{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2007:B7WPVGCOYCMKXSOROBBFS4ECJI","short_pith_number":"pith:B7WPVGCO","schema_version":"1.0","canonical_sha256":"0fecfa984ec098abc9d170425970824a3bea313f2481df12cfb5bb8c3f671ddc","source":{"kind":"arxiv","id":"0711.3999","version":2},"attestation_state":"computed","paper":{"title":"SCET sum rules for B->P and B->V transition form factors","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"F. De Fazio (INFN Bari), Th. Feldmann (Univ. Siegen), T. Hurth (CERN & SLAC)","submitted_at":"2007-11-26T14:50:16Z","abstract_excerpt":"We investigate sum rules for heavy-to-light transition form factors at large recoil derived from correlation functions with interpolating currents for light pseudoscalar or vector fields in soft-collinear effective theory (SCET). We consider both, factorizable and non-factorizable contributions at leading power in the Lambda/m_b expansion and to first order in the strong coupling constant alpha_s, neglecting contributions from 3-particle distribution amplitudes in the B-meson. We pay particular attention to various sources of parametric and systematic uncertainties. We also discuss certain for"},"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":"0711.3999","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2007-11-26T14:50:16Z","cross_cats_sorted":[],"title_canon_sha256":"5596762e878e8621471208cbd7415813221f4d3027750365ccce862266425aee","abstract_canon_sha256":"0c02f9a1fec0eac7f69207dad99b5aff65a34456e28060c1e8259748593f9f6a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:38:00.480895Z","signature_b64":"/9FgZx2tSJzepmGyaByFaKQPSAaPvjBYv/2KhNBIg1bYyflfqM8qM0Npc+kO4gScnoiknnuPu6rDEMhygzeOBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0fecfa984ec098abc9d170425970824a3bea313f2481df12cfb5bb8c3f671ddc","last_reissued_at":"2026-07-04T15:38:00.480462Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:38:00.480462Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"SCET sum rules for B->P and B->V transition form factors","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"F. De Fazio (INFN Bari), Th. Feldmann (Univ. Siegen), T. Hurth (CERN & SLAC)","submitted_at":"2007-11-26T14:50:16Z","abstract_excerpt":"We investigate sum rules for heavy-to-light transition form factors at large recoil derived from correlation functions with interpolating currents for light pseudoscalar or vector fields in soft-collinear effective theory (SCET). We consider both, factorizable and non-factorizable contributions at leading power in the Lambda/m_b expansion and to first order in the strong coupling constant alpha_s, neglecting contributions from 3-particle distribution amplitudes in the B-meson. We pay particular attention to various sources of parametric and systematic uncertainties. We also discuss certain for"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0711.3999","kind":"arxiv","version":2},"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/0711.3999/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":"0711.3999","created_at":"2026-07-04T15:38:00.480532+00:00"},{"alias_kind":"arxiv_version","alias_value":"0711.3999v2","created_at":"2026-07-04T15:38:00.480532+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0711.3999","created_at":"2026-07-04T15:38:00.480532+00:00"},{"alias_kind":"pith_short_12","alias_value":"B7WPVGCOYCMK","created_at":"2026-07-04T15:38:00.480532+00:00"},{"alias_kind":"pith_short_16","alias_value":"B7WPVGCOYCMKXSOR","created_at":"2026-07-04T15:38:00.480532+00:00"},{"alias_kind":"pith_short_8","alias_value":"B7WPVGCO","created_at":"2026-07-04T15:38:00.480532+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2604.26406","citing_title":"Semileptonic $B_q$ decays to heavy tensor mesons","ref_index":25,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/B7WPVGCOYCMKXSOROBBFS4ECJI","json":"https://pith.science/pith/B7WPVGCOYCMKXSOROBBFS4ECJI.json","graph_json":"https://pith.science/api/pith-number/B7WPVGCOYCMKXSOROBBFS4ECJI/graph.json","events_json":"https://pith.science/api/pith-number/B7WPVGCOYCMKXSOROBBFS4ECJI/events.json","paper":"https://pith.science/paper/B7WPVGCO"},"agent_actions":{"view_html":"https://pith.science/pith/B7WPVGCOYCMKXSOROBBFS4ECJI","download_json":"https://pith.science/pith/B7WPVGCOYCMKXSOROBBFS4ECJI.json","view_paper":"https://pith.science/paper/B7WPVGCO","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=0711.3999&json=true","fetch_graph":"https://pith.science/api/pith-number/B7WPVGCOYCMKXSOROBBFS4ECJI/graph.json","fetch_events":"https://pith.science/api/pith-number/B7WPVGCOYCMKXSOROBBFS4ECJI/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/B7WPVGCOYCMKXSOROBBFS4ECJI/action/timestamp_anchor","attest_storage":"https://pith.science/pith/B7WPVGCOYCMKXSOROBBFS4ECJI/action/storage_attestation","attest_author":"https://pith.science/pith/B7WPVGCOYCMKXSOROBBFS4ECJI/action/author_attestation","sign_citation":"https://pith.science/pith/B7WPVGCOYCMKXSOROBBFS4ECJI/action/citation_signature","submit_replication":"https://pith.science/pith/B7WPVGCOYCMKXSOROBBFS4ECJI/action/replication_record"}},"created_at":"2026-07-04T15:38:00.480532+00:00","updated_at":"2026-07-04T15:38:00.480532+00:00"}