{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:YATE2B5FGX6UUJAE5HBF4HBZHI","short_pith_number":"pith:YATE2B5F","schema_version":"1.0","canonical_sha256":"c0264d07a535fd4a2404e9c25e1c393a24261cb17a45f30e18b2962001da8943","source":{"kind":"arxiv","id":"1502.05483","version":3},"attestation_state":"computed","paper":{"title":"$S$-wave resonance contributions to the $B^0_{(s)}\\to J/\\psi\\pi^+\\pi^-$ and $B_s\\to\\pi^+\\pi^-\\mu^+\\mu^-$ decays","license":"http://creativecommons.org/licenses/by/3.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Cai-Dian L\\\"u, Hsiang-nan Li, Wei Wang, Wen-Fei Wang","submitted_at":"2015-02-19T07:24:02Z","abstract_excerpt":"We study $S$-wave resonance contributions to the $B^0_{(s)}\\to J/\\psi\\pi^+\\pi^-$ and $B_s\\to\\pi^+\\pi^-\\ell^+\\ell^-$ decays in the perturbative QCD (PQCD) framework by introducing two-hadron distribution amplitudes for final states. The Breit-Wigner formula for the $f_0(500)$, $f_0(1500)$ and $f_0(1790)$ resonances and the Flatt\\'e model for the $f_0(980)$ resonance are adopted to parameterize the time-like scalar form factors in the two-pion distribution amplitudes, which include both resonant and nonresonant contributions. The resultant branching fraction and differential branching fraction i"},"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":"1502.05483","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/licenses/by/3.0/","primary_cat":"hep-ph","submitted_at":"2015-02-19T07:24:02Z","cross_cats_sorted":[],"title_canon_sha256":"5295395998f370f82864e063132e6c27cb12535649fdf582490948fc4d5d2d20","abstract_canon_sha256":"33add2cccff3a60fed12631e3419336b9dc378ce1089b2ccdbb8b083dcfdb69d"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:03:34.196462Z","signature_b64":"TCay+3P7SgqMlvRnScXexOSCK3m/8jC3YgX6BML44pcJ8ut1wDjeQIjzJkyYoe3XsfQEu879arM17V7h4XofDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c0264d07a535fd4a2404e9c25e1c393a24261cb17a45f30e18b2962001da8943","last_reissued_at":"2026-05-18T02:03:34.195717Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:03:34.195717Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"$S$-wave resonance contributions to the $B^0_{(s)}\\to J/\\psi\\pi^+\\pi^-$ and $B_s\\to\\pi^+\\pi^-\\mu^+\\mu^-$ decays","license":"http://creativecommons.org/licenses/by/3.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Cai-Dian L\\\"u, Hsiang-nan Li, Wei Wang, Wen-Fei Wang","submitted_at":"2015-02-19T07:24:02Z","abstract_excerpt":"We study $S$-wave resonance contributions to the $B^0_{(s)}\\to J/\\psi\\pi^+\\pi^-$ and $B_s\\to\\pi^+\\pi^-\\ell^+\\ell^-$ decays in the perturbative QCD (PQCD) framework by introducing two-hadron distribution amplitudes for final states. The Breit-Wigner formula for the $f_0(500)$, $f_0(1500)$ and $f_0(1790)$ resonances and the Flatt\\'e model for the $f_0(980)$ resonance are adopted to parameterize the time-like scalar form factors in the two-pion distribution amplitudes, which include both resonant and nonresonant contributions. The resultant branching fraction and differential branching fraction i"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1502.05483","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":""},"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":"1502.05483","created_at":"2026-05-18T02:03:34.195834+00:00"},{"alias_kind":"arxiv_version","alias_value":"1502.05483v3","created_at":"2026-05-18T02:03:34.195834+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1502.05483","created_at":"2026-05-18T02:03:34.195834+00:00"},{"alias_kind":"pith_short_12","alias_value":"YATE2B5FGX6U","created_at":"2026-05-18T12:29:50.041715+00:00"},{"alias_kind":"pith_short_16","alias_value":"YATE2B5FGX6UUJAE","created_at":"2026-05-18T12:29:50.041715+00:00"},{"alias_kind":"pith_short_8","alias_value":"YATE2B5F","created_at":"2026-05-18T12:29:50.041715+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/YATE2B5FGX6UUJAE5HBF4HBZHI","json":"https://pith.science/pith/YATE2B5FGX6UUJAE5HBF4HBZHI.json","graph_json":"https://pith.science/api/pith-number/YATE2B5FGX6UUJAE5HBF4HBZHI/graph.json","events_json":"https://pith.science/api/pith-number/YATE2B5FGX6UUJAE5HBF4HBZHI/events.json","paper":"https://pith.science/paper/YATE2B5F"},"agent_actions":{"view_html":"https://pith.science/pith/YATE2B5FGX6UUJAE5HBF4HBZHI","download_json":"https://pith.science/pith/YATE2B5FGX6UUJAE5HBF4HBZHI.json","view_paper":"https://pith.science/paper/YATE2B5F","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1502.05483&json=true","fetch_graph":"https://pith.science/api/pith-number/YATE2B5FGX6UUJAE5HBF4HBZHI/graph.json","fetch_events":"https://pith.science/api/pith-number/YATE2B5FGX6UUJAE5HBF4HBZHI/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/YATE2B5FGX6UUJAE5HBF4HBZHI/action/timestamp_anchor","attest_storage":"https://pith.science/pith/YATE2B5FGX6UUJAE5HBF4HBZHI/action/storage_attestation","attest_author":"https://pith.science/pith/YATE2B5FGX6UUJAE5HBF4HBZHI/action/author_attestation","sign_citation":"https://pith.science/pith/YATE2B5FGX6UUJAE5HBF4HBZHI/action/citation_signature","submit_replication":"https://pith.science/pith/YATE2B5FGX6UUJAE5HBF4HBZHI/action/replication_record"}},"created_at":"2026-05-18T02:03:34.195834+00:00","updated_at":"2026-05-18T02:03:34.195834+00:00"}