Search results for "21.10.Hw"

showing 6 items of 6 documents

Probing the limit of nuclear existence: Proton emission from 159Re

2006

WOS: 000240847400007

Nuclear reactionNuclear and High Energy PhysicsSi detectorsProtonNuclear Theory[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]measured E (p) (t)1 / 201 natural sciences7. Clean energyNuclear physicsEp0103 physical sciencesEnriched targetsNeutronNuclideProton emissionNuclear Experiment010306 general physics106Cd at 300 MeV beam energyPhysicsIsotope010308 nuclear & particles physics21.10.Hw; 21.10.Tg; 23.50.+z; 27.70.+q58Nit1/2NUCLEAR REACTIONS Ni-58+Cd-106 at 300 MeV beam energy13. Climate actionNuclear reactionsGas-filled recoil separatorAtomic physicsNucleonMeasuredRadioactive decayPhysics Letters B
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The ASY-EOS experiment at GSI: Investigating the symmetry energy at supra-saturation densities

2012

The elliptic-flow ratio of neutrons with respect to protons in reactions of neutron rich heavy-ions systems at intermediate energies has been proposed as an observable sensitive to the strength of the symmetry term in the nuclear Equation Of State (EOS) at supra-saturation densities. The recent results obtained from the existing FOPI/LAND data for $^{197}$Au+$^{197}$Au collisions at 400 MeV/nucleon in comparison with the UrQMD model allowed a first estimate of the symmetry term of the EOS but suffer from a considerable statistical uncertainty. In order to obtain an improved data set for Au+Au collisions and to extend the study to other systems, a new experiment was carried out at the GSI la…

Particle physicsHistoryQC1-999Nuclear TheoryFOS: Physical sciencesand isobaric spin 24.10.Pa Thermal and statistical models[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]EducationNuclear physicsPhysics and Astronomy (all)nuclear physics; heavy-ions; symmetry energy; Au+Au collisionsNeutronNuclear Experiment (nucl-ex)Nuclear ExperimentNuclear ExperimentComputingMilieux_MISCELLANEOUSPhysicssezelePhysicsOrder (ring theory)Nuclear equation of stateObservableNuclear Experiment; Nuclear Experiment21.65.-f Nuclear matter 27.80.+w 190(less-than-or-equal-to)A(less-than-or-equal-to)219 24.60.-k Statistical theory and fluctuations 25.75.Gz Particle correlations and fluctuations 21.10.Hw SpinSymmetry (physics)Term (time)Computer Science ApplicationsparityNuclear reactionsSaturation (chemistry)NucleonEnergy (signal processing)
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Emission of fragments in Ca+Ca reaction at 25 MeV/nucleon

2013

We discuss experimental data concerning 40,48Ca+ 40,48Ca reactions at 25 MeV/nucleon; the 4π multi-detector Chimera has been used as detection device. Effects that can be attributed to the neutron to proton ratios (N/Z) degree of freedom have been investigated. From the analysis of experimental data it seems that the neutron richness of the interacting system plays an important role on the evolution of fusion-like sources formed in semi-central collisions. In particular, it is observed that the larger is the neutron content and the larger is the emission of heavy residues. Experimental data have been compared with CoMD-II model calculations; a moderately stiff symmetry energy should be used…

PhysicsHistoryNuclear Theoryand isobaric spin 24.10.Pa Thermal and statistical modelsComputer Science ApplicationsEducationNuclear physicsPhysics and Astronomy (all)parityIsospin25.75.Gz Particle correlations and fluctuations 21.65.-f Nuclear matter 27.40.+z 39(less-than-or-equal-to)A(less-than-or-equal-to)58 21.10.Hw SpinIsobaric processNeutronAtomic physicsNuclear ExperimentNucleon
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Competing T = 0 and T = 1 structures in the N = Z nucleus $^{62}_{31}$Ga

1998

Abstract The low-lying levels in the odd-odd N = Z nucleus 62 Ga have been identified for the first time. These data reveal a cascade of stretched-E2 transitions based on a T =0, 1 + bandhead which decays directly to the T =1, 0 + ground state. The observed levels are interpreted in the context of theshell model, using as a basis, the pf 5/2 g 9/2 orbits with a 56 Ni core.

PhysicsNuclear and High Energy Physics[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]010308 nuclear & particles physicsSHELL modelNsZContext (language use)Nanotechnology01 natural sciencesShell modelCrystallographymedicine.anatomical_structure21.10.-k; 21.10.Hw; 21.60.Cs; 27.50.qeCascadeIsospin0103 physical sciencesIsospinLevelsmedicine010306 general physicsGround stateNucleus
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Discovery of the proton emitting nucleus $^{159}$Re

2007

Fund. para Cienc. Tecnol., FCT, Minist. Cienc. Tecnol.;Fundacao Calouste Gulbenkian;Fundacao Luso-Americana

Si detectorsnuclear spinMeasured E pProtonHadron02 engineering and technologyrhenium[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]7. Clean energyNuclear physicsIsotopes of cadmium0202 electrical engineering electronic engineering information engineeringnuclei with mass number 150 to 189Enriched targetsradioactive decay periodsNuclideIsotopeChemistryNuclear structure020206 networking & telecommunicationsT1/213. Climate action020201 artificial intelligence & image processing23.50.+z; 27.70.+q; 21.10.Tg; 21.10.HwGas-filled recoil separatorNucleonRadioactive decayNuclear reactions 58Ni + 106Cd at 300 MeV beam energyproton emission decay
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Fission Barrier of Superheavy Nuclei and Persistence of Shell Effects at High Spin: Cases of 254No and 220Th

2014

We report on the first measurement of the fission barrier height in a heavy shell-stabilized nucleus. The fission barrier height of 254No is measured to be Bf=6.0±0.5  MeV at spin 15ℏ and, by extrapolation, Bf=6.6±0.9  MeV at spin 0ℏ. This information is deduced from the measured distribution of entry points in the excitation energy versus spin plane. The same measurement is performed for 220Th and only a lower limit of the fission barrier height can be determined: Bf(I)8  MeV. Comparisons with theoretical fission barriers test theories that predict properties of superheavy elements.

superheavy elements[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]fysiikkaComputingMilieux_MISCELLANEOUS27.90.+b 21.10.Hw 24.60.Dr 24.75.+i
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