{"as_of":"2026-08-15T02:13:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:7198e76bb6e66696196968b79190d5464a5cf89c7d004f741c0a7922f8d6e9ce","coverage":[{"denominator":96,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":96,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-14T05:54:36.959162Z","state":"measured"},{"denominator":96,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":96,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-14T06:32:32.682623+00:00","state":"measured"},{"denominator":0,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":0,"source":"paper_references, paper_reference_links","source_observed_at":null,"state":"measured"},{"denominator":1,"lane":"external_citation_measurements","note":"A source-named dated measurement, never combined with another source.","records_observed":0,"source":"cited_works","source_observed_at":null,"state":"measured"}],"external_citation_measurements":[],"inbound":[],"links":{"evidence":"/evidence","html":"/paper/1909.00592/citation-record","integrity":"/paper/1909.00592/integrity","json":"/paper/1909.00592/citation-record.json","paper":"/paper/1909.00592"},"outbound":[{"citation":{"cited_paper":{"arxiv_id":"1207.7214","last_updated":"2012-08-31T19:29:54Z","snapshot_observed_at":"2026-08-12T13:22:06.792849Z","submitted_at":"2012-07-31T11:59:59Z","title":"Observation of a new particle in the search for the Standard Model Higgs boson with the ATLAS detector at the LHC","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1207.7214","snapshot_observed_at":"2026-08-14T05:54:36.620688Z","title":"Observation of a new particle in the search for the Standard Model Higgs boson with the ATLAS detector at the LHC,","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.620688Z"},"links":{"cited_paper":"/paper/1207.7214","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:55f7359f26236c9ac6975c11a26a457360db9303ba09c9616c683e032c7fcd53","observation_id":"d1e40cda-5451-42a3-ab7b-df4fa3618d7d","resolution":{"observed_at":"2026-08-14T05:54:36.620688Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1207.7235","last_updated":"2013-01-28T10:46:38Z","snapshot_observed_at":"2026-08-15T00:51:31.889320Z","submitted_at":"2012-07-31T13:27:18Z","title":"Observation of a new boson at a mass of 125 GeV with the CMS experiment at the LHC","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1207.7235","snapshot_observed_at":"2026-08-14T05:54:36.624694Z","title":"Observation of a New Boson at a Mass of 125 GeV with the CMS Experiment at the LHC,","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.624694Z"},"links":{"cited_paper":"/paper/1207.7235","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:a48237867cc8433f1d260badd96b7617b76be4ecb47151701bfb364c5c51f590","observation_id":"a93bd46d-a34b-46a8-bd97-d30fd4cbee2a","resolution":{"observed_at":"2026-08-14T05:54:36.624694Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1310.8361","last_updated":"2014-01-08T19:07:23Z","snapshot_observed_at":"2026-08-14T23:57:00.191165Z","submitted_at":"2013-10-31T01:50:01Z","title":"Higgs Working Group Report of the Snowmass 2013 Community Planning Study","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1310.8361","snapshot_observed_at":"2026-08-14T05:54:36.628203Z","title":"Working Group Report: Higgs Boson,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.628203Z"},"links":{"cited_paper":"/paper/1310.8361","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:11daa58b1fd27e7858f871b89e5d8f7f2431dd333c38270765934076b534bcaf","observation_id":"28a8f477-5f46-4f25-b798-ded1824daeda","resolution":{"observed_at":"2026-08-14T05:54:36.628203Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1610.07922","last_updated":"2017-05-15T16:42:19Z","snapshot_observed_at":"2026-08-14T21:33:38.030583Z","submitted_at":"2016-10-25T15:30:43Z","title":"Handbook of LHC Higgs Cross Sections: 4. Deciphering the Nature of the Higgs Sector","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1610.07922","snapshot_observed_at":"2026-08-14T05:54:36.631793Z","title":"Handbook of LHC Higgs Cross Sections: 4. Deciphering the Nature of the Higgs Sector,","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.631793Z"},"links":{"cited_paper":"/paper/1610.07922","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:8f2d0678b2b48c9675d4ae7cb620c8b9c29f2b9c3bfa05de0d722360b5da695f","observation_id":"f4a27b09-2ae9-4ad8-9bf8-b8a7411c3a9a","resolution":{"observed_at":"2026-08-14T05:54:36.631793Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1307.1347","last_updated":"2013-11-29T17:03:11Z","snapshot_observed_at":"2026-08-15T00:11:46.803101Z","submitted_at":"2013-07-04T14:26:53Z","title":"Handbook of LHC Higgs Cross Sections: 3. Higgs Properties","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1307.1347","snapshot_observed_at":"2026-08-14T05:54:36.635280Z","title":"Handbook of LHC Higgs Cross Sections: 3. Higgs Properties,","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.635280Z"},"links":{"cited_paper":"/paper/1307.1347","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:491f5ae748845ed1d7449ce16fb2494740d546573ebfeac10a19614abaf901b1","observation_id":"3b2f1c2e-b4f8-464a-804b-e1ad1415b4d5","resolution":{"observed_at":"2026-08-14T05:54:36.635280Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ex/9503002","last_updated":"1995-03-03T14:09:44Z","snapshot_observed_at":"2026-07-07T03:38:34.362538Z","submitted_at":"1995-03-02T23:42:23Z","title":"Observation of Top Quark Production in Pbar-P Collisions","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ex/9503002","snapshot_observed_at":"2026-08-14T05:54:36.638877Z","title":"Observation of top quark production in ¯ pp collisions,","venue":null,"work_id":null,"year":1995},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.638877Z"},"links":{"cited_paper":"/paper/hep-ex/9503002","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:282698bd6ecdf15aa6836f2e6ae3a52eb832baa690668d2690a3836fcafe95d5","observation_id":"5f157701-2e6e-4a39-aacf-a3f031fe72ec","resolution":{"observed_at":"2026-08-14T05:54:36.638877Z","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":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T05:54:36.642832Z","title":"Search for high mass top quark production inp¯p collisions at√s = 1.8 TeV,","venue":null,"work_id":null,"year":1995},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.642832Z"},"links":{"citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:fc01d63e44fe52ad51d2d031911265a6b9c592f917f28d13cf7d28b6cfd037e2","observation_id":"2353e51b-3fa5-416c-a506-ff1b324bda76","resolution":{"observed_at":"2026-08-14T05:54:36.642832Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1411.1054","last_updated":"2015-09-08T18:37:03Z","snapshot_observed_at":"2026-08-14T23:12:55.248171Z","submitted_at":"2014-11-04T21:00:00Z","title":"Possible Futures of Electroweak Precision: ILC, FCC-ee, and CEPC","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1411.1054","snapshot_observed_at":"2026-08-14T05:54:36.646312Z","title":"Possible Futures of Electroweak Precision: ILC, FCC-ee, and CEPC,","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.646312Z"},"links":{"cited_paper":"/paper/1411.1054","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:e4aef1035fa18114b02c8e864116bb80381362474b640ea386df27c9dc51b80a","observation_id":"6a84dd9f-e45a-410a-bb41-16fab175bb3e","resolution":{"observed_at":"2026-08-14T05:54:36.646312Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1504.01726","last_updated":"2015-08-13T08:50:05Z","snapshot_observed_at":"2026-08-14T22:53:23.170086Z","submitted_at":"2015-04-07T14:37:38Z","title":"Physics at the e+ e- Linear Collider","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1504.01726","snapshot_observed_at":"2026-08-14T05:54:36.649675Z","title":"Physics at the e+ e- Linear Collider,","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.649675Z"},"links":{"cited_paper":"/paper/1504.01726","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:9a8936cd73b231cae202425ae23bec1f0b4dc4fd9795acc09e06215af6d99d73","observation_id":"ab075a55-2fbb-41c6-9a10-6ff3009ff997","resolution":{"observed_at":"2026-08-14T05:54:36.649675Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1506.05992","last_updated":"2015-06-26T19:19:08Z","snapshot_observed_at":"2026-08-14T22:43:45.210715Z","submitted_at":"2015-06-19T13:16:34Z","title":"Physics Case for the International Linear Collider","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1506.05992","snapshot_observed_at":"2026-08-14T05:54:36.652790Z","title":"Physics Case for the International Linear Collider,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.652790Z"},"links":{"cited_paper":"/paper/1506.05992","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:939ba07cd5e300bd88eb4dac19914cb6f48e3f4b3a6cbdff63ea36b864763412","observation_id":"c0cffe2c-cd46-4ecf-bc58-e2391a3e0f72","resolution":{"observed_at":"2026-08-14T05:54:36.652790Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1812.06018","last_updated":"2019-05-06T21:54:42Z","snapshot_observed_at":"2026-08-14T17:43:31.322538Z","submitted_at":"2018-12-14T16:51:35Z","title":"The Compact Linear Collider (CLIC) - 2018 Summary Report","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1812.06018","snapshot_observed_at":"2026-08-14T05:54:36.656062Z","title":"The Compact Linear Col- lider (CLIC) - 2018 Summary Report,","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.656062Z"},"links":{"cited_paper":"/paper/1812.06018","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:e260b5f231fdad4be064102629a80eaafda75d20d5476c896e93a32fc72bf2fb","observation_id":"6109c36d-f036-435d-9c8f-763811a09be0","resolution":{"observed_at":"2026-08-14T05:54:36.656062Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1812.07986","last_updated":"2018-12-19T14:56:44Z","snapshot_observed_at":"2026-08-14T17:41:12.841650Z","submitted_at":"2018-12-19T14:56:44Z","title":"The Compact Linear e$^+$e$^-$ Collider (CLIC): Physics Potential","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1812.07986","snapshot_observed_at":"2026-08-14T05:54:36.659440Z","title":"The Compact Linear e +e− Collider (CLIC): Physics Potential,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.659440Z"},"links":{"cited_paper":"/paper/1812.07986","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:f7370236847a487c271d022fa7a3c5aa3aabc76fc7406d136246c609f82f45fe","observation_id":"40ef390a-5528-4707-b8d8-48175b9effd1","resolution":{"observed_at":"2026-08-14T05:54:36.659440Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1903.08655","last_updated":"2019-03-20T16:48:18Z","snapshot_observed_at":"2026-08-14T16:59:20.254746Z","submitted_at":"2019-03-20T16:48:18Z","title":"The Compact Linear Collider (CLIC) - Project Implementation Plan","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1903.08655","snapshot_observed_at":"2026-08-14T05:54:36.662822Z","title":"The Compact Linear Collider (CLIC) - Project Implementation Plan,","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.662822Z"},"links":{"cited_paper":"/paper/1903.08655","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:d9c41288269e17ef7e610dac894f50dadb2c0b36a92a806dfc518e4ef5685eae","observation_id":"3107d262-8d20-40d1-83da-a3b303436083","resolution":{"observed_at":"2026-08-14T05:54:36.662822Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1901.09829","last_updated":"2019-01-28T17:28:27Z","snapshot_observed_at":"2026-08-14T17:24:47.576113Z","submitted_at":"2019-01-28T17:28:27Z","title":"The International Linear Collider. A Global Project","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1901.09829","snapshot_observed_at":"2026-08-14T05:54:36.665947Z","title":"The International Linear Collider. A Global Project,","venue":null,"work_id":null,"year":1901},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.665947Z"},"links":{"cited_paper":"/paper/1901.09829","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:32281add628bca8bc8510d3ae09160043e8a832731b4755b6cd39159d07a79ab","observation_id":"e71b0e6e-fc06-4f69-8fe6-ec464d744b92","resolution":{"observed_at":"2026-08-14T05:54:36.665947Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1306.6352","last_updated":"2013-06-26T20:31:40Z","snapshot_observed_at":"2026-08-15T00:12:41.509313Z","submitted_at":"2013-06-26T20:31:40Z","title":"The International Linear Collider Technical Design Report - Volume 2: Physics","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1306.6352","snapshot_observed_at":"2026-08-14T05:54:36.669257Z","title":"The International Linear Collider Technical Design Report - Volume 2: Physics,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.669257Z"},"links":{"cited_paper":"/paper/1306.6352","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:737c7665c7130be81590ca2e3929ad8445dbbb4c3d021fd19b3d96908539bbbb","observation_id":"8fcb030c-bffb-46a5-b7a9-7f7c29d6a622","resolution":{"observed_at":"2026-08-14T05:54:36.669257Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1306.6327","last_updated":"2013-06-26T19:59:31Z","snapshot_observed_at":"2026-08-15T00:12:42.164853Z","submitted_at":"2013-06-26T19:59:31Z","title":"The International Linear Collider Technical Design Report - Volume 1: Executive Summary","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1306.6327","snapshot_observed_at":"2026-08-14T05:54:36.672755Z","title":"The International Linear Collider Technical Design Report - Volume 1: Executive Summary,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.672755Z"},"links":{"cited_paper":"/paper/1306.6327","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:ffb50e9d321a3e3c9fb597bfc0a2fcf210afd207df7acd53835368d09241ab3f","observation_id":"701253ea-8c17-4517-a006-c4e0d63c201d","resolution":{"observed_at":"2026-08-14T05:54:36.672755Z","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":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T05:54:36.676175Z","title":"CEPC-SPPC Preliminary Conceptual Design Report. 1. Physics and Detector,","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.676175Z"},"links":{"citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:b41b782eac2c12e248a987e15b3222f4dc6f9d5410db1c360359070db853190a","observation_id":"c1f7739b-90a5-4f83-ad75-dd87f6096cbb","resolution":{"observed_at":"2026-08-14T05:54:36.676175Z","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":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T05:54:36.679262Z","title":"CEPC-SPPC Preliminary Conceptual Design Report. 2. Accel- erator,","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.679262Z"},"links":{"citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:899c6077cf4d5b46e4bc2d6ae68d145afdda3d58a88abd53cda014c4ecdfde18","observation_id":"813b2bad-3efb-46c0-90aa-df25ea024bde","resolution":{"observed_at":"2026-08-14T05:54:36.679262Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1308.6176","last_updated":"2013-12-11T17:16:06Z","snapshot_observed_at":"2026-08-15T00:05:11.575016Z","submitted_at":"2013-08-28T14:55:58Z","title":"First Look at the Physics Case of TLEP","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1308.6176","snapshot_observed_at":"2026-08-14T05:54:36.685686Z","title":"First Look at the Physics Case of TLEP,","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.685686Z"},"links":{"cited_paper":"/paper/1308.6176","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:8c8495c48f6c9b5fea4fdc1475f6fa161a3e1210ea3ec20036d614d92bc215a2","observation_id":"3a0563a3-ca40-4934-8131-9698689f79a5","resolution":{"observed_at":"2026-08-14T05:54:36.685686Z","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":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T05:54:36.688814Z","title":"FCC Physics Opportunities : Future Circular Collider Conceptual Design Report Volume 1,","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.688814Z"},"links":{"citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:eee43d9e47fd59c42dc79ecbf6cac930c7494c59d54af13273b4259548f581da","observation_id":"5de536a9-2a39-4c32-9dfa-e520e2cbf1b1","resolution":{"observed_at":"2026-08-14T05:54:36.688814Z","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":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T05:54:36.692051Z","title":"FCC-ee: The Lepton Collider : Future Circular Collider Conceptual Design Report Volume 2,","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.692051Z"},"links":{"citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:07712d9c432a0dfb9eaf457145ad7f2e04e4ab20e20225ae3ce033192b0aa098","observation_id":"85fc6cf2-80db-4c4a-9270-cddb15d05204","resolution":{"observed_at":"2026-08-14T05:54:36.692051Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1902.04070","last_updated":"2019-12-20T10:34:59Z","snapshot_observed_at":"2026-08-14T19:02:39.353559Z","submitted_at":"2019-02-11T09:45:44Z","title":"Standard Model Physics at the HL-LHC and HE-LHC","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1902.04070","snapshot_observed_at":"2026-08-14T05:54:36.695258Z","title":"Standard Model Physics at the HL-LHC and HE-LHC,","venue":null,"work_id":null,"year":1902},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.695258Z"},"links":{"cited_paper":"/paper/1902.04070","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:6c4fbbfac35c7bb05b02cb066f02e277fc0aa4bb50df0fc2aeb5e4992bbf86a4","observation_id":"949baed2-5aa6-4b32-b766-75e789a24984","resolution":{"observed_at":"2026-08-14T05:54:36.695258Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1901.09966","last_updated":"2019-03-02T15:15:16Z","snapshot_observed_at":"2026-08-14T17:28:33.914753Z","submitted_at":"2019-01-20T10:49:04Z","title":"Physics Beyond Colliders at CERN: Beyond the Standard Model Working Group Report","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1901.09966","snapshot_observed_at":"2026-08-14T05:54:36.698539Z","title":"Physics Beyond Colliders at CERN: Beyond the Standard Model Working Group Report,","venue":null,"work_id":null,"year":1901},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.698539Z"},"links":{"cited_paper":"/paper/1901.09966","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:3581bb9ba25f0e65d76f47dad10a80842a8a098e664cce706b8e70052a35036f","observation_id":"bec8a2fc-37c8-4a00-963d-ffc61ab5f637","resolution":{"observed_at":"2026-08-14T05:54:36.698539Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1812.07831","last_updated":"2019-08-13T14:42:45Z","snapshot_observed_at":"2026-08-14T17:41:23.112356Z","submitted_at":"2018-12-19T09:17:35Z","title":"Beyond the Standard Model Physics at the HL-LHC and HE-LHC","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1812.07831","snapshot_observed_at":"2026-08-14T05:54:36.701616Z","title":"Beyond the Standard Model Physics at the HL-LHC and HE-LHC,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.701616Z"},"links":{"cited_paper":"/paper/1812.07831","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:b402342166aee80c8e1628d0227f83b99b3c7b20f703eaf6b163e68e2bca731e","observation_id":"14f01e44-6886-45d2-931b-85db2cef8a7a","resolution":{"observed_at":"2026-08-14T05:54:36.701616Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1904.05637","last_updated":"2020-06-17T09:01:59Z","snapshot_observed_at":"2026-08-14T16:48:07.524868Z","submitted_at":"2019-04-11T11:34:42Z","title":"Top-quark electroweak interactions at high energy","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1904.05637","snapshot_observed_at":"2026-08-14T05:54:36.705240Z","title":"Top-quark electroweak interactions at high energy,","venue":null,"work_id":null,"year":1904},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.705240Z"},"links":{"cited_paper":"/paper/1904.05637","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:4dcedb3273a382d3349e8822adf6ba4df768021d65633f77a0408ebe9131f2d0","observation_id":"2c35ad2c-5690-4e23-bd6c-5589f3cbc757","resolution":{"observed_at":"2026-08-14T05:54:36.705240Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1710.02008","last_updated":"2018-01-09T20:59:08Z","snapshot_observed_at":"2026-08-14T20:26:34.575598Z","submitted_at":"2017-10-05T13:31:27Z","title":"Statistical approach to Higgs couplings in the standard model effective field theory","version":2},"cited_work":{"arxiv_id":"1710.02008","doi":null,"metadata_source":"pith","pith_arxiv_id":"1710.02008","snapshot_observed_at":"2026-08-14T05:54:37.741122Z","title":"Statistical approach to Higgs couplings in the standard model effective field theory","venue":"hep-ph","work_id":"6eec8f33-23be-44a0-96ba-d142dc37941a","year":2017},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.708604Z"},"links":{"cited_paper":"/paper/1710.02008","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:e6310581faa703a68fe7c441c2e2e45414a156395c4b312db3bf699dda4f3077","observation_id":"6461c846-e800-4b39-ac89-f17d015e1d07","resolution":{"observed_at":"2026-08-14T05:54:37.745077Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1809.03520","last_updated":"2022-10-10T11:09:51Z","snapshot_observed_at":"2026-08-14T18:30:29.118006Z","submitted_at":"2018-09-10T18:00:18Z","title":"Probing top-quark couplings indirectly at Higgs factories","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1809.03520","snapshot_observed_at":"2026-08-14T05:54:36.715145Z","title":"Probing top-quark couplings indirectly at Higgs factories,","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":29,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.715145Z"},"links":{"cited_paper":"/paper/1809.03520","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:02378e39271c7f63d2913fd15868528b34dca09713e1bed9e5f77870ec267d8b","observation_id":"2f1a2eab-5394-47e8-926a-0295dff1cb8a","resolution":{"observed_at":"2026-08-14T05:54:36.715145Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1907.10619","last_updated":"2020-12-15T17:18:17Z","snapshot_observed_at":"2026-08-14T16:02:44.344755Z","submitted_at":"2019-07-24T18:00:01Z","title":"The electro-weak couplings of the top and bottom quarks -- global fit and future prospects","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1907.10619","snapshot_observed_at":"2026-08-14T05:54:36.718329Z","title":"The electro-weak couplings of the top and bottom quarks – global fit and future prospects,","venue":null,"work_id":null,"year":1907},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.718329Z"},"links":{"cited_paper":"/paper/1907.10619","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:69aaeb57e84d2cc24d613e492a5d33cf925a93fc1cff1961f95eb8600e8e4324","observation_id":"4fa624e0-578c-4456-992d-1e999344540c","resolution":{"observed_at":"2026-08-14T05:54:36.718329Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1809.09624","last_updated":"2019-04-04T13:19:27Z","snapshot_observed_at":"2026-08-14T18:23:41.250416Z","submitted_at":"2018-09-25T18:00:00Z","title":"Constraining four-fermion operators using rare top decays","version":2},"cited_work":{"arxiv_id":"1809.09624","doi":null,"metadata_source":"pith","pith_arxiv_id":"1809.09624","snapshot_observed_at":"2026-08-14T05:54:37.700574Z","title":"Constraining four-fermion operators using rare top decays","venue":"hep-ph","work_id":"dc8859b9-95f5-414a-bf8d-78a2c49d4255","year":2018},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.721916Z"},"links":{"cited_paper":"/paper/1809.09624","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:774db586389cdaa756550bbf3fe2d0ea6399adad2de584560aa5aeb043200070","observation_id":"bfdddd14-f05b-466f-82c1-fdb71bc64628","resolution":{"observed_at":"2026-08-14T05:54:37.704299Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1802.07237","last_updated":"2018-02-20T18:31:50Z","snapshot_observed_at":"2026-08-14T19:44:03.950078Z","submitted_at":"2018-02-20T18:31:50Z","title":"Interpreting top-quark LHC measurements in the standard-model effective field theory","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1802.07237","snapshot_observed_at":"2026-08-14T05:54:36.728292Z","title":"Interpreting top-quark LHC measurements in the standard- model effective field theory,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.728292Z"},"links":{"cited_paper":"/paper/1802.07237","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:2cfdbbff93213d0e9f3f0a9dd71bed126697642ddd12db9da8589728d0a5e52e","observation_id":"569f9bd0-ec0a-4bad-9748-333a4d4ad48e","resolution":{"observed_at":"2026-08-14T05:54:36.728292Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1706.08945","last_updated":"2018-11-12T14:43:11Z","snapshot_observed_at":"2026-08-14T20:51:18.057104Z","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":"2026-08-14T05:54:36.731563Z","title":"The Standard Model as an Effective Field Theory,","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":34,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.731563Z"},"links":{"cited_paper":"/paper/1706.08945","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:2189be781137dc416f987d5444439a09d361551ef58a64e9f382ef4a1521790c","observation_id":"3630d472-0fcd-4d99-b1a5-bd95c07c0239","resolution":{"observed_at":"2026-08-14T05:54:36.731563Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1906.06949","last_updated":"2019-10-09T09:12:32Z","snapshot_observed_at":"2026-08-14T16:14:38.754207Z","submitted_at":"2019-06-17T11:05:30Z","title":"The Higgs width in the SMEFT","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1906.06949","snapshot_observed_at":"2026-08-14T05:54:36.734821Z","title":"The Higgs width in the SMEFT,","venue":null,"work_id":null,"year":1906},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.734821Z"},"links":{"cited_paper":"/paper/1906.06949","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:9162f46feedba95d06558ce6f6052a9c54c075dd61bedbfe962389b8da1f5254","observation_id":"0f97cbd3-1177-4cb5-b907-3c285443e8f0","resolution":{"observed_at":"2026-08-14T05:54:36.734821Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1702.00951","last_updated":"2017-03-28T17:04:42Z","snapshot_observed_at":"2026-08-14T21:18:09.609017Z","submitted_at":"2017-02-03T10:01:21Z","title":"Constraining Higgs boson effective couplings at electron-positron colliders","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1702.00951","snapshot_observed_at":"2026-08-14T05:54:36.738263Z","title":"Constraining Higgs boson effec- tive couplings at electron-positron colliders,","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":36,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.738263Z"},"links":{"cited_paper":"/paper/1702.00951","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:42efdacd87f0ad9f96afae0e9337c847721ec52527a256abeb9990e96b5eb100","observation_id":"184161a5-aeb5-4508-8322-c1979824554e","resolution":{"observed_at":"2026-08-14T05:54:36.738263Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1805.04697","last_updated":"2018-06-13T07:36:18Z","snapshot_observed_at":"2026-08-14T19:16:07.775303Z","submitted_at":"2018-05-12T10:55:50Z","title":"Study of Higgs Effective Couplings at Electron-Proton Colliders","version":2},"cited_work":{"arxiv_id":"1805.04697","doi":null,"metadata_source":"pith","pith_arxiv_id":"1805.04697","snapshot_observed_at":"2026-08-14T05:54:37.642923Z","title":"Study of Higgs Effective Couplings at Electron-Proton Colliders","venue":"hep-ph","work_id":"b846922d-e962-46d0-8faf-4df5edb94432","year":2018},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":37,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.741771Z"},"links":{"cited_paper":"/paper/1805.04697","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:a4353b9e405ba0ecc4224a5de32af8e89d1bd0746bf9269d3093c975cf105209","observation_id":"c6657e8a-51dc-4873-b335-d0be391bd4ac","resolution":{"observed_at":"2026-08-14T05:54:37.646913Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1702.05753","last_updated":"2017-09-20T12:49:30Z","snapshot_observed_at":"2026-08-14T21:15:49.959295Z","submitted_at":"2017-02-19T14:21:34Z","title":"Probing Higgs boson couplings in H+$\\gamma$ production at the LHC","version":2},"cited_work":{"arxiv_id":"1702.05753","doi":null,"metadata_source":"pith","pith_arxiv_id":"1702.05753","snapshot_observed_at":"2026-08-14T05:54:37.629270Z","title":"Probing Higgs boson couplings in H+$\\gamma$ production at the LHC","venue":"hep-ph","work_id":"1ebcf131-237d-4011-9412-eeb32941c19c","year":2017},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":38,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.745106Z"},"links":{"cited_paper":"/paper/1702.05753","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:c03147fdf6c671d0a7b228c278ff197900fddd1f671b05716955947f523ca219","observation_id":"f21694c6-744a-4eaf-84c4-49d5477be80a","resolution":{"observed_at":"2026-08-14T05:54:37.632909Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1510.04561","last_updated":"2015-10-15T14:51:27Z","snapshot_observed_at":"2026-08-14T22:27:41.715889Z","submitted_at":"2015-10-15T14:51:27Z","title":"Sensitivities of Prospective Future e+e- Colliders to Decoupled New Physics","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1510.04561","snapshot_observed_at":"2026-08-14T05:54:36.748623Z","title":"Sensitivities of Prospective Future e+e- Colliders to Decoupled New Physics,","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":39,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.748623Z"},"links":{"cited_paper":"/paper/1510.04561","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:24760391fa6865a6926189d273799ee6284859c9dd9f403c44bc7950f85d2d8a","observation_id":"af97b2f2-023f-46e1-845e-3729bab2ff0b","resolution":{"observed_at":"2026-08-14T05:54:36.748623Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1711.04046","last_updated":"2018-06-12T08:05:15Z","snapshot_observed_at":"2026-08-14T20:14:45.375299Z","submitted_at":"2017-11-11T00:15:40Z","title":"Probing 6D Operators at Future $e^-e^+$ Colliders","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1711.04046","snapshot_observed_at":"2026-08-14T05:54:36.751862Z","title":"Probing 6D operators at future e?e+ colliders,","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":40,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.751862Z"},"links":{"cited_paper":"/paper/1711.04046","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:0babcad6fd872a8ceaa33f892bab2a0ecc961e0618cb5d82a71dcf47a035abd2","observation_id":"fe94aef7-c19a-4278-bed3-61c7fc359372","resolution":{"observed_at":"2026-08-14T05:54:36.751862Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1701.04804","last_updated":"2017-01-17T18:36:16Z","snapshot_observed_at":"2026-08-14T21:20:46.677269Z","submitted_at":"2017-01-17T18:36:16Z","title":"Dimension-6 Operator Analysis of the CLIC Sensitivity to New Physics","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1701.04804","snapshot_observed_at":"2026-08-14T05:54:36.754957Z","title":"Dimension-6 Operator Analysis of the CLIC Sensitiv- ity to New Physics,","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":41,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.754957Z"},"links":{"cited_paper":"/paper/1701.04804","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:9093ce8b09f6e0296c8a7b91ebb2c765304359714deaa276b8b3ae9d8054d74c","observation_id":"9161ce52-d750-4a20-8671-d3c04f02687a","resolution":{"observed_at":"2026-08-14T05:54:36.754957Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1605.02684","last_updated":"2016-05-09T18:24:04Z","snapshot_observed_at":"2026-08-14T21:58:11.922223Z","submitted_at":"2016-05-09T18:24:04Z","title":"Les Houches 2015: Physics at TeV colliders - new physics working group report","version":1},"cited_work":{"arxiv_id":"1605.02684","doi":null,"metadata_source":"pith","pith_arxiv_id":"1605.02684","snapshot_observed_at":"2026-08-14T05:54:37.589164Z","title":"Les Houches 2015: Physics at TeV colliders - new physics working group report","venue":"hep-ph","work_id":"b7c56c02-0e5e-4c6a-be85-cfeb5edc95a6","year":2016},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":42,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.758121Z"},"links":{"cited_paper":"/paper/1605.02684","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:797f5c635053777b1b2d71c115bf4f306c11fdf1a1925a07ef99bfea1940e1ea","observation_id":"c77742d1-86c4-477d-80d0-2b8c5f802fa9","resolution":{"observed_at":"2026-08-14T05:54:37.592804Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1501.05939","last_updated":"2015-01-23T20:58:27Z","snapshot_observed_at":"2026-08-14T23:02:55.609104Z","submitted_at":"2015-01-23T20:58:27Z","title":"Probing top-Z dipole moments at the LHC and ILC","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1501.05939","snapshot_observed_at":"2026-08-14T05:54:36.761403Z","title":"Probing top-Z dipole moments at the LHC and ILC,","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":43,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.761403Z"},"links":{"cited_paper":"/paper/1501.05939","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:213e8ba7437c8ed3de6999284c7f14f138c12bf4f4cab9b0f21c9189c1097299","observation_id":"91c55c73-b56d-419a-a12b-a041007352d4","resolution":{"observed_at":"2026-08-14T05:54:36.761403Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1404.1005","last_updated":"2015-08-25T13:30:52Z","snapshot_observed_at":"2026-08-14T23:38:45.717364Z","submitted_at":"2014-04-03T16:55:23Z","title":"Constraining couplings of the top quarks to the Z boson in ttbar+Z production at the LHC","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1404.1005","snapshot_observed_at":"2026-08-14T05:54:36.764684Z","title":"Constraining couplings of top quarks to the Z boson in tt + Z production at the LHC,","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":44,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.764684Z"},"links":{"cited_paper":"/paper/1404.1005","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:4b889404f9580de456c9c54ad69baaedb37357c4367a019703779686f2afa860","observation_id":"cb150660-49bd-493e-8da2-fad9bd3ee982","resolution":{"observed_at":"2026-08-14T05:54:36.764684Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1704.02333","last_updated":"2017-09-05T13:07:02Z","snapshot_observed_at":"2026-08-14T21:07:45.038900Z","submitted_at":"2017-04-07T18:16:59Z","title":"The leptonic future of the Higgs","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1704.02333","snapshot_observed_at":"2026-08-14T05:54:36.767911Z","title":"The leptonic future of the Higgs,","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":45,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.767911Z"},"links":{"cited_paper":"/paper/1704.02333","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:06e517a2cf5d94de661768ac0cf77e5e3a5653efd232a6031f6b9bda35ba8010","observation_id":"c10612c6-0df7-476b-96f7-30ce14fdb346","resolution":{"observed_at":"2026-08-14T05:54:36.767911Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1512.03360","last_updated":"2018-07-04T08:58:55Z","snapshot_observed_at":"2026-08-14T22:19:06.336088Z","submitted_at":"2015-12-10T18:32:43Z","title":"Constraining top quark effective theory in the LHC Run II era","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1512.03360","snapshot_observed_at":"2026-08-14T05:54:36.771000Z","title":"Constraining top quark effective theory in the LHC Run II era,","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":46,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.771000Z"},"links":{"cited_paper":"/paper/1512.03360","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:9fd85e12019c9178ae9d8ff7e4cb1dd95e929290e92fdc1c6f12d26b0cda2e17","observation_id":"ba667b24-d295-4ac1-9851-2c22d7566e74","resolution":{"observed_at":"2026-08-14T05:54:36.771000Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1506.08845","last_updated":"2015-11-30T11:16:55Z","snapshot_observed_at":"2026-08-14T22:42:27.783656Z","submitted_at":"2015-06-29T20:19:24Z","title":"A global fit of top quark effective theory to data","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1506.08845","snapshot_observed_at":"2026-08-14T05:54:36.774312Z","title":"Global fit of top quark effective theory to data,","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":47,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.774312Z"},"links":{"cited_paper":"/paper/1506.08845","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:cab16ac38e38094af8f3079f8e319b998d2e7f634e70f48f8728dfda42e403fe","observation_id":"e1fedb82-53f0-45f9-acc6-699a22db5fae","resolution":{"observed_at":"2026-08-14T05:54:36.774312Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1307.8102","last_updated":"2013-07-30T19:49:47Z","snapshot_observed_at":"2026-08-15T00:08:28.659247Z","submitted_at":"2013-07-30T19:49:47Z","title":"A precise determination of top quark electro-weak couplings at the ILC operating at $\\roots=500\\,\\GeV$","version":1},"cited_work":{"arxiv_id":"1307.8102","doi":null,"metadata_source":"pith","pith_arxiv_id":"1307.8102","snapshot_observed_at":"2026-08-14T05:54:37.526201Z","title":"A precise determination of top quark electro-weak couplings at the ILC operating at $\\roots=500\\,\\GeV$","venue":"hep-ex","work_id":"172251e6-e4de-48f2-acc2-f6a97e114672","year":2013},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":48,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.777524Z"},"links":{"cited_paper":"/paper/1307.8102","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:2db71b3d4663c150cec5e2d0b73a1747240d9724dab168b21e90934914056387","observation_id":"543694bc-d6e4-45fe-ac73-5ae5172bee4a","resolution":{"observed_at":"2026-08-14T05:54:37.530184Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1407.3792","last_updated":"2014-07-14T20:00:04Z","snapshot_observed_at":"2026-08-14T23:26:47.043667Z","submitted_at":"2014-07-14T20:00:04Z","title":"The global electroweak fit at NNLO and prospects for the LHC and ILC","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1407.3792","snapshot_observed_at":"2026-08-14T05:54:36.780846Z","title":"The global electroweak fit at NNLO and prospects for the LHC and ILC,","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":49,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.780846Z"},"links":{"cited_paper":"/paper/1407.3792","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:78745e69e92236fff5020503834816a75a51d9d884080fccd62101b24c47635e","observation_id":"75217c5f-48bb-4e69-b53b-2ca10e2c09dd","resolution":{"observed_at":"2026-08-14T05:54:36.780846Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1709.06492","last_updated":"2017-12-20T12:59:55Z","snapshot_observed_at":"2026-08-14T20:31:43.218832Z","submitted_at":"2017-09-19T15:51:50Z","title":"The SMEFTsim package, theory and tools","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1709.06492","snapshot_observed_at":"2026-08-14T05:54:36.784090Z","title":"The SMEFTsim package, theory and tools,","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":50,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.784090Z"},"links":{"cited_paper":"/paper/1709.06492","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:dee71ce959ba611338b1ffd5de0f590a5429f7edcca8cce4579e5146628a8909","observation_id":"0b2f0128-c3d9-4134-9eb9-58e67c20bdec","resolution":{"observed_at":"2026-08-14T05:54:36.784090Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1901.05979","last_updated":"2019-02-04T23:54:42Z","snapshot_observed_at":"2026-08-14T17:29:26.186087Z","submitted_at":"2019-01-17T19:00:26Z","title":"New Physics in Double Higgs Production at Future $e^+ e^-$ Colliders","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1901.05979","snapshot_observed_at":"2026-08-14T05:54:36.787230Z","title":"New physics in double Higgs production at future e +e? colliders,","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":51,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.787230Z"},"links":{"cited_paper":"/paper/1901.05979","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:96875570cdd89fa8ff235c8aa255eed62627458d2d37c5ea5bb9c9fc7e810a3d","observation_id":"0f676281-0c17-4193-9056-8d6930ce81e7","resolution":{"observed_at":"2026-08-14T05:54:36.787230Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0006032","last_updated":"2000-06-04T19:49:58Z","snapshot_observed_at":"2026-08-10T21:44:08.897465Z","submitted_at":"2000-06-02T18:41:17Z","title":"CP Violation in Top Physics","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0006032","snapshot_observed_at":"2026-08-14T05:54:36.790576Z","title":"CP violation in top physics,","venue":null,"work_id":null,"year":2001},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":52,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.790576Z"},"links":{"cited_paper":"/paper/hep-ph/0006032","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:8126f9115b799497d682b19432bf3a6aabf4244816625ee5b09b7334c8199ac0","observation_id":"50a7c4bf-ca8f-4ba4-8a9a-1e641a3a6662","resolution":{"observed_at":"2026-08-14T05:54:36.790576Z","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":"2026-08-14T23:39:39.614377Z","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":"2026-08-14T05:54:36.793762Z","title":"Precision Measurements of Higgs Couplings: Implications for New Physics Scales,","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":53,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.793762Z"},"links":{"cited_paper":"/paper/1403.7191","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:4bf2bac2bf6d0eb14d892ad5ff36ba3907b0e13022c6838c1ac3ae6635fc57cf","observation_id":"ddcc7063-3186-4b01-81cb-29a208ca8c06","resolution":{"observed_at":"2026-08-14T05:54:36.793762Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1412.6654","last_updated":"2015-04-27T17:44:55Z","snapshot_observed_at":"2026-08-14T23:06:39.251219Z","submitted_at":"2014-12-20T14:12:14Z","title":"Pinning down top dipole moments with ultra-boosted tops","version":2},"cited_work":{"arxiv_id":"1412.6654","doi":null,"metadata_source":"pith","pith_arxiv_id":"1412.6654","snapshot_observed_at":"2026-08-14T05:54:37.371288Z","title":"Pinning down top dipole moments with ultra-boosted tops","venue":"hep-ph","work_id":"a5fd8455-8a7e-4e51-aa5d-e4e2f0a49285","year":2014},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":54,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.797386Z"},"links":{"cited_paper":"/paper/1412.6654","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:933f1c9972bf23a95da9cbe4626dc1e71e508fced73ab75b42ed980d09e09e16","observation_id":"3b264342-3f21-4ed5-a8fa-a8c852078e0f","resolution":{"observed_at":"2026-08-14T05:54:37.374899Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"0801.1939","last_updated":"2008-03-16T08:25:09Z","snapshot_observed_at":"2026-07-06T01:33:42.320597Z","submitted_at":"2008-01-13T07:14:01Z","title":"Probing of $Wtb$ Anomalous Couplings via the $tW$ Channel of Single Top Production","version":3},"cited_work":{"arxiv_id":"0801.1939","doi":null,"metadata_source":"pith","pith_arxiv_id":"0801.1939","snapshot_observed_at":"2026-08-14T05:54:37.358246Z","title":"Probing of $Wtb$ Anomalous Couplings via the $tW$ Channel of Single Top Production","venue":"hep-ph","work_id":"040ab7c0-25c4-42b7-b45e-13a904be2f57","year":2008},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":55,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.801138Z"},"links":{"cited_paper":"/paper/0801.1939","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:b7360f613b70c88455321f8c7b29ea9cd0a9927fc60b65eb230f8ad371c3a434","observation_id":"617913cc-1ba8-4aa8-8c42-76c7c58a4259","resolution":{"observed_at":"2026-08-14T05:54:37.361979Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1410.7703","last_updated":"2014-10-28T17:15:16Z","snapshot_observed_at":"2026-08-14T23:13:57.179177Z","submitted_at":"2014-10-28T17:15:16Z","title":"The Effective Standard Model after LHC Run I","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1410.7703","snapshot_observed_at":"2026-08-14T05:54:36.804663Z","title":"The Effective Standard Model after LHC Run I,","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":56,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.804663Z"},"links":{"cited_paper":"/paper/1410.7703","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:e5efa1f48d42530ae5f55e9d057726af8d67e46124f9b638d3cc088ba2a8239b","observation_id":"492fb964-35e2-44f2-aef8-dacbac908c33","resolution":{"observed_at":"2026-08-14T05:54:36.804663Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1511.05170","last_updated":"2016-07-27T10:51:23Z","snapshot_observed_at":"2026-08-14T22:22:42.158365Z","submitted_at":"2015-11-16T21:03:18Z","title":"Higgs coupling measurements at the LHC","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1511.05170","snapshot_observed_at":"2026-08-14T05:54:36.808474Z","title":"Higgs coupling measurements at the LHC,","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":57,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.808474Z"},"links":{"cited_paper":"/paper/1511.05170","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:e787a7864e6b8a303078846ae6c4a28b98fa340ba3947fc9ef30da0d3ad4e03b","observation_id":"8a39178a-cb31-412f-ad2f-eb1690a7a002","resolution":{"observed_at":"2026-08-14T05:54:36.808474Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1404.3667","last_updated":"2014-07-03T17:39:21Z","snapshot_observed_at":"2026-08-14T23:37:34.113436Z","submitted_at":"2014-04-14T17:51:30Z","title":"Complete Higgs Sector Constraints on Dimension-6 Operators","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1404.3667","snapshot_observed_at":"2026-08-14T05:54:36.811482Z","title":"Complete Higgs Sector Constraints on Dimension-6 Operators,","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":58,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.811482Z"},"links":{"cited_paper":"/paper/1404.3667","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:626c7e3264ac8f5449a33f8200f154cecbfdcbeeeaeb830c59b1d8ecb3686c33","observation_id":"ef7175aa-61e2-4be5-a56c-4c19fa3a4dd2","resolution":{"observed_at":"2026-08-14T05:54:36.811482Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1707.03890","last_updated":"2018-05-16T12:32:37Z","snapshot_observed_at":"2026-08-14T20:48:00.924383Z","submitted_at":"2017-07-12T19:56:50Z","title":"Constraints on Higgs effective couplings in $H\\nu \\bar{\\nu}$ production of CLIC at 380 GeV","version":2},"cited_work":{"arxiv_id":"1707.03890","doi":null,"metadata_source":"pith","pith_arxiv_id":"1707.03890","snapshot_observed_at":"2026-08-14T05:54:37.327681Z","title":"Constraints on Higgs effective couplings in $H\\nu \\bar{\\nu}$ production of CLIC at 380 GeV","venue":"hep-ph","work_id":"381f4eef-d51e-4702-a619-97d4f3f470e9","year":2017},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":59,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.815201Z"},"links":{"cited_paper":"/paper/1707.03890","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:df57091a2649b280b96240b9964beedfeed04f22d9d4c6802f4a46e4efc568fb","observation_id":"b0939d24-96b2-4bda-85c0-4161ac17d2e5","resolution":{"observed_at":"2026-08-14T05:54:37.331684Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1901.04784","last_updated":"2019-09-19T08:12:40Z","snapshot_observed_at":"2026-08-15T00:38:55.966943Z","submitted_at":"2019-01-15T12:13:53Z","title":"Testing for observability of Higgs effective couplings in triphoton production at FCC-hh","version":3},"cited_work":{"arxiv_id":"1901.04784","doi":null,"metadata_source":"pith","pith_arxiv_id":"1901.04784","snapshot_observed_at":"2026-08-14T05:54:37.314373Z","title":"Testing for observability of Higgs effective couplings in triphoton production at FCC-hh","venue":"hep-ph","work_id":"44af41cb-4fd7-4f98-8a35-200b7f0b43c7","year":2019},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":60,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.818498Z"},"links":{"cited_paper":"/paper/1901.04784","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:f5966bd15bed6ef6c3f2e968b16ea283bd8e716e1fa38fcb7e53cd01305e5387","observation_id":"cea07e40-85ab-484d-b209-0d5fe6b13562","resolution":{"observed_at":"2026-08-14T05:54:37.318076Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1807.04306","last_updated":"2018-07-11T18:13:12Z","snapshot_observed_at":"2026-08-14T18:53:03.402006Z","submitted_at":"2018-07-11T18:13:12Z","title":"Probing Higgs boson couplings in $t\\bar{t}b\\bar{b}$ production at the LHC","version":1},"cited_work":{"arxiv_id":"1807.04306","doi":null,"metadata_source":"pith","pith_arxiv_id":"1807.04306","snapshot_observed_at":"2026-08-14T05:54:37.301485Z","title":"Probing Higgs boson couplings in $t\\bar{t}b\\bar{b}$ production at the LHC","venue":"hep-ph","work_id":"1f3bfe44-8a2a-48fe-9b63-5dc9170b9932","year":2018},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":61,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.822475Z"},"links":{"cited_paper":"/paper/1807.04306","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:74867006190ba596e40feb092b881a5dc2933ee6cf56ccc882df5b4a43517980","observation_id":"ca7ff139-686c-4b78-b4ed-3911312d2f94","resolution":{"observed_at":"2026-08-14T05:54:37.305053Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1511.03674","last_updated":"2016-01-15T15:16:44Z","snapshot_observed_at":"2026-08-14T22:23:50.575645Z","submitted_at":"2015-11-11T21:00:29Z","title":"Strong tW Scattering at the LHC","version":2},"cited_work":{"arxiv_id":"1511.03674","doi":null,"metadata_source":"pith","pith_arxiv_id":"1511.03674","snapshot_observed_at":"2026-08-14T05:54:37.288644Z","title":"Strong tW Scattering at the LHC","venue":"hep-ph","work_id":"3b7c4d5b-4ef7-4f4a-8960-e3d5b2e9d7d6","year":2015},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":62,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.825732Z"},"links":{"cited_paper":"/paper/1511.03674","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:8c2de794ef75a9311be16673172d938442d93d9e92e233a22a1fb94476614813","observation_id":"c99175e5-d42a-4967-bc3b-f08e49be919a","resolution":{"observed_at":"2026-08-14T05:54:37.292159Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1611.09879","last_updated":"2017-07-11T12:14:56Z","snapshot_observed_at":"2026-08-14T21:27:59.412321Z","submitted_at":"2016-11-29T21:12:56Z","title":"The $Z$ decay width in the SMEFT: $y_t$ and $\\lambda$ corrections at one loop","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1611.09879","snapshot_observed_at":"2026-08-14T05:54:36.830320Z","title":"The Z decay width in the SMEFT: yt andλ cor- rections at one loop,","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":63,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.830320Z"},"links":{"cited_paper":"/paper/1611.09879","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:1e1b8ce76207cb32767e824b4aa583c69711f2cb27ae126f86a5cf5d8e0d3d1f","observation_id":"9143e0ce-0c5b-458b-8006-78930acb5c62","resolution":{"observed_at":"2026-08-14T05:54:36.830320Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1611.01165","last_updated":"2017-08-24T21:22:59Z","snapshot_observed_at":"2026-08-15T00:22:26.225669Z","submitted_at":"2016-11-03T20:00:09Z","title":"Sharpening the shape analysis for higher-dimensional operator searches","version":2},"cited_work":{"arxiv_id":"1611.01165","doi":null,"metadata_source":"pith","pith_arxiv_id":"1611.01165","snapshot_observed_at":"2026-08-14T05:54:37.265407Z","title":"Sharpening the shape analysis for higher-dimensional operator searches","venue":"hep-ph","work_id":"134a4cf9-5111-49c1-a9de-e288339a7558","year":2016},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":64,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.833821Z"},"links":{"cited_paper":"/paper/1611.01165","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:89b01796ee5cf9824a2316a6675f66487ec58e56798a121373385835b956fafc","observation_id":"a3dbe409-b820-407c-b375-d63a70162a71","resolution":{"observed_at":"2026-08-14T05:54:37.269393Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1508.05060","last_updated":"2017-07-14T20:27:31Z","snapshot_observed_at":"2026-08-14T22:35:48.583591Z","submitted_at":"2015-08-20T18:05:05Z","title":"Consistent constraints on the Standard Model Effective Field Theory","version":5},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1508.05060","snapshot_observed_at":"2026-08-14T05:54:36.838126Z","title":"Consistent constraints on the Standard Model Effective Field Theory,","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":65,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.838126Z"},"links":{"cited_paper":"/paper/1508.05060","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:72c577024058fbbd75fdc03446793cbffe9a093f0796155ef6216887dca0eb40","observation_id":"2fcb72de-94ae-4d94-9877-8ee5a76ff8df","resolution":{"observed_at":"2026-08-14T05:54:36.838126Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1807.02121","last_updated":"2018-07-05T18:00:02Z","snapshot_observed_at":"2026-08-14T18:55:16.492846Z","submitted_at":"2018-07-05T18:00:02Z","title":"Global and optimal probes for the top-quark effective field theory at future lepton colliders","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1807.02121","snapshot_observed_at":"2026-08-14T05:54:36.842016Z","title":"Global and optimal probes for the top-quark effective field theory at future lepton colliders,","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":66,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.842016Z"},"links":{"cited_paper":"/paper/1807.02121","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:cc799c6e1950922574362bebbe723100e4cef93f1d071e3c3582c715831e2213","observation_id":"db3c9516-b62e-4567-b55a-d5aa14984c7d","resolution":{"observed_at":"2026-08-14T05:54:36.842016Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1306.6464","last_updated":"2014-01-31T19:52:01Z","snapshot_observed_at":"2026-08-15T00:12:37.878223Z","submitted_at":"2013-06-27T11:03:11Z","title":"A framework for Higgs characterisation","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1306.6464","snapshot_observed_at":"2026-08-14T05:54:36.844940Z","title":"A framework for Higgs characterisation,","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":67,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.844940Z"},"links":{"cited_paper":"/paper/1306.6464","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:99ed50bacaf20116785f12c9b239bb52b5d070d1fe9b276ae6658e1b6a5b0815","observation_id":"c121dcca-2699-4bf1-be33-00bd4ba45461","resolution":{"observed_at":"2026-08-14T05:54:36.844940Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1310.5150","last_updated":"2014-04-16T11:13:40Z","snapshot_observed_at":"2026-08-14T23:58:26.073146Z","submitted_at":"2013-10-18T20:00:06Z","title":"Phenomenology of the Higgs Effective Lagrangian via FeynRules","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1310.5150","snapshot_observed_at":"2026-08-14T05:54:36.848133Z","title":"Phenomenology of the Higgs Effective Lagrangian via FEYNRULES,","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":68,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.848133Z"},"links":{"cited_paper":"/paper/1310.5150","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:92196fd72d666016858fe2eb6505e0fba13efae05115cb2cc015e55dbfc94416","observation_id":"e1f04117-4f83-42e9-9542-4177ec9aae07","resolution":{"observed_at":"2026-08-14T05:54:36.848133Z","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":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T05:54:36.851513Z","title":"Effective Lagrangian Analysis of New Interactions and Flavor Conservation,","venue":null,"work_id":null,"year":1986},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":69,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.851513Z"},"links":{"citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:24040a98ce18e6b2284a679574ec3c1c5dd43def6f02929731a0bcaa727a3ce9","observation_id":"985d5c62-198a-415e-b7b1-0241ac2c4b0b","resolution":{"observed_at":"2026-08-14T05:54:36.851513Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1008.4884","last_updated":"2017-01-15T20:19:22Z","snapshot_observed_at":"2026-08-12T14:13:27.638436Z","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":"2026-08-14T05:54:36.855390Z","title":"Dimension-Six Terms in the Standard Model Lagrangian,","venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":70,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.855390Z"},"links":{"cited_paper":"/paper/1008.4884","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:eeae8b09586782ff706d5f70c4e05fcaa51ed09d2e0cf677793d9c51b1a0f542","observation_id":"6af871c5-35e3-4ff5-8073-bd63305bafeb","resolution":{"observed_at":"2026-08-14T05:54:36.855390Z","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":"10.1103/physrevd.48.2182","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T05:54:36.991640Z","title":"Low-energy effects of new interactions in the electroweak boson sector,","venue":null,"work_id":"0cd12fe0-0e81-47b0-be10-309e691518f1","year":1993},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":71,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.859205Z"},"links":{"citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:a7ab9912229c52bd9975b15475bc2b7c0a72ec35b51c75117b3dc5a1b8f1f98b","observation_id":"64832024-8761-42ab-99e8-55141da8ee36","resolution":{"observed_at":"2026-08-14T05:54:36.996786Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1412.6356","last_updated":"2015-01-27T15:13:35Z","snapshot_observed_at":"2026-08-14T23:06:47.265620Z","submitted_at":"2014-12-19T14:27:18Z","title":"A Systematic Approach to the SILH Lagrangian","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1412.6356","snapshot_observed_at":"2026-08-14T05:54:36.862523Z","title":"A Systematic Approach to the SILH Lagrangian,","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":72,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.862523Z"},"links":{"cited_paper":"/paper/1412.6356","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:60760eaf79544a64012044d6875f5bb25f4fdbdd0c28850fc38ff7fe152048d3","observation_id":"be9e58b1-e2b2-4db8-b830-20593f67c425","resolution":{"observed_at":"2026-08-14T05:54:36.862523Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1504.01707","last_updated":"2015-09-16T15:15:20Z","snapshot_observed_at":"2026-08-14T22:53:21.254590Z","submitted_at":"2015-04-07T19:12:09Z","title":"Note on Anomalous Higgs-Boson Couplings in Effective Field Theory","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1504.01707","snapshot_observed_at":"2026-08-14T05:54:36.865757Z","title":"Note on Anomalous Higgs-Boson Couplings in Effective Field Theory,","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":73,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.865757Z"},"links":{"cited_paper":"/paper/1504.01707","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:576ba16ce2f19fd1a48c791035ac87149c4a95d9cd5347479ac2c07c56f87a99","observation_id":"5d57d840-2cc5-4ace-8879-cd478e417a14","resolution":{"observed_at":"2026-08-14T05:54:36.865757Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1303.3876","last_updated":"2014-03-13T16:22:16Z","snapshot_observed_at":"2026-08-15T00:25:00.224509Z","submitted_at":"2013-03-15T19:34:02Z","title":"Effective Lagrangian for a light Higgs-like scalar","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1303.3876","snapshot_observed_at":"2026-08-14T05:54:36.868989Z","title":"Effective La- grangian for a light Higgs-like scalar,","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":74,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.868989Z"},"links":{"cited_paper":"/paper/1303.3876","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:644b3a369c7df0cdaefa73c9da19af78115b08520d1c1a65103b1fa15c829c7d","observation_id":"0a699017-932f-48b0-ba18-0b7c76b6176e","resolution":{"observed_at":"2026-08-14T05:54:36.868989Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1704.01782","last_updated":"2017-10-25T07:21:38Z","snapshot_observed_at":"2026-08-14T21:08:01.073513Z","submitted_at":"2017-04-06T11:04:39Z","title":"Top quark electroweak couplings at future lepton colliders","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1704.01782","snapshot_observed_at":"2026-08-14T05:54:36.872832Z","title":"Top quark electroweak couplings at future lepton colliders,","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":75,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.872832Z"},"links":{"cited_paper":"/paper/1704.01782","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:395b0190cae719dae8eee57e746c5a5d743b5cad45bca024397c70533cd8b3b0","observation_id":"c88b5b83-844e-4c82-922a-b9f826a18363","resolution":{"observed_at":"2026-08-14T05:54:36.872832Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1711.02547","last_updated":"2018-08-14T19:02:22Z","snapshot_observed_at":"2026-08-14T20:16:04.097891Z","submitted_at":"2017-11-07T15:33:20Z","title":"Measurement of the cross section for top quark pair production in association with a W or Z boson in proton-proton collisions at $\\sqrt{s} =$ 13 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1711.02547","snapshot_observed_at":"2026-08-14T05:54:36.876531Z","title":"Measurement of the cross section for top quark pair production in association with a W or Z boson in proton-proton collisions at √s = 13 TeV,","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":76,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.876531Z"},"links":{"cited_paper":"/paper/1711.02547","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:77fd02eba3ed03a399e5b1d71bda478042e414f1dadadd23b6cc3e7f2dfa55de","observation_id":"8d2b20ed-c276-4b00-b051-97493eb823c3","resolution":{"observed_at":"2026-08-14T05:54:36.876531Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1907.11270","last_updated":"2020-03-20T14:55:05Z","snapshot_observed_at":"2026-08-14T16:02:13.238484Z","submitted_at":"2019-07-25T18:44:30Z","title":"Measurement of top quark pair production in association with a Z boson in proton-proton collisions at $\\sqrt{s} =$ 13 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1907.11270","snapshot_observed_at":"2026-08-14T05:54:36.880084Z","title":"Measurement of top quark pair production in association with a Z boson in proton-proton collisions at √s = 13 TeV,","venue":null,"work_id":null,"year":1907},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":77,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.880084Z"},"links":{"cited_paper":"/paper/1907.11270","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:e48ebc36897ff8bef831dbb46cbd7b840bd988a4692d6eddac7d88830bddb48e","observation_id":"77df2a6e-f6e8-44ee-9714-49f408202127","resolution":{"observed_at":"2026-08-14T05:54:36.880084Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1901.05965","last_updated":"2019-04-02T13:31:24Z","snapshot_observed_at":"2026-08-14T17:29:27.823074Z","submitted_at":"2019-01-17T19:00:00Z","title":"A Monte Carlo global analysis of the Standard Model Effective Field Theory: the top quark sector","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1901.05965","snapshot_observed_at":"2026-08-14T05:54:36.883410Z","title":"A Monte Carlo global analysis of the Standard Model Effective Field Theory: the top quark sector,","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":78,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.883410Z"},"links":{"cited_paper":"/paper/1901.05965","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:1568982af141be8a87a501933913f40a6ea3aab9e6656f639d702b0e4566d534","observation_id":"c8a70498-f506-4d71-891e-a7c7b6e2a44f","resolution":{"observed_at":"2026-08-14T05:54:36.883410Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1910.03606","last_updated":"2019-10-08T18:01:30Z","snapshot_observed_at":"2026-08-07T05:47:30.365831Z","submitted_at":"2019-10-08T18:01:30Z","title":"O new physics, where art thou? A global search in the top sector","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1910.03606","snapshot_observed_at":"2026-08-14T05:54:36.886889Z","title":"O new physics, where art thou? A global search in the top sector,","venue":null,"work_id":null,"year":1910},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":79,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.886889Z"},"links":{"cited_paper":"/paper/1910.03606","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:f0e5ffc30ea9fe8a5451ae40681d1df14773e95692b981e26588d572430c9825","observation_id":"c500d3a8-5e60-4e52-b159-f63697bcbe87","resolution":{"observed_at":"2026-08-14T05:54:36.886889Z","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":"2026-08-14T19:38:04.184859Z","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":"2026-08-14T05:54:36.890639Z","title":"Ellis, C","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":80,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.890639Z"},"links":{"cited_paper":"/paper/1803.03252","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:26e6963258f01115f8aa57e5d4d1077cfc390568114018bf72a648d2e3d12422","observation_id":"5559c9dd-da48-4588-9660-a5a06d460f91","resolution":{"observed_at":"2026-08-14T05:54:36.890639Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1106.0522","last_updated":"2011-06-02T21:48:32Z","snapshot_observed_at":"2026-08-14T15:09:00.831441Z","submitted_at":"2011-06-02T21:48:32Z","title":"MadGraph 5 : Going Beyond","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1106.0522","snapshot_observed_at":"2026-08-14T05:54:36.894108Z","title":"MadGraph 5 : Going Beyond,","venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":81,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.894108Z"},"links":{"cited_paper":"/paper/1106.0522","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:fd74fc7ec9d6382810c237f33de93b2d550ce449b1397c635243df2abd608e87","observation_id":"e03656a4-40a9-4656-9d34-789cfb98a2d5","resolution":{"observed_at":"2026-08-14T05:54:36.894108Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1402.1178","last_updated":"2015-08-23T07:22:18Z","snapshot_observed_at":"2026-08-14T23:45:41.487759Z","submitted_at":"2014-02-05T21:02:01Z","title":"Computing decay rates for new physics theories with FeynRules and MadGraph5/aMC@NLO","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1402.1178","snapshot_observed_at":"2026-08-14T05:54:36.897214Z","title":"Computing decay rates for new physics theories with FeynRules and MadGraph 5 aMC@NLO,","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":82,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.897214Z"},"links":{"cited_paper":"/paper/1402.1178","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:d27e859b48f7f7363006bbdae767b1049d7b4acfd6288e5fb131b647f3e53be1","observation_id":"f52634d8-b8cb-48bd-ad70-17f47744f938","resolution":{"observed_at":"2026-08-14T05:54:36.897214Z","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":"2026-08-14T01:28:40.957968Z","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":"2026-08-14T05:54:36.900693Z","title":"The automated computation of tree-level and next-to-leading order differen- tial cross sections, and their matching to parton shower simulations,","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":83,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.900693Z"},"links":{"cited_paper":"/paper/1405.0301","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:6c2471cde52f4e173e31e57cfb71d9e87b9ecce50c73a9e9d1f4201891cdd471","observation_id":"ac708f3c-c488-4459-be15-37c5f827283f","resolution":{"observed_at":"2026-08-14T05:54:36.900693Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1310.1921","last_updated":"2014-05-11T21:04:33Z","snapshot_observed_at":"2026-08-14T23:59:52.057480Z","submitted_at":"2013-10-07T20:00:02Z","title":"FeynRules 2.0 - A complete toolbox for tree-level phenomenology","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1310.1921","snapshot_observed_at":"2026-08-14T05:54:36.905018Z","title":"FeynRules 2.0 - A complete toolbox for tree-level phenomenology,","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":84,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.905018Z"},"links":{"cited_paper":"/paper/1310.1921","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:a94852a4411c36897813e3f1825656943ef49450aed7c8e96f0b99d7568d7ab2","observation_id":"91be9b14-8260-41cd-ae55-f50e12343e1d","resolution":{"observed_at":"2026-08-14T05:54:36.905018Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1108.2040","last_updated":"2012-07-31T19:07:51Z","snapshot_observed_at":"2026-08-14T11:21:58.290807Z","submitted_at":"2011-08-09T20:27:49Z","title":"UFO - The Universal FeynRules Output","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1108.2040","snapshot_observed_at":"2026-08-14T05:54:36.908537Z","title":"UFO - The Universal FeynRules Output,","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":85,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.908537Z"},"links":{"cited_paper":"/paper/1108.2040","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:9258a8a929ea4ef2d7b1f85a8c4a3b3bf771fccd8c5562c628222992dac8bd68","observation_id":"fbca4c1f-3e7d-49d7-8735-2fd031eebed1","resolution":{"observed_at":"2026-08-14T05:54:36.908537Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0611129","last_updated":"2006-11-09T20:29:52Z","snapshot_observed_at":"2026-08-03T16:02:44.815697Z","submitted_at":"2006-11-09T20:29:52Z","title":"Matching matrix elements and shower evolution for top-quark production in hadronic collisions","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0611129","snapshot_observed_at":"2026-08-14T05:54:36.912824Z","title":"Matching matrix elements and shower evolution for top-quark production in hadronic collisions,","venue":null,"work_id":null,"year":2007},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":86,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.912824Z"},"links":{"cited_paper":"/paper/hep-ph/0611129","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:1e54f458ccd4aa5e14ecb5b34cd4d97a0a9b45a95910362678d8c04d3e447dc0","observation_id":"27855966-87c9-4007-b536-e42507800008","resolution":{"observed_at":"2026-08-14T05:54:36.912824Z","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":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T05:54:36.916388Z","title":"Review of Particle Physics,","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":87,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.916388Z"},"links":{"citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:a72254ee5395af51b9dad5cac583d8e08ecaade27d801c9f6b66ae9c2fbde12e","observation_id":"102ce6ff-d430-460a-8a64-2220afeaac33","resolution":{"observed_at":"2026-08-14T05:54:36.916388Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1410.3012","last_updated":"2014-10-11T17:01:19Z","snapshot_observed_at":"2026-08-14T12:01:16.893295Z","submitted_at":"2014-10-11T17:01:19Z","title":"An Introduction to PYTHIA 8.2","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1410.3012","snapshot_observed_at":"2026-08-14T05:54:36.919783Z","title":"An Introduction to PYTHIA 8.2,","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":88,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.919783Z"},"links":{"cited_paper":"/paper/1410.3012","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:bf01cbc601e9ed6da478927691acac418686df6ad64416f9570fb3dac356bd71","observation_id":"20c21137-c1b6-4d33-87b5-17df27967ffa","resolution":{"observed_at":"2026-08-14T05:54:36.919783Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0710.3820","last_updated":"2007-10-20T06:46:11Z","snapshot_observed_at":"2026-08-12T13:28:29.305631Z","submitted_at":"2007-10-20T06:46:11Z","title":"A Brief Introduction to PYTHIA 8.1","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0710.3820","snapshot_observed_at":"2026-08-14T05:54:36.923638Z","title":"A Brief Introduction to PYTHIA 8.1,","venue":null,"work_id":null,"year":2008},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":89,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.923638Z"},"links":{"cited_paper":"/paper/0710.3820","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:9dc9f5fc1096625fe207bffbdeaf7b20c172db3566246baca0f787f68323536a","observation_id":"748d3a0f-57b7-4e30-b6d9-9c8eed5f5c9f","resolution":{"observed_at":"2026-08-14T05:54:36.923638Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1307.6346","last_updated":"2014-03-21T10:44:52Z","snapshot_observed_at":"2026-07-06T03:19:01.779441Z","submitted_at":"2013-07-24T09:28:24Z","title":"DELPHES 3, A modular framework for fast simulation of a generic collider experiment","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1307.6346","snapshot_observed_at":"2026-08-14T05:54:36.927562Z","title":"DELPHES 3, A modular frame- work for fast simulation of a generic collider experiment,","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":90,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.927562Z"},"links":{"cited_paper":"/paper/1307.6346","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:f984a9df51e6858dcbd72417fbcd6c20fcd4182c6609b5290f4b6c69b68dabea","observation_id":"c51cac41-985b-4e7d-b012-df676654f413","resolution":{"observed_at":"2026-08-14T05:54:36.927562Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1306.6329","last_updated":"2013-06-26T19:59:42Z","snapshot_observed_at":"2026-08-15T00:12:42.826196Z","submitted_at":"2013-06-26T19:59:42Z","title":"The International Linear Collider Technical Design Report - Volume 4: Detectors","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1306.6329","snapshot_observed_at":"2026-08-14T05:54:36.930852Z","title":"The International Linear Collider Technical Design Report - Volume 4: Detectors,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":91,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.930852Z"},"links":{"cited_paper":"/paper/1306.6329","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:3a01a5d00ccd48ea55e8e23e451099aaef888e911738190f879a24ce20c6cf04","observation_id":"d48007ae-37d0-4d7d-a378-01c9d043421d","resolution":{"observed_at":"2026-08-14T05:54:36.930852Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"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":"2026-08-14T05:54:36.934562Z","title":"The anti- kt jet clustering algorithm,","venue":null,"work_id":null,"year":2008},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":92,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.934562Z"},"links":{"cited_paper":"/paper/0802.1189","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:c8570a4a0ea955a3ece92af0e9032423756fb88382a60bd02c090acb74263a97","observation_id":"b5a9a1e0-c8cd-42b2-88d9-4d866ebd8750","resolution":{"observed_at":"2026-08-14T05:54:36.934562Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1111.6097","last_updated":"2011-11-25T20:37:47Z","snapshot_observed_at":"2026-08-15T00:01:17.738963Z","submitted_at":"2011-11-25T20:37:47Z","title":"FastJet user manual","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1111.6097","snapshot_observed_at":"2026-08-14T05:54:36.938307Z","title":"FastJet User Manual,","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":93,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.938307Z"},"links":{"cited_paper":"/paper/1111.6097","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:dcd45b9da707fa7f4c9311d37fe7e446ca58c998c3fc5bf0661371e78027c510","observation_id":"66430c0d-e493-44b6-b618-f4b827d0dd3f","resolution":{"observed_at":"2026-08-14T05:54:36.938307Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"physics/0703039","last_updated":"2009-07-07T20:15:27Z","snapshot_observed_at":"2026-08-10T10:24:20.107880Z","submitted_at":"2007-03-04T19:45:41Z","title":"TMVA - Toolkit for Multivariate Data Analysis","version":5},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"physics/0703039","snapshot_observed_at":"2026-08-14T05:54:36.941681Z","title":"TMVA - Toolkit for Multivariate Data Analysis,","venue":null,"work_id":null,"year":2007},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":94,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.941681Z"},"links":{"cited_paper":"/paper/physics/0703039","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:e28d989b0db32b2db20df2429b8a81b26de49f217c4c79ada4352e63492cc5f0","observation_id":"d54ecf68-2fa0-4492-8d15-725ec1d2c2b8","resolution":{"observed_at":"2026-08-14T05:54:36.941681Z","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":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T05:54:36.945637Z","title":"Current developments in TMVA: An outlook to TMVA4,","venue":null,"work_id":null,"year":2008},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":95,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.945637Z"},"links":{"citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:d20a74d3078eef4498700e43b2449bd5d6ecdb7e443b73d39212125dc50df793","observation_id":"4f856cce-87a0-485e-a030-852c282d52cc","resolution":{"observed_at":"2026-08-14T05:54:36.945637Z","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":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T05:54:36.949510Z","title":"TMVA: Toolkit for multivariate data analysis,","venue":null,"work_id":null,"year":2009},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":96,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.949510Z"},"links":{"citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:79add9d4160bb5ff501e1b841b487c45530d5aa8bed19561893a8b91411604df","observation_id":"140d5245-3028-4f70-97d8-ddc8454a6cde","resolution":{"observed_at":"2026-08-14T05:54:36.949510Z","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":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T05:54:36.952706Z","title":"The toolkit for multivariate data analysis, TMVA 4,","venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":97,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.952706Z"},"links":{"citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:45557c4e26bfe95c4de0eed19a42f7803f56602d723da843146fd5daec9c6d66","observation_id":"53bcf472-e99a-4865-8481-e60e79fb7c10","resolution":{"observed_at":"2026-08-14T05:54:36.952706Z","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":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T05:54:36.955789Z","title":"TMVA Toolkit for multivariate data analysis in ROOT,","venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":98,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.955789Z"},"links":{"citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:38cf85674966d9ec585a424a9057a835b8a68766d6e5e9db7059c9d5cf5e5b9a","observation_id":"64cb463b-4a9b-455f-b462-91f4bf3e06d3","resolution":{"observed_at":"2026-08-14T05:54:36.955789Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0703164","last_updated":"2007-06-19T21:22:14Z","snapshot_observed_at":"2026-07-07T04:14:06.742598Z","submitted_at":"2007-03-15T18:25:44Z","title":"The Strongly-Interacting Light Higgs","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0703164","snapshot_observed_at":"2026-08-14T05:54:36.959162Z","title":"The Strongly-Interacting Light Higgs,","venue":null,"work_id":null,"year":2007},"citing_paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","version":2},"reference_index":99,"source":"pdf_text","source_observed_at":"2026-08-14T05:54:36.959162Z"},"links":{"cited_paper":"/paper/hep-ph/0703164","citing_paper":"/paper/1909.00592"},"observation_digest":"sha256:798fb6b5a7abf6e8b0c8c426a0a6d2c4cc25d311c2230f7393608fc2690dd44b","observation_id":"eeaa5fd7-a67a-40e6-b88a-41ddc1076975","resolution":{"observed_at":"2026-08-14T05:54:36.959162Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"paper":{"arxiv_id":"1909.00592","last_updated":"2020-05-17T14:53:09Z","latest_version":2,"primary_category":"hep-ph","snapshot_observed_at":"2026-08-14T15:22:17.420568Z","submitted_at":"2019-09-02T08:23:09Z","title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders"},"reference_resolution":{"displayed":96,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":82,"verified_exact":14,"verified_fuzzy":0},"total_outbound_references":96},"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":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"thesis":"As of 15 August 2026, this Paper Citation Record lists 96 of 96 outbound references and 0 inbound Pith citation observations for arXiv:1909.00592."}