{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1995:WXVXVH3ZYY4ZQHDZZXLJQTOEVI","short_pith_number":"pith:WXVXVH3Z","schema_version":"1.0","canonical_sha256":"b5eb7a9f79c639981c79cdd6984dc4aa0a026730993b1a17893a2ecd8c9b15d3","source":{"kind":"arxiv","id":"hep-ph/9501281","version":1},"attestation_state":"computed","paper":{"title":"Effective Hamiltonian for $B \\ra X_s e^+ e^-$ Beyond Leading Logarithms in the NDR and HV Schemes","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A.J. Buras, M. Muenz","submitted_at":"1995-01-12T12:45:31Z","abstract_excerpt":"We calculate the next-to-leading QCD corrections to the effective Hamiltonian for \\Bsee in the NDR and HV schemes. We give for the first time analytic expressions for the Wilson Coefficient of the operator $Q_9 = (\\bar s b)_{V-A}(\\bar e e)_V$ in the NDR and HV schemes. Calculating the relevant matrix elements of local operators in the spectator model we demonstrate the scheme independence of the resulting short distance contribution to the physical amplitude. Keeping consistently only leading and next-to-leading terms, we find an analytic formula for the differential dilepton invariant mass di"},"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/9501281","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1995-01-12T12:45:31Z","cross_cats_sorted":[],"title_canon_sha256":"cbef11b6da0da671ed8aa4c2086218d2dc477a959d5ce3380467a21fc6649826","abstract_canon_sha256":"ae183e498d5891007e723a22bf9c6b63d2878246354d7f070afc082e0053b922"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:06:34.930458Z","signature_b64":"hRrzxfDu6mFt/+UTvXQEwK4igQ/4VAowvn80nDvswql4RgkvQTa2v7hHRp+FWNl749HLG1loMthexCP/5kSaBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b5eb7a9f79c639981c79cdd6984dc4aa0a026730993b1a17893a2ecd8c9b15d3","last_reissued_at":"2026-05-18T01:06:34.929783Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:06:34.929783Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Effective Hamiltonian for $B \\ra X_s e^+ e^-$ Beyond Leading Logarithms in the NDR and HV Schemes","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A.J. Buras, M. Muenz","submitted_at":"1995-01-12T12:45:31Z","abstract_excerpt":"We calculate the next-to-leading QCD corrections to the effective Hamiltonian for \\Bsee in the NDR and HV schemes. We give for the first time analytic expressions for the Wilson Coefficient of the operator $Q_9 = (\\bar s b)_{V-A}(\\bar e e)_V$ in the NDR and HV schemes. Calculating the relevant matrix elements of local operators in the spectator model we demonstrate the scheme independence of the resulting short distance contribution to the physical amplitude. Keeping consistently only leading and next-to-leading terms, we find an analytic formula for the differential dilepton invariant mass di"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9501281","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":"hep-ph/9501281","created_at":"2026-05-18T01:06:34.929882+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9501281v1","created_at":"2026-05-18T01:06:34.929882+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9501281","created_at":"2026-05-18T01:06:34.929882+00:00"},{"alias_kind":"pith_short_12","alias_value":"WXVXVH3ZYY4Z","created_at":"2026-05-18T12:25:47.700082+00:00"},{"alias_kind":"pith_short_16","alias_value":"WXVXVH3ZYY4ZQHDZ","created_at":"2026-05-18T12:25:47.700082+00:00"},{"alias_kind":"pith_short_8","alias_value":"WXVXVH3Z","created_at":"2026-05-18T12:25:47.700082+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2409.16961","citing_title":"Correlative study of flavor anomalies and dark matter in the light of scalar leptoquark","ref_index":68,"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 the 2HDM","ref_index":49,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/WXVXVH3ZYY4ZQHDZZXLJQTOEVI","json":"https://pith.science/pith/WXVXVH3ZYY4ZQHDZZXLJQTOEVI.json","graph_json":"https://pith.science/api/pith-number/WXVXVH3ZYY4ZQHDZZXLJQTOEVI/graph.json","events_json":"https://pith.science/api/pith-number/WXVXVH3ZYY4ZQHDZZXLJQTOEVI/events.json","paper":"https://pith.science/paper/WXVXVH3Z"},"agent_actions":{"view_html":"https://pith.science/pith/WXVXVH3ZYY4ZQHDZZXLJQTOEVI","download_json":"https://pith.science/pith/WXVXVH3ZYY4ZQHDZZXLJQTOEVI.json","view_paper":"https://pith.science/paper/WXVXVH3Z","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/9501281&json=true","fetch_graph":"https://pith.science/api/pith-number/WXVXVH3ZYY4ZQHDZZXLJQTOEVI/graph.json","fetch_events":"https://pith.science/api/pith-number/WXVXVH3ZYY4ZQHDZZXLJQTOEVI/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/WXVXVH3ZYY4ZQHDZZXLJQTOEVI/action/timestamp_anchor","attest_storage":"https://pith.science/pith/WXVXVH3ZYY4ZQHDZZXLJQTOEVI/action/storage_attestation","attest_author":"https://pith.science/pith/WXVXVH3ZYY4ZQHDZZXLJQTOEVI/action/author_attestation","sign_citation":"https://pith.science/pith/WXVXVH3ZYY4ZQHDZZXLJQTOEVI/action/citation_signature","submit_replication":"https://pith.science/pith/WXVXVH3ZYY4ZQHDZZXLJQTOEVI/action/replication_record"}},"created_at":"2026-05-18T01:06:34.929882+00:00","updated_at":"2026-05-18T01:06:34.929882+00:00"}