{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:DUG4C3BCXW3HXS6OUZTBONGMO2","short_pith_number":"pith:DUG4C3BC","schema_version":"1.0","canonical_sha256":"1d0dc16c22bdb67bcbcea6661734cc76b2cc815d59d27128cc395fa5da6e20a1","source":{"kind":"arxiv","id":"2404.17246","version":1},"attestation_state":"computed","paper":{"title":"Canonical interpretation of the newly observed $J^P =1^+$ structure $X(2085)$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Guan-Ying Wang, Qi-Fang L\\\"u, Sheng-Chao Zhang, Tian-Ge Li","submitted_at":"2024-04-26T08:38:55Z","abstract_excerpt":"Inspired by the newly observed $X(2085)$ by the BESIII Collaboration, we study the strong decay behaviors of excited axialvector strange mesons within the quark pair creation model. Our results indicate that the $K_1(1793)/K_1(1861)$ can be regarded as the same $K_1(2P)$ state, and the $K_1(1911)$ is assigned as the $K_1(2P^\\prime)$ state. Considering the mass, spin-parity, and decay behaviors, we interpret the newly observed $X(2085)$ as the radially excited $K_1(3P)$ state, which mainly decays into the $\\rho(1450) K$, $\\omega(1420)K$, $\\pi K^*(1410)$, $\\rho K_1(1270)$, and $\\rho K^*(892)$ fi"},"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":"2404.17246","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2024-04-26T08:38:55Z","cross_cats_sorted":[],"title_canon_sha256":"4b8cd65e07d5141f889591eb00a60bf738af2e42909d85c24c264494c5333773","abstract_canon_sha256":"6b4d639a595014c91b994f9c1934d9823b7ce07aae70a9242c75f6463e0484fb"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T08:12:35.194541Z","signature_b64":"cUj7g8bdH9jDqIImvI+2DM1XBRRYk2ZCdYO3dLEzTRFq+hmqdW3OdDCp389kZuEDhxBDKY6fsH122EChiFTgDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1d0dc16c22bdb67bcbcea6661734cc76b2cc815d59d27128cc395fa5da6e20a1","last_reissued_at":"2026-07-05T08:12:35.194131Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T08:12:35.194131Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Canonical interpretation of the newly observed $J^P =1^+$ structure $X(2085)$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Guan-Ying Wang, Qi-Fang L\\\"u, Sheng-Chao Zhang, Tian-Ge Li","submitted_at":"2024-04-26T08:38:55Z","abstract_excerpt":"Inspired by the newly observed $X(2085)$ by the BESIII Collaboration, we study the strong decay behaviors of excited axialvector strange mesons within the quark pair creation model. Our results indicate that the $K_1(1793)/K_1(1861)$ can be regarded as the same $K_1(2P)$ state, and the $K_1(1911)$ is assigned as the $K_1(2P^\\prime)$ state. Considering the mass, spin-parity, and decay behaviors, we interpret the newly observed $X(2085)$ as the radially excited $K_1(3P)$ state, which mainly decays into the $\\rho(1450) K$, $\\omega(1420)K$, $\\pi K^*(1410)$, $\\rho K_1(1270)$, and $\\rho K^*(892)$ fi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2404.17246","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2404.17246/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":"2404.17246","created_at":"2026-07-05T08:12:35.194185+00:00"},{"alias_kind":"arxiv_version","alias_value":"2404.17246v1","created_at":"2026-07-05T08:12:35.194185+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2404.17246","created_at":"2026-07-05T08:12:35.194185+00:00"},{"alias_kind":"pith_short_12","alias_value":"DUG4C3BCXW3H","created_at":"2026-07-05T08:12:35.194185+00:00"},{"alias_kind":"pith_short_16","alias_value":"DUG4C3BCXW3HXS6O","created_at":"2026-07-05T08:12:35.194185+00:00"},{"alias_kind":"pith_short_8","alias_value":"DUG4C3BC","created_at":"2026-07-05T08:12:35.194185+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/DUG4C3BCXW3HXS6OUZTBONGMO2","json":"https://pith.science/pith/DUG4C3BCXW3HXS6OUZTBONGMO2.json","graph_json":"https://pith.science/api/pith-number/DUG4C3BCXW3HXS6OUZTBONGMO2/graph.json","events_json":"https://pith.science/api/pith-number/DUG4C3BCXW3HXS6OUZTBONGMO2/events.json","paper":"https://pith.science/paper/DUG4C3BC"},"agent_actions":{"view_html":"https://pith.science/pith/DUG4C3BCXW3HXS6OUZTBONGMO2","download_json":"https://pith.science/pith/DUG4C3BCXW3HXS6OUZTBONGMO2.json","view_paper":"https://pith.science/paper/DUG4C3BC","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2404.17246&json=true","fetch_graph":"https://pith.science/api/pith-number/DUG4C3BCXW3HXS6OUZTBONGMO2/graph.json","fetch_events":"https://pith.science/api/pith-number/DUG4C3BCXW3HXS6OUZTBONGMO2/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/DUG4C3BCXW3HXS6OUZTBONGMO2/action/timestamp_anchor","attest_storage":"https://pith.science/pith/DUG4C3BCXW3HXS6OUZTBONGMO2/action/storage_attestation","attest_author":"https://pith.science/pith/DUG4C3BCXW3HXS6OUZTBONGMO2/action/author_attestation","sign_citation":"https://pith.science/pith/DUG4C3BCXW3HXS6OUZTBONGMO2/action/citation_signature","submit_replication":"https://pith.science/pith/DUG4C3BCXW3HXS6OUZTBONGMO2/action/replication_record"}},"created_at":"2026-07-05T08:12:35.194185+00:00","updated_at":"2026-07-05T08:12:35.194185+00:00"}