{"paper":{"title":"Analysis of the $\\Omega_c(3000)$, $\\Omega_c(3050)$, $\\Omega_c(3066)$, $\\Omega_c(3090)$ and $\\Omega_c(3119)$ with QCD sum rules","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Zhi-Gang Wang","submitted_at":"2017-04-06T14:22:18Z","abstract_excerpt":"In this article, we assign the $\\Omega_c(3000)$, $\\Omega_c(3050)$, $\\Omega_c(3066)$, $\\Omega_c(3090)$ and $\\Omega_c(3119)$ to be the P-wave baryon states with $J^P={\\frac{1}{2}}^-$, ${\\frac{1}{2}}^-$, ${\\frac{3}{2}}^-$, ${\\frac{3}{2}}^-$ and ${\\frac{5}{2}}^-$, respectively, and study them with the QCD sum rules by introducing an explicit relative P-wave between the two $s$ quarks. The predictions support assigning the $\\Omega_c(3050)$, $\\Omega_c(3066)$, $\\Omega_c(3090)$ and $\\Omega_c(3119)$ to be the P-wave baryon states with $J^P={\\frac{1}{2}}^-$, ${\\frac{3}{2}}^-$, ${\\frac{3}{2}}^-$ and ${\\f"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1704.01854","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"}