{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2001:SLDN3N5IYBD6PAAXP6JUDETXQ5","short_pith_number":"pith:SLDN3N5I","schema_version":"1.0","canonical_sha256":"92c6ddb7a8c047e780177f93419277874870a5706f30fefd3f0e14c2e304fbb4","source":{"kind":"arxiv","id":"hep-ph/0104034","version":2},"attestation_state":"computed","paper":{"title":"Quark mass effects in B -> Xs gamma","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Mikolaj Misiak, Paolo Gambino","submitted_at":"2001-04-03T14:23:22Z","abstract_excerpt":"The charm-loop contribution to B -> Xs gamma is found to be numerically dominant and very stable under logarithmic QCD corrections. The strong enhancement of the branching ratio by QCD logarithms is mainly due to the b-quark mass evolution in the top-quark sector. These observations allow us to achieve better control over residual scale dependence at the next-to-leading order. Furthermore, we observe that the sensitivity of the matrix element < Xs gamma | (sc)_(V-A)(cb)_(V-A) | b > to mc/mb is the source of a sizeable uncertainty that has not been properly taken into account in previous analys"},"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/0104034","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2001-04-03T14:23:22Z","cross_cats_sorted":[],"title_canon_sha256":"512962be3d39ea577da8c19fbdd8bf27cb3517ee876cdc80e7f6668915461580","abstract_canon_sha256":"f60af96eff93f46fd493c7cbe0c7522d8edf56d431d7a241f181842a2d1d94a0"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:18:18.038295Z","signature_b64":"AatQwHuxFmqgGssidovlhcAnvlMEHgRMu4UAdZafS6YH+TfjHc7hXlpSyEnFqcKcQox7d8IB/ZZGrSO9QFkkAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"92c6ddb7a8c047e780177f93419277874870a5706f30fefd3f0e14c2e304fbb4","last_reissued_at":"2026-07-04T15:18:18.037897Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:18:18.037897Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Quark mass effects in B -> Xs gamma","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Mikolaj Misiak, Paolo Gambino","submitted_at":"2001-04-03T14:23:22Z","abstract_excerpt":"The charm-loop contribution to B -> Xs gamma is found to be numerically dominant and very stable under logarithmic QCD corrections. The strong enhancement of the branching ratio by QCD logarithms is mainly due to the b-quark mass evolution in the top-quark sector. These observations allow us to achieve better control over residual scale dependence at the next-to-leading order. Furthermore, we observe that the sensitivity of the matrix element < Xs gamma | (sc)_(V-A)(cb)_(V-A) | b > to mc/mb is the source of a sizeable uncertainty that has not been properly taken into account in previous analys"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0104034","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/hep-ph/0104034/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/0104034","created_at":"2026-07-04T15:18:18.037958+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0104034v2","created_at":"2026-07-04T15:18:18.037958+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0104034","created_at":"2026-07-04T15:18:18.037958+00:00"},{"alias_kind":"pith_short_12","alias_value":"SLDN3N5IYBD6","created_at":"2026-07-04T15:18:18.037958+00:00"},{"alias_kind":"pith_short_16","alias_value":"SLDN3N5IYBD6PAAX","created_at":"2026-07-04T15:18:18.037958+00:00"},{"alias_kind":"pith_short_8","alias_value":"SLDN3N5I","created_at":"2026-07-04T15:18:18.037958+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/SLDN3N5IYBD6PAAXP6JUDETXQ5","json":"https://pith.science/pith/SLDN3N5IYBD6PAAXP6JUDETXQ5.json","graph_json":"https://pith.science/api/pith-number/SLDN3N5IYBD6PAAXP6JUDETXQ5/graph.json","events_json":"https://pith.science/api/pith-number/SLDN3N5IYBD6PAAXP6JUDETXQ5/events.json","paper":"https://pith.science/paper/SLDN3N5I"},"agent_actions":{"view_html":"https://pith.science/pith/SLDN3N5IYBD6PAAXP6JUDETXQ5","download_json":"https://pith.science/pith/SLDN3N5IYBD6PAAXP6JUDETXQ5.json","view_paper":"https://pith.science/paper/SLDN3N5I","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/0104034&json=true","fetch_graph":"https://pith.science/api/pith-number/SLDN3N5IYBD6PAAXP6JUDETXQ5/graph.json","fetch_events":"https://pith.science/api/pith-number/SLDN3N5IYBD6PAAXP6JUDETXQ5/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/SLDN3N5IYBD6PAAXP6JUDETXQ5/action/timestamp_anchor","attest_storage":"https://pith.science/pith/SLDN3N5IYBD6PAAXP6JUDETXQ5/action/storage_attestation","attest_author":"https://pith.science/pith/SLDN3N5IYBD6PAAXP6JUDETXQ5/action/author_attestation","sign_citation":"https://pith.science/pith/SLDN3N5IYBD6PAAXP6JUDETXQ5/action/citation_signature","submit_replication":"https://pith.science/pith/SLDN3N5IYBD6PAAXP6JUDETXQ5/action/replication_record"}},"created_at":"2026-07-04T15:18:18.037958+00:00","updated_at":"2026-07-04T15:18:18.037958+00:00"}