{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2021:MQNR3NIMNXLUBAOGELGRGD6DIS","short_pith_number":"pith:MQNR3NIM","schema_version":"1.0","canonical_sha256":"641b1db50c6dd74081c622cd130fc3448967caf5f58f15544d8f81898b68545b","source":{"kind":"arxiv","id":"2103.04956","version":2},"attestation_state":"computed","paper":{"title":"Measurements of production cross sections of the Higgs boson in the four-lepton final state in proton-proton collisions at $\\sqrt{s} = $ 13 TeV","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"CMS Collaboration","submitted_at":"2021-03-08T18:25:33Z","abstract_excerpt":"Production cross sections of the Higgs boson are measured in the H $\\to$ ZZ $\\to$ $4\\ell$ ($\\ell$ $=$ e, $\\mu$) decay channel. A data sample of proton-proton collisions at a center-of-mass energy of 13 TeV, collected by the CMS detector at the LHC and corresponding to an integrated luminosity of 137 fb$^{-1}$ is used. The signal strength modifier $\\mu$, defined as the ratio of the Higgs boson production rate in the $4\\ell$ channel to the standard model (SM) expectation, is measured to be $\\mu$ $=$ 0.94 $\\pm$ 0.07 (stat) ${}^{+0.09}_{-0.08}$ (syst) at a fixed value of $m_\\mathrm{H}$ $=$ 125.38 "},"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":"2103.04956","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ex","submitted_at":"2021-03-08T18:25:33Z","cross_cats_sorted":[],"title_canon_sha256":"0b91c206ff373e065584afa98eea3de412dd3ebf19b983f6793674f4f12edd6f","abstract_canon_sha256":"b0273b7226b9cb3364ebce219be1657b619053c25a9a7f30cac80c678c1ffe54"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T02:46:12.536388Z","signature_b64":"+GH5mQGDoHJfz5XKdWxA09ie+NKcEaW8c/AbcL/+J5i84xLXGrtdoi381vnNP6FJrEOOU1LfnAH7kcpI5JwtAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"641b1db50c6dd74081c622cd130fc3448967caf5f58f15544d8f81898b68545b","last_reissued_at":"2026-07-05T02:46:12.535885Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T02:46:12.535885Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Measurements of production cross sections of the Higgs boson in the four-lepton final state in proton-proton collisions at $\\sqrt{s} = $ 13 TeV","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"CMS Collaboration","submitted_at":"2021-03-08T18:25:33Z","abstract_excerpt":"Production cross sections of the Higgs boson are measured in the H $\\to$ ZZ $\\to$ $4\\ell$ ($\\ell$ $=$ e, $\\mu$) decay channel. A data sample of proton-proton collisions at a center-of-mass energy of 13 TeV, collected by the CMS detector at the LHC and corresponding to an integrated luminosity of 137 fb$^{-1}$ is used. The signal strength modifier $\\mu$, defined as the ratio of the Higgs boson production rate in the $4\\ell$ channel to the standard model (SM) expectation, is measured to be $\\mu$ $=$ 0.94 $\\pm$ 0.07 (stat) ${}^{+0.09}_{-0.08}$ (syst) at a fixed value of $m_\\mathrm{H}$ $=$ 125.38 "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2103.04956","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/2103.04956/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":"2103.04956","created_at":"2026-07-05T02:46:12.535963+00:00"},{"alias_kind":"arxiv_version","alias_value":"2103.04956v2","created_at":"2026-07-05T02:46:12.535963+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2103.04956","created_at":"2026-07-05T02:46:12.535963+00:00"},{"alias_kind":"pith_short_12","alias_value":"MQNR3NIMNXLU","created_at":"2026-07-05T02:46:12.535963+00:00"},{"alias_kind":"pith_short_16","alias_value":"MQNR3NIMNXLUBAOG","created_at":"2026-07-05T02:46:12.535963+00:00"},{"alias_kind":"pith_short_8","alias_value":"MQNR3NIM","created_at":"2026-07-05T02:46:12.535963+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2605.19016","citing_title":"Measurements of the Higgs boson production, fiducial and differential cross-sections in the four lepton decay channel using 164 fb$^{-1}$ of data collected at $\\sqrt{s}$ = 13.6 TeV with the ATLAS dete","ref_index":13,"is_internal_anchor":false},{"citing_arxiv_id":"2605.19016","citing_title":"Measurements of the Higgs boson production, fiducial and differential cross-sections in the four lepton decay channel using 164 fb$^{-1}$ of data collected at $\\sqrt{s}$ = 13.6 TeV with the ATLAS dete","ref_index":13,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/MQNR3NIMNXLUBAOGELGRGD6DIS","json":"https://pith.science/pith/MQNR3NIMNXLUBAOGELGRGD6DIS.json","graph_json":"https://pith.science/api/pith-number/MQNR3NIMNXLUBAOGELGRGD6DIS/graph.json","events_json":"https://pith.science/api/pith-number/MQNR3NIMNXLUBAOGELGRGD6DIS/events.json","paper":"https://pith.science/paper/MQNR3NIM"},"agent_actions":{"view_html":"https://pith.science/pith/MQNR3NIMNXLUBAOGELGRGD6DIS","download_json":"https://pith.science/pith/MQNR3NIMNXLUBAOGELGRGD6DIS.json","view_paper":"https://pith.science/paper/MQNR3NIM","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2103.04956&json=true","fetch_graph":"https://pith.science/api/pith-number/MQNR3NIMNXLUBAOGELGRGD6DIS/graph.json","fetch_events":"https://pith.science/api/pith-number/MQNR3NIMNXLUBAOGELGRGD6DIS/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/MQNR3NIMNXLUBAOGELGRGD6DIS/action/timestamp_anchor","attest_storage":"https://pith.science/pith/MQNR3NIMNXLUBAOGELGRGD6DIS/action/storage_attestation","attest_author":"https://pith.science/pith/MQNR3NIMNXLUBAOGELGRGD6DIS/action/author_attestation","sign_citation":"https://pith.science/pith/MQNR3NIMNXLUBAOGELGRGD6DIS/action/citation_signature","submit_replication":"https://pith.science/pith/MQNR3NIMNXLUBAOGELGRGD6DIS/action/replication_record"}},"created_at":"2026-07-05T02:46:12.535963+00:00","updated_at":"2026-07-05T02:46:12.535963+00:00"}