{"paper":{"title":"Complete set of polarization transfer observables for the ${}^{16}{\\rm O}(\\vec{p},\\vec{n}){}^{16}{\\rm F}$ reaction at 296 MeV and 0 degrees","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-ex","authors_text":"H. Okamura, K. Hatanaka, M. Dozono, M. Ichimura, M. Okamoto, M. Takaki, T. Noro, T. Wakasa, Y. Sakemi","submitted_at":"2011-05-12T12:41:59Z","abstract_excerpt":"We report measurements of the cross section and a complete set of polarization transfer observables for the ${}^{16}{\\rm O}(\\vec{p},\\vec{n}){}^{16}{\\rm F}$ reaction at a bombarding energy of $T_p$ = 296 MeV and a reaction angle of $\\theta_{\\rm lab}$ = $0^{\\circ}$.\n  The data are compared with distorted-wave impulse approximation calculations employing the large configuration-space shell-model (SM) wave functions.\n  The well-known Gamow-Teller and spin-dipole (SD) states at excitation energies of $E_x$ $\\lesssim$ 8 MeV have been reasonably reproduced by the calculations except for the spin--par"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1105.2449","kind":"arxiv","version":2},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"}