{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:DKCQ6FWTOQ6YG646J2OIGH4FY6","short_pith_number":"pith:DKCQ6FWT","schema_version":"1.0","canonical_sha256":"1a850f16d3743d837b9e4e9c831f85c7a9598b12ebb900f4e60ba90633890cd7","source":{"kind":"arxiv","id":"2407.15594","version":2},"attestation_state":"computed","paper":{"title":"Measurement of single top-quark production in association with a $W$ boson in $pp$ collisions at $\\sqrt{s} = 13$ TeV with the ATLAS detector","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"The ATLAS Collaboration","submitted_at":"2024-07-22T12:32:46Z","abstract_excerpt":"The inclusive cross-section for the production of a single top quark in association with a $W$ boson is measured using 140 fb$^{-1}$ of proton-proton collision data collected with the ATLAS detector at $\\sqrt{s} = 13$ TeV. Events containing two charged leptons and at least one jet identified as originating from a $b$-quark are selected. A multivariate discriminant is constructed to separate the $tW$ signal from the $t\\bar{t}$ background. The cross-section is extracted using a profile likelihood fit to the signal and control regions and it is measured to be $\\sigma_{tW} = 75^{+15}_{-14}$ pb, in"},"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":"2407.15594","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ex","submitted_at":"2024-07-22T12:32:46Z","cross_cats_sorted":[],"title_canon_sha256":"58ae7fcdb8f2892e0b03790a8e4eaa7d88c5d783b7610c581104335d64b14e80","abstract_canon_sha256":"4d769161355e95ac8689757e309309edf43f30a99a38809119885590b690f6c9"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T09:37:39.368112Z","signature_b64":"dhnEUmRK4j8pL/JjtZfGHWTF3RTQ6zC1Unjplz1aPrGjmy/uitPwxzwj5iORA1CSnb2n5KxuqK5nIMZICXKxBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1a850f16d3743d837b9e4e9c831f85c7a9598b12ebb900f4e60ba90633890cd7","last_reissued_at":"2026-07-05T09:37:39.367709Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T09:37:39.367709Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Measurement of single top-quark production in association with a $W$ boson in $pp$ collisions at $\\sqrt{s} = 13$ TeV with the ATLAS detector","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"The ATLAS Collaboration","submitted_at":"2024-07-22T12:32:46Z","abstract_excerpt":"The inclusive cross-section for the production of a single top quark in association with a $W$ boson is measured using 140 fb$^{-1}$ of proton-proton collision data collected with the ATLAS detector at $\\sqrt{s} = 13$ TeV. Events containing two charged leptons and at least one jet identified as originating from a $b$-quark are selected. A multivariate discriminant is constructed to separate the $tW$ signal from the $t\\bar{t}$ background. The cross-section is extracted using a profile likelihood fit to the signal and control regions and it is measured to be $\\sigma_{tW} = 75^{+15}_{-14}$ pb, in"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2407.15594","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/2407.15594/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":"2407.15594","created_at":"2026-07-05T09:37:39.367768+00:00"},{"alias_kind":"arxiv_version","alias_value":"2407.15594v2","created_at":"2026-07-05T09:37:39.367768+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2407.15594","created_at":"2026-07-05T09:37:39.367768+00:00"},{"alias_kind":"pith_short_12","alias_value":"DKCQ6FWTOQ6Y","created_at":"2026-07-05T09:37:39.367768+00:00"},{"alias_kind":"pith_short_16","alias_value":"DKCQ6FWTOQ6YG646","created_at":"2026-07-05T09:37:39.367768+00:00"},{"alias_kind":"pith_short_8","alias_value":"DKCQ6FWT","created_at":"2026-07-05T09:37:39.367768+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2607.06199","citing_title":"Simultaneous efficiency measurements of $b$- and $c$-jets in $t\\bar{t}$ events from $\\sqrt{s}=13.6$ TeV $pp$ collision data collected with the ATLAS detector","ref_index":75,"is_internal_anchor":true},{"citing_arxiv_id":"2601.21040","citing_title":"Constraining dimension-6 SMEFT with higher-order predictions for $p p \\to t W$","ref_index":73,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/DKCQ6FWTOQ6YG646J2OIGH4FY6","json":"https://pith.science/pith/DKCQ6FWTOQ6YG646J2OIGH4FY6.json","graph_json":"https://pith.science/api/pith-number/DKCQ6FWTOQ6YG646J2OIGH4FY6/graph.json","events_json":"https://pith.science/api/pith-number/DKCQ6FWTOQ6YG646J2OIGH4FY6/events.json","paper":"https://pith.science/paper/DKCQ6FWT"},"agent_actions":{"view_html":"https://pith.science/pith/DKCQ6FWTOQ6YG646J2OIGH4FY6","download_json":"https://pith.science/pith/DKCQ6FWTOQ6YG646J2OIGH4FY6.json","view_paper":"https://pith.science/paper/DKCQ6FWT","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2407.15594&json=true","fetch_graph":"https://pith.science/api/pith-number/DKCQ6FWTOQ6YG646J2OIGH4FY6/graph.json","fetch_events":"https://pith.science/api/pith-number/DKCQ6FWTOQ6YG646J2OIGH4FY6/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/DKCQ6FWTOQ6YG646J2OIGH4FY6/action/timestamp_anchor","attest_storage":"https://pith.science/pith/DKCQ6FWTOQ6YG646J2OIGH4FY6/action/storage_attestation","attest_author":"https://pith.science/pith/DKCQ6FWTOQ6YG646J2OIGH4FY6/action/author_attestation","sign_citation":"https://pith.science/pith/DKCQ6FWTOQ6YG646J2OIGH4FY6/action/citation_signature","submit_replication":"https://pith.science/pith/DKCQ6FWTOQ6YG646J2OIGH4FY6/action/replication_record"}},"created_at":"2026-07-05T09:37:39.367768+00:00","updated_at":"2026-07-05T09:37:39.367768+00:00"}