Phys.Rev. C 92, 024314 (2015)

G.Co, V.De Donno, M.Anguiano, R.N.Bernard, A.M.Lallena

Electric quadrupole and magnetic dipole moments of odd nuclei near the magic ones in a self-consistent approach

NUCLEAR STRUCTURE ^16,22,24O, ^40,48,60Ca, ⁹⁰Zr, ^100,132Sn, ²⁰⁸Pb; calculated energies and B(E2) of first 2+ states, energies and B(M1) of low-lying 1+ states using D1M and D1S Gogny interactions, and comparison with experimental data. Hartree-Fock and random phase approximation (RPA) calculations.

NUCLEAR MOMENTS ^15,21,23N, ^17,23,25F, ^{15,17,21,23,25}O, ^39,47,59K, ^41,49,61Sc, ^{39,41,47,49,59,61}Ca, ⁸⁹Y, ⁹¹Nb, ^89,91Zr, ^99,131In, ^101,133Sb, ^{99,101,131,133}Sn, ²⁰⁷Tl, ²⁰⁹Bi, ^207,209Pb; calculated magnetic dipole and electric quadrupole moments of ground states and in some cases excited states using D1M and D1S Gogny interactions and ^16,22,24O, ^40,48,60Ca, ⁹⁰Zr, ^100,132Sn, ²⁰⁸Pb as core nuclei and associated single-particle states. Hartree-Fock random phase approximation (RPA), independent particle model (IPM) first-order perturbation theory, and finite Fermi systems (FFS) calculations.

doi: 10.1103/PhysRevC.92.024314