{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2023:EL5JEIKEXS3PHDHNJCATI3KCX7","short_pith_number":"pith:EL5JEIKE","schema_version":"1.0","canonical_sha256":"22fa922144bcb6f38ced4881346d42bffd9166ad7e4ffbc53b8e6c893e57725e","source":{"kind":"arxiv","id":"2309.05631","version":3},"attestation_state":"computed","paper":{"title":"Next-to-leading order QCD corrections to the form factors of $B$ to scalar meson decays","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Bo-Xuan Shi, Cai-Dian L\\\"u, Long-Shun Lu, Xue-Ying Han, Yue-Long Shen","submitted_at":"2023-09-11T17:20:26Z","abstract_excerpt":"We calculate the next-to-leading order QCD corrections to $B$ to scalar meson form factors from QCD light-cone sum rules with $B$ meson light-cone distribution amplitudes. We demonstrate that the $B$ meson-to-vacuum correlation functions can be factorized into the convolution of short-distance coefficients and light-cone distribution amplitudes at the one-loop level and find that only $\\phi_B^+(\\omega,\\mu)$ contributes to the form factors. We then employ the $z$-parameterization combined with constraints from strong coupling constants to reconstruct the $q^2$ dependence of the form factors in "},"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":"2309.05631","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2023-09-11T17:20:26Z","cross_cats_sorted":[],"title_canon_sha256":"b84a3483d957990d8422815bfb29c92d62556fc55ebd360fa03e524255a2f872","abstract_canon_sha256":"972edb0976bc84a34a6a401d53d0a659ce4c6042c0d41bfb959cccc4e822765e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T07:01:05.459690Z","signature_b64":"TIq8BnvuRmhN2iL3NYUuJ9OHMTdGM/AZItYid/pPWQvgfSfy9N46zu9fkWIa9VB6LnU8e9lXPs5XeldsnaCUDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"22fa922144bcb6f38ced4881346d42bffd9166ad7e4ffbc53b8e6c893e57725e","last_reissued_at":"2026-07-05T07:01:05.459087Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T07:01:05.459087Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Next-to-leading order QCD corrections to the form factors of $B$ to scalar meson decays","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Bo-Xuan Shi, Cai-Dian L\\\"u, Long-Shun Lu, Xue-Ying Han, Yue-Long Shen","submitted_at":"2023-09-11T17:20:26Z","abstract_excerpt":"We calculate the next-to-leading order QCD corrections to $B$ to scalar meson form factors from QCD light-cone sum rules with $B$ meson light-cone distribution amplitudes. We demonstrate that the $B$ meson-to-vacuum correlation functions can be factorized into the convolution of short-distance coefficients and light-cone distribution amplitudes at the one-loop level and find that only $\\phi_B^+(\\omega,\\mu)$ contributes to the form factors. We then employ the $z$-parameterization combined with constraints from strong coupling constants to reconstruct the $q^2$ dependence of the form factors in "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2309.05631","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/2309.05631/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":"2309.05631","created_at":"2026-07-05T07:01:05.459158+00:00"},{"alias_kind":"arxiv_version","alias_value":"2309.05631v3","created_at":"2026-07-05T07:01:05.459158+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2309.05631","created_at":"2026-07-05T07:01:05.459158+00:00"},{"alias_kind":"pith_short_12","alias_value":"EL5JEIKEXS3P","created_at":"2026-07-05T07:01:05.459158+00:00"},{"alias_kind":"pith_short_16","alias_value":"EL5JEIKEXS3PHDHN","created_at":"2026-07-05T07:01:05.459158+00:00"},{"alias_kind":"pith_short_8","alias_value":"EL5JEIKE","created_at":"2026-07-05T07:01:05.459158+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/EL5JEIKEXS3PHDHNJCATI3KCX7","json":"https://pith.science/pith/EL5JEIKEXS3PHDHNJCATI3KCX7.json","graph_json":"https://pith.science/api/pith-number/EL5JEIKEXS3PHDHNJCATI3KCX7/graph.json","events_json":"https://pith.science/api/pith-number/EL5JEIKEXS3PHDHNJCATI3KCX7/events.json","paper":"https://pith.science/paper/EL5JEIKE"},"agent_actions":{"view_html":"https://pith.science/pith/EL5JEIKEXS3PHDHNJCATI3KCX7","download_json":"https://pith.science/pith/EL5JEIKEXS3PHDHNJCATI3KCX7.json","view_paper":"https://pith.science/paper/EL5JEIKE","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2309.05631&json=true","fetch_graph":"https://pith.science/api/pith-number/EL5JEIKEXS3PHDHNJCATI3KCX7/graph.json","fetch_events":"https://pith.science/api/pith-number/EL5JEIKEXS3PHDHNJCATI3KCX7/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/EL5JEIKEXS3PHDHNJCATI3KCX7/action/timestamp_anchor","attest_storage":"https://pith.science/pith/EL5JEIKEXS3PHDHNJCATI3KCX7/action/storage_attestation","attest_author":"https://pith.science/pith/EL5JEIKEXS3PHDHNJCATI3KCX7/action/author_attestation","sign_citation":"https://pith.science/pith/EL5JEIKEXS3PHDHNJCATI3KCX7/action/citation_signature","submit_replication":"https://pith.science/pith/EL5JEIKEXS3PHDHNJCATI3KCX7/action/replication_record"}},"created_at":"2026-07-05T07:01:05.459158+00:00","updated_at":"2026-07-05T07:01:05.459158+00:00"}