{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2005:GKC3AQMAPKDV4OB375I6WFZY77","short_pith_number":"pith:GKC3AQMA","schema_version":"1.0","canonical_sha256":"3285b041807a875e383bff51eb1738ffecbdd014d3f1c44d4040758829ca4bcd","source":{"kind":"arxiv","id":"hep-ph/0508104","version":3},"attestation_state":"computed","paper":{"title":"Charmless hadronic B decays involving scalar mesons: Implications to the nature of light scalar mesons","license":"","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Chun-Khiang Chua, Hai-Yang Cheng, Kwei-Chou Yang","submitted_at":"2005-08-09T18:44:28Z","abstract_excerpt":"The hadronic charmless B decays into a scalar meson and a pseudoscalar meson are studied within the framework of QCD factorization. Although the light scalar mesons $f_0(980)$ and $a_0(980)$ are widely perceived as primarily the four-quark bound states, in practice it is difficult to make quantitative predictions based on the four-quark picture for light scalars. Hence, predictions are made in the 2-quark model for the scalar mesons. Based on the QCD sum rule method, we have derived the leading-twist light-cone distribution amplitudes of scalar mesons and their decay constants. The short-dista"},"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/0508104","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2005-08-09T18:44:28Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"3e5616e71133d6b571275032251628434d8fe5cf45a346466bd7b21838031176","abstract_canon_sha256":"788d8caada0b8d46d0254973c5f47932c872d178da62a2f3964e98ba55a1c3ba"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:17:46.521491Z","signature_b64":"2OoA2NjcM6B50ufF3xz/Mn2NkonH8/z+JPPSyeswvZy13gWh591rnoRvlYLoorUlieCxfWqiYHGmimnYYVTqDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3285b041807a875e383bff51eb1738ffecbdd014d3f1c44d4040758829ca4bcd","last_reissued_at":"2026-07-04T15:17:46.521007Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:17:46.521007Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Charmless hadronic B decays involving scalar mesons: Implications to the nature of light scalar mesons","license":"","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Chun-Khiang Chua, Hai-Yang Cheng, Kwei-Chou Yang","submitted_at":"2005-08-09T18:44:28Z","abstract_excerpt":"The hadronic charmless B decays into a scalar meson and a pseudoscalar meson are studied within the framework of QCD factorization. Although the light scalar mesons $f_0(980)$ and $a_0(980)$ are widely perceived as primarily the four-quark bound states, in practice it is difficult to make quantitative predictions based on the four-quark picture for light scalars. Hence, predictions are made in the 2-quark model for the scalar mesons. Based on the QCD sum rule method, we have derived the leading-twist light-cone distribution amplitudes of scalar mesons and their decay constants. The short-dista"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0508104","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/hep-ph/0508104/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/0508104","created_at":"2026-07-04T15:17:46.521068+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0508104v3","created_at":"2026-07-04T15:17:46.521068+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0508104","created_at":"2026-07-04T15:17:46.521068+00:00"},{"alias_kind":"pith_short_12","alias_value":"GKC3AQMAPKDV","created_at":"2026-07-04T15:17:46.521068+00:00"},{"alias_kind":"pith_short_16","alias_value":"GKC3AQMAPKDV4OB3","created_at":"2026-07-04T15:17:46.521068+00:00"},{"alias_kind":"pith_short_8","alias_value":"GKC3AQMA","created_at":"2026-07-04T15:17:46.521068+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2605.07997","citing_title":"Symmetry-Breaking Effects on Form Factors and Observables in $B \\to K_0^*(1430)\\mu^+\\mu^-$ Decay","ref_index":78,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/GKC3AQMAPKDV4OB375I6WFZY77","json":"https://pith.science/pith/GKC3AQMAPKDV4OB375I6WFZY77.json","graph_json":"https://pith.science/api/pith-number/GKC3AQMAPKDV4OB375I6WFZY77/graph.json","events_json":"https://pith.science/api/pith-number/GKC3AQMAPKDV4OB375I6WFZY77/events.json","paper":"https://pith.science/paper/GKC3AQMA"},"agent_actions":{"view_html":"https://pith.science/pith/GKC3AQMAPKDV4OB375I6WFZY77","download_json":"https://pith.science/pith/GKC3AQMAPKDV4OB375I6WFZY77.json","view_paper":"https://pith.science/paper/GKC3AQMA","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/0508104&json=true","fetch_graph":"https://pith.science/api/pith-number/GKC3AQMAPKDV4OB375I6WFZY77/graph.json","fetch_events":"https://pith.science/api/pith-number/GKC3AQMAPKDV4OB375I6WFZY77/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/GKC3AQMAPKDV4OB375I6WFZY77/action/timestamp_anchor","attest_storage":"https://pith.science/pith/GKC3AQMAPKDV4OB375I6WFZY77/action/storage_attestation","attest_author":"https://pith.science/pith/GKC3AQMAPKDV4OB375I6WFZY77/action/author_attestation","sign_citation":"https://pith.science/pith/GKC3AQMAPKDV4OB375I6WFZY77/action/citation_signature","submit_replication":"https://pith.science/pith/GKC3AQMAPKDV4OB375I6WFZY77/action/replication_record"}},"created_at":"2026-07-04T15:17:46.521068+00:00","updated_at":"2026-07-04T15:17:46.521068+00:00"}