{"paper":{"title":"Measurements of $^{152}$Gd(p,$\\gamma$)$^{153}$Tb and $^{152}$Gd(p,n)$^{152}$Tb reaction cross sections for the astrophysical $\\gamma$ process","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-ex","authors_text":"C. Yal\\c{c}{\\i}n, E. Somorjai, Gy. Gy\\\"urky, J. Farkas, N. \\\"Ozkan, R. T. G\\\"uray, T. Rauscher, Z. Hal\\'asz, Zs. F\\\"ul\\\"op","submitted_at":"2015-04-29T11:52:28Z","abstract_excerpt":"The total cross sections for the $^{152}$Gd(p,$\\gamma$)$^{153}$Tb and $^{152}$Gd(p,n)$^{152}$Tb reactions have been measured by the activation method at effective center-of-mass energies \\mbox{$3.47 \\leq E_\\mathrm{c.m.}^\\mathrm{eff}\\leq 7.94$ MeV} and \\mbox{$4.96 \\leq E_\\mathrm{c.m.}^\\mathrm{eff} \\leq 7.94$ MeV}, respectively. The targets were prepared by evaporation of 30.6\\% isotopically enriched $^{152}$Gd oxide on aluminum backing foils, and bombarded with proton beams provided by a cyclotron accelerator. The cross sections were deduced from the observed $\\gamma$-ray activity, which was de"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1504.07820","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"}