AbstractLow-lying high-spin yrast states in the exotic odd–odd isotopes 124–128Sb (Z=51) and 118–128In (Z=49), studied for the first time, show a striking difference in their observed γ-ray decay. With a single valence proton particle/hole occupying the g7/2/g9/2 spin-orbit partners, dominant electric quadrupole transitions occur in Sb as opposed to magnetic dipole transitions in In. The observed properties are explained on the basis of general principles of symmetry and with large-scale shell-model calculations, and reveal novel aspects of the competition between the neutron–proton interaction and the like-nucleon pairing interaction
International audienceBackground: The Z=50 shell closure, near N=82, is unique in the sense that it ...
International audienceBackground: The Z=50 shell closure, near N=82, is unique in the sense that it ...
International audienceBackground: The Z=50 shell closure, near N=82, is unique in the sense that it ...
Low-lying high-spin yrast states in the exotic odd–odd isotopes 124–128Sb (Z=51) and 118–128In (Z=49...
Expérience GANIL/VAMOS/EXOGAMInternational audienceLow-lying high-spin yrast states in the exotic od...
Expérience GANIL/VAMOS/EXOGAMInternational audienceLow-lying high-spin yrast states in the exotic od...
Expérience GANIL/VAMOS/EXOGAMInternational audienceLow-lying high-spin yrast states in the exotic od...
Expérience GANIL/VAMOS/EXOGAMInternational audienceLow-lying high-spin yrast states in the exotic od...
AbstractLow-lying high-spin yrast states in the exotic odd–odd isotopes 124–128Sb (Z=51) and 118–128...
Expérience GANIL/VAMOS/EXOGAMInternational audienceLow-lying high-spin yrast states in the exotic od...
Low-lying high-spin yrast states in the exotic odd–odd isotopes 124–128Sb (Z=51) and 118–128In (Z=49...
Background: The Z=50 shell closure, near N=82, is unique in the sense that it is the only shell clos...
International audienceBackground: The Z=50 shell closure, near N=82, is unique in the sense that it ...
International audienceBackground: The Z=50 shell closure, near N=82, is unique in the sense that it ...
International audienceBackground: The Z=50 shell closure, near N=82, is unique in the sense that it ...
International audienceBackground: The Z=50 shell closure, near N=82, is unique in the sense that it ...
International audienceBackground: The Z=50 shell closure, near N=82, is unique in the sense that it ...
International audienceBackground: The Z=50 shell closure, near N=82, is unique in the sense that it ...
Low-lying high-spin yrast states in the exotic odd–odd isotopes 124–128Sb (Z=51) and 118–128In (Z=49...
Expérience GANIL/VAMOS/EXOGAMInternational audienceLow-lying high-spin yrast states in the exotic od...
Expérience GANIL/VAMOS/EXOGAMInternational audienceLow-lying high-spin yrast states in the exotic od...
Expérience GANIL/VAMOS/EXOGAMInternational audienceLow-lying high-spin yrast states in the exotic od...
Expérience GANIL/VAMOS/EXOGAMInternational audienceLow-lying high-spin yrast states in the exotic od...
AbstractLow-lying high-spin yrast states in the exotic odd–odd isotopes 124–128Sb (Z=51) and 118–128...
Expérience GANIL/VAMOS/EXOGAMInternational audienceLow-lying high-spin yrast states in the exotic od...
Low-lying high-spin yrast states in the exotic odd–odd isotopes 124–128Sb (Z=51) and 118–128In (Z=49...
Background: The Z=50 shell closure, near N=82, is unique in the sense that it is the only shell clos...
International audienceBackground: The Z=50 shell closure, near N=82, is unique in the sense that it ...
International audienceBackground: The Z=50 shell closure, near N=82, is unique in the sense that it ...
International audienceBackground: The Z=50 shell closure, near N=82, is unique in the sense that it ...
International audienceBackground: The Z=50 shell closure, near N=82, is unique in the sense that it ...
International audienceBackground: The Z=50 shell closure, near N=82, is unique in the sense that it ...
International audienceBackground: The Z=50 shell closure, near N=82, is unique in the sense that it ...