{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:O6SZTKVMSH7H5CN5BHBIMHSSDH","short_pith_number":"pith:O6SZTKVM","schema_version":"1.0","canonical_sha256":"77a599aaac91fe7e89bd09c2861e5219fe1e990794e6d304c07ad170fb09ccde","source":{"kind":"arxiv","id":"2509.19038","version":1},"attestation_state":"computed","paper":{"title":"A search for electroweak $t\\bar{t}Wj$ production in multileptonic final states at $\\sqrt{s} = 13$ TeV with the ATLAS detector and bounds on effective field theory operators","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"ATLAS Collaboration","submitted_at":"2025-09-23T14:09:07Z","abstract_excerpt":"A search is presented for the electroweak production of a top quark pair in association with a $W$ boson and at least one additional jet, known as the ${t\\bar{t}W\\kern-0.2em j_{\\mathrm{EW}}}$ process. This process has embedded within it a $tW$-scattering vertex, which is probed directly for the first time. The collision data were collected with the ATLAS detector during Run 2 of the LHC and correspond to an integrated luminosity of 140 $\\mathrm{fb^{-1}}$ at $\\sqrt{s}=13$~TeV. The search uses same-charge pairs of electrons and muons together with jets, of which at least one is $b$-tagged. The p"},"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":"2509.19038","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ex","submitted_at":"2025-09-23T14:09:07Z","cross_cats_sorted":[],"title_canon_sha256":"436d4890ced17d0d258834740161d7d4974d131e6d4c62ab193197c4d5ea0ae4","abstract_canon_sha256":"ba7b864d00147e5deb6d17e6b1ce972e9f41e969ef97829a1280af1f2c74f124"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-07T02:17:10.349958Z","signature_b64":"UUPMWoU5JMCVtiuu+i3LRNlrz52wVJ8jgXPAA17N8YCrjDRjo2ejLOPCmrPmmrc3gQ1B634+A/adXR1eMvygAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"77a599aaac91fe7e89bd09c2861e5219fe1e990794e6d304c07ad170fb09ccde","last_reissued_at":"2026-07-07T02:17:10.349112Z","signature_status":"signed_v1","first_computed_at":"2026-07-07T02:17:10.349112Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"A search for electroweak $t\\bar{t}Wj$ production in multileptonic final states at $\\sqrt{s} = 13$ TeV with the ATLAS detector and bounds on effective field theory operators","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"ATLAS Collaboration","submitted_at":"2025-09-23T14:09:07Z","abstract_excerpt":"A search is presented for the electroweak production of a top quark pair in association with a $W$ boson and at least one additional jet, known as the ${t\\bar{t}W\\kern-0.2em j_{\\mathrm{EW}}}$ process. This process has embedded within it a $tW$-scattering vertex, which is probed directly for the first time. The collision data were collected with the ATLAS detector during Run 2 of the LHC and correspond to an integrated luminosity of 140 $\\mathrm{fb^{-1}}$ at $\\sqrt{s}=13$~TeV. The search uses same-charge pairs of electrons and muons together with jets, of which at least one is $b$-tagged. The p"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2509.19038","kind":"arxiv","version":1},"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/2509.19038/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":"2509.19038","created_at":"2026-07-07T02:17:10.349224+00:00"},{"alias_kind":"arxiv_version","alias_value":"2509.19038v1","created_at":"2026-07-07T02:17:10.349224+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2509.19038","created_at":"2026-07-07T02:17:10.349224+00:00"},{"alias_kind":"pith_short_12","alias_value":"O6SZTKVMSH7H","created_at":"2026-07-07T02:17:10.349224+00:00"},{"alias_kind":"pith_short_16","alias_value":"O6SZTKVMSH7H5CN5","created_at":"2026-07-07T02:17:10.349224+00:00"},{"alias_kind":"pith_short_8","alias_value":"O6SZTKVM","created_at":"2026-07-07T02:17:10.349224+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2604.11586","citing_title":"Rare top quark production and top quark properties in ATLAS and CMS","ref_index":4,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/O6SZTKVMSH7H5CN5BHBIMHSSDH","json":"https://pith.science/pith/O6SZTKVMSH7H5CN5BHBIMHSSDH.json","graph_json":"https://pith.science/api/pith-number/O6SZTKVMSH7H5CN5BHBIMHSSDH/graph.json","events_json":"https://pith.science/api/pith-number/O6SZTKVMSH7H5CN5BHBIMHSSDH/events.json","paper":"https://pith.science/paper/O6SZTKVM"},"agent_actions":{"view_html":"https://pith.science/pith/O6SZTKVMSH7H5CN5BHBIMHSSDH","download_json":"https://pith.science/pith/O6SZTKVMSH7H5CN5BHBIMHSSDH.json","view_paper":"https://pith.science/paper/O6SZTKVM","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2509.19038&json=true","fetch_graph":"https://pith.science/api/pith-number/O6SZTKVMSH7H5CN5BHBIMHSSDH/graph.json","fetch_events":"https://pith.science/api/pith-number/O6SZTKVMSH7H5CN5BHBIMHSSDH/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/O6SZTKVMSH7H5CN5BHBIMHSSDH/action/timestamp_anchor","attest_storage":"https://pith.science/pith/O6SZTKVMSH7H5CN5BHBIMHSSDH/action/storage_attestation","attest_author":"https://pith.science/pith/O6SZTKVMSH7H5CN5BHBIMHSSDH/action/author_attestation","sign_citation":"https://pith.science/pith/O6SZTKVMSH7H5CN5BHBIMHSSDH/action/citation_signature","submit_replication":"https://pith.science/pith/O6SZTKVMSH7H5CN5BHBIMHSSDH/action/replication_record"}},"created_at":"2026-07-07T02:17:10.349224+00:00","updated_at":"2026-07-07T02:17:10.349224+00:00"}