{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:MFV2CKN3U53QV5XNE7EPLYAVOB","short_pith_number":"pith:MFV2CKN3","schema_version":"1.0","canonical_sha256":"616ba129bba7770af6ed27c8f5e0157063eda72f66a39266fe23da04bd0403ee","source":{"kind":"arxiv","id":"1107.0975","version":2},"attestation_state":"computed","paper":{"title":"Updated Status of the Global Electroweak Fit and Constraints on New Physics","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A. Hoecker, D. Kennedy, J. Haller, J. Stelzer, K. Moenig, M. Baak, M. Goebel, M. Schott","submitted_at":"2011-07-05T20:00:05Z","abstract_excerpt":"We present an update of the Standard Model fit to electroweak precision data. We include newest experimental results on the top quark mass, the W mass and width, and the Higgs boson mass bounds from LEP, Tevatron and the LHC. We also include a new determination of the electromagnetic coupling strength at the Z pole. We find for the Higgs boson mass (91 +30 -23) GeV and (120 +12 -5) GeV when not including and including the direct Higgs searches, respectively. From the latter fit we indirectly determine the W mass to be (80.360 +0.014 -0.013) GeV. We exploit the data to determine experimental co"},"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":"1107.0975","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2011-07-05T20:00:05Z","cross_cats_sorted":[],"title_canon_sha256":"b66f67cac5425042d38fe79568cf25b307d1ad677613db22daa2756f0c1d7f25","abstract_canon_sha256":"c059e16a338f3a0eee31fbf6d99e986a90bedb1c79cac40cca5b0230f34831ac"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T04:42:28.342363Z","signature_b64":"uTT/CGO//DyXw2cxe5CPPlo4XRr9oiFp5YW/x/zT8xocwR5/dKi9RWv67Am4z+nT2mjDEy5hO55PyG6K7OAuBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"616ba129bba7770af6ed27c8f5e0157063eda72f66a39266fe23da04bd0403ee","last_reissued_at":"2026-07-05T04:42:28.341845Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T04:42:28.341845Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Updated Status of the Global Electroweak Fit and Constraints on New Physics","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A. Hoecker, D. Kennedy, J. Haller, J. Stelzer, K. Moenig, M. Baak, M. Goebel, M. Schott","submitted_at":"2011-07-05T20:00:05Z","abstract_excerpt":"We present an update of the Standard Model fit to electroweak precision data. We include newest experimental results on the top quark mass, the W mass and width, and the Higgs boson mass bounds from LEP, Tevatron and the LHC. We also include a new determination of the electromagnetic coupling strength at the Z pole. We find for the Higgs boson mass (91 +30 -23) GeV and (120 +12 -5) GeV when not including and including the direct Higgs searches, respectively. From the latter fit we indirectly determine the W mass to be (80.360 +0.014 -0.013) GeV. We exploit the data to determine experimental co"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1107.0975","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/1107.0975/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":"1107.0975","created_at":"2026-07-05T04:42:28.341905+00:00"},{"alias_kind":"arxiv_version","alias_value":"1107.0975v2","created_at":"2026-07-05T04:42:28.341905+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1107.0975","created_at":"2026-07-05T04:42:28.341905+00:00"},{"alias_kind":"pith_short_12","alias_value":"MFV2CKN3U53Q","created_at":"2026-07-05T04:42:28.341905+00:00"},{"alias_kind":"pith_short_16","alias_value":"MFV2CKN3U53QV5XN","created_at":"2026-07-05T04:42:28.341905+00:00"},{"alias_kind":"pith_short_8","alias_value":"MFV2CKN3","created_at":"2026-07-05T04:42:28.341905+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/MFV2CKN3U53QV5XNE7EPLYAVOB","json":"https://pith.science/pith/MFV2CKN3U53QV5XNE7EPLYAVOB.json","graph_json":"https://pith.science/api/pith-number/MFV2CKN3U53QV5XNE7EPLYAVOB/graph.json","events_json":"https://pith.science/api/pith-number/MFV2CKN3U53QV5XNE7EPLYAVOB/events.json","paper":"https://pith.science/paper/MFV2CKN3"},"agent_actions":{"view_html":"https://pith.science/pith/MFV2CKN3U53QV5XNE7EPLYAVOB","download_json":"https://pith.science/pith/MFV2CKN3U53QV5XNE7EPLYAVOB.json","view_paper":"https://pith.science/paper/MFV2CKN3","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1107.0975&json=true","fetch_graph":"https://pith.science/api/pith-number/MFV2CKN3U53QV5XNE7EPLYAVOB/graph.json","fetch_events":"https://pith.science/api/pith-number/MFV2CKN3U53QV5XNE7EPLYAVOB/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/MFV2CKN3U53QV5XNE7EPLYAVOB/action/timestamp_anchor","attest_storage":"https://pith.science/pith/MFV2CKN3U53QV5XNE7EPLYAVOB/action/storage_attestation","attest_author":"https://pith.science/pith/MFV2CKN3U53QV5XNE7EPLYAVOB/action/author_attestation","sign_citation":"https://pith.science/pith/MFV2CKN3U53QV5XNE7EPLYAVOB/action/citation_signature","submit_replication":"https://pith.science/pith/MFV2CKN3U53QV5XNE7EPLYAVOB/action/replication_record"}},"created_at":"2026-07-05T04:42:28.341905+00:00","updated_at":"2026-07-05T04:42:28.341905+00:00"}