{"as_of":"2026-08-06T16:56:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:c63e056975b43d0363000de54509cf8d7760c94779538e080fdb0eb3ee844523","coverage":[{"denominator":0,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":0,"source":"paper_references, paper_reference_links","source_observed_at":null,"state":"measured"},{"denominator":10,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":10,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-06T06:34:29.942622+00:00","state":"measured"},{"denominator":10,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":10,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-05T16:04:16.913222Z","state":"measured"},{"denominator":1,"lane":"external_citation_measurements","note":"A source-named dated measurement, never combined with another source.","records_observed":1,"source":"pith","source_observed_at":"2026-08-05T02:28:24.338817Z","state":"measured"}],"external_citation_measurements":[{"count":164,"observed_at":"2026-08-05T02:28:24.338817Z","source":"pith"}],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"1711.02116","last_updated":"2018-02-09T14:49:00Z","snapshot_observed_at":"2026-08-02T23:41:35.458402Z","submitted_at":"2017-11-06T19:11:23Z","title":"Large NLO corrections in $t\\bar{t}W^{\\pm}$ and $t\\bar{t}t\\bar{t}$ hadroproduction from supposedly subleading EW contributions","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1711.02116","snapshot_observed_at":"2026-08-05T16:04:16.913222Z","title":"Large NLO corrections int ¯tW ± andt ¯tt¯t hadroproduction from supposedly subleading EW contributions,","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2508.19137","last_updated":"2025-09-10T17:58:12Z","snapshot_observed_at":"2026-08-06T14:23:25.490873Z","submitted_at":"2025-08-26T15:41:21Z","title":"Triple top baryon $\\Omega_{ttt}$","version":2},"reference_index":51,"source":"pdf_text","source_observed_at":"2026-08-05T16:04:16.913222Z"},"links":{"cited_paper":"/paper/1711.02116","citing_paper":"/paper/2508.19137"},"observation_digest":"sha256:9851f4637703aa0eb4659c84a34c66bdc14d8ea03f4f3d87ee636bc5227354ee","observation_id":"edcffb71-786a-4538-a0d2-a5e5faaed557","resolution":{"observed_at":"2026-08-05T16:04:16.913222Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1711.02116","last_updated":"2018-02-09T14:49:00Z","snapshot_observed_at":"2026-08-02T23:41:35.458402Z","submitted_at":"2017-11-06T19:11:23Z","title":"Large NLO corrections in $t\\bar{t}W^{\\pm}$ and $t\\bar{t}t\\bar{t}$ hadroproduction from supposedly subleading EW contributions","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1711.02116","snapshot_observed_at":"2026-08-04T15:42:07.860929Z","title":"Frederix, D","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2509.19038","last_updated":"2025-09-23T14:09:07Z","snapshot_observed_at":"2026-08-04T15:41:57.019062Z","submitted_at":"2025-09-23T14:09:07Z","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","version":1},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-04T15:42:07.860929Z"},"links":{"cited_paper":"/paper/1711.02116","citing_paper":"/paper/2509.19038"},"observation_digest":"sha256:7912658baf68d80df6191f3a026df136b491e8c583de60ed11ef829d9dce07a5","observation_id":"6ecf8d86-add7-41fc-8e12-4cc2ba042383","resolution":{"observed_at":"2026-08-04T15:42:07.860929Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1711.02116","last_updated":"2018-02-09T14:49:00Z","snapshot_observed_at":"2026-08-02T23:41:35.458402Z","submitted_at":"2017-11-06T19:11:23Z","title":"Large NLO corrections in $t\\bar{t}W^{\\pm}$ and $t\\bar{t}t\\bar{t}$ hadroproduction from supposedly subleading EW contributions","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1711.02116","snapshot_observed_at":"2026-08-04T13:34:57.610117Z","title":"Frederix, D","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2510.00686","last_updated":"2026-05-26T10:36:09Z","snapshot_observed_at":"2026-08-04T13:34:56.161899Z","submitted_at":"2025-10-01T09:08:33Z","title":"Phenomenology of a Kinetic Higgs Portal","version":2},"reference_index":56,"source":"pdf_text","source_observed_at":"2026-08-04T13:34:57.610117Z"},"links":{"cited_paper":"/paper/1711.02116","citing_paper":"/paper/2510.00686"},"observation_digest":"sha256:931e1a39e08302b4859a88a2b80f2b1d4a4dc5046e08a382eb289636ee936ad8","observation_id":"0c073f87-84c8-4dc5-8a3f-a5774b5aa103","resolution":{"observed_at":"2026-08-04T13:34:57.610117Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1711.02116","last_updated":"2018-02-09T14:49:00Z","snapshot_observed_at":"2026-08-02T23:41:35.458402Z","submitted_at":"2017-11-06T19:11:23Z","title":"Large NLO corrections in $t\\bar{t}W^{\\pm}$ and $t\\bar{t}t\\bar{t}$ hadroproduction from supposedly subleading EW contributions","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1711.02116","snapshot_observed_at":"2026-08-04T07:59:10.470394Z","title":"Frederix, D","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2510.23755","last_updated":"2026-07-19T03:02:11Z","snapshot_observed_at":"2026-08-06T03:12:50.223235Z","submitted_at":"2025-10-27T18:41:11Z","title":"Measurement of the Higgs boson production in association with top quarks in multilepton final states in $pp$ collisions at $\\sqrt{s}=13$ TeV with the ATLAS detector","version":2},"reference_index":75,"source":"pdf_text","source_observed_at":"2026-08-04T07:59:10.470394Z"},"links":{"cited_paper":"/paper/1711.02116","citing_paper":"/paper/2510.23755"},"observation_digest":"sha256:a6049caf499929d799efba847e94bdc698558bbabd85c996b73e972e3cddce70","observation_id":"80c97e45-d968-4e62-921b-444009476c6f","resolution":{"observed_at":"2026-08-04T07:59:10.470394Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1711.02116","last_updated":"2018-02-09T14:49:00Z","snapshot_observed_at":"2026-08-02T23:41:35.458402Z","submitted_at":"2017-11-06T19:11:23Z","title":"Large NLO corrections in $t\\bar{t}W^{\\pm}$ and $t\\bar{t}t\\bar{t}$ hadroproduction from supposedly subleading EW contributions","version":2},"cited_work":{"arxiv_id":"1711.02116","doi":"10.1007/jhep02(2018)031","metadata_source":"pith","pith_arxiv_id":"1711.02116","snapshot_observed_at":"2026-08-05T02:49:54.815029Z","title":"Large NLO corrections in $t\\bar{t}W^{\\pm}$ and $t\\bar{t}t\\bar{t}$ hadroproduction from supposedly subleading EW contributions","venue":"hep-ph","work_id":"0931dec7-1b05-4a16-a2d7-731c0461de86","year":2017},"citing_paper":{"arxiv_id":"2605.18382","last_updated":"2026-05-18T13:27:32Z","snapshot_observed_at":"2026-08-02T20:31:02.423577Z","submitted_at":"2026-05-18T13:27:32Z","title":"Probing SMEFT Operators through $t\\bar{t}t\\bar{t}$ Production with Hyper-Graph Neural Networks at the LHC","version":1},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-05-20T09:37:11.490001Z"},"links":{"cited_paper":"/paper/1711.02116","citing_paper":"/paper/2605.18382"},"observation_digest":"sha256:210a9a1586ec10b22163d0fd6ee3247c8f7781097da0c7d0ce51e32d088727d3","observation_id":"635a0cbc-b615-463b-8446-5328fa7e1b57","resolution":{"observed_at":"2026-05-20T09:38:10.748042Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-06T06:34:29.942622+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-06T06:34:29.942622+00:00","source":"crossref"},{"observed_at":"2026-08-06T06:34:23.284952+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1711.02116","last_updated":"2018-02-09T14:49:00Z","snapshot_observed_at":"2026-08-02T23:41:35.458402Z","submitted_at":"2017-11-06T19:11:23Z","title":"Large NLO corrections in $t\\bar{t}W^{\\pm}$ and $t\\bar{t}t\\bar{t}$ hadroproduction from supposedly subleading EW contributions","version":2},"cited_work":{"arxiv_id":"1711.02116","doi":"10.1007/jhep02(2018)031","metadata_source":"pith","pith_arxiv_id":"1711.02116","snapshot_observed_at":"2026-08-05T02:49:54.815029Z","title":"Large NLO corrections in $t\\bar{t}W^{\\pm}$ and $t\\bar{t}t\\bar{t}$ hadroproduction from supposedly subleading EW contributions","venue":"hep-ph","work_id":"0931dec7-1b05-4a16-a2d7-731c0461de86","year":2017},"citing_paper":{"arxiv_id":"2606.09503","last_updated":"2026-06-08T13:55:41Z","snapshot_observed_at":"2026-08-02T16:50:31.086766Z","submitted_at":"2026-06-08T13:55:41Z","title":"NNLO QCD predictions for $t\\bar t W$ production at hadron colliders","version":1},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-06-27T16:08:21.973424Z"},"links":{"cited_paper":"/paper/1711.02116","citing_paper":"/paper/2606.09503"},"observation_digest":"sha256:4ff07ece1878e662673a224f05f8d631a3a69ab137cf1199d183c2c140a4c1b2","observation_id":"3682089c-0bae-4ff0-ba99-d9f51863d96d","resolution":{"observed_at":"2026-07-03T02:07:34.121028Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-06T06:34:29.942622+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-06T06:34:29.942622+00:00","source":"crossref"},{"observed_at":"2026-08-06T06:34:23.284952+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1711.02116","last_updated":"2018-02-09T14:49:00Z","snapshot_observed_at":"2026-08-02T23:41:35.458402Z","submitted_at":"2017-11-06T19:11:23Z","title":"Large NLO corrections in $t\\bar{t}W^{\\pm}$ and $t\\bar{t}t\\bar{t}$ hadroproduction from supposedly subleading EW contributions","version":2},"cited_work":{"arxiv_id":"1711.02116","doi":"10.1007/jhep02(2018)031","metadata_source":"pith","pith_arxiv_id":"1711.02116","snapshot_observed_at":"2026-08-05T02:49:54.815029Z","title":"Large NLO corrections in $t\\bar{t}W^{\\pm}$ and $t\\bar{t}t\\bar{t}$ hadroproduction from supposedly subleading EW contributions","venue":"hep-ph","work_id":"0931dec7-1b05-4a16-a2d7-731c0461de86","year":2017},"citing_paper":{"arxiv_id":"2606.30862","last_updated":"2026-06-29T19:49:30Z","snapshot_observed_at":"2026-08-03T00:01:57.335606Z","submitted_at":"2026-06-29T19:49:30Z","title":"Search for physics beyond the standard model in four and three top quark production events using proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":137,"source":"pdf_text","source_observed_at":"2026-07-11T11:50:26.030339Z"},"links":{"cited_paper":"/paper/1711.02116","citing_paper":"/paper/2606.30862"},"observation_digest":"sha256:1f9b2c7f893b8222eced097eaefd2a6d729a5b86e3a65167366f380cf658e36a","observation_id":"7e3a8b59-2b5b-403a-aff1-39f237ef4103","resolution":{"observed_at":"2026-07-01T01:25:12.732575Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-06T06:34:29.942622+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-06T06:34:29.942622+00:00","source":"crossref"},{"observed_at":"2026-08-06T06:34:23.284952+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1711.02116","last_updated":"2018-02-09T14:49:00Z","snapshot_observed_at":"2026-08-02T23:41:35.458402Z","submitted_at":"2017-11-06T19:11:23Z","title":"Large NLO corrections in $t\\bar{t}W^{\\pm}$ and $t\\bar{t}t\\bar{t}$ hadroproduction from supposedly subleading EW contributions","version":2},"cited_work":{"arxiv_id":"1711.02116","doi":"10.1007/jhep02(2018)031","metadata_source":"pith","pith_arxiv_id":"1711.02116","snapshot_observed_at":"2026-08-05T02:49:54.815029Z","title":"Large NLO corrections in $t\\bar{t}W^{\\pm}$ and $t\\bar{t}t\\bar{t}$ hadroproduction from supposedly subleading EW contributions","venue":"hep-ph","work_id":"0931dec7-1b05-4a16-a2d7-731c0461de86","year":2017},"citing_paper":{"arxiv_id":"2606.31823","last_updated":"2026-06-30T15:34:16Z","snapshot_observed_at":"2026-07-31T16:42:46.561890Z","submitted_at":"2026-06-30T15:34:16Z","title":"NNLO QCD predictions for $t\\bar{t}W$ production at the LHC","version":1},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-07-01T04:24:31.719981Z"},"links":{"cited_paper":"/paper/1711.02116","citing_paper":"/paper/2606.31823"},"observation_digest":"sha256:5829f57475a2370d98021662dece85f5d671fbcc2671cef48eae8045c94ac552","observation_id":"c8de8831-2a2d-49a7-9f71-f527fe7eef71","resolution":{"observed_at":"2026-07-01T11:35:42.344305Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-06T06:34:29.942622+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-06T06:34:29.942622+00:00","source":"crossref"},{"observed_at":"2026-08-06T06:34:23.284952+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1711.02116","last_updated":"2018-02-09T14:49:00Z","snapshot_observed_at":"2026-08-02T23:41:35.458402Z","submitted_at":"2017-11-06T19:11:23Z","title":"Large NLO corrections in $t\\bar{t}W^{\\pm}$ and $t\\bar{t}t\\bar{t}$ hadroproduction from supposedly subleading EW contributions","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1711.02116","snapshot_observed_at":"2026-08-01T09:38:05.089941Z","title":"Frederix, D","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2607.27323","last_updated":"2026-07-29T18:00:01Z","snapshot_observed_at":"2026-08-03T03:54:38.407308Z","submitted_at":"2026-07-29T18:00:01Z","title":"The inseparable three and four tops","version":1},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-08-01T09:38:05.089941Z"},"links":{"cited_paper":"/paper/1711.02116","citing_paper":"/paper/2607.27323"},"observation_digest":"sha256:20136d870413b99a2cfcba4c3dc67d16259ce612c9b7210456411592e69fc881","observation_id":"dd5b0268-b11c-4391-b4da-65d68622fb3f","resolution":{"observed_at":"2026-08-01T09:38:05.089941Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1711.02116","last_updated":"2018-02-09T14:49:00Z","snapshot_observed_at":"2026-08-02T23:41:35.458402Z","submitted_at":"2017-11-06T19:11:23Z","title":"Large NLO corrections in $t\\bar{t}W^{\\pm}$ and $t\\bar{t}t\\bar{t}$ hadroproduction from supposedly subleading EW contributions","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1711.02116","snapshot_observed_at":"2026-08-05T13:42:47.254295Z","title":"Frederix, D","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2608.03746","last_updated":"2026-08-04T14:39:09Z","snapshot_observed_at":"2026-08-06T15:37:33.585941Z","submitted_at":"2026-08-04T14:39:09Z","title":"Two-loop QCD amplitudes for $t\\bar{t}W$ production at the LHC in the leading-colour approximation","version":1},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-08-05T13:42:47.254295Z"},"links":{"cited_paper":"/paper/1711.02116","citing_paper":"/paper/2608.03746"},"observation_digest":"sha256:083be96492b1fde841fcc550ba6f6b03119c518b1d5a723ca02ce78dae85c66d","observation_id":"2bf11f48-8d8c-4d8e-8844-2d2ff15d3142","resolution":{"observed_at":"2026-08-05T13:42:47.254295Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"links":{"evidence":"/evidence","html":"/paper/1711.02116/citation-record","integrity":"/paper/1711.02116/integrity","json":"/paper/1711.02116/citation-record.json","paper":"/paper/1711.02116"},"outbound":[],"paper":{"arxiv_id":"1711.02116","last_updated":"2018-02-09T14:49:00Z","latest_version":2,"primary_category":"hep-ph","snapshot_observed_at":"2026-08-02T23:41:35.458402Z","submitted_at":"2017-11-06T19:11:23Z","title":"Large NLO corrections in $t\\bar{t}W^{\\pm}$ and $t\\bar{t}t\\bar{t}$ hadroproduction from supposedly subleading EW contributions"},"reference_resolution":{"displayed":0,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":0,"verified_exact":0,"verified_fuzzy":0},"total_outbound_references":0},"refusal":"A citation records a reference. It does not transfer a finding from one paper to another.","schema":"pith.paper-citation-record.v1","standing_sources":[{"observed_at":"2026-08-06T06:34:29.942622+00:00","source":"crossref"},{"observed_at":"2026-08-06T06:34:23.284952+00:00","source":"retraction_watch"}],"thesis":"As of 6 August 2026, this Paper Citation Record lists 0 of 0 outbound references and 10 inbound Pith citation observations for arXiv:1711.02116."}