{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:GGC23XXWCWLAB4H4ZOLL32NTFQ","short_pith_number":"pith:GGC23XXW","schema_version":"1.0","canonical_sha256":"3185addef6159600f0fccb96bde9b32c0d014b0383aad3af5d5aacb157b49ff0","source":{"kind":"arxiv","id":"2503.18593","version":2},"attestation_state":"computed","paper":{"title":"Analysis of three-body hadronic $D$-meson decays","license":"http://creativecommons.org/publicdomain/zero/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Si-Hong Zhou, Xu-Da Zhou","submitted_at":"2025-03-24T11:51:41Z","abstract_excerpt":"Motivated by recent experimental advances in three-body hadronic $D$ decays from BESIII, we present a systematic analysis of $D_{(s)} \\to P_1 (V \\to) P_2 P_3 $ decay processes, where $V$ denotes vector resonances ($\\rho, K^*, \\omega$, $\\phi$) and $P_{1,2,3}$ are light pseudoscalar mesons ($\\pi,K, \\eta^{(\\prime)}$). Using the factorization-assisted topological-amplitude (FAT) approach we calculate the intermediate subprocesses $D_{(s)} \\to P_1 V$, incorporating relativistic Breit-Wigner distributions to model the subsequent $V \\to P_2 P_3$ strong decays. By comprehensively including all relevan"},"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":"2503.18593","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/publicdomain/zero/1.0/","primary_cat":"hep-ph","submitted_at":"2025-03-24T11:51:41Z","cross_cats_sorted":[],"title_canon_sha256":"94782da2a3db607ed264faf57f7ec8485b831a0353a843115ccf881d031a4f74","abstract_canon_sha256":"c08f81aafaa86db127ef4e121490aec2efbd34b329cc286bc76d0c8128df5cc2"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:29:09.602233Z","signature_b64":"7t6JWRna/S8nIg7o0FCHKrTgDA59hLc2FYvK60aF3+0q7rH2t2/+1ZlPfrmIrFeFBtwzdPJoV1apKI6J/2ImCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3185addef6159600f0fccb96bde9b32c0d014b0383aad3af5d5aacb157b49ff0","last_reissued_at":"2026-07-05T11:29:09.601700Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:29:09.601700Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Analysis of three-body hadronic $D$-meson decays","license":"http://creativecommons.org/publicdomain/zero/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Si-Hong Zhou, Xu-Da Zhou","submitted_at":"2025-03-24T11:51:41Z","abstract_excerpt":"Motivated by recent experimental advances in three-body hadronic $D$ decays from BESIII, we present a systematic analysis of $D_{(s)} \\to P_1 (V \\to) P_2 P_3 $ decay processes, where $V$ denotes vector resonances ($\\rho, K^*, \\omega$, $\\phi$) and $P_{1,2,3}$ are light pseudoscalar mesons ($\\pi,K, \\eta^{(\\prime)}$). Using the factorization-assisted topological-amplitude (FAT) approach we calculate the intermediate subprocesses $D_{(s)} \\to P_1 V$, incorporating relativistic Breit-Wigner distributions to model the subsequent $V \\to P_2 P_3$ strong decays. By comprehensively including all relevan"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2503.18593","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2503.18593/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":"2503.18593","created_at":"2026-07-05T11:29:09.601767+00:00"},{"alias_kind":"arxiv_version","alias_value":"2503.18593v2","created_at":"2026-07-05T11:29:09.601767+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2503.18593","created_at":"2026-07-05T11:29:09.601767+00:00"},{"alias_kind":"pith_short_12","alias_value":"GGC23XXWCWLA","created_at":"2026-07-05T11:29:09.601767+00:00"},{"alias_kind":"pith_short_16","alias_value":"GGC23XXWCWLAB4H4","created_at":"2026-07-05T11:29:09.601767+00:00"},{"alias_kind":"pith_short_8","alias_value":"GGC23XXW","created_at":"2026-07-05T11:29:09.601767+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/GGC23XXWCWLAB4H4ZOLL32NTFQ","json":"https://pith.science/pith/GGC23XXWCWLAB4H4ZOLL32NTFQ.json","graph_json":"https://pith.science/api/pith-number/GGC23XXWCWLAB4H4ZOLL32NTFQ/graph.json","events_json":"https://pith.science/api/pith-number/GGC23XXWCWLAB4H4ZOLL32NTFQ/events.json","paper":"https://pith.science/paper/GGC23XXW"},"agent_actions":{"view_html":"https://pith.science/pith/GGC23XXWCWLAB4H4ZOLL32NTFQ","download_json":"https://pith.science/pith/GGC23XXWCWLAB4H4ZOLL32NTFQ.json","view_paper":"https://pith.science/paper/GGC23XXW","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2503.18593&json=true","fetch_graph":"https://pith.science/api/pith-number/GGC23XXWCWLAB4H4ZOLL32NTFQ/graph.json","fetch_events":"https://pith.science/api/pith-number/GGC23XXWCWLAB4H4ZOLL32NTFQ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/GGC23XXWCWLAB4H4ZOLL32NTFQ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/GGC23XXWCWLAB4H4ZOLL32NTFQ/action/storage_attestation","attest_author":"https://pith.science/pith/GGC23XXWCWLAB4H4ZOLL32NTFQ/action/author_attestation","sign_citation":"https://pith.science/pith/GGC23XXWCWLAB4H4ZOLL32NTFQ/action/citation_signature","submit_replication":"https://pith.science/pith/GGC23XXWCWLAB4H4ZOLL32NTFQ/action/replication_record"}},"created_at":"2026-07-05T11:29:09.601767+00:00","updated_at":"2026-07-05T11:29:09.601767+00:00"}