{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:TLNGJZATQZBZFKXBFXQ6BN2A7V","short_pith_number":"pith:TLNGJZAT","schema_version":"1.0","canonical_sha256":"9ada64e413864392aae12de1e0b740fd5e0e0af0e72a562bc9aa85ae982839a8","source":{"kind":"arxiv","id":"2511.09098","version":3},"attestation_state":"computed","paper":{"title":"Analysis of the strong decays of the $Y(4660)$ in tetraquark scenario via the QCD sum rules","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Xiao-Song Yang, Zhi-Gang Wang","submitted_at":"2025-11-12T08:14:49Z","abstract_excerpt":"Motivated by the enigmatic vector charmonium-like states, we investigate the strong decay behaviors of four kinds of vector tetraquark states, which are possible candidates for the $Y(4660)$, within the framework of three-point QCD sum rules based on rigorous quark-hadron duality. We take into account the vacuum condensates up to dimension 5 on the QCD side, and obtain the hadronic coupling constants therefore the partial decay widths of those states. The predicted total width $61.5\\pm7.3\\,\\rm{MeV}$ is in excellent agreement with the experimental data for the $Y(4660)$, which supports its inte"},"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":"2511.09098","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2025-11-12T08:14:49Z","cross_cats_sorted":[],"title_canon_sha256":"23d7feb27dc4b067b58097f9f8a85f921aaed3bb118a90c385ce6ec5e74ffd7b","abstract_canon_sha256":"9b6232727155a3c3374449d4d5bf13aa72c26e41369c6d6adb3348581b4f8562"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-20T00:00:27.741138Z","signature_b64":"YtQ5p6SN0w9ttmLRurEamC+2HQSHvYlrzipD3DLJBzmNaZ4GlyZfb0mxzFf94MLgFGhMDshSklNGO5LmGmRbCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9ada64e413864392aae12de1e0b740fd5e0e0af0e72a562bc9aa85ae982839a8","last_reissued_at":"2026-05-20T00:00:27.740592Z","signature_status":"signed_v1","first_computed_at":"2026-05-20T00:00:27.740592Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Analysis of the strong decays of the $Y(4660)$ in tetraquark scenario via the QCD sum rules","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Xiao-Song Yang, Zhi-Gang Wang","submitted_at":"2025-11-12T08:14:49Z","abstract_excerpt":"Motivated by the enigmatic vector charmonium-like states, we investigate the strong decay behaviors of four kinds of vector tetraquark states, which are possible candidates for the $Y(4660)$, within the framework of three-point QCD sum rules based on rigorous quark-hadron duality. We take into account the vacuum condensates up to dimension 5 on the QCD side, and obtain the hadronic coupling constants therefore the partial decay widths of those states. The predicted total width $61.5\\pm7.3\\,\\rm{MeV}$ is in excellent agreement with the experimental data for the $Y(4660)$, which supports its inte"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2511.09098","kind":"arxiv","version":3},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2511.09098/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2511.09098","created_at":"2026-05-20T00:00:27.740678+00:00"},{"alias_kind":"arxiv_version","alias_value":"2511.09098v3","created_at":"2026-05-20T00:00:27.740678+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2511.09098","created_at":"2026-05-20T00:00:27.740678+00:00"},{"alias_kind":"pith_short_12","alias_value":"TLNGJZATQZBZ","created_at":"2026-05-20T00:00:27.740678+00:00"},{"alias_kind":"pith_short_16","alias_value":"TLNGJZATQZBZFKXB","created_at":"2026-05-20T00:00:27.740678+00:00"},{"alias_kind":"pith_short_8","alias_value":"TLNGJZAT","created_at":"2026-05-20T00:00:27.740678+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2603.18877","citing_title":"Two-body strong decays of the pseudoscalar hidden-charm tetraquark states via the QCD sum rules","ref_index":22,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/TLNGJZATQZBZFKXBFXQ6BN2A7V","json":"https://pith.science/pith/TLNGJZATQZBZFKXBFXQ6BN2A7V.json","graph_json":"https://pith.science/api/pith-number/TLNGJZATQZBZFKXBFXQ6BN2A7V/graph.json","events_json":"https://pith.science/api/pith-number/TLNGJZATQZBZFKXBFXQ6BN2A7V/events.json","paper":"https://pith.science/paper/TLNGJZAT"},"agent_actions":{"view_html":"https://pith.science/pith/TLNGJZATQZBZFKXBFXQ6BN2A7V","download_json":"https://pith.science/pith/TLNGJZATQZBZFKXBFXQ6BN2A7V.json","view_paper":"https://pith.science/paper/TLNGJZAT","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2511.09098&json=true","fetch_graph":"https://pith.science/api/pith-number/TLNGJZATQZBZFKXBFXQ6BN2A7V/graph.json","fetch_events":"https://pith.science/api/pith-number/TLNGJZATQZBZFKXBFXQ6BN2A7V/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/TLNGJZATQZBZFKXBFXQ6BN2A7V/action/timestamp_anchor","attest_storage":"https://pith.science/pith/TLNGJZATQZBZFKXBFXQ6BN2A7V/action/storage_attestation","attest_author":"https://pith.science/pith/TLNGJZATQZBZFKXBFXQ6BN2A7V/action/author_attestation","sign_citation":"https://pith.science/pith/TLNGJZATQZBZFKXBFXQ6BN2A7V/action/citation_signature","submit_replication":"https://pith.science/pith/TLNGJZATQZBZFKXBFXQ6BN2A7V/action/replication_record"}},"created_at":"2026-05-20T00:00:27.740678+00:00","updated_at":"2026-05-20T00:00:27.740678+00:00"}