{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:I3ADJEBSX22FXIXJGOTBVHSBTM","short_pith_number":"pith:I3ADJEBS","schema_version":"1.0","canonical_sha256":"46c0349032beb45ba2e933a61a9e419b3785bbe1ddd963444918e4ca8d355a69","source":{"kind":"arxiv","id":"1402.0923","version":2},"attestation_state":"computed","paper":{"title":"Measurement of inclusive W and Z boson production cross sections in pp collisions at sqrt(s) = 8 TeV","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"CMS Collaboration","submitted_at":"2014-02-05T02:41:31Z","abstract_excerpt":"A measurement of total and fiducial inclusive W and Z boson production cross sections in pp collisions at sqrt(s) = 8 TeV is presented. Electron and muon final states are analyzed in a data sample collected with the CMS detector corresponding to an integrated luminosity of 18.2 +/- 0.5 inverse picobarns. The measured total inclusive cross sections times branching fractions are sigma(pp to W X) B(W to l nu) = 12.21 +/- 0.03 (stat.) +/- 0.24 (syst.) +/- 0.32 (lum.) nb and sigma(pp to Z X) B(Z to l+ l-) = 1.15 +/- 0.01 (stat.) +/- 0.02 (syst.) +/- 0.03 (lum.) nb for the dilepton mass in the range"},"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":"1402.0923","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ex","submitted_at":"2014-02-05T02:41:31Z","cross_cats_sorted":[],"title_canon_sha256":"fd0862c1b1a7e92ff826fa8ddf0697e93d96728a1ab2c45f2a04df59d1aa59d1","abstract_canon_sha256":"746327d800e51ff1fbb2d05378ae6bcd51c023466a2230730b4b176fa0d4201d"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:51:41.617306Z","signature_b64":"Cs+s+VNlwOOnDyDBTyViERMxXn5iZv0o7RKhjwSE2ALs5Jp+mXyMqoj4bmo7YWBxzcfTwkGiH3PNQG0pnUNABA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"46c0349032beb45ba2e933a61a9e419b3785bbe1ddd963444918e4ca8d355a69","last_reissued_at":"2026-05-18T02:51:41.616775Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:51:41.616775Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Measurement of inclusive W and Z boson production cross sections in pp collisions at sqrt(s) = 8 TeV","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"CMS Collaboration","submitted_at":"2014-02-05T02:41:31Z","abstract_excerpt":"A measurement of total and fiducial inclusive W and Z boson production cross sections in pp collisions at sqrt(s) = 8 TeV is presented. Electron and muon final states are analyzed in a data sample collected with the CMS detector corresponding to an integrated luminosity of 18.2 +/- 0.5 inverse picobarns. The measured total inclusive cross sections times branching fractions are sigma(pp to W X) B(W to l nu) = 12.21 +/- 0.03 (stat.) +/- 0.24 (syst.) +/- 0.32 (lum.) nb and sigma(pp to Z X) B(Z to l+ l-) = 1.15 +/- 0.01 (stat.) +/- 0.02 (syst.) +/- 0.03 (lum.) nb for the dilepton mass in the range"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1402.0923","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":""},"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":"1402.0923","created_at":"2026-05-18T02:51:41.616859+00:00"},{"alias_kind":"arxiv_version","alias_value":"1402.0923v2","created_at":"2026-05-18T02:51:41.616859+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1402.0923","created_at":"2026-05-18T02:51:41.616859+00:00"},{"alias_kind":"pith_short_12","alias_value":"I3ADJEBSX22F","created_at":"2026-05-18T12:28:33.132498+00:00"},{"alias_kind":"pith_short_16","alias_value":"I3ADJEBSX22FXIXJ","created_at":"2026-05-18T12:28:33.132498+00:00"},{"alias_kind":"pith_short_8","alias_value":"I3ADJEBS","created_at":"2026-05-18T12:28:33.132498+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2604.12706","citing_title":"Measurement of the $W$-boson production cross-sections in $pp$ collisions at $\\sqrt{s}$ = 13 TeV in the forward region","ref_index":32,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/I3ADJEBSX22FXIXJGOTBVHSBTM","json":"https://pith.science/pith/I3ADJEBSX22FXIXJGOTBVHSBTM.json","graph_json":"https://pith.science/api/pith-number/I3ADJEBSX22FXIXJGOTBVHSBTM/graph.json","events_json":"https://pith.science/api/pith-number/I3ADJEBSX22FXIXJGOTBVHSBTM/events.json","paper":"https://pith.science/paper/I3ADJEBS"},"agent_actions":{"view_html":"https://pith.science/pith/I3ADJEBSX22FXIXJGOTBVHSBTM","download_json":"https://pith.science/pith/I3ADJEBSX22FXIXJGOTBVHSBTM.json","view_paper":"https://pith.science/paper/I3ADJEBS","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1402.0923&json=true","fetch_graph":"https://pith.science/api/pith-number/I3ADJEBSX22FXIXJGOTBVHSBTM/graph.json","fetch_events":"https://pith.science/api/pith-number/I3ADJEBSX22FXIXJGOTBVHSBTM/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/I3ADJEBSX22FXIXJGOTBVHSBTM/action/timestamp_anchor","attest_storage":"https://pith.science/pith/I3ADJEBSX22FXIXJGOTBVHSBTM/action/storage_attestation","attest_author":"https://pith.science/pith/I3ADJEBSX22FXIXJGOTBVHSBTM/action/author_attestation","sign_citation":"https://pith.science/pith/I3ADJEBSX22FXIXJGOTBVHSBTM/action/citation_signature","submit_replication":"https://pith.science/pith/I3ADJEBSX22FXIXJGOTBVHSBTM/action/replication_record"}},"created_at":"2026-05-18T02:51:41.616859+00:00","updated_at":"2026-05-18T02:51:41.616859+00:00"}