{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:BZDJZ6LAY3I3UTDN2SPAZ5NQKV","short_pith_number":"pith:BZDJZ6LA","schema_version":"1.0","canonical_sha256":"0e469cf960c6d1ba4c6dd49e0cf5b055759fc75cba872cb2f41c4ab0b6aa3226","source":{"kind":"arxiv","id":"2404.01290","version":3},"attestation_state":"computed","paper":{"title":"Potential of light-cone sum rules without semiglobal quark-hadron duality","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A. Carvunis, F. Mahmoudi, Y. Monceaux","submitted_at":"2024-04-01T17:57:08Z","abstract_excerpt":"This work addresses the calculation of local form factors involved in the theoretical predictions of semileptonic $B$-meson decays at low $q^2$. We present a new approach to the method of QCD light-cone sum rule with $B$-meson light-cone distribution amplitudes. In our strategy, we bypass the semiglobal quark-hadron duality (QHD) approximation which usually contributes an unknown and potentially large systematic error to the prediction of form factors. We trade this improvement for an increased reliance on higher-order contributions in perturbation theory. Unlike the systematic error from semi"},"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":"2404.01290","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2024-04-01T17:57:08Z","cross_cats_sorted":[],"title_canon_sha256":"bc2e6dd06b6b09f4f7b764d64661155af6df694d5a825e7ca9cd0d12e1b282fa","abstract_canon_sha256":"c7c73ebd1af127c481aafc26a175cc7e981fbc67ff41e8b564e1bd73cbdd2a56"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T09:54:25.889736Z","signature_b64":"auH3YezUzq81O9TlVpL+pK1UyC43eUWLk5uvPzr0fN22Rh2RE7XG/NJO6tHeCFyLZQgrp91eYRk/UiYNM9JZBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0e469cf960c6d1ba4c6dd49e0cf5b055759fc75cba872cb2f41c4ab0b6aa3226","last_reissued_at":"2026-07-05T09:54:25.889284Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T09:54:25.889284Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Potential of light-cone sum rules without semiglobal quark-hadron duality","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A. Carvunis, F. Mahmoudi, Y. Monceaux","submitted_at":"2024-04-01T17:57:08Z","abstract_excerpt":"This work addresses the calculation of local form factors involved in the theoretical predictions of semileptonic $B$-meson decays at low $q^2$. We present a new approach to the method of QCD light-cone sum rule with $B$-meson light-cone distribution amplitudes. In our strategy, we bypass the semiglobal quark-hadron duality (QHD) approximation which usually contributes an unknown and potentially large systematic error to the prediction of form factors. We trade this improvement for an increased reliance on higher-order contributions in perturbation theory. Unlike the systematic error from semi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2404.01290","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/2404.01290/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":"2404.01290","created_at":"2026-07-05T09:54:25.889341+00:00"},{"alias_kind":"arxiv_version","alias_value":"2404.01290v3","created_at":"2026-07-05T09:54:25.889341+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2404.01290","created_at":"2026-07-05T09:54:25.889341+00:00"},{"alias_kind":"pith_short_12","alias_value":"BZDJZ6LAY3I3","created_at":"2026-07-05T09:54:25.889341+00:00"},{"alias_kind":"pith_short_16","alias_value":"BZDJZ6LAY3I3UTDN","created_at":"2026-07-05T09:54:25.889341+00:00"},{"alias_kind":"pith_short_8","alias_value":"BZDJZ6LA","created_at":"2026-07-05T09:54:25.889341+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/BZDJZ6LAY3I3UTDN2SPAZ5NQKV","json":"https://pith.science/pith/BZDJZ6LAY3I3UTDN2SPAZ5NQKV.json","graph_json":"https://pith.science/api/pith-number/BZDJZ6LAY3I3UTDN2SPAZ5NQKV/graph.json","events_json":"https://pith.science/api/pith-number/BZDJZ6LAY3I3UTDN2SPAZ5NQKV/events.json","paper":"https://pith.science/paper/BZDJZ6LA"},"agent_actions":{"view_html":"https://pith.science/pith/BZDJZ6LAY3I3UTDN2SPAZ5NQKV","download_json":"https://pith.science/pith/BZDJZ6LAY3I3UTDN2SPAZ5NQKV.json","view_paper":"https://pith.science/paper/BZDJZ6LA","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2404.01290&json=true","fetch_graph":"https://pith.science/api/pith-number/BZDJZ6LAY3I3UTDN2SPAZ5NQKV/graph.json","fetch_events":"https://pith.science/api/pith-number/BZDJZ6LAY3I3UTDN2SPAZ5NQKV/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/BZDJZ6LAY3I3UTDN2SPAZ5NQKV/action/timestamp_anchor","attest_storage":"https://pith.science/pith/BZDJZ6LAY3I3UTDN2SPAZ5NQKV/action/storage_attestation","attest_author":"https://pith.science/pith/BZDJZ6LAY3I3UTDN2SPAZ5NQKV/action/author_attestation","sign_citation":"https://pith.science/pith/BZDJZ6LAY3I3UTDN2SPAZ5NQKV/action/citation_signature","submit_replication":"https://pith.science/pith/BZDJZ6LAY3I3UTDN2SPAZ5NQKV/action/replication_record"}},"created_at":"2026-07-05T09:54:25.889341+00:00","updated_at":"2026-07-05T09:54:25.889341+00:00"}