{ "id": "nucl-th/0612022", "version": "v1", "published": "2006-12-05T22:32:59.000Z", "updated": "2006-12-05T22:32:59.000Z", "title": "No-Core shell model for A = 47 and A = 49", "authors": [ "J. P. Vary", "A. G. Negoita", "S. Stoica" ], "comment": "17 pages including 14 figures", "categories": [ "nucl-th" ], "abstract": "We apply an {\\it ab-initio} approach to the nuclear structure of odd-mass nuclei straddling $^{48}Ca$. Starting with the NN interaction, that fits two-body scattering and bound state data we evaluate the nuclear properties of $A = 47$ and $A = 49$ nuclei in a no-core approach. Due to model space limitations and the absence of 3-body interactions, we incorporate phenomenological terms determined by fits to $A = 48$ nuclei in a previous effort. Our modified Hamiltonian produces reasonable spectra for these odd mass nuclei. In addition to the differences in single-particle basis states, the absence of a single-particle Hamiltonian in our no-core approach obscures direct comparisons with valence effective NN interactions. Nevertheless, we compare the fp-shell matrix elements of our initial and modified Hamiltonians in the harmonic oscillator basis with a recent model fp-shell interaction, the GXPF1 interaction of Honma, Otsuka, Brown and Mizusaki. Notable differences emerge from these comparisons. In particular, our diagonal two-body $T = 0$ matrix elements are, on average, about 800-900keV more attractive. Furthermore, while our initial and modified NN Hamiltonian fp-shell matrix elements are strongly correlated, there is much less correlation with the GXPF1 matrix elements.", "revisions": [ { "version": "v1", "updated": "2006-12-05T22:32:59.000Z" } ], "analyses": { "keywords": [ "no-core shell model", "hamiltonian produces reasonable spectra", "no-core approach obscures direct comparisons", "interaction", "nn hamiltonian fp-shell matrix elements" ], "note": { "typesetting": "TeX", "pages": 17, "language": "en", "license": "arXiv", "status": "editable", "inspire": 733653, "adsabs": "2006nucl.th..12022V" } } }