{ "id": "1504.02594", "version": "v1", "published": "2015-04-10T09:05:16.000Z", "updated": "2015-04-10T09:05:16.000Z", "title": "Proton and neutron correlations in $^{10}$B", "authors": [ "Yoshiko Kanada-En'yo", "Hiroyuki Morita", "Fumiharu Kobayashi" ], "comment": "12 pages 9 figures", "categories": [ "nucl-th" ], "abstract": "We investigate positive-parity states of $^{10}$B with the calculation of antisymmetrized molecular dynamics focusing on $pn$ pair correlations. We discuss effects of the spin-orbit interaction on energy spectra and $pn$ correlations of the $J^\\pi T=1^+_10$, $=3^+_10$, and $0^+_11$ states. The $1^+_10$ state has almost no energy gain of the spin-orbit interaction, whereas the $3^+_10$ state gains the spin-orbit interaction energy largely to come down to the ground state. We interpret a part of the two-body spin-orbit interaction in the adopted effective interactions as a contribution of the genuine $NNN$ force, and find it to be essential for the level ordering of the $3^+_10$ and $1^+_10$ states in $^{10}$B. We also apply a $2\\alpha+pn$ model to discuss effects of the spin-orbit interaction on $T=0$ and $T=1$ $pn$ pairs around the 2$\\alpha$ core. In the spin-aligned $J^\\pi T=3^+0$ state, the spin-orbit interaction affects the $(ST)=(10)$ pair attractively and keeps the pair close to the core, whereas, in the $1^+0$ state, it gives a minor effect to the $(ST)=(10)$ pair. In the $0^+1$ state, the $(ST)=(01)$ pair is somewhat dissociated by the spin-orbit interaction.", "revisions": [ { "version": "v1", "updated": "2015-04-10T09:05:16.000Z" } ], "analyses": { "subjects": [ "21.10.-k", "21.30.Fe", "21.60.Gx", "27.20.+n" ], "keywords": [ "neutron correlations", "two-body spin-orbit interaction", "spin-orbit interaction affects", "spin-orbit interaction energy", "minor effect" ], "publication": { "doi": "10.1103/PhysRevC.91.054323" }, "note": { "typesetting": "TeX", "pages": 12, "language": "en", "license": "arXiv", "status": "editable", "inspire": 1358970 } } }