{"paper":{"title":"New pathway to bypass the 15O waiting point","license":"","headline":"","cross_cats":[],"primary_cat":"nucl-ex","authors_text":"A. Buta, A. Coc, A. Lefebvre-Schuhl, C. Stodel, D. Pantelica, E. Berthoumieux, F. de Oliveira Santos, F. Negoita, G. Dumitru, I. Ray, I. Stefan, J.C. Ang\\'elique, J.C. Thomas, J. Kiener, J.M. Daugas, L. Perrot, M. Ang\\'elique, M. Fadil, M.G. Pellegriti, M.G. Saint Laurent, M. Lenhardt, M. Lewitowicz, M. Stanoiu, O. Roig, O. Sorlin, R. Borcea, S. Gr\\'evy, T. Davinson, V. Tatischeff","submitted_at":"2006-03-22T12:50:51Z","abstract_excerpt":"We propose the sequential reaction process $^{15}$O($p$,$\\gamma)(\\beta^{+}$)$^{16}$O as a new pathway to bypass of the $^{15}$O waiting point. This exotic reaction is found to have a surprisingly high cross section, approximately 10$^{10}$ times higher than the $^{15}$O($p$,$\\beta^{+}$)$^{16}$O. These cross sections were calculated after precise measurements of energies and widths of the proton-unbound $^{16}$F low lying states, obtained using the H($^{15}$O,p)$^{15}$O reaction. The large $(p,\\gamma)(\\beta^{+})$ cross section can be understood to arise from the more efficient feeding of the lo"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"nucl-ex/0603020","kind":"arxiv","version":3},"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"}