{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2007:MU6UUQIJF35HJFELFH6ITFDGTZ","short_pith_number":"pith:MU6UUQIJ","schema_version":"1.0","canonical_sha256":"653d4a41092efa74948b29fc8994669e669111f35e5769e0ef93b6dc1f14ef8f","source":{"kind":"arxiv","id":"0705.4392","version":2},"attestation_state":"computed","paper":{"title":"Finite-Mass Effects on Inclusive B-Meson Hadroproduction","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"B.A. Kniehl, G. Kramer, H. Spiesberger, I. Schienbein","submitted_at":"2007-05-30T13:26:09Z","abstract_excerpt":"We calculate the transverse-momentum (p_T) distribution for the inclusive hadroproduction of B mesons at intermediate values of p_T at next-to-leading order (NLO) in a dedicated finite-mass scheme using realistic non-perturbative fragmentation functions that are obtained through a global fit to e^+e^- data from CERN LEP1 and SLAC SLC exploiting their universality and scaling violations. We find that finite-mass effects moderately enhance the cross section, by about 20% at p_T = 2 m_b, and rapidly fade out with increasing value of p_T, so that the zero-mass prediction is reached. We also perfor"},"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":"0705.4392","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2007-05-30T13:26:09Z","cross_cats_sorted":[],"title_canon_sha256":"a8168538375a83a42d016033973f73c6724bd55343779a1efb4c431902c936ad","abstract_canon_sha256":"a1b11ef79e035100551f7c81f0df611e013d93845b62246628a8b4a37e446438"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:23:35.509863Z","signature_b64":"5jDK8Lm9BmPCvioEJTtPOCg2aUz7GXtKMPPUygslSgw+rERklrssUhtHHGeKmG4QJo0xCDjmJKis/RnMKVKBAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"653d4a41092efa74948b29fc8994669e669111f35e5769e0ef93b6dc1f14ef8f","last_reissued_at":"2026-07-04T15:23:35.509322Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:23:35.509322Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Finite-Mass Effects on Inclusive B-Meson Hadroproduction","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"B.A. Kniehl, G. Kramer, H. Spiesberger, I. Schienbein","submitted_at":"2007-05-30T13:26:09Z","abstract_excerpt":"We calculate the transverse-momentum (p_T) distribution for the inclusive hadroproduction of B mesons at intermediate values of p_T at next-to-leading order (NLO) in a dedicated finite-mass scheme using realistic non-perturbative fragmentation functions that are obtained through a global fit to e^+e^- data from CERN LEP1 and SLAC SLC exploiting their universality and scaling violations. We find that finite-mass effects moderately enhance the cross section, by about 20% at p_T = 2 m_b, and rapidly fade out with increasing value of p_T, so that the zero-mass prediction is reached. We also perfor"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0705.4392","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/0705.4392/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":"0705.4392","created_at":"2026-07-04T15:23:35.509399+00:00"},{"alias_kind":"arxiv_version","alias_value":"0705.4392v2","created_at":"2026-07-04T15:23:35.509399+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0705.4392","created_at":"2026-07-04T15:23:35.509399+00:00"},{"alias_kind":"pith_short_12","alias_value":"MU6UUQIJF35H","created_at":"2026-07-04T15:23:35.509399+00:00"},{"alias_kind":"pith_short_16","alias_value":"MU6UUQIJF35HJFEL","created_at":"2026-07-04T15:23:35.509399+00:00"},{"alias_kind":"pith_short_8","alias_value":"MU6UUQIJ","created_at":"2026-07-04T15:23:35.509399+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2605.16019","citing_title":"Inclusive charm and bottom quark pair production cross sections at hadron colliders at next-to-next-to-leading-order accuracy","ref_index":23,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/MU6UUQIJF35HJFELFH6ITFDGTZ","json":"https://pith.science/pith/MU6UUQIJF35HJFELFH6ITFDGTZ.json","graph_json":"https://pith.science/api/pith-number/MU6UUQIJF35HJFELFH6ITFDGTZ/graph.json","events_json":"https://pith.science/api/pith-number/MU6UUQIJF35HJFELFH6ITFDGTZ/events.json","paper":"https://pith.science/paper/MU6UUQIJ"},"agent_actions":{"view_html":"https://pith.science/pith/MU6UUQIJF35HJFELFH6ITFDGTZ","download_json":"https://pith.science/pith/MU6UUQIJF35HJFELFH6ITFDGTZ.json","view_paper":"https://pith.science/paper/MU6UUQIJ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=0705.4392&json=true","fetch_graph":"https://pith.science/api/pith-number/MU6UUQIJF35HJFELFH6ITFDGTZ/graph.json","fetch_events":"https://pith.science/api/pith-number/MU6UUQIJF35HJFELFH6ITFDGTZ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/MU6UUQIJF35HJFELFH6ITFDGTZ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/MU6UUQIJF35HJFELFH6ITFDGTZ/action/storage_attestation","attest_author":"https://pith.science/pith/MU6UUQIJF35HJFELFH6ITFDGTZ/action/author_attestation","sign_citation":"https://pith.science/pith/MU6UUQIJF35HJFELFH6ITFDGTZ/action/citation_signature","submit_replication":"https://pith.science/pith/MU6UUQIJF35HJFELFH6ITFDGTZ/action/replication_record"}},"created_at":"2026-07-04T15:23:35.509399+00:00","updated_at":"2026-07-04T15:23:35.509399+00:00"}