{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2002:IJOIMRRKRGAUFC5XGJTPHJIPR2","short_pith_number":"pith:IJOIMRRK","schema_version":"1.0","canonical_sha256":"425c86462a8981428bb73266f3a50f8e940458ef7cf3cd55e18eb5eeb60b7f42","source":{"kind":"arxiv","id":"hep-ex/0210031","version":2},"attestation_state":"computed","paper":{"title":"Inclusive Analysis of the b Quark Fragmentation Function in Z Decays at LEP","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"The OPAL collaboration","submitted_at":"2002-10-11T14:36:10Z","abstract_excerpt":"A study of b quark hadronisation is presented using inclusively reconstructed B hadrons in about four million hadronic Z decays recorded in 1992-2000 with the OPAL detector at LEP. The data are compared to different theoretical models, and fragmentation function parameters of these models are fitted. The average scaled energy of weakly decaying B hadrons is determined to be <xe>=0.7193+-0.0016(stat)+0.0036-0.0031(syst)"},"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/0210031","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ex","submitted_at":"2002-10-11T14:36:10Z","cross_cats_sorted":[],"title_canon_sha256":"e60e6305c5cf35be1c0ce03d699041a5187f09c576c7e65cdf555d4b39b6423e","abstract_canon_sha256":"0cfa631f8917b6b4c181b3049307e5a13f9a65e0c9519796d8489733a46f2b15"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:47:32.237563Z","signature_b64":"uV4Ga9NV4oK8mI3Sye847akvh6xWNHRfgrfuzgSuQNxMjaL0FyMLdW//RDxGODFasgasr573j1h63wySktRFDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"425c86462a8981428bb73266f3a50f8e940458ef7cf3cd55e18eb5eeb60b7f42","last_reissued_at":"2026-05-18T03:47:32.237136Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:47:32.237136Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Inclusive Analysis of the b Quark Fragmentation Function in Z Decays at LEP","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"The OPAL collaboration","submitted_at":"2002-10-11T14:36:10Z","abstract_excerpt":"A study of b quark hadronisation is presented using inclusively reconstructed B hadrons in about four million hadronic Z decays recorded in 1992-2000 with the OPAL detector at LEP. The data are compared to different theoretical models, and fragmentation function parameters of these models are fitted. The average scaled energy of weakly decaying B hadrons is determined to be <xe>=0.7193+-0.0016(stat)+0.0036-0.0031(syst)"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ex/0210031","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-ex/0210031","created_at":"2026-05-18T03:47:32.237198+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ex/0210031v2","created_at":"2026-05-18T03:47:32.237198+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ex/0210031","created_at":"2026-05-18T03:47:32.237198+00:00"},{"alias_kind":"pith_short_12","alias_value":"IJOIMRRKRGAU","created_at":"2026-05-18T12:25:50.845339+00:00"},{"alias_kind":"pith_short_16","alias_value":"IJOIMRRKRGAUFC5X","created_at":"2026-05-18T12:25:50.845339+00:00"},{"alias_kind":"pith_short_8","alias_value":"IJOIMRRK","created_at":"2026-05-18T12:25:50.845339+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":3,"sample":[{"citing_arxiv_id":"2511.10666","citing_title":"Jet fragmentation function and groomed substructure of bottom quark jets in proton-proton collisions at 5.02 TeV","ref_index":22,"is_internal_anchor":true},{"citing_arxiv_id":"2511.10216","citing_title":"Measurement of charged-hadron distributions in heavy-flavor jets in proton-proton collisions at $\\sqrt{s}$=13 TeV","ref_index":16,"is_internal_anchor":true},{"citing_arxiv_id":"2511.23091","citing_title":"Measurement of the top-quark mass using decays with a $J/\\psi$ meson at $\\sqrt{s}=$13 TeV with the ATLAS detector","ref_index":49,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/IJOIMRRKRGAUFC5XGJTPHJIPR2","json":"https://pith.science/pith/IJOIMRRKRGAUFC5XGJTPHJIPR2.json","graph_json":"https://pith.science/api/pith-number/IJOIMRRKRGAUFC5XGJTPHJIPR2/graph.json","events_json":"https://pith.science/api/pith-number/IJOIMRRKRGAUFC5XGJTPHJIPR2/events.json","paper":"https://pith.science/paper/IJOIMRRK"},"agent_actions":{"view_html":"https://pith.science/pith/IJOIMRRKRGAUFC5XGJTPHJIPR2","download_json":"https://pith.science/pith/IJOIMRRKRGAUFC5XGJTPHJIPR2.json","view_paper":"https://pith.science/paper/IJOIMRRK","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ex/0210031&json=true","fetch_graph":"https://pith.science/api/pith-number/IJOIMRRKRGAUFC5XGJTPHJIPR2/graph.json","fetch_events":"https://pith.science/api/pith-number/IJOIMRRKRGAUFC5XGJTPHJIPR2/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/IJOIMRRKRGAUFC5XGJTPHJIPR2/action/timestamp_anchor","attest_storage":"https://pith.science/pith/IJOIMRRKRGAUFC5XGJTPHJIPR2/action/storage_attestation","attest_author":"https://pith.science/pith/IJOIMRRKRGAUFC5XGJTPHJIPR2/action/author_attestation","sign_citation":"https://pith.science/pith/IJOIMRRKRGAUFC5XGJTPHJIPR2/action/citation_signature","submit_replication":"https://pith.science/pith/IJOIMRRKRGAUFC5XGJTPHJIPR2/action/replication_record"}},"created_at":"2026-05-18T03:47:32.237198+00:00","updated_at":"2026-05-18T03:47:32.237198+00:00"}