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We calculate the mass and residue of $\\Omega(2012)$ state by employing the QCD sum rule method. Comparison of the obtained results with the experimental data allows us to interpret this state as $1P$ orbital excitation of the ground state $\\Omega$ baryon, i.e. with quantum numbers $J^P=\\frac{3}{2}^-$."},"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":"1806.01626","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-06-05T12:16:43Z","cross_cats_sorted":["hep-ex","hep-lat"],"title_canon_sha256":"272870e1b2ffcdea9c5674c0bf8310f91668e610448cbe0894c0dfbc5721c1ac","abstract_canon_sha256":"20d6f49d9018b2426f9c7273ef9406f2b71f051de10b56671217c0ac331c219a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:09:11.469588Z","signature_b64":"772TuL9PokguoQ65MYa9lqATux6rbmuwkuONcDMcW8+7QABoWTQBtIdI+mmEU2EhGHQ3qkQmYdzTuSlLSo7iBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"08ca2961416331c7a890e3e2a5d25804dd37bfd8dbe45c3f273d1a1007d36e3d","last_reissued_at":"2026-05-18T00:09:11.469133Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:09:11.469133Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Interpretation of the newly discovered $\\Omega$(2012)","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","hep-lat"],"primary_cat":"hep-ph","authors_text":"H. Sundu, K. Azizi, T. M. Aliev, Y. Sarac","submitted_at":"2018-06-05T12:16:43Z","abstract_excerpt":"Very recently Belle Collaboration reported observation of a narrow state called $\\Omega(2012)$ with mass $2012.4 \\pm 0.7$~(stat)~$\\pm 0.6$(syst)~MeV and width $6.4^{+2.5}_{-2.0}$~(stat)~$\\pm 1.6$~(syst)~MeV. We calculate the mass and residue of $\\Omega(2012)$ state by employing the QCD sum rule method. Comparison of the obtained results with the experimental data allows us to interpret this state as $1P$ orbital excitation of the ground state $\\Omega$ baryon, i.e. with quantum numbers $J^P=\\frac{3}{2}^-$."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1806.01626","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1806.01626","created_at":"2026-05-18T00:09:11.469207+00:00"},{"alias_kind":"arxiv_version","alias_value":"1806.01626v2","created_at":"2026-05-18T00:09:11.469207+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1806.01626","created_at":"2026-05-18T00:09:11.469207+00:00"},{"alias_kind":"pith_short_12","alias_value":"BDFCSYKBMMY4","created_at":"2026-05-18T12:32:13.499390+00:00"},{"alias_kind":"pith_short_16","alias_value":"BDFCSYKBMMY4PKEQ","created_at":"2026-05-18T12:32:13.499390+00:00"},{"alias_kind":"pith_short_8","alias_value":"BDFCSYKB","created_at":"2026-05-18T12:32:13.499390+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2604.25630","citing_title":"Probing the hadronic molecular nature of the $\\Omega(2012)$, $\\Omega(2380)$, and $\\Omega_c(3120)$ via femtoscopy correlation functions","ref_index":28,"is_internal_anchor":false},{"citing_arxiv_id":"2604.25630","citing_title":"Probing the hadronic molecular nature of the $\\Omega(2012)$, $\\Omega(2380)$, and $\\Omega_c(3120)$ via femtoscopy correlation functions","ref_index":28,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/BDFCSYKBMMY4PKEQ4PRKLUSYAT","json":"https://pith.science/pith/BDFCSYKBMMY4PKEQ4PRKLUSYAT.json","graph_json":"https://pith.science/api/pith-number/BDFCSYKBMMY4PKEQ4PRKLUSYAT/graph.json","events_json":"https://pith.science/api/pith-number/BDFCSYKBMMY4PKEQ4PRKLUSYAT/events.json","paper":"https://pith.science/paper/BDFCSYKB"},"agent_actions":{"view_html":"https://pith.science/pith/BDFCSYKBMMY4PKEQ4PRKLUSYAT","download_json":"https://pith.science/pith/BDFCSYKBMMY4PKEQ4PRKLUSYAT.json","view_paper":"https://pith.science/paper/BDFCSYKB","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1806.01626&json=true","fetch_graph":"https://pith.science/api/pith-number/BDFCSYKBMMY4PKEQ4PRKLUSYAT/graph.json","fetch_events":"https://pith.science/api/pith-number/BDFCSYKBMMY4PKEQ4PRKLUSYAT/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/BDFCSYKBMMY4PKEQ4PRKLUSYAT/action/timestamp_anchor","attest_storage":"https://pith.science/pith/BDFCSYKBMMY4PKEQ4PRKLUSYAT/action/storage_attestation","attest_author":"https://pith.science/pith/BDFCSYKBMMY4PKEQ4PRKLUSYAT/action/author_attestation","sign_citation":"https://pith.science/pith/BDFCSYKBMMY4PKEQ4PRKLUSYAT/action/citation_signature","submit_replication":"https://pith.science/pith/BDFCSYKBMMY4PKEQ4PRKLUSYAT/action/replication_record"}},"created_at":"2026-05-18T00:09:11.469207+00:00","updated_at":"2026-05-18T00:09:11.469207+00:00"}