{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1993:NXBW6V7TWND72AYBCWWGP3LB7L","short_pith_number":"pith:NXBW6V7T","schema_version":"1.0","canonical_sha256":"6dc36f57f3b347fd030115ac67ed61facfe4bb7e82c1d1447e8ec411ff9569ce","source":{"kind":"arxiv","id":"hep-ph/9312318","version":2},"attestation_state":"computed","paper":{"title":"Leptoproduction of Heavy Quarks I-- General Formalism and Kinematics of Charged Current and Neutral Current Production Processes","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Fredrick I. Olness, M. A. G. Aivazis, Wu-Ki Tung","submitted_at":"1993-12-21T04:42:47Z","abstract_excerpt":"Existing calculations of heavy quark production in charged-current and neutral current lepton-hadron scattering are formulated differently because of the artificial distinction of ``light'' and ``heavy'' quarks made in the traditional approach. A proper QCD formalism valid for a wide kinematic range from near threshold to energies much higher then the quark mass should treat these processes in a uniform way. We formulate a unified approach to both types of leptoproduction processes based on the conventional factorization theorem. In this paper, we present the general framework with complete ki"},"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/9312318","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1993-12-21T04:42:47Z","cross_cats_sorted":[],"title_canon_sha256":"e2a1ab46de9082ae833dbb6bfbbf65df7f2338978b7ecbcf96df2bc8e0ed8b89","abstract_canon_sha256":"c0c6691c83f31bf3c5c2b497926ebb052a678910e81db0c5e6871eab79f1b8ee"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:37:54.211655Z","signature_b64":"9iMbsZ7PsekEXALQW+tol1KiZXlhrZNsPQc/CtCPOX1yMDbp63GLyWFYxzcgEJLFltuGbTCtVDErX/BjVAqvCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6dc36f57f3b347fd030115ac67ed61facfe4bb7e82c1d1447e8ec411ff9569ce","last_reissued_at":"2026-05-18T04:37:54.211024Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:37:54.211024Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Leptoproduction of Heavy Quarks I-- General Formalism and Kinematics of Charged Current and Neutral Current Production Processes","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Fredrick I. Olness, M. A. G. Aivazis, Wu-Ki Tung","submitted_at":"1993-12-21T04:42:47Z","abstract_excerpt":"Existing calculations of heavy quark production in charged-current and neutral current lepton-hadron scattering are formulated differently because of the artificial distinction of ``light'' and ``heavy'' quarks made in the traditional approach. A proper QCD formalism valid for a wide kinematic range from near threshold to energies much higher then the quark mass should treat these processes in a uniform way. We formulate a unified approach to both types of leptoproduction processes based on the conventional factorization theorem. In this paper, we present the general framework with complete ki"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9312318","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":""},"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/9312318","created_at":"2026-05-18T04:37:54.211116+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9312318v2","created_at":"2026-05-18T04:37:54.211116+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9312318","created_at":"2026-05-18T04:37:54.211116+00:00"},{"alias_kind":"pith_short_12","alias_value":"NXBW6V7TWND7","created_at":"2026-05-18T12:25:47.102015+00:00"},{"alias_kind":"pith_short_16","alias_value":"NXBW6V7TWND72AYB","created_at":"2026-05-18T12:25:47.102015+00:00"},{"alias_kind":"pith_short_8","alias_value":"NXBW6V7T","created_at":"2026-05-18T12:25:47.102015+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":2,"sample":[{"citing_arxiv_id":"1912.10053","citing_title":"New CTEQ global analysis of quantum chromodynamics with high-precision data from the LHC","ref_index":118,"is_internal_anchor":true},{"citing_arxiv_id":"2605.05880","citing_title":"Top-associated Higgs-boson production using perturbative fragmentation functions at next-to-leading-order","ref_index":39,"is_internal_anchor":true},{"citing_arxiv_id":"2605.05880","citing_title":"Top-associated Higgs-boson production using perturbative fragmentation functions at next-to-leading-order","ref_index":39,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/NXBW6V7TWND72AYBCWWGP3LB7L","json":"https://pith.science/pith/NXBW6V7TWND72AYBCWWGP3LB7L.json","graph_json":"https://pith.science/api/pith-number/NXBW6V7TWND72AYBCWWGP3LB7L/graph.json","events_json":"https://pith.science/api/pith-number/NXBW6V7TWND72AYBCWWGP3LB7L/events.json","paper":"https://pith.science/paper/NXBW6V7T"},"agent_actions":{"view_html":"https://pith.science/pith/NXBW6V7TWND72AYBCWWGP3LB7L","download_json":"https://pith.science/pith/NXBW6V7TWND72AYBCWWGP3LB7L.json","view_paper":"https://pith.science/paper/NXBW6V7T","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/9312318&json=true","fetch_graph":"https://pith.science/api/pith-number/NXBW6V7TWND72AYBCWWGP3LB7L/graph.json","fetch_events":"https://pith.science/api/pith-number/NXBW6V7TWND72AYBCWWGP3LB7L/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/NXBW6V7TWND72AYBCWWGP3LB7L/action/timestamp_anchor","attest_storage":"https://pith.science/pith/NXBW6V7TWND72AYBCWWGP3LB7L/action/storage_attestation","attest_author":"https://pith.science/pith/NXBW6V7TWND72AYBCWWGP3LB7L/action/author_attestation","sign_citation":"https://pith.science/pith/NXBW6V7TWND72AYBCWWGP3LB7L/action/citation_signature","submit_replication":"https://pith.science/pith/NXBW6V7TWND72AYBCWWGP3LB7L/action/replication_record"}},"created_at":"2026-05-18T04:37:54.211116+00:00","updated_at":"2026-05-18T04:37:54.211116+00:00"}