) at such low energies.

Nuclear and High Energy PhysicsNuclear TheoryQC1-999relativistic [quantum molecular dynamics]hiukkasfysiikka7. Clean energy01 natural sciencesNuclear physicsscattering [heavy ion]low [energy]0103 physical sciencestransport theoryddc:530numerical calculations010306 general physicsNuclear ExperimentNuclear theoryNuclear Experiment1.23 GeV/nucleonPhysicsdensity010308 nuclear & particles physicsPhysicsShear viscosityrelativistic heavy ion collisionsEntropy densityHADESflowHarmonicsviscosityHigh Energy Physics::ExperimentGranularityentropy
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Is Seniority a Partial Dynamic Symmetry in the First $\nu g_{9/2}$ Shell?

2018

The low-lying structures of the midshell νg9/2 Ni isotopes 72Ni and 74Ni have been investigated at the RIBF facility in RIKEN within the EURICA collaboration. Previously unobserved low-lying states were accessed for the first time following β decay of the mother nuclei 72Co and 74Co. As a result, we provide a complete picture in terms of the seniority scheme up to the first (8+) levels for both nuclei. The experimental results are compared to shell-model calculations in order to define to what extent the seniority quantum number is preserved in the first neutron g9/2 shell. We find that the disappearance of the seniority isomerism in the (81+) states can be explained by a lowering of the se…

Nuclear and High Energy PhysicsNuclear Theory[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]Hadron[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciences29.30.Kv23.40.-sNuclear physics21.60.Cs0103 physical sciencesNeutronSeniority[ PHYS.NEXP ] Physics [physics]/Nuclear Experiment [nucl-ex]010306 general physicsNuclear Experiment[ PHYS.NUCL ] Physics [physics]/Nuclear Theory [nucl-th]Spin-½Physics010308 nuclear & particles physics23.20.LvFermionQuantum numberlcsh:QC1-999Atomic physicsNucleonlcsh:PhysicsRadioactive decay
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Isospin mixing and the continuum coupling in weakly bound nuclei

2009

The isospin breaking effects due to the Coulomb interaction in weakly-bound nuclei are studied using the Gamow Shell Model, a complex-energy configuration interaction approach which simultaneously takes into account many-body correlations between valence nucleons and continuum effects. We investigate the near-threshold behavior of one-nucleon spectroscopic factors and the structure of wave functions along an isomultiplet. Illustrative calculations are carried out for the T=1 isobaric triplet. By using a shell-model Hamiltonian consisting of an isoscalar nuclear interaction and the Coulomb term, we demonstrate that for weakly bound or unbound systems the structure of isobaric analog states v…

Nuclear and High Energy PhysicsNuclear Theory[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]IsoscalarNuclear TheoryFOS: Physical sciences01 natural sciencesNuclear Theory (nucl-th)symbols.namesakeQuantum mechanics0103 physical sciencesCoulombSymmetry breakingMirror nucleiNuclear Experiment010306 general physicsWave functionPhysics010308 nuclear & particles physics3. Good healthIsospinsymbols21.10.Sf 21.60.Cs 24.10.Cn 21.10.JxAtomic physicsHamiltonian (quantum mechanics)Nucleon
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Electromagnetic moments of scandium isotopes and $N=28$ isotones in the distinctive $0f_{7/2}$ orbit

2022

The electric quadrupole moment of $^{49}$Sc was measured by collinear laser spectroscopy at CERN-ISOLDE to be $Q_{\rm s}=-0.159(8)$ $e$b, and a nearly tenfold improvement in precision was reached for the electromagnetic moments of $^{47,49}$Sc. The single-particle behavior and nucleon-nucleon correlations are investigated with the electromagnetic moments of $Z=21$ isotopes and $N=28$ isotones as valence neutrons and protons fill the distinctive $0f_{7/2}$ orbit, respectively, located between magic numbers, 20 and 28. The experimental data are interpreted with shell-model calculations using an effective interaction, and ab-initio valence-space in-medium similarity renormalization group calcu…

Nuclear and High Energy PhysicsNuclear Theorynucl-thCollinear laser spectroscopyNuclear TheoryFOS: Physical sciencesAstronomy & Astrophysicsnucl-exComputer Science::Digital LibrariesPhysics Particles & FieldsElectromagnetic momentsNuclear Theory (nucl-th)Nuclear Physics - ExperimentNuclear Experiment (nucl-ex)Nuclear ExperimentNuclear ExperimentisotoopitScience & TechnologyPhysicsNUCLEAR MOMENTSQUADRUPOLE-MOMENTSPhysics NuclearNucleon-nucleon correlationNuclear Physics - TheoryPhysical SciencesSHELL-MODELCOLLECTIVITYPräzisionsexperimente - Abteilung BlaumydinfysiikkaskandiumAb-initio calculation
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Weak kaon production off the nucleon and Watson's theorem

2021

We have improved the tree-level model of Ref arXiv:1004.5484 [hep-ph] for weak production of kaons off nucleons by partially restoring unitarity. This is achieved by imposing Watson's theorem to the dominant vector and axial-vector contributions in appropriate angular momentum and isospin quantum number sectors. The observable consequences of this procedure are investigated.

Nuclear and High Energy PhysicsParticle physicsAngular momentumNuclear TheoryQC1-999Nuclear TheoryFOS: Physical sciences01 natural sciencesHigh Energy Physics - ExperimentNuclear Theory (nucl-th)High Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)0103 physical sciencesNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentNuclear ExperimentPhysicsUnitarity010308 nuclear & particles physicsWatsonPhysicsHigh Energy Physics::PhenomenologyObservableQuantum numberHigh Energy Physics - PhenomenologyIsospinProduction (computer science)NucleonPhysics Letters B
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