{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2010:EKAXSJBO3X4CICPCOTSIFU6RNV","short_pith_number":"pith:EKAXSJBO","schema_version":"1.0","canonical_sha256":"228179242eddf82409e274e482d3d16d67dc4f294cf474da85c85d7ccf7c8a8d","source":{"kind":"arxiv","id":"1001.4162","version":3},"attestation_state":"computed","paper":{"title":"Combination of Tevatron searches for the standard model Higgs boson in the W+W- decay mode","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"et al, the CDF, the D0 Collaborations: T. Aaltonen","submitted_at":"2010-01-25T20:20:59Z","abstract_excerpt":"We combine searches by the CDF and D0 collaborations for a Higgs boson decaying to W+W-. The data correspond to an integrated total luminosity of 4.8 (CDF) and 5.4 (D0) fb-1 of p-pbar collisions at sqrt{s}=1.96 TeV at the Fermilab Tevatron collider. No excess is observed above background expectation, and resulting limits on Higgs boson production exclude a standard-model Higgs boson in the mass range 162-166 GeV at the 95% C.L."},"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":"1001.4162","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ex","submitted_at":"2010-01-25T20:20:59Z","cross_cats_sorted":[],"title_canon_sha256":"c54f3fe649aab89366ae45c6a8fc2564d51abc8d46339cd93835a21175254344","abstract_canon_sha256":"7f0b4c3cb4c012d062cca9df04ad62cc0c81fb13352c8b5bdd8f75cba4c5aee0"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:48:01.694581Z","signature_b64":"hnnE6gm+OXQku+DgGlAZIHlfOOrDhBVdSTBu5u6Ifzaam0KvWW8ZWIUAzvI78EUtRSLKe8lF7Zf79TUFMiT6Aw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"228179242eddf82409e274e482d3d16d67dc4f294cf474da85c85d7ccf7c8a8d","last_reissued_at":"2026-05-18T03:48:01.694193Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:48:01.694193Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Combination of Tevatron searches for the standard model Higgs boson in the W+W- decay mode","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"et al, the CDF, the D0 Collaborations: T. Aaltonen","submitted_at":"2010-01-25T20:20:59Z","abstract_excerpt":"We combine searches by the CDF and D0 collaborations for a Higgs boson decaying to W+W-. The data correspond to an integrated total luminosity of 4.8 (CDF) and 5.4 (D0) fb-1 of p-pbar collisions at sqrt{s}=1.96 TeV at the Fermilab Tevatron collider. No excess is observed above background expectation, and resulting limits on Higgs boson production exclude a standard-model Higgs boson in the mass range 162-166 GeV at the 95% C.L."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1001.4162","kind":"arxiv","version":3},"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":"1001.4162","created_at":"2026-05-18T03:48:01.694260+00:00"},{"alias_kind":"arxiv_version","alias_value":"1001.4162v3","created_at":"2026-05-18T03:48:01.694260+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1001.4162","created_at":"2026-05-18T03:48:01.694260+00:00"},{"alias_kind":"pith_short_12","alias_value":"EKAXSJBO3X4C","created_at":"2026-05-18T12:26:06.534383+00:00"},{"alias_kind":"pith_short_16","alias_value":"EKAXSJBO3X4CICPC","created_at":"2026-05-18T12:26:06.534383+00:00"},{"alias_kind":"pith_short_8","alias_value":"EKAXSJBO","created_at":"2026-05-18T12:26:06.534383+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"1007.1727","citing_title":"Asymptotic formulae for likelihood-based tests of new physics","ref_index":10,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/EKAXSJBO3X4CICPCOTSIFU6RNV","json":"https://pith.science/pith/EKAXSJBO3X4CICPCOTSIFU6RNV.json","graph_json":"https://pith.science/api/pith-number/EKAXSJBO3X4CICPCOTSIFU6RNV/graph.json","events_json":"https://pith.science/api/pith-number/EKAXSJBO3X4CICPCOTSIFU6RNV/events.json","paper":"https://pith.science/paper/EKAXSJBO"},"agent_actions":{"view_html":"https://pith.science/pith/EKAXSJBO3X4CICPCOTSIFU6RNV","download_json":"https://pith.science/pith/EKAXSJBO3X4CICPCOTSIFU6RNV.json","view_paper":"https://pith.science/paper/EKAXSJBO","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1001.4162&json=true","fetch_graph":"https://pith.science/api/pith-number/EKAXSJBO3X4CICPCOTSIFU6RNV/graph.json","fetch_events":"https://pith.science/api/pith-number/EKAXSJBO3X4CICPCOTSIFU6RNV/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/EKAXSJBO3X4CICPCOTSIFU6RNV/action/timestamp_anchor","attest_storage":"https://pith.science/pith/EKAXSJBO3X4CICPCOTSIFU6RNV/action/storage_attestation","attest_author":"https://pith.science/pith/EKAXSJBO3X4CICPCOTSIFU6RNV/action/author_attestation","sign_citation":"https://pith.science/pith/EKAXSJBO3X4CICPCOTSIFU6RNV/action/citation_signature","submit_replication":"https://pith.science/pith/EKAXSJBO3X4CICPCOTSIFU6RNV/action/replication_record"}},"created_at":"2026-05-18T03:48:01.694260+00:00","updated_at":"2026-05-18T03:48:01.694260+00:00"}