0000000000345428

AUTHOR

R. S. Slepnev

showing 5 related works from this author

T=5/2 states in 9Li: Isobaric analog states of 9He

2003

The thick target inverse kinematic method was applied to the study of isobaric analog states in the neutron-rich nucleus 9Li. For this purpose, an excitation function for 8He+p elastic scattering was measured in the center-of-momentum energy range from 1.6 to 5.8 MeV. Three T=5/2 states in 9Li (isobaric analogs of 9He) were observed. Restrictions on the spin-parity assignments are provided according to R-matrix calculations, and conclusions regarding the structure of 9He are given. peerReviewed

nuclear physicsNuclear TheoryNuclear Experimentydinfysiikka
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Structure of exotic 7He and 9He

2004

The heavy helium isotopes 7,9 He were studied via their isobaric analog states (IAS) in 7,9 Li. The IAS were populated via resonance reactions of protons with radioactive beams of 6,8 He. The isospin-conserving neutron decay of T=3/2 resonances in 7 Li and proton decay of T=5/2 resonances in 9 Li were measured. New spectroscopic information on these states were obtained, and compared with the properties of levels in 7,9 He.

Nuclear physicsPhysicsNuclear and High Energy PhysicsProton decayNuclear TheoryIsobaric processResonanceNeutronAtomic physicsNuclear ExperimentIsotopes of heliumNuclear Physics A
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T=5/2states in9Li:Isobaric analog states of9He

2003

The thick target inverse kinematic method was applied to the study of isobaric analog states in the neutron-rich nucleus ${}^{9}\mathrm{Li}.$ For this purpose, an excitation function for ${}^{8}\mathrm{He}+p$ elastic scattering was measured in the center-of-momentum energy range from 1.6 to 5.8 MeV. Three $T=5/2$ states in ${}^{9}\mathrm{Li}$ (isobaric analogs of ${}^{9}\mathrm{He})$ were observed. Restrictions on the spin-parity assignments are provided according to R-matrix calculations, and conclusions regarding the structure of ${}^{9}\mathrm{He}$ are given.

Excitation functionPhysicsElastic scatteringNuclear and High Energy PhysicsNuclear TheoryInverseIsobaric processAtomic physicsNuclear ExperimentEnergy (signal processing)Physical Review C
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Lifetime of 26S and a limit for its 2p decay energy

2010

Unknown isotope 26S, expected to decay by two-proton (2p) emission, was studied theoretically and was searched experimentally. The structure of this nucleus was examined within the relativistic mean field (RMF) approach. A method for taking into account the many-body structure in the three-body decay calculations was developed. The results of the RMF calculations were used as an input for the three-cluster decay model worked out to study a possible 2p decay branch of this nucleus. The experimental search for 26S was performed in fragmentation reactions of a 50.3 A MeV 32S beam. No events of 26S or 25P (a presumably proton-unstable subsystem of 26S) were observed. Based on the obtained produ…

PhysicsNuclear and High Energy PhysicsIsotopeNuclear TheoryGeneral Physics and AstronomyFOS: Physical sciencesMain branchNuclear physicsmedicine.anatomical_structureMean field theoryFragmentation (mass spectrometry)Decay energyPicosecondmedicineNuclear Experiment (nucl-ex)Nuclear ExperimentNuclear ExperimentNucleus
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Isobaric analog states as a tool for spectroscopy of exotic nuclei

2005

Abstract Spectroscopy of neutron rich exotic isotopes via their isobaric analog states (IAS) in less exotic nuclei is discussed. Several different experimental techniques, which can be applied to search for IAS of exotic isotopes, are described. Successful application of these techniques to the studies of heavy helium isotopes 7 He and 9 He led to the observation of unknown IAS in 7 Li and 9 Li. Spectroscopic information for these states were obtained, and implication of these findings to the structure of 7,9 He is considered.

Elastic scatteringNuclear physicsNuclear reactionNuclear and High Energy PhysicsIsotopeChemistryIsobaric processNeutronAtomic physicsNuclear ExperimentSpectroscopyInstrumentationIsotopes of heliumNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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