{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2010:GDCPQD3C45FXHOL4GEZ42BVZ76","short_pith_number":"pith:GDCPQD3C","schema_version":"1.0","canonical_sha256":"30c4f80f62e74b73b97c3133cd06b9ff8fba3584bc8a758ef19a8bcfb0b4ca8b","source":{"kind":"arxiv","id":"1001.4468","version":2},"attestation_state":"computed","paper":{"title":"Inclusive Search for Standard Model Higgs Boson Production in the WW Decay Channel using the CDF II Detector","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"et al, The CDF Collaboration: T. Aaltonen","submitted_at":"2010-01-25T19:36:12Z","abstract_excerpt":"We present a search for standard model (SM) Higgs boson production using ppbar collision data at sqrt(s) = 1.96 TeV, collected with the CDF II detector and corresponding to an integrated luminosity of 4.8 fb-1. We search for Higgs bosons produced in all processes with a significant production rate and decaying to two W bosons. We find no evidence for SM Higgs boson production and place upper limits at the 95% confidence level on the SM production cross section (sigma(H)) for values of the Higgs boson mass (m_H) in the range from 110 to 200 GeV. These limits are the most stringent for m_H > 130"},"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":"1001.4468","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ex","submitted_at":"2010-01-25T19:36:12Z","cross_cats_sorted":[],"title_canon_sha256":"007ca79f8fe2358958ce04f2bff41a695ac269c347ac65a738743b24464fcc0c","abstract_canon_sha256":"39a2b253aaae70e71e56ad19f8d25a8e2660163ed7d33affed5ca2be52399c6d"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T17:28:17.326083Z","signature_b64":"unli/levCbqqi6BxZBYbZ69J9mzW5dbXsMxvXqOI+3aYqICAr/FSuQdrCTUrp0nqUUmFICGAXeAVZblL2rgzBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"30c4f80f62e74b73b97c3133cd06b9ff8fba3584bc8a758ef19a8bcfb0b4ca8b","last_reissued_at":"2026-07-04T17:28:17.325596Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T17:28:17.325596Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Inclusive Search for Standard Model Higgs Boson Production in the WW Decay Channel using the CDF II Detector","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"et al, The CDF Collaboration: T. Aaltonen","submitted_at":"2010-01-25T19:36:12Z","abstract_excerpt":"We present a search for standard model (SM) Higgs boson production using ppbar collision data at sqrt(s) = 1.96 TeV, collected with the CDF II detector and corresponding to an integrated luminosity of 4.8 fb-1. We search for Higgs bosons produced in all processes with a significant production rate and decaying to two W bosons. We find no evidence for SM Higgs boson production and place upper limits at the 95% confidence level on the SM production cross section (sigma(H)) for values of the Higgs boson mass (m_H) in the range from 110 to 200 GeV. These limits are the most stringent for m_H > 130"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1001.4468","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/1001.4468/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":"1001.4468","created_at":"2026-07-04T17:28:17.325661+00:00"},{"alias_kind":"arxiv_version","alias_value":"1001.4468v2","created_at":"2026-07-04T17:28:17.325661+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1001.4468","created_at":"2026-07-04T17:28:17.325661+00:00"},{"alias_kind":"pith_short_12","alias_value":"GDCPQD3C45FX","created_at":"2026-07-04T17:28:17.325661+00:00"},{"alias_kind":"pith_short_16","alias_value":"GDCPQD3C45FXHOL4","created_at":"2026-07-04T17:28:17.325661+00:00"},{"alias_kind":"pith_short_8","alias_value":"GDCPQD3C","created_at":"2026-07-04T17:28:17.325661+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/GDCPQD3C45FXHOL4GEZ42BVZ76","json":"https://pith.science/pith/GDCPQD3C45FXHOL4GEZ42BVZ76.json","graph_json":"https://pith.science/api/pith-number/GDCPQD3C45FXHOL4GEZ42BVZ76/graph.json","events_json":"https://pith.science/api/pith-number/GDCPQD3C45FXHOL4GEZ42BVZ76/events.json","paper":"https://pith.science/paper/GDCPQD3C"},"agent_actions":{"view_html":"https://pith.science/pith/GDCPQD3C45FXHOL4GEZ42BVZ76","download_json":"https://pith.science/pith/GDCPQD3C45FXHOL4GEZ42BVZ76.json","view_paper":"https://pith.science/paper/GDCPQD3C","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1001.4468&json=true","fetch_graph":"https://pith.science/api/pith-number/GDCPQD3C45FXHOL4GEZ42BVZ76/graph.json","fetch_events":"https://pith.science/api/pith-number/GDCPQD3C45FXHOL4GEZ42BVZ76/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/GDCPQD3C45FXHOL4GEZ42BVZ76/action/timestamp_anchor","attest_storage":"https://pith.science/pith/GDCPQD3C45FXHOL4GEZ42BVZ76/action/storage_attestation","attest_author":"https://pith.science/pith/GDCPQD3C45FXHOL4GEZ42BVZ76/action/author_attestation","sign_citation":"https://pith.science/pith/GDCPQD3C45FXHOL4GEZ42BVZ76/action/citation_signature","submit_replication":"https://pith.science/pith/GDCPQD3C45FXHOL4GEZ42BVZ76/action/replication_record"}},"created_at":"2026-07-04T17:28:17.325661+00:00","updated_at":"2026-07-04T17:28:17.325661+00:00"}