{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:W34SJA5XE62UDYZXV5IDHXETQ5","short_pith_number":"pith:W34SJA5X","schema_version":"1.0","canonical_sha256":"b6f92483b727b541e337af5033dc93874640bcc1d233363323b7120e07e735ec","source":{"kind":"arxiv","id":"1807.06485","version":1},"attestation_state":"computed","paper":{"title":"Strong decay modes $\\bar{K}\\Xi$ and $\\bar{K}\\Xi\\pi$ of the $\\Omega(2012)$ in the $\\bar{K}\\Xi(1530)$ and $\\eta\\Omega$ molecular scenario","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Ju-Jun Xie, Jun-Xu Lu, Li-Sheng Geng, Ming-Zhu Liu, Yin Huang","submitted_at":"2018-07-17T15:07:43Z","abstract_excerpt":"We study the $\\bar{K} \\Xi$ decay mode of the newly observed $\\Omega(2012)$ assuming that the $\\Omega(2012)$ is a dynamically generated state with spin-parity $J^P = 3/2^-$ from the coupled channel $S$-wave interactions of $\\bar{K}\\Xi(1530)$ and $\\eta \\Omega$. In addition we also calculate its $K\\pi\\Xi$ three-body decay mode. It is shown that the so-obtained total decay width is in fair agreement with the experimental data. We compare our results with those of other recent studies and highlight differences among them."},"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":"1807.06485","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-07-17T15:07:43Z","cross_cats_sorted":[],"title_canon_sha256":"d92b994f6ee062fe96bec0102d2b3153681a9b2a4535821fa1a7a0a6082b242b","abstract_canon_sha256":"0691cb8480f78b4aa18c6d51a1f0cc8e7ac5e6a621cbf01182b69976f3aad957"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:02:33.770812Z","signature_b64":"mVKF5h77V7MSGSgR99EPP3L+6jV6L9p6IzF90H3HMffA2jJj2X7YN/tokRzNZZuIwhCS8g+FodXYeBVbdS8fBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b6f92483b727b541e337af5033dc93874640bcc1d233363323b7120e07e735ec","last_reissued_at":"2026-05-18T00:02:33.770204Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:02:33.770204Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Strong decay modes $\\bar{K}\\Xi$ and $\\bar{K}\\Xi\\pi$ of the $\\Omega(2012)$ in the $\\bar{K}\\Xi(1530)$ and $\\eta\\Omega$ molecular scenario","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Ju-Jun Xie, Jun-Xu Lu, Li-Sheng Geng, Ming-Zhu Liu, Yin Huang","submitted_at":"2018-07-17T15:07:43Z","abstract_excerpt":"We study the $\\bar{K} \\Xi$ decay mode of the newly observed $\\Omega(2012)$ assuming that the $\\Omega(2012)$ is a dynamically generated state with spin-parity $J^P = 3/2^-$ from the coupled channel $S$-wave interactions of $\\bar{K}\\Xi(1530)$ and $\\eta \\Omega$. In addition we also calculate its $K\\pi\\Xi$ three-body decay mode. It is shown that the so-obtained total decay width is in fair agreement with the experimental data. We compare our results with those of other recent studies and highlight differences among them."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1807.06485","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1807.06485","created_at":"2026-05-18T00:02:33.770288+00:00"},{"alias_kind":"arxiv_version","alias_value":"1807.06485v1","created_at":"2026-05-18T00:02:33.770288+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1807.06485","created_at":"2026-05-18T00:02:33.770288+00:00"},{"alias_kind":"pith_short_12","alias_value":"W34SJA5XE62U","created_at":"2026-05-18T12:32:59.047623+00:00"},{"alias_kind":"pith_short_16","alias_value":"W34SJA5XE62UDYZX","created_at":"2026-05-18T12:32:59.047623+00:00"},{"alias_kind":"pith_short_8","alias_value":"W34SJA5X","created_at":"2026-05-18T12:32:59.047623+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":34,"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":34,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/W34SJA5XE62UDYZXV5IDHXETQ5","json":"https://pith.science/pith/W34SJA5XE62UDYZXV5IDHXETQ5.json","graph_json":"https://pith.science/api/pith-number/W34SJA5XE62UDYZXV5IDHXETQ5/graph.json","events_json":"https://pith.science/api/pith-number/W34SJA5XE62UDYZXV5IDHXETQ5/events.json","paper":"https://pith.science/paper/W34SJA5X"},"agent_actions":{"view_html":"https://pith.science/pith/W34SJA5XE62UDYZXV5IDHXETQ5","download_json":"https://pith.science/pith/W34SJA5XE62UDYZXV5IDHXETQ5.json","view_paper":"https://pith.science/paper/W34SJA5X","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1807.06485&json=true","fetch_graph":"https://pith.science/api/pith-number/W34SJA5XE62UDYZXV5IDHXETQ5/graph.json","fetch_events":"https://pith.science/api/pith-number/W34SJA5XE62UDYZXV5IDHXETQ5/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/W34SJA5XE62UDYZXV5IDHXETQ5/action/timestamp_anchor","attest_storage":"https://pith.science/pith/W34SJA5XE62UDYZXV5IDHXETQ5/action/storage_attestation","attest_author":"https://pith.science/pith/W34SJA5XE62UDYZXV5IDHXETQ5/action/author_attestation","sign_citation":"https://pith.science/pith/W34SJA5XE62UDYZXV5IDHXETQ5/action/citation_signature","submit_replication":"https://pith.science/pith/W34SJA5XE62UDYZXV5IDHXETQ5/action/replication_record"}},"created_at":"2026-05-18T00:02:33.770288+00:00","updated_at":"2026-05-18T00:02:33.770288+00:00"}