{"paper":{"title":"New Results from the Studies of the $N(1440)1/2^+$, $N(1520)3/2^-$, and $\\Delta(1620)1/2^-$ Resonances in Exclusive $ep \\to e'p' \\pi^+ \\pi^-$ Electroproduction with the CLAS Detector","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"nucl-ex","authors_text":"B.S.Ishkhanov, D.S.Carman, E.L.Isupov, E.N.Golovatch, G.V.Fedotov, Iu.Skorodumina, K.Hicks, L.Elouadrhiri, R.W.Gothe, V.D.Burkert, V.I.Mokeev","submitted_at":"2015-09-17T22:14:52Z","abstract_excerpt":"The transition helicity amplitudes from the proton ground state to the $N(1440)1/2^+$, $N(1520)3/2^-$, and $\\Delta(1620)1/2^-$ resonances ($\\gamma_vpN^*$ electrocouplings) were determined from the analysis of nine independent one-fold differential $\\pi^+ \\pi^- p$ electroproduction cross sections off a proton target, taken with CLAS at photon virtualities 0.5 GeV$^2$ $< Q^2 <$ 1.5 GeV$^2$. The phenomenological reaction model employed for separation of the resonant and non-resonant contributions to this exclusive channel was further developed. The $N(1440)1/2^+$, $N(1520)3/2^-$, and $\\Delta(1620"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1509.05460","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"}