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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"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"1704.01854","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-04-06T14:22:18Z","cross_cats_sorted":[],"title_canon_sha256":"ef63a1eb95b7a8158bd4210bcccd5fdb12c4b59147918323c8c09ff23a8160d0","abstract_canon_sha256":"56c15bea83e1e09885a4f2d2ae4ab251ac495f6a26869d20c01a693e920ea4fc"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:44:08.697159Z","signature_b64":"jo8j+kiZQ6mGbsWMikFCmXAhQZdZwNs3oW6RtTTO6RH4nPKm/Sx2VJV3rNRvvJsyeiDpW80aCmIFPVyuU0IvCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8cd7327ae5c98f8f14d37f01869642e729f89ab677d1dcd37db4776e465f86cd","last_reissued_at":"2026-05-18T00:44:08.696692Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:44:08.696692Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"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. 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