{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:MLOW5YPLYZMOHGQ26K2OTIFMYP","short_pith_number":"pith:MLOW5YPL","schema_version":"1.0","canonical_sha256":"62dd6ee1ebc658e39a1af2b4e9a0acc3c3f699df56d6241eb6655c39f82faf16","source":{"kind":"arxiv","id":"2208.00924","version":2},"attestation_state":"computed","paper":{"title":"Measurement of inclusive and differential cross sections for single top quark production in association with a W boson 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":"2022-08-01T15:12:46Z","abstract_excerpt":"Measurements of the inclusive and normalised differential cross sections are presented for the production of single top quarks in association with a W boson in proton-proton collisions at a centre-of-mass energy of 13 TeV. The data used were recorded with the CMS detector at the LHC during 2016-2018, and correspond to an integrated luminosity of 138 fb$^{-1}$. Events containing one electron and one muon in the final state are analysed. For the inclusive measurement, a multivariate discriminant, exploiting the kinematic properties of the events is used to separate the signal from the dominant $"},"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":"2208.00924","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ex","submitted_at":"2022-08-01T15:12:46Z","cross_cats_sorted":[],"title_canon_sha256":"56014a329b846067c79be6d6cb81e1a731560dfb811b2765c8e3853956a56a6a","abstract_canon_sha256":"edd5c5e77196abd741b77f35ce8727cba93adbe789f4af605796b761dbf052f6"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T06:32:33.771155Z","signature_b64":"0l/1zvJEbtcqra3cmOu08NIS+QIhPidK6ECyHKho7E3LvaveWEweQx2hxnvi7dCz4Xn9/rcd1LQ5p3WD8PmcDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"62dd6ee1ebc658e39a1af2b4e9a0acc3c3f699df56d6241eb6655c39f82faf16","last_reissued_at":"2026-07-05T06:32:33.770643Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T06:32:33.770643Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Measurement of inclusive and differential cross sections for single top quark production in association with a W boson 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":"2022-08-01T15:12:46Z","abstract_excerpt":"Measurements of the inclusive and normalised differential cross sections are presented for the production of single top quarks in association with a W boson in proton-proton collisions at a centre-of-mass energy of 13 TeV. The data used were recorded with the CMS detector at the LHC during 2016-2018, and correspond to an integrated luminosity of 138 fb$^{-1}$. Events containing one electron and one muon in the final state are analysed. For the inclusive measurement, a multivariate discriminant, exploiting the kinematic properties of the events is used to separate the signal from the dominant $"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2208.00924","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/2208.00924/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":"2208.00924","created_at":"2026-07-05T06:32:33.770702+00:00"},{"alias_kind":"arxiv_version","alias_value":"2208.00924v2","created_at":"2026-07-05T06:32:33.770702+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2208.00924","created_at":"2026-07-05T06:32:33.770702+00:00"},{"alias_kind":"pith_short_12","alias_value":"MLOW5YPLYZMO","created_at":"2026-07-05T06:32:33.770702+00:00"},{"alias_kind":"pith_short_16","alias_value":"MLOW5YPLYZMOHGQ2","created_at":"2026-07-05T06:32:33.770702+00:00"},{"alias_kind":"pith_short_8","alias_value":"MLOW5YPL","created_at":"2026-07-05T06:32:33.770702+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2601.21040","citing_title":"Constraining dimension-6 SMEFT with higher-order predictions for $p p \\to t W$","ref_index":72,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/MLOW5YPLYZMOHGQ26K2OTIFMYP","json":"https://pith.science/pith/MLOW5YPLYZMOHGQ26K2OTIFMYP.json","graph_json":"https://pith.science/api/pith-number/MLOW5YPLYZMOHGQ26K2OTIFMYP/graph.json","events_json":"https://pith.science/api/pith-number/MLOW5YPLYZMOHGQ26K2OTIFMYP/events.json","paper":"https://pith.science/paper/MLOW5YPL"},"agent_actions":{"view_html":"https://pith.science/pith/MLOW5YPLYZMOHGQ26K2OTIFMYP","download_json":"https://pith.science/pith/MLOW5YPLYZMOHGQ26K2OTIFMYP.json","view_paper":"https://pith.science/paper/MLOW5YPL","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2208.00924&json=true","fetch_graph":"https://pith.science/api/pith-number/MLOW5YPLYZMOHGQ26K2OTIFMYP/graph.json","fetch_events":"https://pith.science/api/pith-number/MLOW5YPLYZMOHGQ26K2OTIFMYP/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/MLOW5YPLYZMOHGQ26K2OTIFMYP/action/timestamp_anchor","attest_storage":"https://pith.science/pith/MLOW5YPLYZMOHGQ26K2OTIFMYP/action/storage_attestation","attest_author":"https://pith.science/pith/MLOW5YPLYZMOHGQ26K2OTIFMYP/action/author_attestation","sign_citation":"https://pith.science/pith/MLOW5YPLYZMOHGQ26K2OTIFMYP/action/citation_signature","submit_replication":"https://pith.science/pith/MLOW5YPLYZMOHGQ26K2OTIFMYP/action/replication_record"}},"created_at":"2026-07-05T06:32:33.770702+00:00","updated_at":"2026-07-05T06:32:33.770702+00:00"}