{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:JUSLE4FPLCKX4IGARZ6ASVXLQS","short_pith_number":"pith:JUSLE4FP","schema_version":"1.0","canonical_sha256":"4d24b270af58957e20c08e7c0956eb849be905e0f8aab02a20e41dfa5f900340","source":{"kind":"arxiv","id":"1511.09036","version":1},"attestation_state":"computed","paper":{"title":"Perturbative Corrections to $\\Lambda_b \\to \\Lambda$ Form Factors from QCD Light-Cone Sum Rules","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","hep-lat"],"primary_cat":"hep-ph","authors_text":"Yue-Long Shen, Yu-Ming Wang","submitted_at":"2015-11-29T16:24:10Z","abstract_excerpt":"We compute radiative corrections to $\\Lambda_b \\to \\Lambda$ from factors, at next-to-leading logarithmic accuracy, from QCD light-cone sum rules with $\\Lambda_b$-baryon distribution amplitudes. Employing the diagrammatic approach factorization of the vacuum-to-$\\Lambda_b$-baryon correlation function is justified at leading power in $\\Lambda/m_b$, with the aid of the method of regions. Hard functions entering the factorization formulae are identical to the corresponding matching coefficients of heavy-to-light currents from QCD onto soft-collinear effective theory. The universal jet function fro"},"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":"1511.09036","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2015-11-29T16:24:10Z","cross_cats_sorted":["hep-ex","hep-lat"],"title_canon_sha256":"9df142048d3b0004e86f3ad5d583da7e2cf7ee732bb07e81e6e9bd2ce225e99d","abstract_canon_sha256":"db4e40fd174468e67394a2190d3c47f93934b606dc141271cd52221fc7737136"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:18:30.491670Z","signature_b64":"HCRdNb8nUj0ZO0Z8qP6t+7MsxobNNpOqiIKg4mkvzPLFPBqWRNyLmpP9azFQ4zAyNWVraFoHJOCQYSt0xmsGAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4d24b270af58957e20c08e7c0956eb849be905e0f8aab02a20e41dfa5f900340","last_reissued_at":"2026-05-18T01:18:30.491070Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:18:30.491070Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Perturbative Corrections to $\\Lambda_b \\to \\Lambda$ Form Factors from QCD Light-Cone Sum Rules","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","hep-lat"],"primary_cat":"hep-ph","authors_text":"Yue-Long Shen, Yu-Ming Wang","submitted_at":"2015-11-29T16:24:10Z","abstract_excerpt":"We compute radiative corrections to $\\Lambda_b \\to \\Lambda$ from factors, at next-to-leading logarithmic accuracy, from QCD light-cone sum rules with $\\Lambda_b$-baryon distribution amplitudes. Employing the diagrammatic approach factorization of the vacuum-to-$\\Lambda_b$-baryon correlation function is justified at leading power in $\\Lambda/m_b$, with the aid of the method of regions. Hard functions entering the factorization formulae are identical to the corresponding matching coefficients of heavy-to-light currents from QCD onto soft-collinear effective theory. The universal jet function fro"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1511.09036","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":""},"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":"1511.09036","created_at":"2026-05-18T01:18:30.491156+00:00"},{"alias_kind":"arxiv_version","alias_value":"1511.09036v1","created_at":"2026-05-18T01:18:30.491156+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1511.09036","created_at":"2026-05-18T01:18:30.491156+00:00"},{"alias_kind":"pith_short_12","alias_value":"JUSLE4FPLCKX","created_at":"2026-05-18T12:29:27.538025+00:00"},{"alias_kind":"pith_short_16","alias_value":"JUSLE4FPLCKX4IGA","created_at":"2026-05-18T12:29:27.538025+00:00"},{"alias_kind":"pith_short_8","alias_value":"JUSLE4FP","created_at":"2026-05-18T12:29:27.538025+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":2,"sample":[{"citing_arxiv_id":"2512.19429","citing_title":"Semileptonic neutral current decays of $\\Xi_b$ with dileptons or dineutrinos in the final state","ref_index":70,"is_internal_anchor":true},{"citing_arxiv_id":"2602.04311","citing_title":"Analysis of the semileptonic decays $\\Sigma_b\\to\\Sigma_cl\\bar{\\nu}_l$, $\\Xi'_b\\to\\Xi'_cl\\bar{\\nu}_l$ and $\\Omega_b\\to\\Omega_cl\\bar{\\nu}_l$ in QCD sum rules","ref_index":13,"is_internal_anchor":true},{"citing_arxiv_id":"2604.15834","citing_title":"Comprehensive analyses of rare $ \\Lambda_b \\rightarrow \\Lambda \\ell^+ \\ell^-$, $\\Sigma_b \\rightarrow \\Sigma \\ell^+ \\ell^-$ and $\\Xi_b \\rightarrow \\Xi \\ell^+ \\ell^-$ decays in 2HDM","ref_index":54,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/JUSLE4FPLCKX4IGARZ6ASVXLQS","json":"https://pith.science/pith/JUSLE4FPLCKX4IGARZ6ASVXLQS.json","graph_json":"https://pith.science/api/pith-number/JUSLE4FPLCKX4IGARZ6ASVXLQS/graph.json","events_json":"https://pith.science/api/pith-number/JUSLE4FPLCKX4IGARZ6ASVXLQS/events.json","paper":"https://pith.science/paper/JUSLE4FP"},"agent_actions":{"view_html":"https://pith.science/pith/JUSLE4FPLCKX4IGARZ6ASVXLQS","download_json":"https://pith.science/pith/JUSLE4FPLCKX4IGARZ6ASVXLQS.json","view_paper":"https://pith.science/paper/JUSLE4FP","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1511.09036&json=true","fetch_graph":"https://pith.science/api/pith-number/JUSLE4FPLCKX4IGARZ6ASVXLQS/graph.json","fetch_events":"https://pith.science/api/pith-number/JUSLE4FPLCKX4IGARZ6ASVXLQS/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/JUSLE4FPLCKX4IGARZ6ASVXLQS/action/timestamp_anchor","attest_storage":"https://pith.science/pith/JUSLE4FPLCKX4IGARZ6ASVXLQS/action/storage_attestation","attest_author":"https://pith.science/pith/JUSLE4FPLCKX4IGARZ6ASVXLQS/action/author_attestation","sign_citation":"https://pith.science/pith/JUSLE4FPLCKX4IGARZ6ASVXLQS/action/citation_signature","submit_replication":"https://pith.science/pith/JUSLE4FPLCKX4IGARZ6ASVXLQS/action/replication_record"}},"created_at":"2026-05-18T01:18:30.491156+00:00","updated_at":"2026-05-18T01:18:30.491156+00:00"}