{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:NCGUWDSGOIJJUD3YSF7XF3R2DO","short_pith_number":"pith:NCGUWDSG","schema_version":"1.0","canonical_sha256":"688d4b0e4672129a0f78917f72ee3a1b8daa619cff00f1d121ff12667cf72314","source":{"kind":"arxiv","id":"1201.4611","version":1},"attestation_state":"computed","paper":{"title":"Search for a Standard Model Higgs boson decaying to b quarks and produced in association with Z/W bosons with the CMS detector","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"Astrophysics, Batavia, Department of Physics, Fermi National Accelerator Laboratory, FL USA, Gainesville, IL USA), Institute for High Energy Physics, Michele De Gruttola (University of Florida","submitted_at":"2012-01-22T22:52:08Z","abstract_excerpt":"A search for the standard model Higgs boson is performed in a data sample corresponding to an integrated luminosity of 1.1 fb$^{-1}$, recorded by the CMS detector in proton-proton collisions at the LHC with a 7 TeV center-of-mass energy. The following modes are studied: W($\\mu \\nu$)H, W(e$\\nu$)H, Z($\\mu \\mu$)H, Z(ee)H and Z($\\nu \\nu$)H, with the Higgs decaying to bb pairs. 95% C.L. upper limits on the VH production cross section are derived for a Higgs mass between 110 and 135 GeV. The expected (observed) upper limit at 115 GeV is found to be 5.7 (8.3) times the standard model expectation."},"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":"1201.4611","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ex","submitted_at":"2012-01-22T22:52:08Z","cross_cats_sorted":[],"title_canon_sha256":"c77e083aa6e37071a61cfb43c1ae40c4fc9c55d654f08deec16a4f447fd397ab","abstract_canon_sha256":"2c5797ce1ec8b3deea581abc07a18e2e6f0087716c8e7afbc8d06ee3dbd36581"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:58:43.749899Z","signature_b64":"qBqM4OKLq99bEZeWIy6GkoQwvVLN6ItouqNIdvDFrlFDG8h78YGZSx2e/CSmuHo8iPTDHMflP0FNj8CWu59OAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"688d4b0e4672129a0f78917f72ee3a1b8daa619cff00f1d121ff12667cf72314","last_reissued_at":"2026-05-18T01:58:43.749176Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:58:43.749176Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Search for a Standard Model Higgs boson decaying to b quarks and produced in association with Z/W bosons with the CMS detector","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"Astrophysics, Batavia, Department of Physics, Fermi National Accelerator Laboratory, FL USA, Gainesville, IL USA), Institute for High Energy Physics, Michele De Gruttola (University of Florida","submitted_at":"2012-01-22T22:52:08Z","abstract_excerpt":"A search for the standard model Higgs boson is performed in a data sample corresponding to an integrated luminosity of 1.1 fb$^{-1}$, recorded by the CMS detector in proton-proton collisions at the LHC with a 7 TeV center-of-mass energy. The following modes are studied: W($\\mu \\nu$)H, W(e$\\nu$)H, Z($\\mu \\mu$)H, Z(ee)H and Z($\\nu \\nu$)H, with the Higgs decaying to bb pairs. 95% C.L. upper limits on the VH production cross section are derived for a Higgs mass between 110 and 135 GeV. The expected (observed) upper limit at 115 GeV is found to be 5.7 (8.3) times the standard model expectation."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1201.4611","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":"1201.4611","created_at":"2026-05-18T01:58:43.749305+00:00"},{"alias_kind":"arxiv_version","alias_value":"1201.4611v1","created_at":"2026-05-18T01:58:43.749305+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1201.4611","created_at":"2026-05-18T01:58:43.749305+00:00"},{"alias_kind":"pith_short_12","alias_value":"NCGUWDSGOIJJ","created_at":"2026-05-18T12:27:16.716162+00:00"},{"alias_kind":"pith_short_16","alias_value":"NCGUWDSGOIJJUD3Y","created_at":"2026-05-18T12:27:16.716162+00:00"},{"alias_kind":"pith_short_8","alias_value":"NCGUWDSG","created_at":"2026-05-18T12:27:16.716162+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/NCGUWDSGOIJJUD3YSF7XF3R2DO","json":"https://pith.science/pith/NCGUWDSGOIJJUD3YSF7XF3R2DO.json","graph_json":"https://pith.science/api/pith-number/NCGUWDSGOIJJUD3YSF7XF3R2DO/graph.json","events_json":"https://pith.science/api/pith-number/NCGUWDSGOIJJUD3YSF7XF3R2DO/events.json","paper":"https://pith.science/paper/NCGUWDSG"},"agent_actions":{"view_html":"https://pith.science/pith/NCGUWDSGOIJJUD3YSF7XF3R2DO","download_json":"https://pith.science/pith/NCGUWDSGOIJJUD3YSF7XF3R2DO.json","view_paper":"https://pith.science/paper/NCGUWDSG","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1201.4611&json=true","fetch_graph":"https://pith.science/api/pith-number/NCGUWDSGOIJJUD3YSF7XF3R2DO/graph.json","fetch_events":"https://pith.science/api/pith-number/NCGUWDSGOIJJUD3YSF7XF3R2DO/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/NCGUWDSGOIJJUD3YSF7XF3R2DO/action/timestamp_anchor","attest_storage":"https://pith.science/pith/NCGUWDSGOIJJUD3YSF7XF3R2DO/action/storage_attestation","attest_author":"https://pith.science/pith/NCGUWDSGOIJJUD3YSF7XF3R2DO/action/author_attestation","sign_citation":"https://pith.science/pith/NCGUWDSGOIJJUD3YSF7XF3R2DO/action/citation_signature","submit_replication":"https://pith.science/pith/NCGUWDSGOIJJUD3YSF7XF3R2DO/action/replication_record"}},"created_at":"2026-05-18T01:58:43.749305+00:00","updated_at":"2026-05-18T01:58:43.749305+00:00"}