{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2010:URKOXVAKMPNPJZUKAW3P64N5RA","short_pith_number":"pith:URKOXVAK","schema_version":"1.0","canonical_sha256":"a454ebd40a63daf4e68a05b6ff71bd88175c74c65e690924f1bde4aac5b8f536","source":{"kind":"arxiv","id":"1003.2826","version":1},"attestation_state":"computed","paper":{"title":"Combination of CDF and D0 Results on the Width of the W boson","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"The Tevatron Electroweak Working Group","submitted_at":"2010-03-14T21:51:16Z","abstract_excerpt":"We summarize and combine  direct measurements of the width of the W boson in data collected by the Tevatron experiments CDF and D0 at Fermilab. Results from CDF and D0 RunI (1992-1995)  have been combined with  the CDF 200 pb^-1 results from the first period of RunII (2001-2004) and the recent 1 fb^-1 result in the electron channel from D0 (2002-2006). The results are corrected  for any inconsistencies in parton distribution functions and assumptions about electroweak parameters used in the different analyses.  The resulting Tevatron average for the width of the W boson is Gamma_W =  2,046 +- "},"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":"1003.2826","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ex","submitted_at":"2010-03-14T21:51:16Z","cross_cats_sorted":[],"title_canon_sha256":"c01215c7ff9f8efaf80873259d57bbf7c8d24436edaf0768a5eb90f5d65d5551","abstract_canon_sha256":"aa313ee889964c1184bcaf76181de022f88233de4685c0fde70f42c2798c5523"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:48:01.592256Z","signature_b64":"2iyewDrUGAnnnorPa76kdBpVNe4ouV8V12cOTycJJHbnImZpX+b8Yh99/Ig522jCBQonYjQR8v15bFYC1w9+Bw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a454ebd40a63daf4e68a05b6ff71bd88175c74c65e690924f1bde4aac5b8f536","last_reissued_at":"2026-05-18T03:48:01.591835Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:48:01.591835Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Combination of CDF and D0 Results on the Width of the W boson","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"The Tevatron Electroweak Working Group","submitted_at":"2010-03-14T21:51:16Z","abstract_excerpt":"We summarize and combine  direct measurements of the width of the W boson in data collected by the Tevatron experiments CDF and D0 at Fermilab. Results from CDF and D0 RunI (1992-1995)  have been combined with  the CDF 200 pb^-1 results from the first period of RunII (2001-2004) and the recent 1 fb^-1 result in the electron channel from D0 (2002-2006). The results are corrected  for any inconsistencies in parton distribution functions and assumptions about electroweak parameters used in the different analyses.  The resulting Tevatron average for the width of the W boson is Gamma_W =  2,046 +- "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1003.2826","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":"1003.2826","created_at":"2026-05-18T03:48:01.591903+00:00"},{"alias_kind":"arxiv_version","alias_value":"1003.2826v1","created_at":"2026-05-18T03:48:01.591903+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1003.2826","created_at":"2026-05-18T03:48:01.591903+00:00"},{"alias_kind":"pith_short_12","alias_value":"URKOXVAKMPNP","created_at":"2026-05-18T12:26:15.391820+00:00"},{"alias_kind":"pith_short_16","alias_value":"URKOXVAKMPNPJZUK","created_at":"2026-05-18T12:26:15.391820+00:00"},{"alias_kind":"pith_short_8","alias_value":"URKOXVAK","created_at":"2026-05-18T12:26:15.391820+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2504.02958","citing_title":"Combined effective field theory interpretation of Higgs boson, electroweak vector boson, top quark, and multi-jet measurements","ref_index":79,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/URKOXVAKMPNPJZUKAW3P64N5RA","json":"https://pith.science/pith/URKOXVAKMPNPJZUKAW3P64N5RA.json","graph_json":"https://pith.science/api/pith-number/URKOXVAKMPNPJZUKAW3P64N5RA/graph.json","events_json":"https://pith.science/api/pith-number/URKOXVAKMPNPJZUKAW3P64N5RA/events.json","paper":"https://pith.science/paper/URKOXVAK"},"agent_actions":{"view_html":"https://pith.science/pith/URKOXVAKMPNPJZUKAW3P64N5RA","download_json":"https://pith.science/pith/URKOXVAKMPNPJZUKAW3P64N5RA.json","view_paper":"https://pith.science/paper/URKOXVAK","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1003.2826&json=true","fetch_graph":"https://pith.science/api/pith-number/URKOXVAKMPNPJZUKAW3P64N5RA/graph.json","fetch_events":"https://pith.science/api/pith-number/URKOXVAKMPNPJZUKAW3P64N5RA/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/URKOXVAKMPNPJZUKAW3P64N5RA/action/timestamp_anchor","attest_storage":"https://pith.science/pith/URKOXVAKMPNPJZUKAW3P64N5RA/action/storage_attestation","attest_author":"https://pith.science/pith/URKOXVAKMPNPJZUKAW3P64N5RA/action/author_attestation","sign_citation":"https://pith.science/pith/URKOXVAKMPNPJZUKAW3P64N5RA/action/citation_signature","submit_replication":"https://pith.science/pith/URKOXVAKMPNPJZUKAW3P64N5RA/action/replication_record"}},"created_at":"2026-05-18T03:48:01.591903+00:00","updated_at":"2026-05-18T03:48:01.591903+00:00"}