{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2001:D4M5YV4BU6QFBSAFP32VS3KLKE","short_pith_number":"pith:D4M5YV4B","schema_version":"1.0","canonical_sha256":"1f19dc5781a7a050c8057ef5596d4b51025c06a20f6e23c0a0527089fa404ab3","source":{"kind":"arxiv","id":"hep-ex/0102049","version":1},"attestation_state":"computed","paper":{"title":"Precise Measurement of Dimuon Production Cross-Sections in muon neutrino Fe and muon antineutrino Fe Deep Inelastic Scattering at the Tevatron","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"et al, NuTeV Collaboration: M. Goncharov, P.Spentzouris","submitted_at":"2001-02-26T16:41:12Z","abstract_excerpt":"We present measurements of the semi-inclusive cross-sections for muon neutrino and muon antineutrino-nucleon deep inelastic scattering interactions with two oppositely charged muons in the final state. These events dominantly arise from production of a charm quark during the scattering process. The measurement was obtained from the analysis of 5102 muon neutrino-induced and 1458 muon antineutrino-induced events collected with the NuTeV detector exposed to a sign-selected beam at the Fermilab Tevatron. We also extract a cross-section measurement from a re-analysis of 5030 muon neutrino-induced "},"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-ex/0102049","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ex","submitted_at":"2001-02-26T16:41:12Z","cross_cats_sorted":[],"title_canon_sha256":"640fd761dc60cfbb2a766e5042be4e249252e798aac6fc3a03bebfc04ad0aa4c","abstract_canon_sha256":"d1e349c3a33e6dd1225862a38afa6bbf560aa5ce7d6cb9330d521d3a4f2f236f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:29:22.294347Z","signature_b64":"JiL4NWNIsYZOYIUMHJzobnIxBwbycowr/34epmyy4KBbU+6JA1o/YxXXnAPrK0dbxVB5SaypdKmCykZfuPXZCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1f19dc5781a7a050c8057ef5596d4b51025c06a20f6e23c0a0527089fa404ab3","last_reissued_at":"2026-07-04T15:29:22.293912Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:29:22.293912Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Precise Measurement of Dimuon Production Cross-Sections in muon neutrino Fe and muon antineutrino Fe Deep Inelastic Scattering at the Tevatron","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"et al, NuTeV Collaboration: M. Goncharov, P.Spentzouris","submitted_at":"2001-02-26T16:41:12Z","abstract_excerpt":"We present measurements of the semi-inclusive cross-sections for muon neutrino and muon antineutrino-nucleon deep inelastic scattering interactions with two oppositely charged muons in the final state. These events dominantly arise from production of a charm quark during the scattering process. The measurement was obtained from the analysis of 5102 muon neutrino-induced and 1458 muon antineutrino-induced events collected with the NuTeV detector exposed to a sign-selected beam at the Fermilab Tevatron. We also extract a cross-section measurement from a re-analysis of 5030 muon neutrino-induced "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ex/0102049","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-ex/0102049/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-ex/0102049","created_at":"2026-07-04T15:29:22.293988+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ex/0102049v1","created_at":"2026-07-04T15:29:22.293988+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ex/0102049","created_at":"2026-07-04T15:29:22.293988+00:00"},{"alias_kind":"pith_short_12","alias_value":"D4M5YV4BU6QF","created_at":"2026-07-04T15:29:22.293988+00:00"},{"alias_kind":"pith_short_16","alias_value":"D4M5YV4BU6QFBSAF","created_at":"2026-07-04T15:29:22.293988+00:00"},{"alias_kind":"pith_short_8","alias_value":"D4M5YV4B","created_at":"2026-07-04T15:29:22.293988+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":7,"internal_anchor_count":7,"sample":[{"citing_arxiv_id":"2606.26056","citing_title":"Impact of parity-violating deep-inelastic scattering on the weak mixing angle and high-$x$ parton distributions","ref_index":38,"is_internal_anchor":true},{"citing_arxiv_id":"2606.08830","citing_title":"Nuclear parton distributions and nuclear shadowing","ref_index":133,"is_internal_anchor":true},{"citing_arxiv_id":"1907.08147","citing_title":"Updates of PDFs in the MMHT framework","ref_index":6,"is_internal_anchor":true},{"citing_arxiv_id":"2412.12076","citing_title":"Predictions for dimuon production in high-energy neutrino-proton collisions using the color dipole model","ref_index":12,"is_internal_anchor":true},{"citing_arxiv_id":"2510.26260","citing_title":"Letter of Intent: The Forward Physics Facility","ref_index":27,"is_internal_anchor":true},{"citing_arxiv_id":"1912.10053","citing_title":"New CTEQ global analysis of quantum chromodynamics with high-precision data from the LHC","ref_index":70,"is_internal_anchor":true},{"citing_arxiv_id":"2507.16913","citing_title":"A linear PDF model for Bayesian inference","ref_index":60,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/D4M5YV4BU6QFBSAFP32VS3KLKE","json":"https://pith.science/pith/D4M5YV4BU6QFBSAFP32VS3KLKE.json","graph_json":"https://pith.science/api/pith-number/D4M5YV4BU6QFBSAFP32VS3KLKE/graph.json","events_json":"https://pith.science/api/pith-number/D4M5YV4BU6QFBSAFP32VS3KLKE/events.json","paper":"https://pith.science/paper/D4M5YV4B"},"agent_actions":{"view_html":"https://pith.science/pith/D4M5YV4BU6QFBSAFP32VS3KLKE","download_json":"https://pith.science/pith/D4M5YV4BU6QFBSAFP32VS3KLKE.json","view_paper":"https://pith.science/paper/D4M5YV4B","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ex/0102049&json=true","fetch_graph":"https://pith.science/api/pith-number/D4M5YV4BU6QFBSAFP32VS3KLKE/graph.json","fetch_events":"https://pith.science/api/pith-number/D4M5YV4BU6QFBSAFP32VS3KLKE/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/D4M5YV4BU6QFBSAFP32VS3KLKE/action/timestamp_anchor","attest_storage":"https://pith.science/pith/D4M5YV4BU6QFBSAFP32VS3KLKE/action/storage_attestation","attest_author":"https://pith.science/pith/D4M5YV4BU6QFBSAFP32VS3KLKE/action/author_attestation","sign_citation":"https://pith.science/pith/D4M5YV4BU6QFBSAFP32VS3KLKE/action/citation_signature","submit_replication":"https://pith.science/pith/D4M5YV4BU6QFBSAFP32VS3KLKE/action/replication_record"}},"created_at":"2026-07-04T15:29:22.293988+00:00","updated_at":"2026-07-04T15:29:22.293988+00:00"}