The single particle (hole) energies in "1"0"0Sn, as extrapolated by a shell model analysis of the neighbouring nuclei, show a remarkable similarity to those in "3"6Ni, one major shell lower. This is borne out in nearly identical I"#pi#=2"+ excitation energies, implying E(2"+)#approx =#3 MeV in "1"0"0Sn, and a large neutron effective E2 charge #epsilon##>=#1.6#epsilon#. In contrast a small proton polarisation charge #delta##epsilon##<=#0.3#epsilon# is found, pointing to a large isovector charge. Mean field predictions for single particle energies show substantial deviations from the experimental extrapolation. From the experimental two-proton hole spectrum in "9"8Cd an im...
Odd-mass gadolinium isotopes around N = 90 were populated by the (p,d) reaction, utilizing 25-MeV pr...
The monopole effect resulting from the interaction between the magic core and the valence particles ...
One of the most successful descriptions of the structure of atomic nuclei is the spherical shell mo...
The single particle (hole) energies in "1"0"0Sn, as extrapolated by a shell model ana...
The status of experimental approach to "1"0"0Sn and "7"8Ni is reviewed. Rev...
The three neutron-deficient nuclei "9"4Pd, "9"8Cd and "1"0"4Sn in...
The present status of experimental approach to "1"0"0Sn in the spectroscopy of excite...
The spectra of nuclides involving few valence particles or holes far from β¯ stability are important...
Excited states in "9"8Cd, two proton holes from "1"0"0Sn, were identified a...
We perform an analysis of a binding energy difference called δV pn(N,Z)-14[E(Z,N)-E(Z,N-2)-E(Z-2,N)+...
Atomic nuclei are finite quantum systems composed of two distinct types of fermion--protons and neut...
Atomic nuclei are finite quantum systems composed of two distinct types of fermion - protons and neu...
We perform an analysis of a binding energy difference called δVpn(N,Z)≡-1/4[E(Z,N)-E(Z,N-2)-E(Z-2,N)...
The structure of atomic nuclei depends on the interactions of its constituents, protons and neutrons...
International audienceIt has been shown that the neutron 2d5/2 orbital has to be included in shell-m...
Odd-mass gadolinium isotopes around N = 90 were populated by the (p,d) reaction, utilizing 25-MeV pr...
The monopole effect resulting from the interaction between the magic core and the valence particles ...
One of the most successful descriptions of the structure of atomic nuclei is the spherical shell mo...
The single particle (hole) energies in "1"0"0Sn, as extrapolated by a shell model ana...
The status of experimental approach to "1"0"0Sn and "7"8Ni is reviewed. Rev...
The three neutron-deficient nuclei "9"4Pd, "9"8Cd and "1"0"4Sn in...
The present status of experimental approach to "1"0"0Sn in the spectroscopy of excite...
The spectra of nuclides involving few valence particles or holes far from β¯ stability are important...
Excited states in "9"8Cd, two proton holes from "1"0"0Sn, were identified a...
We perform an analysis of a binding energy difference called δV pn(N,Z)-14[E(Z,N)-E(Z,N-2)-E(Z-2,N)+...
Atomic nuclei are finite quantum systems composed of two distinct types of fermion--protons and neut...
Atomic nuclei are finite quantum systems composed of two distinct types of fermion - protons and neu...
We perform an analysis of a binding energy difference called δVpn(N,Z)≡-1/4[E(Z,N)-E(Z,N-2)-E(Z-2,N)...
The structure of atomic nuclei depends on the interactions of its constituents, protons and neutrons...
International audienceIt has been shown that the neutron 2d5/2 orbital has to be included in shell-m...
Odd-mass gadolinium isotopes around N = 90 were populated by the (p,d) reaction, utilizing 25-MeV pr...
The monopole effect resulting from the interaction between the magic core and the valence particles ...
One of the most successful descriptions of the structure of atomic nuclei is the spherical shell mo...