{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2003:TRRKH5DMQTL5VT5ARIT2GP5NX5","short_pith_number":"pith:TRRKH5DM","schema_version":"1.0","canonical_sha256":"9c62a3f46c84d7dacfa08a27a33fadbf55938618cff9aaac83860ab162c5fda2","source":{"kind":"arxiv","id":"hep-ph/0310084","version":1},"attestation_state":"computed","paper":{"title":"Nonfactorizable contributions in B decays to charmonium: the case of $B^- \\to K^- h_c$","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"F. De Fazio, P. Colangelo, T.N. Pham","submitted_at":"2003-10-07T14:39:46Z","abstract_excerpt":"Nonleptonic $B$ to charmonium decays generally show deviations from the factorization predictions. For example, the mode $B^- \\to K^- \\chi_{c0}$ has been experimentally observed with sizeable branching fraction while its factorized amplitude vanishes. We investigate the role of rescattering effects mediated by intermediate charmed meson production in this class of decay modes, and consider $B^- \\to K^- h_c$ with $h_c$ the $J^{PC}=1^{+-}$ $\\bar c c$ meson. Using an effective lagrangian describing interactions of pairs of heavy-light $Q{\\bar q}$ mesons with a quarkonium state, we relate this mod"},"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/0310084","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2003-10-07T14:39:46Z","cross_cats_sorted":[],"title_canon_sha256":"44dfcf77d350c9f205d0341948f26abc6e999f22a7819a7a60a45db2886addbf","abstract_canon_sha256":"0cfa48dd12fd7a99896d3d6a697e3c781a7dfeb32dc64d9602f59682abc21247"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:40:54.867129Z","signature_b64":"yTPdupstBD0OVrDp26j9LOlYD0f81HkZUz0d/1Ml/FNuVUain6kko28cKpj7LVumK0h0js3Ub+r99nItOP2oDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9c62a3f46c84d7dacfa08a27a33fadbf55938618cff9aaac83860ab162c5fda2","last_reissued_at":"2026-07-04T16:40:54.866729Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:40:54.866729Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Nonfactorizable contributions in B decays to charmonium: the case of $B^- \\to K^- h_c$","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"F. De Fazio, P. Colangelo, T.N. Pham","submitted_at":"2003-10-07T14:39:46Z","abstract_excerpt":"Nonleptonic $B$ to charmonium decays generally show deviations from the factorization predictions. For example, the mode $B^- \\to K^- \\chi_{c0}$ has been experimentally observed with sizeable branching fraction while its factorized amplitude vanishes. We investigate the role of rescattering effects mediated by intermediate charmed meson production in this class of decay modes, and consider $B^- \\to K^- h_c$ with $h_c$ the $J^{PC}=1^{+-}$ $\\bar c c$ meson. Using an effective lagrangian describing interactions of pairs of heavy-light $Q{\\bar q}$ mesons with a quarkonium state, we relate this mod"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0310084","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/hep-ph/0310084/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":"hep-ph/0310084","created_at":"2026-07-04T16:40:54.866792+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0310084v1","created_at":"2026-07-04T16:40:54.866792+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0310084","created_at":"2026-07-04T16:40:54.866792+00:00"},{"alias_kind":"pith_short_12","alias_value":"TRRKH5DMQTL5","created_at":"2026-07-04T16:40:54.866792+00:00"},{"alias_kind":"pith_short_16","alias_value":"TRRKH5DMQTL5VT5A","created_at":"2026-07-04T16:40:54.866792+00:00"},{"alias_kind":"pith_short_8","alias_value":"TRRKH5DM","created_at":"2026-07-04T16:40:54.866792+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2606.13278","citing_title":"Resolving the CP Asymmetry Puzzle in $B$ Decays with Unitarized Final-State Interactions","ref_index":33,"is_internal_anchor":true},{"citing_arxiv_id":"2604.10944","citing_title":"Study of $\\chi_{cJ}\\to \\eta \\eta \\eta^\\prime$ via intermediate charmed meson loop mechanisms and its implications for non-observation of $\\eta_1(1855)$ in $\\chi_{cJ}$ decays","ref_index":56,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/TRRKH5DMQTL5VT5ARIT2GP5NX5","json":"https://pith.science/pith/TRRKH5DMQTL5VT5ARIT2GP5NX5.json","graph_json":"https://pith.science/api/pith-number/TRRKH5DMQTL5VT5ARIT2GP5NX5/graph.json","events_json":"https://pith.science/api/pith-number/TRRKH5DMQTL5VT5ARIT2GP5NX5/events.json","paper":"https://pith.science/paper/TRRKH5DM"},"agent_actions":{"view_html":"https://pith.science/pith/TRRKH5DMQTL5VT5ARIT2GP5NX5","download_json":"https://pith.science/pith/TRRKH5DMQTL5VT5ARIT2GP5NX5.json","view_paper":"https://pith.science/paper/TRRKH5DM","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/0310084&json=true","fetch_graph":"https://pith.science/api/pith-number/TRRKH5DMQTL5VT5ARIT2GP5NX5/graph.json","fetch_events":"https://pith.science/api/pith-number/TRRKH5DMQTL5VT5ARIT2GP5NX5/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/TRRKH5DMQTL5VT5ARIT2GP5NX5/action/timestamp_anchor","attest_storage":"https://pith.science/pith/TRRKH5DMQTL5VT5ARIT2GP5NX5/action/storage_attestation","attest_author":"https://pith.science/pith/TRRKH5DMQTL5VT5ARIT2GP5NX5/action/author_attestation","sign_citation":"https://pith.science/pith/TRRKH5DMQTL5VT5ARIT2GP5NX5/action/citation_signature","submit_replication":"https://pith.science/pith/TRRKH5DMQTL5VT5ARIT2GP5NX5/action/replication_record"}},"created_at":"2026-07-04T16:40:54.866792+00:00","updated_at":"2026-07-04T16:40:54.866792+00:00"}