{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2010:EKQJ7MNZDCLKPBVPZE3FKU347G","short_pith_number":"pith:EKQJ7MNZ","schema_version":"1.0","canonical_sha256":"22a09fb1b91896a786afc93655537cf98048922e5babf0b8869d3873fb6f5472","source":{"kind":"arxiv","id":"1001.4481","version":3},"attestation_state":"computed","paper":{"title":"Search for Higgs boson production in dilepton and missing energy final states with 5.4 fb-1 of p-pbar collisions at sqrt(s) =1.96 TeV","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"the D0 Collaboration","submitted_at":"2010-01-25T16:40:59Z","abstract_excerpt":"A search for the standard model Higgs boson is presented using events with two charged leptons and large missing transverse energy selected from 5.4 fb-1 of integrated luminosity in p-pbar collisions at sqrt(s)=1.96 TeV collected with the D0 detector at the Fermilab Tevatron Collider. No significant excess of events above background predictions is found, and observed (expected) upper limits at 95% confidence level on the rate of Higgs boson production are derived that are a factor of 1.55 (1.36) above the predicted standard model cross section at Higgs boson mass of 165 GeV."},"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":"1001.4481","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ex","submitted_at":"2010-01-25T16:40:59Z","cross_cats_sorted":[],"title_canon_sha256":"89195825b90d49d86a739cf2fc9f1cf8097de75ec0fa2372d3ff28036077e5a7","abstract_canon_sha256":"660c36972b44f32948a4e90fb73d80525d140ed9cab7b965610e55766a8b3bba"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:48:01.689410Z","signature_b64":"L/xrERt5uw3Mu8vj01s6Ov/6u/0Y0ZhAV0Q3Ak4Rhu9r8blUoYNFHAxfX2aK5XkHigZ7p6pgifPyPc5cWhgsAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"22a09fb1b91896a786afc93655537cf98048922e5babf0b8869d3873fb6f5472","last_reissued_at":"2026-05-18T03:48:01.689022Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:48:01.689022Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Search for Higgs boson production in dilepton and missing energy final states with 5.4 fb-1 of p-pbar collisions at sqrt(s) =1.96 TeV","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"the D0 Collaboration","submitted_at":"2010-01-25T16:40:59Z","abstract_excerpt":"A search for the standard model Higgs boson is presented using events with two charged leptons and large missing transverse energy selected from 5.4 fb-1 of integrated luminosity in p-pbar collisions at sqrt(s)=1.96 TeV collected with the D0 detector at the Fermilab Tevatron Collider. No significant excess of events above background predictions is found, and observed (expected) upper limits at 95% confidence level on the rate of Higgs boson production are derived that are a factor of 1.55 (1.36) above the predicted standard model cross section at Higgs boson mass of 165 GeV."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1001.4481","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":"1001.4481","created_at":"2026-05-18T03:48:01.689078+00:00"},{"alias_kind":"arxiv_version","alias_value":"1001.4481v3","created_at":"2026-05-18T03:48:01.689078+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1001.4481","created_at":"2026-05-18T03:48:01.689078+00:00"},{"alias_kind":"pith_short_12","alias_value":"EKQJ7MNZDCLK","created_at":"2026-05-18T12:26:06.534383+00:00"},{"alias_kind":"pith_short_16","alias_value":"EKQJ7MNZDCLKPBVP","created_at":"2026-05-18T12:26:06.534383+00:00"},{"alias_kind":"pith_short_8","alias_value":"EKQJ7MNZ","created_at":"2026-05-18T12:26:06.534383+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/EKQJ7MNZDCLKPBVPZE3FKU347G","json":"https://pith.science/pith/EKQJ7MNZDCLKPBVPZE3FKU347G.json","graph_json":"https://pith.science/api/pith-number/EKQJ7MNZDCLKPBVPZE3FKU347G/graph.json","events_json":"https://pith.science/api/pith-number/EKQJ7MNZDCLKPBVPZE3FKU347G/events.json","paper":"https://pith.science/paper/EKQJ7MNZ"},"agent_actions":{"view_html":"https://pith.science/pith/EKQJ7MNZDCLKPBVPZE3FKU347G","download_json":"https://pith.science/pith/EKQJ7MNZDCLKPBVPZE3FKU347G.json","view_paper":"https://pith.science/paper/EKQJ7MNZ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1001.4481&json=true","fetch_graph":"https://pith.science/api/pith-number/EKQJ7MNZDCLKPBVPZE3FKU347G/graph.json","fetch_events":"https://pith.science/api/pith-number/EKQJ7MNZDCLKPBVPZE3FKU347G/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/EKQJ7MNZDCLKPBVPZE3FKU347G/action/timestamp_anchor","attest_storage":"https://pith.science/pith/EKQJ7MNZDCLKPBVPZE3FKU347G/action/storage_attestation","attest_author":"https://pith.science/pith/EKQJ7MNZDCLKPBVPZE3FKU347G/action/author_attestation","sign_citation":"https://pith.science/pith/EKQJ7MNZDCLKPBVPZE3FKU347G/action/citation_signature","submit_replication":"https://pith.science/pith/EKQJ7MNZDCLKPBVPZE3FKU347G/action/replication_record"}},"created_at":"2026-05-18T03:48:01.689078+00:00","updated_at":"2026-05-18T03:48:01.689078+00:00"}