{"as_of":"2026-08-11T19:51:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:cd3415198273d70921bb599392a3005b026cda0af7dbe17c8612d842d7d292c7","coverage":[{"denominator":63,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":63,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-11T10:58:56.198881Z","state":"measured"},{"denominator":65,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":65,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-11T06:34:44.6726+00:00","state":"measured"},{"denominator":2,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":2,"source":"paper_references, paper_reference_links","source_observed_at":"2026-07-11T20:37:53.493266Z","state":"measured"},{"denominator":1,"lane":"external_citation_measurements","note":"A source-named dated measurement, never combined with another source.","records_observed":0,"source":"arxiv_reference","source_observed_at":"2026-05-19T15:57:49.689856Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"2412.16020","last_updated":"2025-06-03T08:19:02Z","snapshot_observed_at":"2026-08-11T10:50:33.964800Z","submitted_at":"2024-12-20T16:10:03Z","title":"Dimension-8 operators in $W^+W^-$ production via gluon fusion","version":2},"cited_work":{"arxiv_id":"2412.16020","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2412.16020","snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Gillies, A","venue":null,"work_id":"a1f57c3f-061c-4d53-97f2-8c1b03305c5f","year":null},"citing_paper":{"arxiv_id":"2605.15262","last_updated":"2026-05-14T18:00:00Z","snapshot_observed_at":"2026-08-01T16:34:36.445112Z","submitted_at":"2026-05-14T18:00:00Z","title":"USMEFT as a tool for discovery of universal new physics at high luminosity LHC","version":1},"reference_index":42,"source":"pdf_text","source_observed_at":"2026-05-19T15:54:46.892619Z"},"links":{"cited_paper":"/paper/2412.16020","citing_paper":"/paper/2605.15262"},"observation_digest":"sha256:b2970748f7af7821d565b0223ae863c6753af0c736ca298b0b5d85968dbaab63","observation_id":"72d181bf-5cad-4f39-88da-a8534f9ecaa0","resolution":{"observed_at":"2026-05-19T15:57:49.694551Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2412.16020","last_updated":"2025-06-03T08:19:02Z","snapshot_observed_at":"2026-08-11T10:50:33.964800Z","submitted_at":"2024-12-20T16:10:03Z","title":"Dimension-8 operators in $W^+W^-$ production via gluon fusion","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2412.16020","snapshot_observed_at":"2026-07-11T20:37:53.493266Z","title":"Gillies, A","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2607.04251","last_updated":"2026-07-05T12:02:09Z","snapshot_observed_at":"2026-08-01T18:28:25.038234Z","submitted_at":"2026-07-05T12:02:09Z","title":"Anomalous triple gauge couplings in the light of dimension-8 operators in $W^+W^-$","version":1},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-07-11T20:37:53.493266Z"},"links":{"cited_paper":"/paper/2412.16020","citing_paper":"/paper/2607.04251"},"observation_digest":"sha256:4a92242037f5a30e27d8197864fb6726deef7d3757d25f08daae4d74830940ce","observation_id":"5f4588da-4a88-48f9-9493-8c310025fedb","resolution":{"observed_at":"2026-07-11T20:37:53.493266Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"links":{"evidence":"/evidence","html":"/paper/2412.16020/citation-record","integrity":"/paper/2412.16020/integrity","json":"/paper/2412.16020/citation-record.json","paper":"/paper/2412.16020"},"outbound":[{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-11T10:58:57.055462Z","title":"collaboration, Summary Plots for Heavy Particle Searches and Long-lived Particle Searches - March 2023 ,","venue":null,"work_id":"1e428d61-42d4-4ba6-be16-26fe5ccba5ba","year":2023},"citing_paper":{"arxiv_id":"2412.16020","last_updated":"2025-06-03T08:19:02Z","snapshot_observed_at":"2026-08-11T10:50:33.964800Z","submitted_at":"2024-12-20T16:10:03Z","title":"Dimension-8 operators in $W^+W^-$ production via gluon fusion","version":2},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-08-11T10:58:55.959520Z"},"links":{"citing_paper":"/paper/2412.16020"},"observation_digest":"sha256:811c955c70755291bb45e8712580b499a9dd6edddb4869df71c3f2479a890599","observation_id":"c25ec315-c03d-4ad7-a8ab-c694a07fc9c7","resolution":{"observed_at":"2026-08-11T10:58:57.059270Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2405.18661","last_updated":"2025-04-08T17:57:05Z","snapshot_observed_at":"2026-08-11T02:01:29.495658Z","submitted_at":"2024-05-28T23:54:05Z","title":"Stairway to discovery: a report on the CMS programme of cross section measurements from millibarns to femtobarns","version":2},"cited_work":{"arxiv_id":"2405.18661","doi":null,"metadata_source":"pith","pith_arxiv_id":"2405.18661","snapshot_observed_at":"2026-08-11T10:58:56.877644Z","title":"Stairway to discovery: a report on the CMS programme of cross section measurements from millibarns to femtobarns","venue":"hep-ex","work_id":"5eb3e654-9121-4bfc-9266-eeccb88b7998","year":2024},"citing_paper":{"arxiv_id":"2412.16020","last_updated":"2025-06-03T08:19:02Z","snapshot_observed_at":"2026-08-11T10:50:33.964800Z","submitted_at":"2024-12-20T16:10:03Z","title":"Dimension-8 operators in $W^+W^-$ production via gluon fusion","version":2},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-08-11T10:58:55.963796Z"},"links":{"cited_paper":"/paper/2405.18661","citing_paper":"/paper/2412.16020"},"observation_digest":"sha256:9f7b04d54f02d16424b598db7d55d49adcb2621082f27bd624c5e692cff3f001","observation_id":"9f334fa4-c7ab-460e-92ff-76204ab68377","resolution":{"observed_at":"2026-08-11T10:58:56.881675Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1909.02845","last_updated":"2020-02-11T07:45:49Z","snapshot_observed_at":"2026-08-09T06:35:35.956579Z","submitted_at":"2019-09-06T12:16:38Z","title":"Combined measurements of Higgs boson production and decay using up to $80$ fb$^{-1}$ of proton-proton collision data at $\\sqrt{s}=$ 13 TeV collected with the ATLAS experiment","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1909.02845","snapshot_observed_at":"2026-08-11T10:58:55.968430Z","title":"Aad et al., Combined measurements of Higgs boson production and decay using up to 80 fb−1 of proton-proton collision data at √s = 13 TeV collected with the ATLAS experiment , Phys","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2412.16020","last_updated":"2025-06-03T08:19:02Z","snapshot_observed_at":"2026-08-11T10:50:33.964800Z","submitted_at":"2024-12-20T16:10:03Z","title":"Dimension-8 operators in $W^+W^-$ production via gluon fusion","version":2},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-08-11T10:58:55.968430Z"},"links":{"cited_paper":"/paper/1909.02845","citing_paper":"/paper/2412.16020"},"observation_digest":"sha256:be69f00360edead243829494e3cc2b218b540097cdec5696435c24abdabcd387","observation_id":"f4a932ac-cb13-4e19-9019-6b5731c604c2","resolution":{"observed_at":"2026-08-11T10:58:55.968430Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-11T10:58:57.045018Z","title":null,"venue":null,"work_id":"e862aa76-09cf-4ccf-8dcf-f018114d096c","year":null},"citing_paper":{"arxiv_id":"2412.16020","last_updated":"2025-06-03T08:19:02Z","snapshot_observed_at":"2026-08-11T10:50:33.964800Z","submitted_at":"2024-12-20T16:10:03Z","title":"Dimension-8 operators in $W^+W^-$ production via gluon fusion","version":2},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-11T10:58:55.972546Z"},"links":{"citing_paper":"/paper/2412.16020"},"observation_digest":"sha256:3dbc01be80393771e5a0fbbdad12ff3c5aa737a3a71c384bf88556017d1455fa","observation_id":"86212921-67b9-44c5-ad5d-921249110239","resolution":{"observed_at":"2026-08-11T10:58:57.048666Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1706.08945","last_updated":"2018-11-12T14:43:11Z","snapshot_observed_at":"2026-07-06T02:11:23.670680Z","submitted_at":"2017-06-27T17:17:52Z","title":"The Standard Model as an Effective Field Theory","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1706.08945","snapshot_observed_at":"2026-08-11T10:58:55.976682Z","title":"Brivio and M","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2412.16020","last_updated":"2025-06-03T08:19:02Z","snapshot_observed_at":"2026-08-11T10:50:33.964800Z","submitted_at":"2024-12-20T16:10:03Z","title":"Dimension-8 operators in $W^+W^-$ production via gluon fusion","version":2},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-08-11T10:58:55.976682Z"},"links":{"cited_paper":"/paper/1706.08945","citing_paper":"/paper/2412.16020"},"observation_digest":"sha256:92e1bd10cf401e104cf6258688169ad9fed6fff16261ed00fcbb7c75531c9f4b","observation_id":"1314dd6f-4095-490f-b13a-afb169a0d959","resolution":{"observed_at":"2026-08-11T10:58:55.976682Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-11T10:58:57.033966Z","title":"Buchm¨ uller and D","venue":null,"work_id":"60b19e8e-66fa-4df8-8fa1-1f2c64eadad4","year":1986},"citing_paper":{"arxiv_id":"2412.16020","last_updated":"2025-06-03T08:19:02Z","snapshot_observed_at":"2026-08-11T10:50:33.964800Z","submitted_at":"2024-12-20T16:10:03Z","title":"Dimension-8 operators in $W^+W^-$ production via gluon fusion","version":2},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-11T10:58:55.981094Z"},"links":{"citing_paper":"/paper/2412.16020"},"observation_digest":"sha256:954eab5ca3762d8d90f42775fa496ccd94c9e1f03828760cc54d089432fe3edf","observation_id":"5ebcebe6-e914-4297-bf7a-30fc1eb75054","resolution":{"observed_at":"2026-08-11T10:58:57.037994Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1008.4884","last_updated":"2017-01-15T20:19:22Z","snapshot_observed_at":"2026-07-06T02:11:23.670680Z","submitted_at":"2010-08-28T19:19:07Z","title":"Dimension-Six Terms in the Standard Model Lagrangian","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1008.4884","snapshot_observed_at":"2026-08-11T10:58:55.984996Z","title":"Grzadkowski, M","venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"2412.16020","last_updated":"2025-06-03T08:19:02Z","snapshot_observed_at":"2026-08-11T10:50:33.964800Z","submitted_at":"2024-12-20T16:10:03Z","title":"Dimension-8 operators in $W^+W^-$ production via gluon fusion","version":2},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-11T10:58:55.984996Z"},"links":{"cited_paper":"/paper/1008.4884","citing_paper":"/paper/2412.16020"},"observation_digest":"sha256:c48e436268c290e73ee656802f14fbe31fea07e245f76c844d97df7518a9b077","observation_id":"b1269ed6-dc36-4b37-83fe-5b3f697a52c4","resolution":{"observed_at":"2026-08-11T10:58:55.984996Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2307.04784","last_updated":"2023-07-10T18:00:00Z","snapshot_observed_at":"2026-08-05T00:04:20.860288Z","submitted_at":"2023-07-10T18:00:00Z","title":"Positivity-causality competition: a road to ultimate EFT consistency constraints","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2307.04784","snapshot_observed_at":"2026-08-11T10:58:55.989202Z","title":"Carrillo Gonz´ alez, C","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2412.16020","last_updated":"2025-06-03T08:19:02Z","snapshot_observed_at":"2026-08-11T10:50:33.964800Z","submitted_at":"2024-12-20T16:10:03Z","title":"Dimension-8 operators in $W^+W^-$ production via gluon fusion","version":2},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-11T10:58:55.989202Z"},"links":{"cited_paper":"/paper/2307.04784","citing_paper":"/paper/2412.16020"},"observation_digest":"sha256:179058532f18e3160c6a965193f65cc41fef8dfbbb7bddeeb8a1adb9ee3cb716","observation_id":"7b81c8df-30d4-4fc3-a6a8-fcf1a3bb586d","resolution":{"observed_at":"2026-08-11T10:58:55.989202Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/0602178","last_updated":"2006-03-31T22:47:25Z","snapshot_observed_at":"2026-07-07T04:56:41.885342Z","submitted_at":"2006-02-20T20:30:07Z","title":"Causality, Analyticity and an IR Obstruction to UV Completion","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/0602178","snapshot_observed_at":"2026-08-11T10:58:55.993529Z","title":"Adams, N","venue":null,"work_id":null,"year":2006},"citing_paper":{"arxiv_id":"2412.16020","last_updated":"2025-06-03T08:19:02Z","snapshot_observed_at":"2026-08-11T10:50:33.964800Z","submitted_at":"2024-12-20T16:10:03Z","title":"Dimension-8 operators in $W^+W^-$ production via gluon fusion","version":2},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-11T10:58:55.993529Z"},"links":{"cited_paper":"/paper/hep-th/0602178","citing_paper":"/paper/2412.16020"},"observation_digest":"sha256:ce404825c3a3c26e1cba6b449862bde4d173e5ef7df07b23d585d1f951767e36","observation_id":"34986123-af50-446a-bb99-697888f0bd72","resolution":{"observed_at":"2026-08-11T10:58:55.993529Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1803.03252","last_updated":"2018-06-15T19:56:02Z","snapshot_observed_at":"2026-07-06T06:27:19.598924Z","submitted_at":"2018-03-08T18:49:48Z","title":"Updated Global SMEFT Fit to Higgs, Diboson and Electroweak Data","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1803.03252","snapshot_observed_at":"2026-08-11T10:58:55.997052Z","title":"Ellis, C","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2412.16020","last_updated":"2025-06-03T08:19:02Z","snapshot_observed_at":"2026-08-11T10:50:33.964800Z","submitted_at":"2024-12-20T16:10:03Z","title":"Dimension-8 operators in $W^+W^-$ production via gluon fusion","version":2},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-11T10:58:55.997052Z"},"links":{"cited_paper":"/paper/1803.03252","citing_paper":"/paper/2412.16020"},"observation_digest":"sha256:0f7247495aa378f2db6ece1eb6f96722c722e09e2daa2ee071b7ad25f3a66c71","observation_id":"8a61efe3-6e8f-4925-8832-92356a837bae","resolution":{"observed_at":"2026-08-11T10:58:55.997052Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1604.03105","last_updated":"2016-04-25T17:13:51Z","snapshot_observed_at":"2026-08-09T06:13:34.053486Z","submitted_at":"2016-04-11T20:00:00Z","title":"The Gauge-Higgs Legacy of the LHC Run I","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1604.03105","snapshot_observed_at":"2026-08-11T10:58:56.000413Z","title":"Butter, O","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2412.16020","last_updated":"2025-06-03T08:19:02Z","snapshot_observed_at":"2026-08-11T10:50:33.964800Z","submitted_at":"2024-12-20T16:10:03Z","title":"Dimension-8 operators in $W^+W^-$ production via gluon fusion","version":2},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-08-11T10:58:56.000413Z"},"links":{"cited_paper":"/paper/1604.03105","citing_paper":"/paper/2412.16020"},"observation_digest":"sha256:8674fb84ad5149131a113dc00c68019c68ce494768095e86e52a9edaa4d0813a","observation_id":"7c03bfee-a684-43ee-829b-21ca3c99b60a","resolution":{"observed_at":"2026-08-11T10:58:56.000413Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1610.07572","last_updated":"2017-09-21T11:57:03Z","snapshot_observed_at":"2026-07-06T05:15:48.443232Z","submitted_at":"2016-10-24T19:37:06Z","title":"Multi-Boson Interactions at the LHC","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1610.07572","snapshot_observed_at":"2026-08-11T10:58:56.003649Z","title":null,"venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2412.16020","last_updated":"2025-06-03T08:19:02Z","snapshot_observed_at":"2026-08-11T10:50:33.964800Z","submitted_at":"2024-12-20T16:10:03Z","title":"Dimension-8 operators in $W^+W^-$ production via gluon fusion","version":2},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-08-11T10:58:56.003649Z"},"links":{"cited_paper":"/paper/1610.07572","citing_paper":"/paper/2412.16020"},"observation_digest":"sha256:2df21ac368dd3b8df9dd20c320a32ad38f7d56bc3e6031d6f499bc588d90a15d","observation_id":"fa6ce9fd-d06f-45b2-b43c-58d476448033","resolution":{"observed_at":"2026-08-11T10:58:56.003649Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1610.01618","last_updated":"2017-11-16T03:53:20Z","snapshot_observed_at":"2026-07-06T05:13:30.860932Z","submitted_at":"2016-10-05T20:01:07Z","title":"Time to Go Beyond Triple-Gauge-Boson-Coupling Interpretation of $W$ Pair Production","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1610.01618","snapshot_observed_at":"2026-08-11T10:58:56.007008Z","title":"Zhang, Time to Go Beyond Triple-Gauge-Boson-Coupling Interpretation of W Pair Production, Phys","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2412.16020","last_updated":"2025-06-03T08:19:02Z","snapshot_observed_at":"2026-08-11T10:50:33.964800Z","submitted_at":"2024-12-20T16:10:03Z","title":"Dimension-8 operators in $W^+W^-$ production via gluon fusion","version":2},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-11T10:58:56.007008Z"},"links":{"cited_paper":"/paper/1610.01618","citing_paper":"/paper/2412.16020"},"observation_digest":"sha256:3a428f4f37bfe13f4e809bb6db01e7528ac1bbf2f93cb9494c11de4db4f800ac","observation_id":"b908dadb-a9dc-44ba-9105-00b6a4a4e1a0","resolution":{"observed_at":"2026-08-11T10:58:56.007008Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1708.03332","last_updated":"2017-10-17T14:13:08Z","snapshot_observed_at":"2026-08-06T23:10:42.786258Z","submitted_at":"2017-08-10T18:00:03Z","title":"An NLO QCD effective field theory analysis of $W^+_{}W^-_{}$ production at the LHC including fermionic operators","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1708.03332","snapshot_observed_at":"2026-08-11T10:58:56.010853Z","title":"Baglio, S","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2412.16020","last_updated":"2025-06-03T08:19:02Z","snapshot_observed_at":"2026-08-11T10:50:33.964800Z","submitted_at":"2024-12-20T16:10:03Z","title":"Dimension-8 operators in $W^+W^-$ production via gluon fusion","version":2},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-11T10:58:56.010853Z"},"links":{"cited_paper":"/paper/1708.03332","citing_paper":"/paper/2412.16020"},"observation_digest":"sha256:9b993d84c813ca1b8c7a45d0c58e3de01469fad33c25775ff9e840fd44760109","observation_id":"dc4f7453-c6d7-4dc7-bd00-d83a62abd5cb","resolution":{"observed_at":"2026-08-11T10:58:56.010853Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1812.00214","last_updated":"2019-02-12T17:52:15Z","snapshot_observed_at":"2026-07-06T07:18:24.861528Z","submitted_at":"2018-12-01T15:25:02Z","title":"NLO Effects in EFT Fits to $W^+W^-$ Production at the LHC","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1812.00214","snapshot_observed_at":"2026-08-11T10:58:56.014729Z","title":"Baglio, S","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2412.16020","last_updated":"2025-06-03T08:19:02Z","snapshot_observed_at":"2026-08-11T10:50:33.964800Z","submitted_at":"2024-12-20T16:10:03Z","title":"Dimension-8 operators in $W^+W^-$ production via gluon fusion","version":2},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-08-11T10:58:56.014729Z"},"links":{"cited_paper":"/paper/1812.00214","citing_paper":"/paper/2412.16020"},"observation_digest":"sha256:9d98377a24c5e6d5a488436dee32fa4421818f4d4173c4304f6a6c7c1bad7132","observation_id":"79ff7db6-76cd-41fd-b5f7-baecb8917863","resolution":{"observed_at":"2026-08-11T10:58:56.014729Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1909.11576","last_updated":"2019-12-11T18:55:41Z","snapshot_observed_at":"2026-08-10T00:03:35.825283Z","submitted_at":"2019-09-23T18:00:00Z","title":"QCD Corrections in SMEFT Fits to $WZ$ and $WW$ Production","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1909.11576","snapshot_observed_at":"2026-08-11T10:58:56.018713Z","title":"Baglio, S","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2412.16020","last_updated":"2025-06-03T08:19:02Z","snapshot_observed_at":"2026-08-11T10:50:33.964800Z","submitted_at":"2024-12-20T16:10:03Z","title":"Dimension-8 operators in $W^+W^-$ production via gluon fusion","version":2},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-08-11T10:58:56.018713Z"},"links":{"cited_paper":"/paper/1909.11576","citing_paper":"/paper/2412.16020"},"observation_digest":"sha256:6c3173f30dbe00bec3a02cbe967c9229892593556f12e5191b190dfa05505e9d","observation_id":"2cb315fc-1090-4200-9a44-117fa2533201","resolution":{"observed_at":"2026-08-11T10:58:56.018713Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2108.03199","last_updated":"2022-04-11T08:38:06Z","snapshot_observed_at":"2026-07-06T11:36:14.208411Z","submitted_at":"2021-08-06T16:42:22Z","title":"A sensitivity study of VBS and diboson WW to dimension-6 EFT operators at the LHC","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2108.03199","snapshot_observed_at":"2026-08-11T10:58:56.023084Z","title":"Bellan et al., A sensitivity study of VBS and diboson WW to dimension-6 EFT operators at the LHC , JHEP 05 (2022) 039, [ 2108.03199]","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2412.16020","last_updated":"2025-06-03T08:19:02Z","snapshot_observed_at":"2026-08-11T10:50:33.964800Z","submitted_at":"2024-12-20T16:10:03Z","title":"Dimension-8 operators in $W^+W^-$ production via gluon fusion","version":2},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-08-11T10:58:56.023084Z"},"links":{"cited_paper":"/paper/2108.03199","citing_paper":"/paper/2412.16020"},"observation_digest":"sha256:4c163517d4fe879eb8984de1822ded4b49efc790116aa7b0551291befbda20f5","observation_id":"32674a27-c3e2-4845-8ca6-ccdc827463da","resolution":{"observed_at":"2026-08-11T10:58:56.023084Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2108.04828","last_updated":"2021-12-27T13:59:28Z","snapshot_observed_at":"2026-08-11T12:15:43.788765Z","submitted_at":"2021-08-10T18:00:01Z","title":"Electroweak legacy of the LHC Run II","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2108.04828","snapshot_observed_at":"2026-08-11T10:58:56.027166Z","title":null,"venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2412.16020","last_updated":"2025-06-03T08:19:02Z","snapshot_observed_at":"2026-08-11T10:50:33.964800Z","submitted_at":"2024-12-20T16:10:03Z","title":"Dimension-8 operators in $W^+W^-$ production via gluon fusion","version":2},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-08-11T10:58:56.027166Z"},"links":{"cited_paper":"/paper/2108.04828","citing_paper":"/paper/2412.16020"},"observation_digest":"sha256:793732546bbb51afa2dfe1c0fa25ca9f49ff5f2e636fe30e9ea680729302d639","observation_id":"5adde8a7-2174-4960-9946-ff16b19e6a97","resolution":{"observed_at":"2026-08-11T10:58:56.027166Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1205.4231","last_updated":"2012-05-18T19:58:08Z","snapshot_observed_at":"2026-07-06T02:11:23.670680Z","submitted_at":"2012-05-18T19:58:08Z","title":"Effective Field Theory: A Modern Approach to Anomalous Couplings","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1205.4231","snapshot_observed_at":"2026-08-11T10:58:56.031005Z","title":"Degrande, N","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2412.16020","last_updated":"2025-06-03T08:19:02Z","snapshot_observed_at":"2026-08-11T10:50:33.964800Z","submitted_at":"2024-12-20T16:10:03Z","title":"Dimension-8 operators in $W^+W^-$ production via gluon fusion","version":2},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-08-11T10:58:56.031005Z"},"links":{"cited_paper":"/paper/1205.4231","citing_paper":"/paper/2412.16020"},"observation_digest":"sha256:11a1ef2e355414989e1ea8b1b0a870ed99aac7923447cbbc4e1e8191dd16c43b","observation_id":"fc16079f-ea25-46b0-92ec-e74fb81c8af9","resolution":{"observed_at":"2026-08-11T10:58:56.031005Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1609.06312","last_updated":"2017-02-13T16:09:22Z","snapshot_observed_at":"2026-08-11T11:04:28.652527Z","submitted_at":"2016-09-20T20:00:01Z","title":"Anomalous Triple Gauge Couplings in the Effective Field Theory Approach at the LHC","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1609.06312","snapshot_observed_at":"2026-08-11T10:58:56.034180Z","title":"Falkowski, M","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2412.16020","last_updated":"2025-06-03T08:19:02Z","snapshot_observed_at":"2026-08-11T10:50:33.964800Z","submitted_at":"2024-12-20T16:10:03Z","title":"Dimension-8 operators in $W^+W^-$ production via gluon fusion","version":2},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-08-11T10:58:56.034180Z"},"links":{"cited_paper":"/paper/1609.06312","citing_paper":"/paper/2412.16020"},"observation_digest":"sha256:7ee595a2c1e4f38a0c3c24fd3905b7af32fd5ee3836aa9b77150b43224a4b608","observation_id":"69395e5d-3225-4449-881a-bf7a07962f4b","resolution":{"observed_at":"2026-08-11T10:58:56.034180Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1902.11262","last_updated":"2019-08-05T18:56:51Z","snapshot_observed_at":"2026-08-11T14:34:27.457392Z","submitted_at":"2019-02-28T18:09:00Z","title":"Jet Substructure Measurements of Interference in Non-Interfering SMEFT Effects","version":2},"cited_work":{"arxiv_id":"1902.11262","doi":null,"metadata_source":"pith","pith_arxiv_id":"1902.11262","snapshot_observed_at":"2026-08-11T10:58:56.703977Z","title":"Jet Substructure Measurements of Interference in Non-Interfering SMEFT Effects","venue":"hep-ph","work_id":"1b015e79-4a95-4d2e-b07c-29bf0f18b779","year":2019},"citing_paper":{"arxiv_id":"2412.16020","last_updated":"2025-06-03T08:19:02Z","snapshot_observed_at":"2026-08-11T10:50:33.964800Z","submitted_at":"2024-12-20T16:10:03Z","title":"Dimension-8 operators in $W^+W^-$ production via gluon fusion","version":2},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-08-11T10:58:56.038213Z"},"links":{"cited_paper":"/paper/1902.11262","citing_paper":"/paper/2412.16020"},"observation_digest":"sha256:9bb356e07ddad486c7fde502c3fbc60a25e1a560ac53ab6cbf86e192af07532c","observation_id":"642a97b9-281d-4be1-9d32-f7aa3b595f78","resolution":{"observed_at":"2026-08-11T10:58:56.708433Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2112.06729","last_updated":"2022-05-08T15:43:02Z","snapshot_observed_at":"2026-07-06T12:18:11.444272Z","submitted_at":"2021-12-13T15:33:04Z","title":"Hadron Collider Probes of the Quartic Couplings of Gluons to the Photon and $Z$ Boson","version":4},"cited_work":{"arxiv_id":"2112.06729","doi":null,"metadata_source":"pith","pith_arxiv_id":"2112.06729","snapshot_observed_at":"2026-08-11T10:58:56.687890Z","title":"Hadron Collider Probes of the Quartic Couplings of Gluons to the Photon and $Z$ Boson","venue":"hep-ph","work_id":"a2827cd4-c8b9-43ea-8c5b-64b23dbc534f","year":2021},"citing_paper":{"arxiv_id":"2412.16020","last_updated":"2025-06-03T08:19:02Z","snapshot_observed_at":"2026-08-11T10:50:33.964800Z","submitted_at":"2024-12-20T16:10:03Z","title":"Dimension-8 operators in $W^+W^-$ production via gluon fusion","version":2},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-08-11T10:58:56.041786Z"},"links":{"cited_paper":"/paper/2112.06729","citing_paper":"/paper/2412.16020"},"observation_digest":"sha256:88aea6410b9c24b362efe799fcb00bb62b3f23842e77c6494b1378bd7e756a16","observation_id":"2b3f77f6-0b22-4d40-9cbd-833466709f4c","resolution":{"observed_at":"2026-08-11T10:58:56.692109Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2312.09867","last_updated":"2023-12-15T15:11:14Z","snapshot_observed_at":"2026-07-06T17:02:54.291288Z","submitted_at":"2023-12-15T15:11:14Z","title":"A case study of SMEFT $\\mathcal O(1/\\Lambda^4)$ effects in diboson processes: $pp \\to W^\\pm(\\ell^\\pm \\nu) \\gamma$","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2312.09867","snapshot_observed_at":"2026-08-11T10:58:56.045516Z","title":"Martin, A case study of SMEFT O 1/Λ4 effects in diboson processes: pp → W(ℓν )γ, JHEP 05 (2024) 223, [ 2312.09867]","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2412.16020","last_updated":"2025-06-03T08:19:02Z","snapshot_observed_at":"2026-08-11T10:50:33.964800Z","submitted_at":"2024-12-20T16:10:03Z","title":"Dimension-8 operators in $W^+W^-$ production via gluon fusion","version":2},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-08-11T10:58:56.045516Z"},"links":{"cited_paper":"/paper/2312.09867","citing_paper":"/paper/2412.16020"},"observation_digest":"sha256:dc1e9fc18102f4891ec9a0c0cae57b4cbf2de38a7a56f3401572182f95a9f09c","observation_id":"b23c0b0a-2f5d-4ac2-887d-84f2a60b6019","resolution":{"observed_at":"2026-08-11T10:58:56.045516Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2303.10493","last_updated":"2023-04-04T08:40:30Z","snapshot_observed_at":"2026-08-01T15:47:12.771172Z","submitted_at":"2023-03-18T20:11:58Z","title":"Impact of Dimension-8 SMEFT operators on Diboson Productions","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2303.10493","snapshot_observed_at":"2026-08-11T10:58:56.049209Z","title":"Degrande and H.-L","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2412.16020","last_updated":"2025-06-03T08:19:02Z","snapshot_observed_at":"2026-08-11T10:50:33.964800Z","submitted_at":"2024-12-20T16:10:03Z","title":"Dimension-8 operators in $W^+W^-$ production via gluon fusion","version":2},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-08-11T10:58:56.049209Z"},"links":{"cited_paper":"/paper/2303.10493","citing_paper":"/paper/2412.16020"},"observation_digest":"sha256:95ad2d906ceb99057c921cd869023e8fc2ad3922c4c15fbdbe3f93f80c9bb1b4","observation_id":"178e385e-5e3b-4623-b966-72f637b89017","resolution":{"observed_at":"2026-08-11T10:58:56.049209Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1602.05141","last_updated":"2016-02-16T19:07:22Z","snapshot_observed_at":"2026-08-03T18:51:39.644898Z","submitted_at":"2016-02-16T19:07:22Z","title":"Anomalous coupling, top-mass and parton-shower effects in ${W^+W^-}$ production","version":1},"cited_work":{"arxiv_id":"1602.05141","doi":null,"metadata_source":"pith","pith_arxiv_id":"1602.05141","snapshot_observed_at":"2026-08-11T10:58:56.652486Z","title":"Anomalous coupling, top-mass and parton-shower effects in ${W^+W^-}$ production","venue":"hep-ph","work_id":"acd93682-4b69-4d4d-8f1a-05ce68802b94","year":2016},"citing_paper":{"arxiv_id":"2412.16020","last_updated":"2025-06-03T08:19:02Z","snapshot_observed_at":"2026-08-11T10:50:33.964800Z","submitted_at":"2024-12-20T16:10:03Z","title":"Dimension-8 operators in $W^+W^-$ production via gluon fusion","version":2},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-08-11T10:58:56.052867Z"},"links":{"cited_paper":"/paper/1602.05141","citing_paper":"/paper/2412.16020"},"observation_digest":"sha256:0cc4e0aa31b558c64c8d0081ddd475f180ddfaa76ed96ec7c96d996e1e480c98","observation_id":"c4b2923c-52b5-49c6-8eb1-d96d39f1ec3c","resolution":{"observed_at":"2026-08-11T10:58:56.657192Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2306.09963","last_updated":"2024-11-07T15:06:21Z","snapshot_observed_at":"2026-08-10T01:20:08.146566Z","submitted_at":"2023-06-16T16:45:13Z","title":"Diboson production in the SMEFT from gluon fusion","version":2},"cited_work":{"arxiv_id":"2306.09963","doi":null,"metadata_source":"pith","pith_arxiv_id":"2306.09963","snapshot_observed_at":"2026-08-11T10:58:56.637617Z","title":"Diboson production in the SMEFT from gluon fusion","venue":"hep-ph","work_id":"7dbd0a85-1762-4520-89b5-5b236f8a4bea","year":2023},"citing_paper":{"arxiv_id":"2412.16020","last_updated":"2025-06-03T08:19:02Z","snapshot_observed_at":"2026-08-11T10:50:33.964800Z","submitted_at":"2024-12-20T16:10:03Z","title":"Dimension-8 operators in $W^+W^-$ production via gluon fusion","version":2},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-08-11T10:58:56.056581Z"},"links":{"cited_paper":"/paper/2306.09963","citing_paper":"/paper/2412.16020"},"observation_digest":"sha256:38d5988d1bd4dd1829119abffd099e93e890e3fbd16a11ed5086c4cbbdbeaffc","observation_id":"6b79436b-cb81-4211-af5f-4d2f01f91c24","resolution":{"observed_at":"2026-08-11T10:58:56.641813Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1309.5273","last_updated":"2014-03-28T14:30:25Z","snapshot_observed_at":"2026-07-06T03:23:33.025529Z","submitted_at":"2013-09-20T14:08:28Z","title":"Probing Higgs couplings with high p_T Higgs production","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1309.5273","snapshot_observed_at":"2026-08-11T10:58:56.060295Z","title":"Azatov and A","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2412.16020","last_updated":"2025-06-03T08:19:02Z","snapshot_observed_at":"2026-08-11T10:50:33.964800Z","submitted_at":"2024-12-20T16:10:03Z","title":"Dimension-8 operators in $W^+W^-$ production via gluon fusion","version":2},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-08-11T10:58:56.060295Z"},"links":{"cited_paper":"/paper/1309.5273","citing_paper":"/paper/2412.16020"},"observation_digest":"sha256:5186af9f463ef923071a968a70ecc4e064a07ce6155d859f482454ea19e18509","observation_id":"3f136cb0-599a-494f-abf1-9abdcc26a08f","resolution":{"observed_at":"2026-08-11T10:58:56.060295Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1312.3317","last_updated":"2014-04-09T23:12:55Z","snapshot_observed_at":"2026-07-06T03:30:38.831652Z","submitted_at":"2013-12-11T20:57:43Z","title":"Very boosted Higgs in gluon fusion","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1312.3317","snapshot_observed_at":"2026-08-11T10:58:56.064015Z","title":"Grojean, E","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2412.16020","last_updated":"2025-06-03T08:19:02Z","snapshot_observed_at":"2026-08-11T10:50:33.964800Z","submitted_at":"2024-12-20T16:10:03Z","title":"Dimension-8 operators in $W^+W^-$ production via gluon fusion","version":2},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-08-11T10:58:56.064015Z"},"links":{"cited_paper":"/paper/1312.3317","citing_paper":"/paper/2412.16020"},"observation_digest":"sha256:4b06a8cd236c3f974defcc658a6a9a8ed04ad8570ce2ec1ae35476aa7f68b5de","observation_id":"ba34cdaa-0cee-4fae-81c0-9faf928f1dd5","resolution":{"observed_at":"2026-08-11T10:58:56.064015Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1308.4771","last_updated":"2013-08-22T06:28:40Z","snapshot_observed_at":"2026-07-06T03:21:10.650690Z","submitted_at":"2013-08-22T06:28:40Z","title":"Probing top-partners in Higgs + jets","version":1},"cited_work":{"arxiv_id":"1308.4771","doi":null,"metadata_source":"pith","pith_arxiv_id":"1308.4771","snapshot_observed_at":"2026-08-11T10:58:56.601314Z","title":"Probing top-partners in Higgs + jets","venue":"hep-ph","work_id":"9c937274-17c2-404e-b719-58b955db1e36","year":2013},"citing_paper":{"arxiv_id":"2412.16020","last_updated":"2025-06-03T08:19:02Z","snapshot_observed_at":"2026-08-11T10:50:33.964800Z","submitted_at":"2024-12-20T16:10:03Z","title":"Dimension-8 operators in $W^+W^-$ production via gluon fusion","version":2},"reference_index":29,"source":"pdf_text","source_observed_at":"2026-08-11T10:58:56.068028Z"},"links":{"cited_paper":"/paper/1308.4771","citing_paper":"/paper/2412.16020"},"observation_digest":"sha256:a7f6dcd78b980f5fbd987d6ca02e58369a3bea0a04fa4fe693d6625659a7666b","observation_id":"62f1226e-0547-4964-a76f-969c1ab2fac4","resolution":{"observed_at":"2026-08-11T10:58:56.605256Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1406.6338","last_updated":"2015-03-10T17:37:46Z","snapshot_observed_at":"2026-07-06T03:47:11.838220Z","submitted_at":"2014-06-24T19:17:09Z","title":"Taming the off-shell Higgs boson","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1406.6338","snapshot_observed_at":"2026-08-11T10:58:56.071746Z","title":"Azatov, C","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2412.16020","last_updated":"2025-06-03T08:19:02Z","snapshot_observed_at":"2026-08-11T10:50:33.964800Z","submitted_at":"2024-12-20T16:10:03Z","title":"Dimension-8 operators in $W^+W^-$ production via gluon fusion","version":2},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-08-11T10:58:56.071746Z"},"links":{"cited_paper":"/paper/1406.6338","citing_paper":"/paper/2412.16020"},"observation_digest":"sha256:6e816740862e35ca0fa0f318404d53fef9ca9a7314959a173c5a961710e27635","observation_id":"41ff7364-7902-4eee-a3eb-6d689e5a8ca0","resolution":{"observed_at":"2026-08-11T10:58:56.071746Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1608.00977","last_updated":"2018-04-30T12:52:12Z","snapshot_observed_at":"2026-07-06T05:05:47.694853Z","submitted_at":"2016-08-02T20:00:05Z","title":"Resolving gluon fusion loops at current and future hadron colliders","version":3},"cited_work":{"arxiv_id":"1608.00977","doi":null,"metadata_source":"pith","pith_arxiv_id":"1608.00977","snapshot_observed_at":"2026-08-11T10:58:56.574538Z","title":"Resolving gluon fusion loops at current and future hadron colliders","venue":"hep-ph","work_id":"62845fef-5dda-4892-a3ea-9fd6eb48f5ee","year":2016},"citing_paper":{"arxiv_id":"2412.16020","last_updated":"2025-06-03T08:19:02Z","snapshot_observed_at":"2026-08-11T10:50:33.964800Z","submitted_at":"2024-12-20T16:10:03Z","title":"Dimension-8 operators in $W^+W^-$ production via gluon fusion","version":2},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-08-11T10:58:56.075549Z"},"links":{"cited_paper":"/paper/1608.00977","citing_paper":"/paper/2412.16020"},"observation_digest":"sha256:53aca47e7d95f9d851dc417a4f1b3b126fd816bed8c608909eb84825a4d25844","observation_id":"49b54eca-d0ef-4d2f-9a49-02fbe41b8586","resolution":{"observed_at":"2026-08-11T10:58:56.578639Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2404.12809","last_updated":"2024-10-28T10:02:33Z","snapshot_observed_at":"2026-07-06T18:02:40.943221Z","submitted_at":"2024-04-19T11:43:33Z","title":"Mapping the SMEFT at High-Energy Colliders: from LEP and the (HL-)LHC to the FCC-ee","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2404.12809","snapshot_observed_at":"2026-08-11T10:58:56.079353Z","title":"Celada, T","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2412.16020","last_updated":"2025-06-03T08:19:02Z","snapshot_observed_at":"2026-08-11T10:50:33.964800Z","submitted_at":"2024-12-20T16:10:03Z","title":"Dimension-8 operators in $W^+W^-$ production via gluon fusion","version":2},"reference_index":32,"source":"pdf_text","source_observed_at":"2026-08-11T10:58:56.079353Z"},"links":{"cited_paper":"/paper/2404.12809","citing_paper":"/paper/2412.16020"},"observation_digest":"sha256:3d8ccf019b22c801e9ccfd06ba09e22d62493d4045abc8c2722317d356fe00d4","observation_id":"e71c1133-822a-48a6-8347-9831b3f6c451","resolution":{"observed_at":"2026-08-11T10:58:56.079353Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2105.00006","last_updated":"2021-10-31T16:08:27Z","snapshot_observed_at":"2026-08-09T12:33:54.696381Z","submitted_at":"2021-04-30T18:00:01Z","title":"Combined SMEFT interpretation of Higgs, diboson, and top quark data from the LHC","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2105.00006","snapshot_observed_at":"2026-08-11T10:58:56.083090Z","title":null,"venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2412.16020","last_updated":"2025-06-03T08:19:02Z","snapshot_observed_at":"2026-08-11T10:50:33.964800Z","submitted_at":"2024-12-20T16:10:03Z","title":"Dimension-8 operators in $W^+W^-$ production via gluon fusion","version":2},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-08-11T10:58:56.083090Z"},"links":{"cited_paper":"/paper/2105.00006","citing_paper":"/paper/2412.16020"},"observation_digest":"sha256:1daafa7f09518e602957397b4a58bc25bef49a406d9a9dcebeae1ba2ffdcebe4","observation_id":"e7636366-cd7e-4b8b-bc9a-b2879fbb754f","resolution":{"observed_at":"2026-08-11T10:58:56.083090Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1912.00068","last_updated":"2020-02-26T11:13:13Z","snapshot_observed_at":"2026-07-06T08:40:59.491813Z","submitted_at":"2019-11-29T21:03:01Z","title":"NNLO QCD+NLO EW with MATRIX+OpenLoops: precise predictions for vector-boson pair production","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1912.00068","snapshot_observed_at":"2026-08-11T10:58:56.087067Z","title":"Grazzini, S","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2412.16020","last_updated":"2025-06-03T08:19:02Z","snapshot_observed_at":"2026-08-11T10:50:33.964800Z","submitted_at":"2024-12-20T16:10:03Z","title":"Dimension-8 operators in $W^+W^-$ production via gluon fusion","version":2},"reference_index":34,"source":"pdf_text","source_observed_at":"2026-08-11T10:58:56.087067Z"},"links":{"cited_paper":"/paper/1912.00068","citing_paper":"/paper/2412.16020"},"observation_digest":"sha256:d7f018e065b8e1514ebffb71b98553504d98aa04b51e391ff6c6a5d99af4fe7c","observation_id":"781b3f0f-f177-457b-b5f9-b58ed8553351","resolution":{"observed_at":"2026-08-11T10:58:56.087067Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1705.00598","last_updated":"2017-12-22T13:21:04Z","snapshot_observed_at":"2026-07-06T05:40:07.126075Z","submitted_at":"2017-05-01T17:29:02Z","title":"NLO QCD+EW predictions for $2\\ell2\\nu$ diboson signatures at the LHC","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1705.00598","snapshot_observed_at":"2026-08-11T10:58:56.091031Z","title":"Kallweit, J","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2412.16020","last_updated":"2025-06-03T08:19:02Z","snapshot_observed_at":"2026-08-11T10:50:33.964800Z","submitted_at":"2024-12-20T16:10:03Z","title":"Dimension-8 operators in $W^+W^-$ production via gluon fusion","version":2},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-08-11T10:58:56.091031Z"},"links":{"cited_paper":"/paper/1705.00598","citing_paper":"/paper/2412.16020"},"observation_digest":"sha256:24b4660fbae2a4b7b2ad4476bd48544411a4d06676b800c763f0a28bbc6cbbe3","observation_id":"deb4640d-6e0e-443a-b61c-e53e447b1735","resolution":{"observed_at":"2026-08-11T10:58:56.091031Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2406.15640","last_updated":"2025-01-30T20:14:23Z","snapshot_observed_at":"2026-08-03T10:40:20.555034Z","submitted_at":"2024-06-21T20:35:18Z","title":"Electroweak corrections and EFT operators in $W^+W^-$ production at the LHC","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2406.15640","snapshot_observed_at":"2026-08-11T10:58:56.094743Z","title":"Banerjee, D","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2412.16020","last_updated":"2025-06-03T08:19:02Z","snapshot_observed_at":"2026-08-11T10:50:33.964800Z","submitted_at":"2024-12-20T16:10:03Z","title":"Dimension-8 operators in $W^+W^-$ production via gluon fusion","version":2},"reference_index":36,"source":"pdf_text","source_observed_at":"2026-08-11T10:58:56.094743Z"},"links":{"cited_paper":"/paper/2406.15640","citing_paper":"/paper/2412.16020"},"observation_digest":"sha256:08b484a7a5d06600a002f6632b501c5dffc0416ef9586ab5004989f5879d713b","observation_id":"d269c834-1519-4bfd-83bc-97def21ecae8","resolution":{"observed_at":"2026-08-11T10:58:56.094743Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1510.00372","last_updated":"2015-11-12T20:46:08Z","snapshot_observed_at":"2026-07-06T04:31:44.421146Z","submitted_at":"2015-10-01T19:22:32Z","title":"Low-derivative operators of the Standard Model effective field theory via Hilbert series methods","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1510.00372","snapshot_observed_at":"2026-08-11T10:58:56.099415Z","title":"Lehman and A","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2412.16020","last_updated":"2025-06-03T08:19:02Z","snapshot_observed_at":"2026-08-11T10:50:33.964800Z","submitted_at":"2024-12-20T16:10:03Z","title":"Dimension-8 operators in $W^+W^-$ production via gluon fusion","version":2},"reference_index":37,"source":"pdf_text","source_observed_at":"2026-08-11T10:58:56.099415Z"},"links":{"cited_paper":"/paper/1510.00372","citing_paper":"/paper/2412.16020"},"observation_digest":"sha256:4855d2cc09383c15867b850ba05402a6eacb043239a340b7bfd1881bdd9d196d","observation_id":"b7abe4ae-4c1a-46b9-ab2c-8c7eef30f740","resolution":{"observed_at":"2026-08-11T10:58:56.099415Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-11T10:58:57.022825Z","title":null,"venue":null,"work_id":"19dabf8c-2510-40c2-a2c8-b72de42de9bc","year":null},"citing_paper":{"arxiv_id":"2412.16020","last_updated":"2025-06-03T08:19:02Z","snapshot_observed_at":"2026-08-11T10:50:33.964800Z","submitted_at":"2024-12-20T16:10:03Z","title":"Dimension-8 operators in $W^+W^-$ production via gluon fusion","version":2},"reference_index":38,"source":"pdf_text","source_observed_at":"2026-08-11T10:58:56.103065Z"},"links":{"citing_paper":"/paper/2412.16020"},"observation_digest":"sha256:cd59eb937cb3919a940b3e0b16561954728f8d8fe5fec8d960d83699bd3274c7","observation_id":"23e07277-857d-421a-8f58-06ed6c196dbc","resolution":{"observed_at":"2026-08-11T10:58:57.026618Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2304.09883","last_updated":"2023-07-13T13:54:13Z","snapshot_observed_at":"2026-08-10T17:58:05.417883Z","submitted_at":"2023-04-19T18:00:00Z","title":"UFO 2.0 -- The Universal Feynman Output format","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2304.09883","snapshot_observed_at":"2026-08-11T10:58:56.106908Z","title":"Darm´ e et al.,UFO 2.0: the ‘Universal Feynman Output’ format , Eur","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2412.16020","last_updated":"2025-06-03T08:19:02Z","snapshot_observed_at":"2026-08-11T10:50:33.964800Z","submitted_at":"2024-12-20T16:10:03Z","title":"Dimension-8 operators in $W^+W^-$ production via gluon fusion","version":2},"reference_index":39,"source":"pdf_text","source_observed_at":"2026-08-11T10:58:56.106908Z"},"links":{"cited_paper":"/paper/2304.09883","citing_paper":"/paper/2412.16020"},"observation_digest":"sha256:857512d6cddca7d666fd6ea727cc9bd718aa487f2c680f9327fe14ecd7f52a6a","observation_id":"36813b1d-1a15-4843-955e-a3f96d24656b","resolution":{"observed_at":"2026-08-11T10:58:56.106908Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1405.0301","last_updated":"2014-07-21T09:46:15Z","snapshot_observed_at":"2026-07-06T02:11:23.670680Z","submitted_at":"2014-05-01T20:24:46Z","title":"The automated computation of tree-level and next-to-leading order differential cross sections, and their matching to parton shower simulations","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1405.0301","snapshot_observed_at":"2026-08-11T10:58:56.111082Z","title":"Alwall, R","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2412.16020","last_updated":"2025-06-03T08:19:02Z","snapshot_observed_at":"2026-08-11T10:50:33.964800Z","submitted_at":"2024-12-20T16:10:03Z","title":"Dimension-8 operators in $W^+W^-$ production via gluon fusion","version":2},"reference_index":40,"source":"pdf_text","source_observed_at":"2026-08-11T10:58:56.111082Z"},"links":{"cited_paper":"/paper/1405.0301","citing_paper":"/paper/2412.16020"},"observation_digest":"sha256:6f469a03a2d481c0332e1d598397072f93070ef3758fbcf1ec2259ef86f9f0a3","observation_id":"067cd3e6-2ca1-4a9f-ad45-daaef4078e96","resolution":{"observed_at":"2026-08-11T10:58:56.111082Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2004.04545","last_updated":"2020-08-08T20:52:14Z","snapshot_observed_at":"2026-08-07T22:46:31.018151Z","submitted_at":"2020-04-09T14:11:59Z","title":"$CP$ Properties of Higgs Boson Interactions with Top Quarks in the $t\\bar{t}H$ and $tH$ Processes Using $H \\rightarrow \\gamma\\gamma$ with the ATLAS Detector","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2004.04545","snapshot_observed_at":"2026-08-11T10:58:56.114541Z","title":"Aad et al., CP Properties of Higgs Boson Interactions with Top Quarks in the t¯tH and tH Processes Using H → γγ with the ATLAS Detector, Phys","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2412.16020","last_updated":"2025-06-03T08:19:02Z","snapshot_observed_at":"2026-08-11T10:50:33.964800Z","submitted_at":"2024-12-20T16:10:03Z","title":"Dimension-8 operators in $W^+W^-$ production via gluon fusion","version":2},"reference_index":41,"source":"pdf_text","source_observed_at":"2026-08-11T10:58:56.114541Z"},"links":{"cited_paper":"/paper/2004.04545","citing_paper":"/paper/2412.16020"},"observation_digest":"sha256:177f695002019129b98b97cb11a42d81de62424650ec23dd2d3d1ea7b6824d99","observation_id":"e3ec7220-57a9-419c-8658-7cf4ea3ae307","resolution":{"observed_at":"2026-08-11T10:58:56.114541Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2109.13808","last_updated":"2022-07-27T14:47:00Z","snapshot_observed_at":"2026-07-06T11:52:15.682202Z","submitted_at":"2021-09-28T15:36:13Z","title":"Constraints on Higgs boson properties using $WW^{*}(\\rightarrow e\\nu\\mu\\nu) jj$ production in 36.1 fb$^{-1}$ of $\\sqrt{s}$=13 TeV $pp$ collisions with the ATLAS detector","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2109.13808","snapshot_observed_at":"2026-08-11T10:58:56.118100Z","title":"Aad et al., Constraints on Higgs boson properties using W W∗(→ eνµν )jj production in 36.1 fb−1 of √s = 13 TeV pp collisions with the ATLAS detector, Eur","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2412.16020","last_updated":"2025-06-03T08:19:02Z","snapshot_observed_at":"2026-08-11T10:50:33.964800Z","submitted_at":"2024-12-20T16:10:03Z","title":"Dimension-8 operators in $W^+W^-$ production via gluon fusion","version":2},"reference_index":42,"source":"pdf_text","source_observed_at":"2026-08-11T10:58:56.118100Z"},"links":{"cited_paper":"/paper/2109.13808","citing_paper":"/paper/2412.16020"},"observation_digest":"sha256:aa89cd93f1cbbfa6d7b6878803d2f065730b1eced5416d75a3c19f496cb16a60","observation_id":"c012d3b8-7f75-4d12-bc64-57033fb697a9","resolution":{"observed_at":"2026-08-11T10:58:56.118100Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2303.05974","last_updated":"2024-04-16T14:30:14Z","snapshot_observed_at":"2026-08-10T06:03:29.788312Z","submitted_at":"2023-03-10T15:11:20Z","title":"Probing the $CP$ nature of the top-Higgs Yukawa coupling in $t\\bar{t}H$ and $tH$ events with $H \\to b\\bar{b}$ decays using the ATLAS detector at the LHC","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2303.05974","snapshot_observed_at":"2026-08-11T10:58:56.121883Z","title":"Aad et al., Probing the CP nature of the top–Higgs Yukawa coupling in tt¯H and tH events with H →bb¯ decays using the ATLAS detector at the LHC , Phys","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2412.16020","last_updated":"2025-06-03T08:19:02Z","snapshot_observed_at":"2026-08-11T10:50:33.964800Z","submitted_at":"2024-12-20T16:10:03Z","title":"Dimension-8 operators in $W^+W^-$ production via gluon fusion","version":2},"reference_index":43,"source":"pdf_text","source_observed_at":"2026-08-11T10:58:56.121883Z"},"links":{"cited_paper":"/paper/2303.05974","citing_paper":"/paper/2412.16020"},"observation_digest":"sha256:8011e61b3cfd250ca54c672bc3eee23392142fd7599c66417780144512d943a8","observation_id":"87ab656f-8de7-42c8-b56e-03e6c17f3d52","resolution":{"observed_at":"2026-08-11T10:58:56.121883Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1905.06646","last_updated":"2019-08-12T17:04:12Z","snapshot_observed_at":"2026-07-06T07:53:26.275932Z","submitted_at":"2019-05-16T10:29:52Z","title":"BSM WW production with a jet veto","version":3},"cited_work":{"arxiv_id":"1905.06646","doi":null,"metadata_source":"pith","pith_arxiv_id":"1905.06646","snapshot_observed_at":"2026-08-11T10:58:56.444806Z","title":"BSM WW production with a jet veto","venue":"hep-ph","work_id":"355738e3-dc9c-4970-88d5-c7b3162086b6","year":2019},"citing_paper":{"arxiv_id":"2412.16020","last_updated":"2025-06-03T08:19:02Z","snapshot_observed_at":"2026-08-11T10:50:33.964800Z","submitted_at":"2024-12-20T16:10:03Z","title":"Dimension-8 operators in $W^+W^-$ production via gluon fusion","version":2},"reference_index":44,"source":"pdf_text","source_observed_at":"2026-08-11T10:58:56.125439Z"},"links":{"cited_paper":"/paper/1905.06646","citing_paper":"/paper/2412.16020"},"observation_digest":"sha256:5e6f2fc7505da7b083bd5e85f4216119a6769f07822dd234589161d7b2f0c8e2","observation_id":"f2948372-753a-4cc4-bcbd-134dc7836743","resolution":{"observed_at":"2026-08-11T10:58:56.449393Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"0802.1189","last_updated":"2008-04-21T21:44:17Z","snapshot_observed_at":"2026-07-06T01:34:46.001237Z","submitted_at":"2008-02-08T18:17:17Z","title":"The anti-k_t jet clustering algorithm","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0802.1189","snapshot_observed_at":"2026-08-11T10:58:56.129129Z","title":"Cacciari, G","venue":null,"work_id":null,"year":2008},"citing_paper":{"arxiv_id":"2412.16020","last_updated":"2025-06-03T08:19:02Z","snapshot_observed_at":"2026-08-11T10:50:33.964800Z","submitted_at":"2024-12-20T16:10:03Z","title":"Dimension-8 operators in $W^+W^-$ production via gluon fusion","version":2},"reference_index":45,"source":"pdf_text","source_observed_at":"2026-08-11T10:58:56.129129Z"},"links":{"cited_paper":"/paper/0802.1189","citing_paper":"/paper/2412.16020"},"observation_digest":"sha256:094a4b0cd75e0fe8c6e68046b27dd86a5dfa1a87ed5842bd25ca949feda1c5f0","observation_id":"587ad0c9-3b81-4cc0-b657-daaabd2c6a01","resolution":{"observed_at":"2026-08-11T10:58:56.129129Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1905.04242","last_updated":"2019-11-04T14:21:19Z","snapshot_observed_at":"2026-07-06T07:52:13.448801Z","submitted_at":"2019-05-10T16:23:38Z","title":"Measurement of fiducial and differential $W^+W^-$ production cross-sections at $\\sqrt{s}=$13 TeV with the ATLAS detector","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1905.04242","snapshot_observed_at":"2026-08-11T10:58:56.133042Z","title":"Aaboud et al., Measurement of fiducial and differential W +W − production cross-sections at √s = 13 TeV with the ATLAS detector , Eur","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2412.16020","last_updated":"2025-06-03T08:19:02Z","snapshot_observed_at":"2026-08-11T10:50:33.964800Z","submitted_at":"2024-12-20T16:10:03Z","title":"Dimension-8 operators in $W^+W^-$ production via gluon fusion","version":2},"reference_index":46,"source":"pdf_text","source_observed_at":"2026-08-11T10:58:56.133042Z"},"links":{"cited_paper":"/paper/1905.04242","citing_paper":"/paper/2412.16020"},"observation_digest":"sha256:39bd612b017f4ea6ae7442ff0214a32aa3e5fbfe6f1ad4dd9cfc4b58f6143644","observation_id":"7046d395-4172-4734-b123-bcc389aee726","resolution":{"observed_at":"2026-08-11T10:58:56.133042Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1408.5243","last_updated":"2014-08-22T09:39:26Z","snapshot_observed_at":"2026-07-06T02:11:23.670680Z","submitted_at":"2014-08-22T09:39:26Z","title":"$W^+W^-$ production at hadron colliders in NNLO QCD","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1408.5243","snapshot_observed_at":"2026-08-11T10:58:56.136765Z","title":"Gehrmann, M","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2412.16020","last_updated":"2025-06-03T08:19:02Z","snapshot_observed_at":"2026-08-11T10:50:33.964800Z","submitted_at":"2024-12-20T16:10:03Z","title":"Dimension-8 operators in $W^+W^-$ production via gluon fusion","version":2},"reference_index":47,"source":"pdf_text","source_observed_at":"2026-08-11T10:58:56.136765Z"},"links":{"cited_paper":"/paper/1408.5243","citing_paper":"/paper/2412.16020"},"observation_digest":"sha256:76898d308a197e55c8f5c4ae64872588885acf7fe855ccd078223e132ffb99f7","observation_id":"55d20f75-6a0d-4986-b5ec-c136cbacfd17","resolution":{"observed_at":"2026-08-11T10:58:56.136765Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1605.02716","last_updated":"2016-05-09T19:53:37Z","snapshot_observed_at":"2026-07-06T04:55:39.926609Z","submitted_at":"2016-05-09T19:53:37Z","title":"$W^+W^-$ production at the LHC: fiducial cross sections and distributions in NNLO QCD","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1605.02716","snapshot_observed_at":"2026-08-11T10:58:56.140853Z","title":"Grazzini, S","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2412.16020","last_updated":"2025-06-03T08:19:02Z","snapshot_observed_at":"2026-08-11T10:50:33.964800Z","submitted_at":"2024-12-20T16:10:03Z","title":"Dimension-8 operators in $W^+W^-$ production via gluon fusion","version":2},"reference_index":48,"source":"pdf_text","source_observed_at":"2026-08-11T10:58:56.140853Z"},"links":{"cited_paper":"/paper/1605.02716","citing_paper":"/paper/2412.16020"},"observation_digest":"sha256:64d9908579c7d997d60b97878d59ceaa50a71afadb9ff432eba2bf2887a08b03","observation_id":"4e836f5f-f856-4deb-a91b-a08b986832b7","resolution":{"observed_at":"2026-08-11T10:58:56.140853Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2002.01877","last_updated":"2020-02-05T17:30:28Z","snapshot_observed_at":"2026-07-06T08:55:06.379560Z","submitted_at":"2020-02-05T17:30:28Z","title":"$W^+W^-$ production at the LHC: NLO QCD corrections to the loop-induced gluon fusion channel","version":1},"cited_work":{"arxiv_id":"2002.01877","doi":null,"metadata_source":"pith","pith_arxiv_id":"2002.01877","snapshot_observed_at":"2026-08-11T10:58:56.386747Z","title":"$W^+W^-$ production at the LHC: NLO QCD corrections to the loop-induced gluon fusion channel","venue":"hep-ph","work_id":"aabd6b0d-2f6a-44f1-8b03-e269c987df9f","year":2020},"citing_paper":{"arxiv_id":"2412.16020","last_updated":"2025-06-03T08:19:02Z","snapshot_observed_at":"2026-08-11T10:50:33.964800Z","submitted_at":"2024-12-20T16:10:03Z","title":"Dimension-8 operators in $W^+W^-$ production via gluon fusion","version":2},"reference_index":49,"source":"pdf_text","source_observed_at":"2026-08-11T10:58:56.144616Z"},"links":{"cited_paper":"/paper/2002.01877","citing_paper":"/paper/2412.16020"},"observation_digest":"sha256:df66ba800b0fb2755a6f004c700aa7e27c90dec4492b36bc2a01327055eb2f92","observation_id":"7a011092-9f31-4f56-bdb1-b1746eadef2f","resolution":{"observed_at":"2026-08-11T10:58:56.390944Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2004.07720","last_updated":"2021-01-22T15:44:08Z","snapshot_observed_at":"2026-08-10T13:12:21.896244Z","submitted_at":"2020-04-16T15:58:15Z","title":"Accurate single- and double-differential resummation of colour-singlet processes with MATRIX+RadISH: $W^+W^-$ production at the LHC","version":2},"cited_work":{"arxiv_id":"2004.07720","doi":null,"metadata_source":"pith","pith_arxiv_id":"2004.07720","snapshot_observed_at":"2026-08-11T10:58:56.370161Z","title":"Accurate single- and double-differential resummation of colour-singlet processes with MATRIX+RadISH: $W^+W^-$ production at the LHC","venue":"hep-ph","work_id":"fbe498f7-b89e-4d11-b2a1-9c31a0ee2f46","year":2020},"citing_paper":{"arxiv_id":"2412.16020","last_updated":"2025-06-03T08:19:02Z","snapshot_observed_at":"2026-08-11T10:50:33.964800Z","submitted_at":"2024-12-20T16:10:03Z","title":"Dimension-8 operators in $W^+W^-$ production via gluon fusion","version":2},"reference_index":50,"source":"pdf_text","source_observed_at":"2026-08-11T10:58:56.148419Z"},"links":{"cited_paper":"/paper/2004.07720","citing_paper":"/paper/2412.16020"},"observation_digest":"sha256:5e3b5eb6b553fd2b0adbd788e1e0b8a92f156416bbbfebc787dbcfdcb8870bf7","observation_id":"f051e26d-049a-4c48-99f3-b860725b0193","resolution":{"observed_at":"2026-08-11T10:58:56.375131Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2301.11768","last_updated":"2023-04-09T16:17:22Z","snapshot_observed_at":"2026-07-06T14:45:19.481734Z","submitted_at":"2023-01-27T15:06:45Z","title":"Jet-veto resummation at N$^3$LL$_\\text{p}$+NNLO in boson production processes","version":2},"cited_work":{"arxiv_id":"2301.11768","doi":null,"metadata_source":"pith","pith_arxiv_id":"2301.11768","snapshot_observed_at":"2026-08-11T10:58:56.353617Z","title":"Jet-veto resummation at N$^3$LL$_\\text{p}$+NNLO in boson production processes","venue":"hep-ph","work_id":"083e4bd9-3adf-4a51-9056-27ffce27cf36","year":2023},"citing_paper":{"arxiv_id":"2412.16020","last_updated":"2025-06-03T08:19:02Z","snapshot_observed_at":"2026-08-11T10:50:33.964800Z","submitted_at":"2024-12-20T16:10:03Z","title":"Dimension-8 operators in $W^+W^-$ production via gluon fusion","version":2},"reference_index":51,"source":"pdf_text","source_observed_at":"2026-08-11T10:58:56.152215Z"},"links":{"cited_paper":"/paper/2301.11768","citing_paper":"/paper/2412.16020"},"observation_digest":"sha256:8a6e51ffe42db86aa3f25b48dc5497c6509396ee86728396167436fd558d031a","observation_id":"e5ba95f7-a1d4-43cb-b08f-60b92080b911","resolution":{"observed_at":"2026-08-11T10:58:56.358146Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2308.11577","last_updated":"2023-08-22T17:27:53Z","snapshot_observed_at":"2026-08-10T09:46:46.278540Z","submitted_at":"2023-08-22T17:27:53Z","title":"NNLO+PS $W^+W^-$ production using jet veto resummation at NNLL$'$","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2308.11577","snapshot_observed_at":"2026-08-11T10:58:56.155655Z","title":"Gavardi, M","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2412.16020","last_updated":"2025-06-03T08:19:02Z","snapshot_observed_at":"2026-08-11T10:50:33.964800Z","submitted_at":"2024-12-20T16:10:03Z","title":"Dimension-8 operators in $W^+W^-$ production via gluon fusion","version":2},"reference_index":52,"source":"pdf_text","source_observed_at":"2026-08-11T10:58:56.155655Z"},"links":{"cited_paper":"/paper/2308.11577","citing_paper":"/paper/2412.16020"},"observation_digest":"sha256:fb3381f45181ce9f5a1c85c7680b5e958dce1f8e1c58e17aa2280ea2eadda5df","observation_id":"3e833201-7b2f-4705-b5ad-3f059cb856d0","resolution":{"observed_at":"2026-08-11T10:58:56.155655Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2402.10503","last_updated":"2024-06-03T09:42:00Z","snapshot_observed_at":"2026-08-10T13:29:18.132601Z","submitted_at":"2024-02-16T08:24:09Z","title":"Automated resummation of electroweak Sudakov logarithms in diboson production at future colliders","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2402.10503","snapshot_observed_at":"2026-08-11T10:58:56.159504Z","title":"Denner and S","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2412.16020","last_updated":"2025-06-03T08:19:02Z","snapshot_observed_at":"2026-08-11T10:50:33.964800Z","submitted_at":"2024-12-20T16:10:03Z","title":"Dimension-8 operators in $W^+W^-$ production via gluon fusion","version":2},"reference_index":53,"source":"pdf_text","source_observed_at":"2026-08-11T10:58:56.159504Z"},"links":{"cited_paper":"/paper/2402.10503","citing_paper":"/paper/2412.16020"},"observation_digest":"sha256:447d35b72503890df9160659ee332143ff68909be78f42bd1c0e5ce241c4e8f6","observation_id":"5793c122-3a61-41fa-a19f-1cd7ebc6e71f","resolution":{"observed_at":"2026-08-11T10:58:56.159504Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1712.07053","last_updated":"2018-05-24T12:40:38Z","snapshot_observed_at":"2026-08-10T11:50:19.873614Z","submitted_at":"2017-12-19T17:08:39Z","title":"Illuminating the photon content of the proton within a global PDF analysis","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1712.07053","snapshot_observed_at":"2026-08-11T10:58:56.163234Z","title":"Bertone, S","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2412.16020","last_updated":"2025-06-03T08:19:02Z","snapshot_observed_at":"2026-08-11T10:50:33.964800Z","submitted_at":"2024-12-20T16:10:03Z","title":"Dimension-8 operators in $W^+W^-$ production via gluon fusion","version":2},"reference_index":54,"source":"pdf_text","source_observed_at":"2026-08-11T10:58:56.163234Z"},"links":{"cited_paper":"/paper/1712.07053","citing_paper":"/paper/2412.16020"},"observation_digest":"sha256:3fabdc251ac041f8b144e97cb3bdd080f3713e09189f3f7ab2024ac1780c40a0","observation_id":"84c9464f-12b3-4232-bb72-841229072da9","resolution":{"observed_at":"2026-08-11T10:58:56.163234Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1107.2117","last_updated":"2012-02-01T11:08:40Z","snapshot_observed_at":"2026-07-06T02:30:42.129649Z","submitted_at":"2011-07-11T20:00:02Z","title":"Theory Uncertainties for Higgs and Other Searches Using Jet Bins","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1107.2117","snapshot_observed_at":"2026-08-11T10:58:56.166941Z","title":null,"venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2412.16020","last_updated":"2025-06-03T08:19:02Z","snapshot_observed_at":"2026-08-11T10:50:33.964800Z","submitted_at":"2024-12-20T16:10:03Z","title":"Dimension-8 operators in $W^+W^-$ production via gluon fusion","version":2},"reference_index":55,"source":"pdf_text","source_observed_at":"2026-08-11T10:58:56.166941Z"},"links":{"cited_paper":"/paper/1107.2117","citing_paper":"/paper/2412.16020"},"observation_digest":"sha256:263b910c580ab2aa7bfe65bc005a7fe0b292bceecde0d12639d84c4f4098a5df","observation_id":"d57f89dc-f8f9-4ca7-a6b2-c2920a6f8ce6","resolution":{"observed_at":"2026-08-11T10:58:56.166941Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1702.04519","last_updated":"2017-10-01T08:47:49Z","snapshot_observed_at":"2026-07-06T05:30:05.815906Z","submitted_at":"2017-02-15T09:43:09Z","title":"Measurement of the $W^+W^-$ production cross section in $pp$ collisions at a centre-of-mass energy of $\\sqrt{s}$ = 13 TeV with the ATLAS experiment","version":2},"cited_work":{"arxiv_id":"1702.04519","doi":null,"metadata_source":"pith","pith_arxiv_id":"1702.04519","snapshot_observed_at":"2026-08-11T10:58:56.294684Z","title":"Measurement of the $W^+W^-$ production cross section in $pp$ collisions at a centre-of-mass energy of $\\sqrt{s}$ = 13 TeV with the ATLAS experiment","venue":"hep-ex","work_id":"ade1cadb-6921-46c6-bda7-d8e186fa0a5d","year":2017},"citing_paper":{"arxiv_id":"2412.16020","last_updated":"2025-06-03T08:19:02Z","snapshot_observed_at":"2026-08-11T10:50:33.964800Z","submitted_at":"2024-12-20T16:10:03Z","title":"Dimension-8 operators in $W^+W^-$ production via gluon fusion","version":2},"reference_index":56,"source":"pdf_text","source_observed_at":"2026-08-11T10:58:56.171342Z"},"links":{"cited_paper":"/paper/1702.04519","citing_paper":"/paper/2412.16020"},"observation_digest":"sha256:6c9e443bbcfb61eaf7c3816f8722eed9a75d85a10e4946ebf9225f6a7e3a4c29","observation_id":"2f633661-f4d5-44fb-9320-f43c9815a83f","resolution":{"observed_at":"2026-08-11T10:58:56.300608Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2208.02686","last_updated":"2023-07-18T18:28:29Z","snapshot_observed_at":"2026-08-10T20:19:34.400034Z","submitted_at":"2022-08-04T14:37:09Z","title":"Search for $CP$ violation in ttH and tH production in multilepton channels in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2208.02686","snapshot_observed_at":"2026-08-11T10:58:56.175400Z","title":"Tumasyan et al., Search for CP violation in ttH and tH production in multilepton channels in proton-proton collisions at √s = 13 TeV , JHEP 07 (2023) 092, [ 2208.02686]","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2412.16020","last_updated":"2025-06-03T08:19:02Z","snapshot_observed_at":"2026-08-11T10:50:33.964800Z","submitted_at":"2024-12-20T16:10:03Z","title":"Dimension-8 operators in $W^+W^-$ production via gluon fusion","version":2},"reference_index":57,"source":"pdf_text","source_observed_at":"2026-08-11T10:58:56.175400Z"},"links":{"cited_paper":"/paper/2208.02686","citing_paper":"/paper/2412.16020"},"observation_digest":"sha256:e482be0517fff6acc499f40fce4e238ab09364387d29742afb8e6b485b6215c1","observation_id":"bc30125e-5802-46e8-805a-a7c6b42f2e5e","resolution":{"observed_at":"2026-08-11T10:58:56.175400Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2007.08542","last_updated":"2021-10-19T12:33:59Z","snapshot_observed_at":"2026-07-06T09:38:53.228850Z","submitted_at":"2020-07-16T18:00:40Z","title":"Indirect $\\mathcal{CP}$ probes of the Higgs-top-quark interaction: current LHC constraints and future opportunities","version":5},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2007.08542","snapshot_observed_at":"2026-08-11T10:58:56.179501Z","title":null,"venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2412.16020","last_updated":"2025-06-03T08:19:02Z","snapshot_observed_at":"2026-08-11T10:50:33.964800Z","submitted_at":"2024-12-20T16:10:03Z","title":"Dimension-8 operators in $W^+W^-$ production via gluon fusion","version":2},"reference_index":58,"source":"pdf_text","source_observed_at":"2026-08-11T10:58:56.179501Z"},"links":{"cited_paper":"/paper/2007.08542","citing_paper":"/paper/2412.16020"},"observation_digest":"sha256:fc8f629b3ce2e3d855ec4bfd109f3c95957abeef5a12b79a1e32cd10304c0eec","observation_id":"4f150829-7490-4389-ba1c-833efb247f8d","resolution":{"observed_at":"2026-08-11T10:58:56.179501Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1902.00134","last_updated":"2019-03-19T11:24:31Z","snapshot_observed_at":"2026-08-05T17:50:22.226547Z","submitted_at":"2019-01-31T23:51:10Z","title":"Higgs Physics at the HL-LHC and HE-LHC","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1902.00134","snapshot_observed_at":"2026-08-11T10:58:56.182949Z","title":"Cepeda et al., Report from Working Group 2: Higgs Physics at the HL-LHC and HE-LHC, CERN Yellow Rep","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2412.16020","last_updated":"2025-06-03T08:19:02Z","snapshot_observed_at":"2026-08-11T10:50:33.964800Z","submitted_at":"2024-12-20T16:10:03Z","title":"Dimension-8 operators in $W^+W^-$ production via gluon fusion","version":2},"reference_index":59,"source":"pdf_text","source_observed_at":"2026-08-11T10:58:56.182949Z"},"links":{"cited_paper":"/paper/1902.00134","citing_paper":"/paper/2412.16020"},"observation_digest":"sha256:ca69403822b0ee3d7fff71bcc7c993f9dfe485e46369f68bf04b2e5792fde45b","observation_id":"52ddfb5d-a85e-44e0-a1c3-a89cc2e958bf","resolution":{"observed_at":"2026-08-11T10:58:56.182949Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1403.7191","last_updated":"2014-04-24T17:49:33Z","snapshot_observed_at":"2026-07-06T03:39:39.812144Z","submitted_at":"2014-03-27T19:54:50Z","title":"Precision Measurements of Higgs Couplings: Implications for New Physics Scales","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1403.7191","snapshot_observed_at":"2026-08-11T10:58:56.187062Z","title":"Englert, A","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2412.16020","last_updated":"2025-06-03T08:19:02Z","snapshot_observed_at":"2026-08-11T10:50:33.964800Z","submitted_at":"2024-12-20T16:10:03Z","title":"Dimension-8 operators in $W^+W^-$ production via gluon fusion","version":2},"reference_index":60,"source":"pdf_text","source_observed_at":"2026-08-11T10:58:56.187062Z"},"links":{"cited_paper":"/paper/1403.7191","citing_paper":"/paper/2412.16020"},"observation_digest":"sha256:606c1f8c5784738c75373387d4cd108753fe56fe581a776fb6cf4990e5e0d396","observation_id":"cafc2634-cbfa-4f0a-ac90-b737530c09a8","resolution":{"observed_at":"2026-08-11T10:58:56.187062Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2009.00119","last_updated":"2020-11-10T14:31:48Z","snapshot_observed_at":"2026-08-11T03:23:18.265128Z","submitted_at":"2020-08-31T21:55:54Z","title":"W$^+$W$^-$ boson pair production in proton-proton collisions at $\\sqrt{s} =$ 13 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2009.00119","snapshot_observed_at":"2026-08-11T10:58:56.190657Z","title":null,"venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2412.16020","last_updated":"2025-06-03T08:19:02Z","snapshot_observed_at":"2026-08-11T10:50:33.964800Z","submitted_at":"2024-12-20T16:10:03Z","title":"Dimension-8 operators in $W^+W^-$ production via gluon fusion","version":2},"reference_index":61,"source":"pdf_text","source_observed_at":"2026-08-11T10:58:56.190657Z"},"links":{"cited_paper":"/paper/2009.00119","citing_paper":"/paper/2412.16020"},"observation_digest":"sha256:6676970c55aa756cea355f9059a445487df585c9a846461ce0aaf8821aa26786","observation_id":"7284f2ae-466a-467c-951a-9ddcc89b0c48","resolution":{"observed_at":"2026-08-11T10:58:56.190657Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-11T10:58:57.011694Z","title":null,"venue":null,"work_id":"712f2d9a-907d-4b20-8e36-c80bed2ca5de","year":null},"citing_paper":{"arxiv_id":"2412.16020","last_updated":"2025-06-03T08:19:02Z","snapshot_observed_at":"2026-08-11T10:50:33.964800Z","submitted_at":"2024-12-20T16:10:03Z","title":"Dimension-8 operators in $W^+W^-$ production via gluon fusion","version":2},"reference_index":62,"source":"pdf_text","source_observed_at":"2026-08-11T10:58:56.195165Z"},"links":{"citing_paper":"/paper/2412.16020"},"observation_digest":"sha256:313db6d0a5207435d8348d7d59931a4dd16fffccd3bfe24fdb3fb12de13b359f","observation_id":"65b1f2ec-d78f-4fe2-830d-457321bae343","resolution":{"observed_at":"2026-08-11T10:58:57.015641Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"0812.1594","last_updated":"2022-05-24T09:22:41Z","snapshot_observed_at":"2026-08-08T17:15:26.165328Z","submitted_at":"2008-12-09T20:49:40Z","title":"Two-component spinor techniques and Feynman rules for quantum field theory and supersymmetry","version":6},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0812.1594","snapshot_observed_at":"2026-08-11T10:58:56.198881Z","title":null,"venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"2412.16020","last_updated":"2025-06-03T08:19:02Z","snapshot_observed_at":"2026-08-11T10:50:33.964800Z","submitted_at":"2024-12-20T16:10:03Z","title":"Dimension-8 operators in $W^+W^-$ production via gluon fusion","version":2},"reference_index":63,"source":"pdf_text","source_observed_at":"2026-08-11T10:58:56.198881Z"},"links":{"cited_paper":"/paper/0812.1594","citing_paper":"/paper/2412.16020"},"observation_digest":"sha256:be228e5f192c9fbb3059f3ed6877838f7f630d8750149312df48b215333b63c7","observation_id":"86f0b3e7-de35-44f2-a2ee-a51d160a1aca","resolution":{"observed_at":"2026-08-11T10:58:56.198881Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"paper":{"arxiv_id":"2412.16020","last_updated":"2025-06-03T08:19:02Z","latest_version":2,"primary_category":"hep-ph","snapshot_observed_at":"2026-08-11T10:50:33.964800Z","submitted_at":"2024-12-20T16:10:03Z","title":"Dimension-8 operators in $W^+W^-$ production via gluon fusion"},"reference_resolution":{"displayed":63,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":49,"verified_exact":12,"verified_fuzzy":2},"total_outbound_references":63},"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":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"thesis":"As of 11 August 2026, this Paper Citation Record lists 63 of 63 outbound references and 2 inbound Pith citation observations for arXiv:2412.16020."}