{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1995:RMJBFYPEMKY6XCNXWC4JD3XCTP","short_pith_number":"pith:RMJBFYPE","schema_version":"1.0","canonical_sha256":"8b1212e1e462b1eb89b7b0b891eee29be0e087a2c620d04286426f22b62d204c","source":{"kind":"arxiv","id":"hep-ph/9506225","version":1},"attestation_state":"computed","paper":{"title":"A MODEL FOR THE CHARMED $D_s^{+}$ MESON DECAYS INTO THREE PIONS","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"M. Gourdin, X. Y. Pham, Y. Y. Keum","submitted_at":"1995-06-02T15:39:21Z","abstract_excerpt":"We propose a phenomenological three component model describing the decay amplitude of the process $D_{s}^{+} \\ra 3\\pi$. The first component is a constant background, the second one is a Breit-Wigner amplitude associated to a quasi two-body $f_{0}(980) \\pi^{+}$ state and the third one another Breit-Wigner amplitude corresponding to a possible quasi two-body $\\rho(770) \\pi$ state. We show that it is possible to reproduce the observed total rate for $D_{s}^{+} \\ra \\pi^{+}\\pi^{+}\\pi^{-}$ as well as the two other measured branching ratios for the non resonant part and the resonant $f_{0}\\pi^{+}$ on"},"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":"hep-ph/9506225","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1995-06-02T15:39:21Z","cross_cats_sorted":[],"title_canon_sha256":"1b2c2b59b537caa32575ac7eb2e1037fb4cae8e56ad1e4881d2b6f6dae92bb6e","abstract_canon_sha256":"c46f90237348b2e90d1f338e7d359b573615323c0aae9edbe0ced8b65dd331ae"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:06:30.227334Z","signature_b64":"JRWoXD37hXuMSKJaruQNk7JZbRRBb2M/N9Ljgbj5OPsIFeLCMEkjGDgpSsqMDv4QgXDDfIOQPwsZx6PR89ALBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8b1212e1e462b1eb89b7b0b891eee29be0e087a2c620d04286426f22b62d204c","last_reissued_at":"2026-05-18T01:06:30.226714Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:06:30.226714Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"A MODEL FOR THE CHARMED $D_s^{+}$ MESON DECAYS INTO THREE PIONS","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"M. Gourdin, X. Y. Pham, Y. Y. Keum","submitted_at":"1995-06-02T15:39:21Z","abstract_excerpt":"We propose a phenomenological three component model describing the decay amplitude of the process $D_{s}^{+} \\ra 3\\pi$. The first component is a constant background, the second one is a Breit-Wigner amplitude associated to a quasi two-body $f_{0}(980) \\pi^{+}$ state and the third one another Breit-Wigner amplitude corresponding to a possible quasi two-body $\\rho(770) \\pi$ state. We show that it is possible to reproduce the observed total rate for $D_{s}^{+} \\ra \\pi^{+}\\pi^{+}\\pi^{-}$ as well as the two other measured branching ratios for the non resonant part and the resonant $f_{0}\\pi^{+}$ on"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9506225","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":"hep-ph/9506225","created_at":"2026-05-18T01:06:30.226797+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9506225v1","created_at":"2026-05-18T01:06:30.226797+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9506225","created_at":"2026-05-18T01:06:30.226797+00:00"},{"alias_kind":"pith_short_12","alias_value":"RMJBFYPEMKY6","created_at":"2026-05-18T12:25:47.700082+00:00"},{"alias_kind":"pith_short_16","alias_value":"RMJBFYPEMKY6XCNX","created_at":"2026-05-18T12:25:47.700082+00:00"},{"alias_kind":"pith_short_8","alias_value":"RMJBFYPE","created_at":"2026-05-18T12:25:47.700082+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/RMJBFYPEMKY6XCNXWC4JD3XCTP","json":"https://pith.science/pith/RMJBFYPEMKY6XCNXWC4JD3XCTP.json","graph_json":"https://pith.science/api/pith-number/RMJBFYPEMKY6XCNXWC4JD3XCTP/graph.json","events_json":"https://pith.science/api/pith-number/RMJBFYPEMKY6XCNXWC4JD3XCTP/events.json","paper":"https://pith.science/paper/RMJBFYPE"},"agent_actions":{"view_html":"https://pith.science/pith/RMJBFYPEMKY6XCNXWC4JD3XCTP","download_json":"https://pith.science/pith/RMJBFYPEMKY6XCNXWC4JD3XCTP.json","view_paper":"https://pith.science/paper/RMJBFYPE","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/9506225&json=true","fetch_graph":"https://pith.science/api/pith-number/RMJBFYPEMKY6XCNXWC4JD3XCTP/graph.json","fetch_events":"https://pith.science/api/pith-number/RMJBFYPEMKY6XCNXWC4JD3XCTP/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/RMJBFYPEMKY6XCNXWC4JD3XCTP/action/timestamp_anchor","attest_storage":"https://pith.science/pith/RMJBFYPEMKY6XCNXWC4JD3XCTP/action/storage_attestation","attest_author":"https://pith.science/pith/RMJBFYPEMKY6XCNXWC4JD3XCTP/action/author_attestation","sign_citation":"https://pith.science/pith/RMJBFYPEMKY6XCNXWC4JD3XCTP/action/citation_signature","submit_replication":"https://pith.science/pith/RMJBFYPEMKY6XCNXWC4JD3XCTP/action/replication_record"}},"created_at":"2026-05-18T01:06:30.226797+00:00","updated_at":"2026-05-18T01:06:30.226797+00:00"}