{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:56PAQ3KUJZUFS64M42ME5ETKJ5","short_pith_number":"pith:56PAQ3KU","schema_version":"1.0","canonical_sha256":"ef9e086d544e68597b8ce6984e926a4f72767b7a42a4e0e487268674414c96d0","source":{"kind":"arxiv","id":"2408.03744","version":2},"attestation_state":"computed","paper":{"title":"Measurement of the inclusive cross sections for W and Z boson production in proton-proton collisions at $\\sqrt{s}$ = 5.02 and 13 TeV","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"CMS Collaboration","submitted_at":"2024-08-07T12:57:33Z","abstract_excerpt":"Measurements of fiducial and total inclusive cross sections for W and Z boson production are presented in proton-proton collisions at $\\sqrt{s}$ = 5.02 and 13 TeV. Electron and muon decay modes ($\\ell$ = e or $\\mu$) are studied in the data collected with the CMS detector in 2017, in dedicated runs with reduced instantaneous luminosity. The data sets correspond to integrated luminosities of 298 $\\pm$ 6 pb$^{-1}$ at 5.02 TeV and 206 $\\pm$ 5 pb$^{-1}$ at 13 TeV. Measured values of the products of the total inclusive cross sections and the branching fractions at 5.02 TeV are $\\sigma$(pp $\\to$ W+X)"},"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":"2408.03744","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ex","submitted_at":"2024-08-07T12:57:33Z","cross_cats_sorted":[],"title_canon_sha256":"37e545a663e1fec6ebc5def0d5b447e754e19f6711e29d160cfc6e6b33d0543b","abstract_canon_sha256":"c4589c3f3edbe54f125431d6a71d725f1ee8cee506c4ecde3caee881c093783e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T10:56:33.808899Z","signature_b64":"rm+2SUfhMbaKk39viLHvHgbaXdyIEiepFaIElY9WjhmkxCOzRrISlnrod4G1EjuC6efR2U3PfRLm7hvXNg9+Ag==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ef9e086d544e68597b8ce6984e926a4f72767b7a42a4e0e487268674414c96d0","last_reissued_at":"2026-07-05T10:56:33.808432Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T10:56:33.808432Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Measurement of the inclusive cross sections for W and Z boson production in proton-proton collisions at $\\sqrt{s}$ = 5.02 and 13 TeV","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"CMS Collaboration","submitted_at":"2024-08-07T12:57:33Z","abstract_excerpt":"Measurements of fiducial and total inclusive cross sections for W and Z boson production are presented in proton-proton collisions at $\\sqrt{s}$ = 5.02 and 13 TeV. Electron and muon decay modes ($\\ell$ = e or $\\mu$) are studied in the data collected with the CMS detector in 2017, in dedicated runs with reduced instantaneous luminosity. The data sets correspond to integrated luminosities of 298 $\\pm$ 6 pb$^{-1}$ at 5.02 TeV and 206 $\\pm$ 5 pb$^{-1}$ at 13 TeV. Measured values of the products of the total inclusive cross sections and the branching fractions at 5.02 TeV are $\\sigma$(pp $\\to$ W+X)"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2408.03744","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/2408.03744/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":"2408.03744","created_at":"2026-07-05T10:56:33.808492+00:00"},{"alias_kind":"arxiv_version","alias_value":"2408.03744v2","created_at":"2026-07-05T10:56:33.808492+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2408.03744","created_at":"2026-07-05T10:56:33.808492+00:00"},{"alias_kind":"pith_short_12","alias_value":"56PAQ3KUJZUF","created_at":"2026-07-05T10:56:33.808492+00:00"},{"alias_kind":"pith_short_16","alias_value":"56PAQ3KUJZUFS64M","created_at":"2026-07-05T10:56:33.808492+00:00"},{"alias_kind":"pith_short_8","alias_value":"56PAQ3KU","created_at":"2026-07-05T10:56:33.808492+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":37,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/56PAQ3KUJZUFS64M42ME5ETKJ5","json":"https://pith.science/pith/56PAQ3KUJZUFS64M42ME5ETKJ5.json","graph_json":"https://pith.science/api/pith-number/56PAQ3KUJZUFS64M42ME5ETKJ5/graph.json","events_json":"https://pith.science/api/pith-number/56PAQ3KUJZUFS64M42ME5ETKJ5/events.json","paper":"https://pith.science/paper/56PAQ3KU"},"agent_actions":{"view_html":"https://pith.science/pith/56PAQ3KUJZUFS64M42ME5ETKJ5","download_json":"https://pith.science/pith/56PAQ3KUJZUFS64M42ME5ETKJ5.json","view_paper":"https://pith.science/paper/56PAQ3KU","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2408.03744&json=true","fetch_graph":"https://pith.science/api/pith-number/56PAQ3KUJZUFS64M42ME5ETKJ5/graph.json","fetch_events":"https://pith.science/api/pith-number/56PAQ3KUJZUFS64M42ME5ETKJ5/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/56PAQ3KUJZUFS64M42ME5ETKJ5/action/timestamp_anchor","attest_storage":"https://pith.science/pith/56PAQ3KUJZUFS64M42ME5ETKJ5/action/storage_attestation","attest_author":"https://pith.science/pith/56PAQ3KUJZUFS64M42ME5ETKJ5/action/author_attestation","sign_citation":"https://pith.science/pith/56PAQ3KUJZUFS64M42ME5ETKJ5/action/citation_signature","submit_replication":"https://pith.science/pith/56PAQ3KUJZUFS64M42ME5ETKJ5/action/replication_record"}},"created_at":"2026-07-05T10:56:33.808492+00:00","updated_at":"2026-07-05T10:56:33.808492+00:00"}