AbstractThe available experimental data on shell evolution indicate that the strength of the spin–orbit single-particle potential may be enhanced in neutron-rich nuclei. We observe that such a simple scheme destroys the harmonic oscillator magic numbers N=8 and 20 and generates new magic numbers like N=6, 14, 16, 32 and 34. The traditional magic numbers like N=28 and 50 and N=14 seen in 22O are eroded in neutron-rich nuclei due to the sensitivity of larger-l orbitals to the depth of the central potential but they are more robust than the harmonic oscillator magic numbers. The N=82 shell closure persists in neutron-rich nuclei while the previously proposed shell closures like N=40 and 70 do not emerge. Both mechanisms contribute to enhancing...
Low-lying high-spin yrast states in the exotic odd–odd isotopes 124–128Sb (Z=51) and 118–128In (Z=49...
AbstractLow-lying high-spin yrast states in the exotic odd–odd isotopes 124–128Sb (Z=51) and 118–128...
The breaking of the isospin symmetry is discussed from the point of view of the nuclear shell-model....
AbstractThe available experimental data on shell evolution indicate that the strength of the spin–or...
40 pages,15 figures, Procceedings Nobel Symposium 2012, accepted for publication in Physica ScriptaI...
We present a quantitative study of the role played by different components characterizing the nucleo...
We report on a quantitative study of the evolution of the nuclear shell structure, in particular, ef...
ReviewThe main purpose of the present manuscript is to review the structural evolution along the iso...
International audienceRecent advances in Large Shell Model calculations allow now to treat extended ...
By the use of the latest experimental data on the spectra of $^{133}$Sb and $^{131}$Sn and on the an...
International audienceThe atomic nucleus is a quantum many-body system whose constituent nucleons (p...
AbstractThe behaviour of the i13/2 and h9/2 single-neutron strength was studied with the (α,He3) rea...
International audienceThe N=28 shell closure is the first arising from the strong spin-orbit interac...
In the framework of the shell model, the evolution of the single particle states with the N/Z ratio ...
The behaviour of the i13 / 2 and h9 / 2 single-neutron strength was studied with the (α, 3He) reacti...
Low-lying high-spin yrast states in the exotic odd–odd isotopes 124–128Sb (Z=51) and 118–128In (Z=49...
AbstractLow-lying high-spin yrast states in the exotic odd–odd isotopes 124–128Sb (Z=51) and 118–128...
The breaking of the isospin symmetry is discussed from the point of view of the nuclear shell-model....
AbstractThe available experimental data on shell evolution indicate that the strength of the spin–or...
40 pages,15 figures, Procceedings Nobel Symposium 2012, accepted for publication in Physica ScriptaI...
We present a quantitative study of the role played by different components characterizing the nucleo...
We report on a quantitative study of the evolution of the nuclear shell structure, in particular, ef...
ReviewThe main purpose of the present manuscript is to review the structural evolution along the iso...
International audienceRecent advances in Large Shell Model calculations allow now to treat extended ...
By the use of the latest experimental data on the spectra of $^{133}$Sb and $^{131}$Sn and on the an...
International audienceThe atomic nucleus is a quantum many-body system whose constituent nucleons (p...
AbstractThe behaviour of the i13/2 and h9/2 single-neutron strength was studied with the (α,He3) rea...
International audienceThe N=28 shell closure is the first arising from the strong spin-orbit interac...
In the framework of the shell model, the evolution of the single particle states with the N/Z ratio ...
The behaviour of the i13 / 2 and h9 / 2 single-neutron strength was studied with the (α, 3He) reacti...
Low-lying high-spin yrast states in the exotic odd–odd isotopes 124–128Sb (Z=51) and 118–128In (Z=49...
AbstractLow-lying high-spin yrast states in the exotic odd–odd isotopes 124–128Sb (Z=51) and 118–128...
The breaking of the isospin symmetry is discussed from the point of view of the nuclear shell-model....