{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2001:RHOHLS3DTJM7NYJGPOLHBCRQM3","short_pith_number":"pith:RHOHLS3D","schema_version":"1.0","canonical_sha256":"89dc75cb639a59f6e1267b96708a3066f9c51eaa6ee1d7f63116fbadffc52dc8","source":{"kind":"arxiv","id":"hep-ph/0110372","version":1},"attestation_state":"computed","paper":{"title":"Remarks on sum rules in the heavy quark limit of QCD","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A. Le Yaouanc, J.-C. Raynal, L. Oliver, O. Pene, V. Morenas","submitted_at":"2001-10-29T16:17:31Z","abstract_excerpt":"We underline a problem existing in the heavy quark limit of QCD concerning the rates of semileptonic B decays into P-wave $D_J(j)$ mesons, where $j = {1 \\over 2}$ (wide states) or $j = {3 \\over 2}$ (narrow states). The leading order sum rules of Bjorken and Uraltsev suggest $\\Gamma [ \\bar{B} \\to D_{0,1} ({1 \\over 2}) \\ell \\nu ] \\ll \\Gamma [ \\bar{B} \\to D_{1,2} ({3 \\over 2}) \\ell \\nu ]$, in contradiction with experiment. The same trend follows also from a sum rule for the subleading $1/m_Q$ curent matrix element correction $\\xi_3(1)$. The problem is made explicit in relativistic quarks models \\"},"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/0110372","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2001-10-29T16:17:31Z","cross_cats_sorted":[],"title_canon_sha256":"2112137089f27f433d6d36331ad6ef83edf6a765bbd12ad3c0d9f99d5cdccad5","abstract_canon_sha256":"21e6c759db12862f04c414d7705d14d4402dbb79abb4bc01ee89e952983d130c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T14:28:05.123201Z","signature_b64":"1DOqov4LRs1J/2g0tOlIPay8Ai5lQYcFmLfltnl588po178sR61RagOT0PJ1IyZEKVjLCE9vqg0U8b83+bi+CA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"89dc75cb639a59f6e1267b96708a3066f9c51eaa6ee1d7f63116fbadffc52dc8","last_reissued_at":"2026-07-04T14:28:05.122788Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T14:28:05.122788Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Remarks on sum rules in the heavy quark limit of QCD","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A. Le Yaouanc, J.-C. Raynal, L. Oliver, O. Pene, V. Morenas","submitted_at":"2001-10-29T16:17:31Z","abstract_excerpt":"We underline a problem existing in the heavy quark limit of QCD concerning the rates of semileptonic B decays into P-wave $D_J(j)$ mesons, where $j = {1 \\over 2}$ (wide states) or $j = {3 \\over 2}$ (narrow states). The leading order sum rules of Bjorken and Uraltsev suggest $\\Gamma [ \\bar{B} \\to D_{0,1} ({1 \\over 2}) \\ell \\nu ] \\ll \\Gamma [ \\bar{B} \\to D_{1,2} ({3 \\over 2}) \\ell \\nu ]$, in contradiction with experiment. The same trend follows also from a sum rule for the subleading $1/m_Q$ curent matrix element correction $\\xi_3(1)$. The problem is made explicit in relativistic quarks models \\"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0110372","kind":"arxiv","version":1},"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/0110372/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/0110372","created_at":"2026-07-04T14:28:05.122846+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0110372v1","created_at":"2026-07-04T14:28:05.122846+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0110372","created_at":"2026-07-04T14:28:05.122846+00:00"},{"alias_kind":"pith_short_12","alias_value":"RHOHLS3DTJM7","created_at":"2026-07-04T14:28:05.122846+00:00"},{"alias_kind":"pith_short_16","alias_value":"RHOHLS3DTJM7NYJG","created_at":"2026-07-04T14:28:05.122846+00:00"},{"alias_kind":"pith_short_8","alias_value":"RHOHLS3D","created_at":"2026-07-04T14:28:05.122846+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/RHOHLS3DTJM7NYJGPOLHBCRQM3","json":"https://pith.science/pith/RHOHLS3DTJM7NYJGPOLHBCRQM3.json","graph_json":"https://pith.science/api/pith-number/RHOHLS3DTJM7NYJGPOLHBCRQM3/graph.json","events_json":"https://pith.science/api/pith-number/RHOHLS3DTJM7NYJGPOLHBCRQM3/events.json","paper":"https://pith.science/paper/RHOHLS3D"},"agent_actions":{"view_html":"https://pith.science/pith/RHOHLS3DTJM7NYJGPOLHBCRQM3","download_json":"https://pith.science/pith/RHOHLS3DTJM7NYJGPOLHBCRQM3.json","view_paper":"https://pith.science/paper/RHOHLS3D","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/0110372&json=true","fetch_graph":"https://pith.science/api/pith-number/RHOHLS3DTJM7NYJGPOLHBCRQM3/graph.json","fetch_events":"https://pith.science/api/pith-number/RHOHLS3DTJM7NYJGPOLHBCRQM3/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/RHOHLS3DTJM7NYJGPOLHBCRQM3/action/timestamp_anchor","attest_storage":"https://pith.science/pith/RHOHLS3DTJM7NYJGPOLHBCRQM3/action/storage_attestation","attest_author":"https://pith.science/pith/RHOHLS3DTJM7NYJGPOLHBCRQM3/action/author_attestation","sign_citation":"https://pith.science/pith/RHOHLS3DTJM7NYJGPOLHBCRQM3/action/citation_signature","submit_replication":"https://pith.science/pith/RHOHLS3DTJM7NYJGPOLHBCRQM3/action/replication_record"}},"created_at":"2026-07-04T14:28:05.122846+00:00","updated_at":"2026-07-04T14:28:05.122846+00:00"}