{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2002:GCVPRZOECUVF2B3XHS4WZXWQKC","short_pith_number":"pith:GCVPRZOE","schema_version":"1.0","canonical_sha256":"30aaf8e5c4152a5d07773cb96cded050a5487d1dfd86d4da9c38e78c69900d05","source":{"kind":"arxiv","id":"hep-ph/0201229","version":1},"attestation_state":"computed","paper":{"title":"The Puzzle of the Bottom Quark Production Cross Section","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Edmond L. Berger","submitted_at":"2002-01-24T00:22:54Z","abstract_excerpt":"The production rate of bottom quarks at hadron colliders exceeds the expectations of next-to-leading order perturbative quantum chromodynamics. An additional contribution from pair-production of light gluinos, of mass 12 to 16 GeV, with two-body decays into bottom quarks and light bottom squarks, yields a differential cross section for bottom quarks in better agreement with data. The masses of the gluino and bottom squark are restricted further by the ratio of like-sign to opposite-sign leptons at hadron colliders. Restrictions on this scenario from other data are summarized, and predictions a"},"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/0201229","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2002-01-24T00:22:54Z","cross_cats_sorted":[],"title_canon_sha256":"7d4ba602b2784c1be936526ddce847ad7c0775aab0fe9ac4eb38de1965e9dccf","abstract_canon_sha256":"b9a612a7ab73713fe10b33da538f9b0355547bc49c023f6abaad00851aac8e2c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:36:38.652475Z","signature_b64":"b8zlZ6phxsppmB7rBm1ChCePFeT3Ir5dvis+08dAfYpI+XKr2sBuv/4mU3uIAnTYBJWOkZHWA8gcyFSfZhstAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"30aaf8e5c4152a5d07773cb96cded050a5487d1dfd86d4da9c38e78c69900d05","last_reissued_at":"2026-05-18T02:36:38.651939Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:36:38.651939Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The Puzzle of the Bottom Quark Production Cross Section","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Edmond L. Berger","submitted_at":"2002-01-24T00:22:54Z","abstract_excerpt":"The production rate of bottom quarks at hadron colliders exceeds the expectations of next-to-leading order perturbative quantum chromodynamics. An additional contribution from pair-production of light gluinos, of mass 12 to 16 GeV, with two-body decays into bottom quarks and light bottom squarks, yields a differential cross section for bottom quarks in better agreement with data. The masses of the gluino and bottom squark are restricted further by the ratio of like-sign to opposite-sign leptons at hadron colliders. Restrictions on this scenario from other data are summarized, and predictions a"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0201229","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/0201229","created_at":"2026-05-18T02:36:38.652023+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0201229v1","created_at":"2026-05-18T02:36:38.652023+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0201229","created_at":"2026-05-18T02:36:38.652023+00:00"},{"alias_kind":"pith_short_12","alias_value":"GCVPRZOECUVF","created_at":"2026-05-18T12:25:50.845339+00:00"},{"alias_kind":"pith_short_16","alias_value":"GCVPRZOECUVF2B3X","created_at":"2026-05-18T12:25:50.845339+00:00"},{"alias_kind":"pith_short_8","alias_value":"GCVPRZOE","created_at":"2026-05-18T12:25:50.845339+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/GCVPRZOECUVF2B3XHS4WZXWQKC","json":"https://pith.science/pith/GCVPRZOECUVF2B3XHS4WZXWQKC.json","graph_json":"https://pith.science/api/pith-number/GCVPRZOECUVF2B3XHS4WZXWQKC/graph.json","events_json":"https://pith.science/api/pith-number/GCVPRZOECUVF2B3XHS4WZXWQKC/events.json","paper":"https://pith.science/paper/GCVPRZOE"},"agent_actions":{"view_html":"https://pith.science/pith/GCVPRZOECUVF2B3XHS4WZXWQKC","download_json":"https://pith.science/pith/GCVPRZOECUVF2B3XHS4WZXWQKC.json","view_paper":"https://pith.science/paper/GCVPRZOE","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/0201229&json=true","fetch_graph":"https://pith.science/api/pith-number/GCVPRZOECUVF2B3XHS4WZXWQKC/graph.json","fetch_events":"https://pith.science/api/pith-number/GCVPRZOECUVF2B3XHS4WZXWQKC/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/GCVPRZOECUVF2B3XHS4WZXWQKC/action/timestamp_anchor","attest_storage":"https://pith.science/pith/GCVPRZOECUVF2B3XHS4WZXWQKC/action/storage_attestation","attest_author":"https://pith.science/pith/GCVPRZOECUVF2B3XHS4WZXWQKC/action/author_attestation","sign_citation":"https://pith.science/pith/GCVPRZOECUVF2B3XHS4WZXWQKC/action/citation_signature","submit_replication":"https://pith.science/pith/GCVPRZOECUVF2B3XHS4WZXWQKC/action/replication_record"}},"created_at":"2026-05-18T02:36:38.652023+00:00","updated_at":"2026-05-18T02:36:38.652023+00:00"}