{"paper":{"title":"Effects of $N(2000)\\, 5/2^+$, $N(2060)\\,5/2^-$, $N(2120)\\,3/2^-$, and $N(2190)\\,7/2^-$ on $K^*\\Lambda$ photoproduction","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","nucl-ex","nucl-th"],"primary_cat":"hep-ph","authors_text":"Atsushi Hosaka, Hyun-Chul Kim, Sang-Ho Kim","submitted_at":"2014-02-07T20:33:48Z","abstract_excerpt":"We reinvestigate $K^*\\Lambda(1116)$ photoproduction off the nucleon target, based on an effective Lagrangian approach. We include higher nucleon resonances such as $N(2000)\\, 5/2^+$, $N(2060)\\,5/2^-$, $N(2120)\\,3/2^-$, and $N(2190)\\,7/2^-$, of which the data are taken from the 2012 edition of Review of Paritcle Physics, in addition to the $t$-channel diagrams ($K$, $K^*$, and $\\kappa$), the $s$-channel nucleon, and $u$-channel hyperon($\\Lambda$, $\\Sigma$, and $\\Sigma^*$) contributions. We find that the $N(2120)\\,3/2^-$ and $N(2190)\\,7/2^-$ resonances are essential in describing the new CLAS da"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1402.1753","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"}