{"paper":{"title":"Spectroscopy of $^{26}$F","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-ex","authors_text":"A. Kerek, A. Krasznahorkay, B. A. Brown, C. Borcea, C. Bourgeois (IPNO), C. Timis, D. Guillemaud-Mueller (IPNO), D. Sohler, F. Azaiez (IPNO), F. Ibrahim (IPNO), F. Negoita, G. Sletten, H. Savajols (GANIL), J. Mrazek, J. Timar, M. G. Porquet (CSNSM), M. G. Saint-Laurent (GANIL), M. Lewitowicz (GANIL), M. Stanoiu (IPNO), O. Sorlin (GANIL), P. Roussel-Chomaz (GANIL), S. Gr\\'evy, S. M. Lukyanov, Yu.-E. Penionzhkevich, Z. Elekes, Zs. Dombradi, Zs. F\\\"ul\\\"op, Zs. Podolyak","submitted_at":"2012-01-05T10:49:05Z","abstract_excerpt":"The structure of the weakly-bound $^{26}_{\\;\\;9}$F$_{17}$ odd-odd nucleus, produced from $^{27,28}$Na nuclei, has been investigated at GANIL by means of the in-beam $\\gamma$-ray spectroscopy technique. A single $\\gamma$-line is observed at 657(7) keV in $^{26}_{9}$F which has been ascribed to the decay of the excited J=$2^+$ state to the J=1$^+$ ground state. The possible presence of intruder negative parity states in $^{26}$F is also discussed."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1201.1111","kind":"arxiv","version":1},"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"}