1997/09/05 by J. Suhonen, J. Toivanen, A. Holt +3 · 1 citation
Physics and Astronomy · #nucl-th
paper · pdf · doi:10.1016/s0375-9474(97)00615-5
published as Nucl.Phys. A628 (1998) 41-61 · Elsevier latex style espart, 26 pages, submitted to Nuclear Physics A
arxiv created 1997/09/05 · arxiv updated 2009/12/01
The microscopic quasiparticle-phonon model, MQPM, is used to study the energy spectra of the odd Z=53 - 63, N=82 isotones. The results are compared with experimental data, with the extreme quasiparticle-phonon limit and with the results of an unrestricted 2s1d0g7/20h11/2 shell model (SM) calculation. The interaction used in these calculations is a realistic two-body G-matrix interaction derived from modern meson-exchange potential models for the nucleon-nucleon interaction. For the shell model all the two-body matrix elements are renormalized by the Q-box method whereas for the MQPM the effective interaction is defined by the G-matrix.