{"as_of":"2026-08-14T20:09:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:33d3f68c09bed9477392edf7dc0e7d0628621c60c889b591022e64e219f52b59","coverage":[{"denominator":245,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":100,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-14T04:24:09.674745Z","state":"measured"},{"denominator":100,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":100,"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/2608.10064/citation-record","integrity":"/paper/2608.10064/integrity","json":"/paper/2608.10064/citation-record.json","paper":"/paper/2608.10064"},"outbound":[{"citation":{"cited_paper":{"arxiv_id":"hep-ex/0509008","last_updated":"2006-02-27T21:07:09Z","snapshot_observed_at":"2026-08-07T03:48:30.361762Z","submitted_at":"2005-09-07T16:45:02Z","title":"Precision Electroweak Measurements on the Z Resonance","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ex/0509008","snapshot_observed_at":"2026-08-14T04:24:07.177149Z","title":"Schaelet al.(ALEPH, DELPHI, L3, OPAL, SLD, LEP Electroweak Working Group, SLD Electroweak Group, SLD Heavy Flavour Group), Phys","venue":null,"work_id":null,"year":2006},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:07.177149Z"},"links":{"cited_paper":"/paper/hep-ex/0509008","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:8ad299d5cc11bcd6d012880eae5b0acde2d1888a94edf093085ab487e96e4e57","observation_id":"1e95eb96-59d8-4ad0-91c4-93e622c8ba4b","resolution":{"observed_at":"2026-08-14T04:24:07.177149Z","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":"2026-08-14T04:24:07.198607Z","title":"Abadaet al.(FCC), Eur","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:07.198607Z"},"links":{"citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:e096bfbd48a6274ffa86eb799c60ad92de551e2ac8fac2bd328a1c1e7d67b28f","observation_id":"030344ce-8c63-474e-bc5b-c585505f61be","resolution":{"observed_at":"2026-08-14T04:24:07.198607Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1811.10545","last_updated":"2018-11-23T16:15:38Z","snapshot_observed_at":"2026-08-14T17:54:40.660786Z","submitted_at":"2018-11-23T16:15:38Z","title":"CEPC Conceptual Design Report: Volume 2 - Physics & Detector","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1811.10545","snapshot_observed_at":"2026-08-14T04:24:07.231891Z","title":"Donget al.(CEPC Study Group), (2018), arXiv:1811.10545 [hep-ex]","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:07.231891Z"},"links":{"cited_paper":"/paper/1811.10545","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:15a9606cdd700c7962815139e9078ebb213e417950e6e01da44453e36050b998","observation_id":"11d11f1c-7bbe-4dde-bde1-c9defb99a3a8","resolution":{"observed_at":"2026-08-14T04:24:07.231891Z","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":"2026-08-14T04:24:07.264643Z","title":"Buchmüller and D","venue":null,"work_id":null,"year":1986},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:07.264643Z"},"links":{"citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:de94bb2508399d8b2c8c354c5f3967be637bad5d3f7cd339750996219cf74f28","observation_id":"6261635a-4272-4c25-a0ed-28a29d4e8edb","resolution":{"observed_at":"2026-08-14T04:24:07.264643Z","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":"2026-08-14T04:24:07.292382Z","title":"Grzadkowski, M","venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:07.292382Z"},"links":{"cited_paper":"/paper/1008.4884","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:1bdf3e0e60fd29d3d95b8b2031fc272dcf8be1d63ca7855abbe6b71008d8e87b","observation_id":"9d8d6063-4e57-4d20-8905-5287e5f123b1","resolution":{"observed_at":"2026-08-14T04:24:07.292382Z","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":"2026-08-13T06:43:55.862289Z","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":"2026-08-14T04:24:07.309747Z","title":"Brivio and M","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:07.309747Z"},"links":{"cited_paper":"/paper/1706.08945","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:bce57ea52d4753c9a1dd91511625c35256ba6083f63c64e69f51ed89380a6b46","observation_id":"0c17c2d4-4fa2-4517-83e4-ece41911310b","resolution":{"observed_at":"2026-08-14T04:24:07.309747Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2303.16922","last_updated":"2023-10-04T08:29:30Z","snapshot_observed_at":"2026-08-13T12:13:50.609284Z","submitted_at":"2023-03-29T18:00:00Z","title":"The Standard Model effective field theory at work","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2303.16922","snapshot_observed_at":"2026-08-14T04:24:07.346613Z","title":"Isidori, F","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:07.346613Z"},"links":{"cited_paper":"/paper/2303.16922","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:e4bd56574d3f11a2f3086ae3093b93243a37db4ca96e9a02810c861cdc41ee09","observation_id":"94d2802d-ac1e-403c-9a42-7e6f942061f1","resolution":{"observed_at":"2026-08-14T04:24:07.346613Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1909.02000","last_updated":"2022-09-26T18:43:01Z","snapshot_observed_at":"2026-08-14T05:01:11.184693Z","submitted_at":"2019-09-04T18:00:00Z","title":"Electroweak and QCD Corrections to $Z$ and $W$ pole observables in the SMEFT","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1909.02000","snapshot_observed_at":"2026-08-14T04:24:07.385628Z","title":"Dawson and P","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:07.385628Z"},"links":{"cited_paper":"/paper/1909.02000","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:6ec59f4310b71e2f768f4b4240fa6d73c2134f3ae733b6e2baa5369f476f42ba","observation_id":"d1cdde95-081d-4449-a8e0-48e0823f1396","resolution":{"observed_at":"2026-08-14T04:24:07.385628Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2201.09887","last_updated":"2022-01-24T19:00:00Z","snapshot_observed_at":"2026-08-14T13:28:29.172627Z","submitted_at":"2022-01-24T19:00:00Z","title":"Flavorful Electroweak Precision Observables in the Standard Model Effective Field Theory","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2201.09887","snapshot_observed_at":"2026-08-14T04:24:07.417460Z","title":"Dawson and P","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:07.417460Z"},"links":{"cited_paper":"/paper/2201.09887","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:bc80a03ab8cffd84bd9a1dd93fbdf7ebfb24fe2f1a0fe0ccfb905b17bfed0b57","observation_id":"5621b6df-9d7e-4e02-a736-632dc5c28b4b","resolution":{"observed_at":"2026-08-14T04:24:07.417460Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2304.00029","last_updated":"2024-12-17T21:48:21Z","snapshot_observed_at":"2026-08-13T12:12:08.509532Z","submitted_at":"2023-03-31T18:00:01Z","title":"The Importance of Flavor in SMEFT Electroweak Precision Fits","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2304.00029","snapshot_observed_at":"2026-08-14T04:24:07.454748Z","title":"Bellafronte, S","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:07.454748Z"},"links":{"cited_paper":"/paper/2304.00029","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:b301dd86aa6cb7efe4cf54cd432318607814532e4731598c6ea1a6e0aa684e5d","observation_id":"fb61842d-71dc-461d-bb57-b910f870831f","resolution":{"observed_at":"2026-08-14T04:24:07.454748Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2503.07724","last_updated":"2025-03-10T18:00:03Z","snapshot_observed_at":"2026-08-07T17:15:51.394036Z","submitted_at":"2025-03-10T18:00:03Z","title":"Analytic results for electroweak precision observables at NLO in SMEFT","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2503.07724","snapshot_observed_at":"2026-08-14T04:24:07.486026Z","title":"Biekötter and B","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:07.486026Z"},"links":{"cited_paper":"/paper/2503.07724","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:69d7e3debf14c87157e4f9b7e91d4da9b177c68b5ef100f5046572b562a1bcec","observation_id":"5bd822c5-db50-4145-9476-ce4b5ba6fcf3","resolution":{"observed_at":"2026-08-14T04:24:07.486026Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2605.18679","last_updated":"2026-07-23T10:36:33Z","snapshot_observed_at":"2026-08-14T02:35:25.009504Z","submitted_at":"2026-05-18T17:21:26Z","title":"NLO EW and QCD dimension-6 SMEFT results for Higgs and gauge boson decays in POPxf format","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2605.18679","snapshot_observed_at":"2026-08-14T04:24:07.523034Z","title":"Bellafronte, S","venue":null,"work_id":null,"year":2026},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:07.523034Z"},"links":{"cited_paper":"/paper/2605.18679","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:8371acecaa6b34de48b7c640efea6fcf7d857292897e2905f3a3fc92ad5a5b06","observation_id":"6f345255-1fec-4600-9097-263cd3c81a66","resolution":{"observed_at":"2026-08-14T04:24:07.523034Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2305.03763","last_updated":"2023-05-05T18:00:20Z","snapshot_observed_at":"2026-08-13T11:48:21.564558Z","submitted_at":"2023-05-05T18:00:20Z","title":"Electroweak input schemes and universal corrections in SMEFT","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2305.03763","snapshot_observed_at":"2026-08-14T04:24:07.554751Z","title":"Biekötter, B","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:07.554751Z"},"links":{"cited_paper":"/paper/2305.03763","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:046daa154e1060c2736817aba91c6ae8391503ba633e5f47c5a433c112d3a878","observation_id":"e68b6c86-cfdf-485a-8ac9-a1efab2d00fe","resolution":{"observed_at":"2026-08-14T04:24:07.554751Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2312.08446","last_updated":"2023-12-13T19:00:02Z","snapshot_observed_at":"2026-08-13T05:03:00.496528Z","submitted_at":"2023-12-13T19:00:02Z","title":"Using the effective weak mixing angle as an input parameter in SMEFT","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2312.08446","snapshot_observed_at":"2026-08-14T04:24:07.597154Z","title":"Biekötter, B","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:07.597154Z"},"links":{"cited_paper":"/paper/2312.08446","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:de28edbf23ddf036a5087c46a70a8c771d046fc7615004a8ef21ca69ca4f0a28","observation_id":"c46f0738-f0c2-4e8c-87df-2b1580e453f2","resolution":{"observed_at":"2026-08-14T04:24:07.597154Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2410.13304","last_updated":"2025-01-15T06:16:37Z","snapshot_observed_at":"2026-08-12T22:21:12.617222Z","submitted_at":"2024-10-17T08:03:29Z","title":"Precision tests of third-generation four-quark operators: one- and two-loop matching","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2410.13304","snapshot_observed_at":"2026-08-14T04:24:07.619229Z","title":"Haisch and L","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:07.619229Z"},"links":{"cited_paper":"/paper/2410.13304","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:8aab85ccd5a9a53f625d5e3fb698226841412d7c859c18ce7eb405798458f032","observation_id":"412e43d4-036e-41a3-af86-5eceb286792c","resolution":{"observed_at":"2026-08-14T04:24:07.619229Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2507.01137","last_updated":"2026-07-04T15:31:04Z","snapshot_observed_at":"2026-08-12T15:20:36.642587Z","submitted_at":"2025-07-01T18:55:30Z","title":"Constraining four-heavy-quark operators with top-quark, Higgs, and electroweak precision data","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2507.01137","snapshot_observed_at":"2026-08-14T04:24:07.654745Z","title":"Di Noi, H","venue":null,"work_id":null,"year":2026},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:07.654745Z"},"links":{"cited_paper":"/paper/2507.01137","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:b3fc2636a0c4caf61501d9f8a0691a5530bfd9ebc6f23b5c03ad3a372b445765","observation_id":"204b6466-c3e5-401a-ada5-f71cb9b0f70c","resolution":{"observed_at":"2026-08-14T04:24:07.654745Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1308.2627","last_updated":"2020-07-15T12:41:06Z","snapshot_observed_at":"2026-08-07T19:35:43.779739Z","submitted_at":"2013-08-12T17:21:12Z","title":"Renormalization Group Evolution of the Standard Model Dimension Six Operators I: Formalism and lambda Dependence","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1308.2627","snapshot_observed_at":"2026-08-14T04:24:07.697160Z","title":null,"venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:07.697160Z"},"links":{"cited_paper":"/paper/1308.2627","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:2ecb377cf7d076b2814bfda86b4c6dd6e5fec22df594d55feaf54b8abb74e201","observation_id":"662badcc-6146-4580-bd79-c9f7dd60362c","resolution":{"observed_at":"2026-08-14T04:24:07.697160Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1310.4838","last_updated":"2020-07-15T12:41:18Z","snapshot_observed_at":"2026-08-06T19:18:12.176848Z","submitted_at":"2013-10-17T20:07:48Z","title":"Renormalization Group Evolution of the Standard Model Dimension Six Operators II: Yukawa Dependence","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1310.4838","snapshot_observed_at":"2026-08-14T04:24:07.725535Z","title":null,"venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:07.725535Z"},"links":{"cited_paper":"/paper/1310.4838","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:1534ff9c549f659d7fde667237c884d20508e1a1f6f23882575b206476c3fe00","observation_id":"ca9e2ff0-bb13-4857-b92f-a3036990c3f0","resolution":{"observed_at":"2026-08-14T04:24:07.725535Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1312.2014","last_updated":"2024-06-13T16:23:18Z","snapshot_observed_at":"2026-08-12T21:44:49.413147Z","submitted_at":"2013-12-06T21:09:00Z","title":"Renormalization Group Evolution of the Standard Model Dimension Six Operators III: Gauge Coupling Dependence and Phenomenology","version":5},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1312.2014","snapshot_observed_at":"2026-08-14T04:24:07.748065Z","title":"Alonso, E","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:07.748065Z"},"links":{"cited_paper":"/paper/1312.2014","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:6c21159a91d94d7f07a6f8f232bda85896f71a13e798cd2d192de3e0f6249638","observation_id":"8d8ea212-be45-4f04-b307-71df44fc12a1","resolution":{"observed_at":"2026-08-14T04:24:07.748065Z","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":"2026-08-14T04:24:07.774829Z","title":null,"venue":null,"work_id":null,"year":2026},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:07.774829Z"},"links":{"citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:d71cc222c56ed305c8cf31e4654d71aeccd1eea6f2e63d062031ce685753b909","observation_id":"d0beb0ac-8cfd-4ab5-8e15-847e48dcdf31","resolution":{"observed_at":"2026-08-14T04:24:07.774829Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1607.03773","last_updated":"2016-07-13T14:39:20Z","snapshot_observed_at":"2026-07-06T05:03:26.896392Z","submitted_at":"2016-07-13T14:39:20Z","title":"Indirect probes of the trilinear Higgs coupling: $gg \\to h$ and $h \\to \\gamma \\gamma$","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1607.03773","snapshot_observed_at":"2026-08-14T04:24:07.811935Z","title":"Gorbahn and U","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:07.811935Z"},"links":{"cited_paper":"/paper/1607.03773","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:c8b42c2fc9469e7b1c4d759389ae2bd5e1bde355e11d93c0302e8b5892263321","observation_id":"3a7b9833-5d54-4785-9f56-d2648567ccb4","resolution":{"observed_at":"2026-08-14T04:24:07.811935Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2005.12917","last_updated":"2020-05-26T18:00:00Z","snapshot_observed_at":"2026-08-11T16:59:44.008739Z","submitted_at":"2020-05-26T18:00:00Z","title":"Structure of two-loop SMEFT anomalous dimensions via on-shell methods","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2005.12917","snapshot_observed_at":"2026-08-14T04:24:07.827234Z","title":null,"venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:07.827234Z"},"links":{"cited_paper":"/paper/2005.12917","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:3e885607c02b04c0d168a013eef4b459299aee6ca6122452679e71485467397f","observation_id":"c31bea0d-632d-4c16-9205-8f02693d7a14","resolution":{"observed_at":"2026-08-14T04:24:07.827234Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2011.02494","last_updated":"2021-01-12T09:17:13Z","snapshot_observed_at":"2026-08-10T20:08:11.410917Z","submitted_at":"2020-11-04T19:00:04Z","title":"Two-Loop anomalous dimensions of QCD operators up to dimension-sixteen and Higgs EFT amplitudes","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2011.02494","snapshot_observed_at":"2026-08-14T04:24:07.847400Z","title":null,"venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:07.847400Z"},"links":{"cited_paper":"/paper/2011.02494","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:aa7805601314e630432c15b035087c42af778d01091f5c0d5f3ce017ddddd8db","observation_id":"76655bcf-59b4-4eca-81ae-8c36fcf79bf4","resolution":{"observed_at":"2026-08-14T04:24:07.847400Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2204.00663","last_updated":"2022-07-08T16:19:56Z","snapshot_observed_at":"2026-08-13T16:10:00.344327Z","submitted_at":"2022-04-01T19:01:47Z","title":"NNLO event generation for $\\boldsymbol{pp \\to Zh \\to \\ell^+\\ell^- b \\bar b}$ production in the SM effective field theory","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2204.00663","snapshot_observed_at":"2026-08-14T04:24:07.882848Z","title":"Haisch, D","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:07.882848Z"},"links":{"cited_paper":"/paper/2204.00663","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:71514446b5b40a604b60fdf311e410d113781b7fe9c8afd275af9697f7dbcb3c","observation_id":"fbc04b7a-7303-4a85-aceb-d9eeb364f1ec","resolution":{"observed_at":"2026-08-14T04:24:07.882848Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2310.18221","last_updated":"2024-03-25T15:04:48Z","snapshot_observed_at":"2026-08-14T11:17:46.966306Z","submitted_at":"2023-10-27T15:50:31Z","title":"On $\\gamma_5$ schemes and the interplay of SMEFT operators in the Higgs-gluon coupling","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2310.18221","snapshot_observed_at":"2026-08-14T04:24:07.904748Z","title":"Di Noi, R","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:07.904748Z"},"links":{"cited_paper":"/paper/2310.18221","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:cfb0083925de5308933ca4e45a41497e9f538e838c9a95dc910692e5221f24df","observation_id":"1586e3c3-da84-4ea7-80a0-49fe72fba9d8","resolution":{"observed_at":"2026-08-14T04:24:07.904748Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2310.19883","last_updated":"2023-11-09T19:25:02Z","snapshot_observed_at":"2026-08-13T05:37:16.560191Z","submitted_at":"2023-10-30T18:00:04Z","title":"Two Loop Renormalization of Scalar Theories using a Geometric Approach","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2310.19883","snapshot_observed_at":"2026-08-14T04:24:07.934866Z","title":null,"venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:07.934866Z"},"links":{"cited_paper":"/paper/2310.19883","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:88ed3cc9e424bc4510188b66b6c61b6f2f65073966cc7cbf391bf607a0e97a04","observation_id":"e722b933-b206-4473-9ede-82a72545e267","resolution":{"observed_at":"2026-08-14T04:24:07.934866Z","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":"2026-08-14T04:24:07.964749Z","title":"Di Noi, R","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:07.964749Z"},"links":{"citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:d4be346fcccb8236ac6ce5c321c5cfa104801f38b9fd731cbe92b831c8a6e857","observation_id":"06d45f4a-54de-4a48-9ce3-4dab50fe0f5d","resolution":{"observed_at":"2026-08-14T04:24:07.964749Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2410.07320","last_updated":"2025-04-08T16:12:15Z","snapshot_observed_at":"2026-08-12T22:26:56.989460Z","submitted_at":"2024-10-09T18:00:01Z","title":"Two-Loop Running in the Bosonic SMEFT Using Functional Methods","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2410.07320","snapshot_observed_at":"2026-08-14T04:24:07.998497Z","title":null,"venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:07.998497Z"},"links":{"cited_paper":"/paper/2410.07320","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:99d3f5332b9d4e6620264b3dcd6b4f4cbc2d608c9e4009b095dff9aa3765e6f2","observation_id":"ca3fcc1c-31a1-4f6d-8532-4d7520778a53","resolution":{"observed_at":"2026-08-14T04:24:07.998497Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2412.13251","last_updated":"2025-06-17T07:33:28Z","snapshot_observed_at":"2026-08-11T16:47:58.161827Z","submitted_at":"2024-12-17T19:00:00Z","title":"Renormalization-group equations of the LEFT at two loops: dimension-five effects","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2412.13251","snapshot_observed_at":"2026-08-14T04:24:08.019828Z","title":"Naterop and P","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":29,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:08.019828Z"},"links":{"cited_paper":"/paper/2412.13251","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:3ebb97c4aab6cdc06c33b6bb2166a5d408eddaeff57a785c2f10a2262c6a1f81","observation_id":"6aaa87f2-072a-44be-a2fc-fa512f76218d","resolution":{"observed_at":"2026-08-14T04:24:08.019828Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2503.01954","last_updated":"2025-03-03T19:00:00Z","snapshot_observed_at":"2026-08-08T13:53:29.441306Z","submitted_at":"2025-03-03T19:00:00Z","title":"Two-loop renormalisation of quark and gluon fields in the SMEFT","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2503.01954","snapshot_observed_at":"2026-08-14T04:24:08.052686Z","title":null,"venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:08.052686Z"},"links":{"cited_paper":"/paper/2503.01954","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:5e019bd508533a1837a6f54253d01c9c1794b890344489c50367eb03f4e1aa08","observation_id":"f13eeb44-604b-4071-979b-0bc11966ea7e","resolution":{"observed_at":"2026-08-14T04:24:08.052686Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2503.06249","last_updated":"2025-04-22T09:47:54Z","snapshot_observed_at":"2026-08-07T17:20:05.841639Z","submitted_at":"2025-03-08T15:17:01Z","title":"Higgs production from anomalous gluon dynamics","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2503.06249","snapshot_observed_at":"2026-08-14T04:24:08.084573Z","title":"Haisch, JHEP06, 004 (2025), arXiv:2503.06249 [hep-ph]","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:08.084573Z"},"links":{"cited_paper":"/paper/2503.06249","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:6ec8e90fd7d4c83f6c42b79be50e63c11126f3ee691d5dc0a30c1140d57b44ec","observation_id":"11f81836-325e-4003-8b47-5de8a0d12b85","resolution":{"observed_at":"2026-08-14T04:24:08.084573Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2504.00792","last_updated":"2025-05-05T20:30:03Z","snapshot_observed_at":"2026-08-07T16:17:26.098162Z","submitted_at":"2025-04-01T13:50:58Z","title":"Two-loop Renormalization Group Equations in the $\\nu$SMEFT","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2504.00792","snapshot_observed_at":"2026-08-14T04:24:08.104751Z","title":"Zhang, JHEP06, 106 (2025), arXiv:2504.00792 [hep-ph]","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":32,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:08.104751Z"},"links":{"cited_paper":"/paper/2504.00792","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:2b390bc107107a8c41ce58a966a0f2abddfb2440e6f73ef85e677709a0ed458a","observation_id":"b7b2fc7d-abfe-451b-b044-119776e780ad","resolution":{"observed_at":"2026-08-14T04:24:08.104751Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2504.18537","last_updated":"2025-04-25T17:59:58Z","snapshot_observed_at":"2026-08-14T18:26:30.651616Z","submitted_at":"2025-04-25T17:59:58Z","title":"Renormalizing Two-Fermion Operators in the SMEFT via Supergeometry","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2504.18537","snapshot_observed_at":"2026-08-14T04:24:08.133607Z","title":null,"venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:08.133607Z"},"links":{"cited_paper":"/paper/2504.18537","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:905a4a7590ff52ecdfd7299d2bb4297b1559616b0c3cb706f33af5781507c411","observation_id":"d4344eb4-58c9-4bd7-8f6a-77e49caecdf8","resolution":{"observed_at":"2026-08-14T04:24:08.133607Z","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":"2026-08-14T04:24:08.154738Z","title":"Naterop and P","venue":null,"work_id":null,"year":2026},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":34,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:08.154738Z"},"links":{"citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:4ffb103601ce06b14b8c7a9de135b82cf630c2b21d001d61e7020464eb598154","observation_id":"0e62a029-9116-4ffc-8aea-1598c9753645","resolution":{"observed_at":"2026-08-14T04:24:08.154738Z","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":"2026-08-14T04:24:08.176049Z","title":"Di Noi and R","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:08.176049Z"},"links":{"citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:9e97f751207b8e9f17bc618339b2e71755363174557aa324e0821b0ac3a4ee20","observation_id":"ba8a8adb-6ca8-4627-aa73-c9f07efd606b","resolution":{"observed_at":"2026-08-14T04:24:08.176049Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2507.20803","last_updated":"2025-07-28T13:10:23Z","snapshot_observed_at":"2026-08-09T10:29:52.423032Z","submitted_at":"2025-07-28T13:10:23Z","title":"Precision tests of third-generation four-quark operators: $gg \\to h$ and $h \\to \\gamma \\gamma$","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2507.20803","snapshot_observed_at":"2026-08-14T04:24:08.197988Z","title":"Haisch and M","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":36,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:08.197988Z"},"links":{"cited_paper":"/paper/2507.20803","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:ceddc38938f3bc0ab06e91fb5be81d2762b5b33ec7265f3cfa2740c8d034b781","observation_id":"85fdd9ce-2b3c-4373-8b1e-77344146a2ba","resolution":{"observed_at":"2026-08-14T04:24:08.197988Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2508.04500","last_updated":"2025-08-06T14:48:31Z","snapshot_observed_at":"2026-08-07T06:45:25.545568Z","submitted_at":"2025-08-06T14:48:31Z","title":"Two-loop renormalisation of quark and gluon fields in the SMEFT in the on-shell scheme","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2508.04500","snapshot_observed_at":"2026-08-14T04:24:08.222832Z","title":null,"venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":37,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:08.222832Z"},"links":{"cited_paper":"/paper/2508.04500","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:5a4559fccdc852d4db8f13ed27fbd47647f886a1691f8a6666648ba4ff4f58d5","observation_id":"3c7b6a00-d13a-49e2-93de-d07425c52e7f","resolution":{"observed_at":"2026-08-14T04:24:08.222832Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2510.14680","last_updated":"2026-06-18T09:44:58Z","snapshot_observed_at":"2026-08-06T07:48:59.939294Z","submitted_at":"2025-10-16T13:43:11Z","title":"Complete two-loop Yukawa-induced running of the Higgs-gluon coupling in SMEFT","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2510.14680","snapshot_observed_at":"2026-08-14T04:24:08.259306Z","title":"Di Noi, B","venue":null,"work_id":null,"year":2026},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":38,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:08.259306Z"},"links":{"cited_paper":"/paper/2510.14680","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:1b598290bc7bf71f7b185d712d0ba9edffa1a4601fb54a911faf9860826c8c0b","observation_id":"2115c176-73d9-4c7e-adfa-b8f9e7030da0","resolution":{"observed_at":"2026-08-14T04:24:08.259306Z","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":"2026-08-14T04:24:08.286160Z","title":"Banik, A","venue":null,"work_id":null,"year":2026},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":39,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:08.286160Z"},"links":{"citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:0c78f115ec49b8d338d55fe29a41e1c2bd4e4cc13a6b1f804ebb326f38dd80ec","observation_id":"e2da8620-87a9-4aef-b7cb-4833d9bed5e2","resolution":{"observed_at":"2026-08-14T04:24:08.286160Z","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":"2026-08-14T04:24:08.322614Z","title":"Henriksson, S","venue":null,"work_id":null,"year":2026},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":40,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:08.322614Z"},"links":{"citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:44cb8fc1f06f9ea0cad79800ab0923e9bf2c5fa82a06a43219dbe2945e989dcd","observation_id":"2cba3817-672d-4e42-a842-d79490419245","resolution":{"observed_at":"2026-08-14T04:24:08.322614Z","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":"2026-08-14T04:24:08.354746Z","title":"Chala and J","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":41,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:08.354746Z"},"links":{"citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:6a9197c58de7b80911626ad1184497451de99eb956c5aa8d5209e87a54d5eccb","observation_id":"1fb332d9-4cd3-4b70-953f-83c80fb2943c","resolution":{"observed_at":"2026-08-14T04:24:08.354746Z","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":"2026-08-14T04:24:08.385949Z","title":"Guedes and J","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":42,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:08.385949Z"},"links":{"citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:1af75935b9c65c467c7ec14555670925816cd71900b9dcf1eb90f0129c648f81","observation_id":"5d885b3a-189b-47e6-868a-b3092d4b29b3","resolution":{"observed_at":"2026-08-14T04:24:08.385949Z","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":"2026-08-14T04:24:08.405937Z","title":null,"venue":null,"work_id":null,"year":2026},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":43,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:08.405937Z"},"links":{"citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:4d40d468ac5848715bb5394dd21945d145a60c15139dbd185ff0ab7fd1e1982c","observation_id":"6fbc3b39-fc66-4be4-8022-abfe4df6c05c","resolution":{"observed_at":"2026-08-14T04:24:08.405937Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2604.16599","last_updated":"2026-04-17T18:00:01Z","snapshot_observed_at":"2026-08-03T01:26:09.520850Z","submitted_at":"2026-04-17T18:00:01Z","title":"The effect of the two-loop SMEFT RGEs at future colliders","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2604.16599","snapshot_observed_at":"2026-08-14T04:24:08.435510Z","title":"Mantani, P","venue":null,"work_id":null,"year":2026},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":44,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:08.435510Z"},"links":{"cited_paper":"/paper/2604.16599","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:f3d752518b7f375a8f9bae30c2fae989b53230a72009b23b67eb01526c13d9c8","observation_id":"d890f7e0-b308-4b7b-9da1-61ffe5540390","resolution":{"observed_at":"2026-08-14T04:24:08.435510Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2604.26817","last_updated":"2026-04-29T15:44:53Z","snapshot_observed_at":"2026-08-13T12:18:56.274740Z","submitted_at":"2026-04-29T15:44:53Z","title":"When Two Loops Matter: Electroweak Precision in the SMEFT","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2604.26817","snapshot_observed_at":"2026-08-14T04:24:08.479451Z","title":null,"venue":null,"work_id":null,"year":2026},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":45,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:08.479451Z"},"links":{"cited_paper":"/paper/2604.26817","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:641bd982e0ffb089b23afd84875b16cdaa263f701843a748dc9704a0f0eecfcc","observation_id":"5fe1e2ea-5284-4df3-b993-9be7cbb606ec","resolution":{"observed_at":"2026-08-14T04:24:08.479451Z","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":"2026-08-14T04:24:08.509171Z","title":"Greljo, A","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":46,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:08.509171Z"},"links":{"citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:4f77e19d7014f209179c69388c4589a046b44bb29f995fceebeffd4c5142b432","observation_id":"b02e1015-a5fb-4f42-a69d-88045e48e849","resolution":{"observed_at":"2026-08-14T04:24:08.509171Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2209.00666","last_updated":"2022-12-29T12:04:09Z","snapshot_observed_at":"2026-08-13T14:34:22.928912Z","submitted_at":"2022-09-01T18:00:12Z","title":"Charting the Higgs self-coupling boundaries","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2209.00666","snapshot_observed_at":"2026-08-14T04:24:08.555851Z","title":"Durieux, M","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":47,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:08.555851Z"},"links":{"cited_paper":"/paper/2209.00666","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:e9d3049b06fa5d1dc5b0ec71cd60248afe14d2f3f99306b2e01c5c8b137afe4b","observation_id":"e2de00ac-83ae-4aba-84ae-9d4c57ab87fd","resolution":{"observed_at":"2026-08-14T04:24:08.555851Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2407.09593","last_updated":"2025-01-22T12:51:09Z","snapshot_observed_at":"2026-08-12T23:23:11.220624Z","submitted_at":"2024-07-12T18:00:00Z","title":"Non-universal probes of composite Higgs models: New bounds and prospects for FCC-ee","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2407.09593","snapshot_observed_at":"2026-08-14T04:24:08.581147Z","title":null,"venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":48,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:08.581147Z"},"links":{"cited_paper":"/paper/2407.09593","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:c7ec52d4c58a862b65dcf75f252368692c1c9b60a9344693a2d3cf9b036c5ccb","observation_id":"6aad6a89-02a6-4e33-805e-eaf307c73363","resolution":{"observed_at":"2026-08-14T04:24:08.581147Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2408.03992","last_updated":"2025-03-10T17:24:15Z","snapshot_observed_at":"2026-08-14T07:27:12.720039Z","submitted_at":"2024-08-07T18:00:01Z","title":"New Physics at Tera-$Z$: Precision Renormalised","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2408.03992","snapshot_observed_at":"2026-08-14T04:24:08.595691Z","title":"Allwicher, M","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":49,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:08.595691Z"},"links":{"cited_paper":"/paper/2408.03992","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:0435d06721724fdc2d478b766bae83cfc2c5a503497fbc0dbcf8be3879e4982e","observation_id":"c5700891-ffa8-4ae1-bd36-ab7bddedf30a","resolution":{"observed_at":"2026-08-14T04:24:08.595691Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2412.14241","last_updated":"2025-08-19T13:18:11Z","snapshot_observed_at":"2026-08-14T19:12:13.359327Z","submitted_at":"2024-12-18T19:00:01Z","title":"Accuracy complements energy: electroweak precision tests at Tera-Z","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2412.14241","snapshot_observed_at":"2026-08-14T04:24:08.634751Z","title":"Maura, B","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":50,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:08.634751Z"},"links":{"cited_paper":"/paper/2412.14241","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:bee74113dc645a60324915a5b701d0166c74e0c62b1742fcccdc9a23443ea85a","observation_id":"50a99683-bb76-4ac5-9733-43e8e50eef4d","resolution":{"observed_at":"2026-08-14T04:24:08.634751Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2503.13719","last_updated":"2025-04-16T14:24:40Z","snapshot_observed_at":"2026-08-07T16:56:34.772238Z","submitted_at":"2025-03-17T20:56:57Z","title":"The Higgs Self-Coupling at FCC-ee","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2503.13719","snapshot_observed_at":"2026-08-14T04:24:08.654766Z","title":"Maura, B","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":51,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:08.654766Z"},"links":{"cited_paper":"/paper/2503.13719","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:c3c733391b5dcb694478806ea510c105ae0f1681ccb25df15246015d445f2550","observation_id":"73c0af1e-c377-4d05-b833-7d5f2ff6044b","resolution":{"observed_at":"2026-08-14T04:24:08.654766Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2504.05974","last_updated":"2025-07-21T12:34:04Z","snapshot_observed_at":"2026-08-11T18:39:52.527372Z","submitted_at":"2025-04-08T12:30:44Z","title":"Higgs trilinear coupling in the standard model effective field theory at the high luminosity LHC and the FCC-ee","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2504.05974","snapshot_observed_at":"2026-08-14T04:24:08.681418Z","title":"ter Hoeve, L","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":52,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:08.681418Z"},"links":{"cited_paper":"/paper/2504.05974","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:9b7f6057ae228f10c41ebe1eea77c90c522d57849e7b55bf8cce941d81e61c18","observation_id":"01bb9aa4-fb41-4dc8-ac97-9a63f3cc2e73","resolution":{"observed_at":"2026-08-14T04:24:08.681418Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2601.13248","last_updated":"2026-05-15T13:04:42Z","snapshot_observed_at":"2026-08-05T10:25:25.231211Z","submitted_at":"2026-01-19T17:35:29Z","title":"Constraining the Higgs potential using multi-Higgs production","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2601.13248","snapshot_observed_at":"2026-08-14T04:24:08.695924Z","title":"Dinget al., (2026), 10.21468/SciPostPhysCommRep.24, arXiv:2601.13248 [hep-ph]","venue":null,"work_id":null,"year":2026},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":53,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:08.695924Z"},"links":{"cited_paper":"/paper/2601.13248","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:03b7c7dcc7a665ef0fd0ad49d837b16953947803309b1ba6ceb53e21139479ae","observation_id":"a8183b18-fa59-4bca-8847-91a234ac3a05","resolution":{"observed_at":"2026-08-14T04:24:08.695924Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1201.6670","last_updated":"2012-06-21T01:25:55Z","snapshot_observed_at":"2026-07-06T02:42:05.078758Z","submitted_at":"2012-01-31T20:21:16Z","title":"Constraints on Non-standard Top Quark Couplings","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1201.6670","snapshot_observed_at":"2026-08-14T04:24:08.724747Z","title":"Zhang, N","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":54,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:08.724747Z"},"links":{"cited_paper":"/paper/1201.6670","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:c438fc09235f99ac22eddc22b0b1cb570f8e43e6116773a015f6ecabb0f20a8a","observation_id":"2f4868ca-c0e3-4d47-9cca-f6c22978dcb7","resolution":{"observed_at":"2026-08-14T04:24:08.724747Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1408.0792","last_updated":"2015-03-01T06:50:54Z","snapshot_observed_at":"2026-07-06T03:50:53.543616Z","submitted_at":"2014-08-04T20:00:00Z","title":"Probing anomalous $t\\bar t Z$ interactions with rare meson decays","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1408.0792","snapshot_observed_at":"2026-08-14T04:24:08.755216Z","title":null,"venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":55,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:08.755216Z"},"links":{"cited_paper":"/paper/1408.0792","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:eda944c03e7698c48d5ca8b09d63598abe826bf95f148acb4315fc89c8e2a466","observation_id":"95fdbd50-6f83-4642-824e-3cf0ca9d77db","resolution":{"observed_at":"2026-08-14T04:24:08.755216Z","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":"2026-07-06T03:40:17.732584Z","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":"2026-08-14T04:24:08.784976Z","title":"Röntsch and M","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":56,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:08.784976Z"},"links":{"cited_paper":"/paper/1404.1005","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:42f85a7ec1acb0b8030f436fdee50ed2315c727426585d88d3bd8fdb24f9cab5","observation_id":"9ccb28b7-a9aa-4161-8747-0bf709a5f9c2","resolution":{"observed_at":"2026-08-14T04:24:08.784976Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1510.01131","last_updated":"2016-02-08T14:35:39Z","snapshot_observed_at":"2026-08-06T17:49:41.141811Z","submitted_at":"2015-10-05T12:47:16Z","title":"Observation of top quark pairs produced in association with a vector boson in pp collisions at sqrt(s) = 8 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1510.01131","snapshot_observed_at":"2026-08-14T04:24:08.807450Z","title":"Khachatryanet al.(CMS), JHEP01, 096 (2016), arXiv:1510.01131 [hep-ex]","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":57,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:08.807450Z"},"links":{"cited_paper":"/paper/1510.01131","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:12f9935d1d489fc06062e15f900202da2307b05731f698e65a2a9b40aebedba3","observation_id":"e4299389-4a3d-46b5-99bd-e92cf58dc6bb","resolution":{"observed_at":"2026-08-14T04:24:08.807450Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1601.08193","last_updated":"2016-01-29T16:54:31Z","snapshot_observed_at":"2026-08-06T22:24:21.675084Z","submitted_at":"2016-01-29T16:54:31Z","title":"Probing top quark neutral couplings in the Standard Model Effective Field Theory at NLO QCD","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1601.08193","snapshot_observed_at":"2026-08-14T04:24:08.824998Z","title":"Bessidskaia Bylund, F","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":58,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:08.824998Z"},"links":{"cited_paper":"/paper/1601.08193","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:3a5349be6ff050e07e5280bdfdf4480035f2aa2b702f6f7743aede1550a0cee1","observation_id":"1f432cb3-f7c2-407c-909c-1c063dce773c","resolution":{"observed_at":"2026-08-14T04:24:08.824998Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1804.07773","last_updated":"2018-04-20T18:00:16Z","snapshot_observed_at":"2026-08-14T19:23:43.494538Z","submitted_at":"2018-04-20T18:00:16Z","title":"Single-top associated production with a $Z$ or $H$ boson at the LHC: the SMEFT interpretation","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1804.07773","snapshot_observed_at":"2026-08-14T04:24:08.864542Z","title":"Degrande, F","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":59,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:08.864542Z"},"links":{"cited_paper":"/paper/1804.07773","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:b4ea3f4037dd46ee6f18e201920f79b961728f1f6012a6aacfd9394f465c4eb6","observation_id":"5df44767-0868-4ecd-9871-819d4303efba","resolution":{"observed_at":"2026-08-14T04:24:08.864542Z","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":"2026-08-14T04:24:08.883841Z","title":null,"venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":60,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:08.883841Z"},"links":{"cited_paper":"/paper/1907.11270","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:a718aa1242e0cfb901ab8e4dfb8e0413dc457d84d48fa3283fdc60b041f75be2","observation_id":"883d4128-d824-4e0a-a2f5-18efbc865c02","resolution":{"observed_at":"2026-08-14T04:24:08.883841Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2106.09690","last_updated":"2021-09-16T07:08:34Z","snapshot_observed_at":"2026-08-09T23:47:47.854886Z","submitted_at":"2021-06-17T17:45:22Z","title":"Observing $t\\bar{t}Z$ spin correlations at the LHC","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2106.09690","snapshot_observed_at":"2026-08-14T04:24:08.934751Z","title":"Ravina, E","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":61,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:08.934751Z"},"links":{"cited_paper":"/paper/2106.09690","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:9a9259818a6ba108afe696dda7a4a70a9410730d8f297e669634db3d38ec50da","observation_id":"1f13b033-63ae-4b34-b244-2d1819ce3468","resolution":{"observed_at":"2026-08-14T04:24:08.934751Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2111.03080","last_updated":"2022-02-14T20:07:03Z","snapshot_observed_at":"2026-08-04T20:21:45.246370Z","submitted_at":"2021-11-04T18:00:04Z","title":"Single top production in association with a $WZ$ pair at the LHC in the SMEFT","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2111.03080","snapshot_observed_at":"2026-08-14T04:24:08.955512Z","title":null,"venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":62,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:08.955512Z"},"links":{"cited_paper":"/paper/2111.03080","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:75172e4b7af58277894a0b98d5127db3677343d8a9c2a280b432040cc5e0a4f2","observation_id":"04ab9f1c-cbae-4896-a252-868bf75bf3f9","resolution":{"observed_at":"2026-08-14T04:24:08.955512Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2208.05986","last_updated":"2023-10-31T21:49:57Z","snapshot_observed_at":"2026-08-13T14:47:00.315962Z","submitted_at":"2022-08-11T18:00:06Z","title":"Boosting New Physics Searches in $t\\bar{t}Z$ and $tZj$ Production with Angular Moments","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2208.05986","snapshot_observed_at":"2026-08-14T04:24:08.963067Z","title":"Mammen Abraham and D","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":63,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:08.963067Z"},"links":{"cited_paper":"/paper/2208.05986","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:4cce540c7ccbc552a7343750b7ca8a1816b3f054d9de84aeb7b32a10a5148ce6","observation_id":"dff6f8a6-9b48-4b83-890a-cfdc7a13118c","resolution":{"observed_at":"2026-08-14T04:24:08.963067Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2504.05919","last_updated":"2026-07-13T13:34:49Z","snapshot_observed_at":"2026-08-07T16:07:34.415351Z","submitted_at":"2025-04-08T11:18:22Z","title":"Measurement of high-mass $t\\bar{t}\\ell^{+}\\ell^{-}$ production and lepton flavour universality-inspired effective field theory interpretations at $\\sqrt{s}=13$ TeV with the ATLAS detector","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2504.05919","snapshot_observed_at":"2026-08-14T04:24:09.024750Z","title":"Aadet al.(ATLAS), Eur","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":64,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:09.024750Z"},"links":{"cited_paper":"/paper/2504.05919","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:8ecea2adbd7ad4f42c82ebfecb9ca27b7f9c129a1366cb27da549cc912162d34","observation_id":"e45314bd-aa23-4bd9-8dd8-4cf438d55818","resolution":{"observed_at":"2026-08-14T04:24:09.024750Z","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":"2026-08-14T04:24:09.045537Z","title":"Cornet-Gomez, V","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":65,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:09.045537Z"},"links":{"citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:f45fd04cbc0651fce1a25b6352dcfca17e0c11b078aeea61609303921761e0ab","observation_id":"63ee708c-4759-4c3f-905f-5a704671f1d2","resolution":{"observed_at":"2026-08-14T04:24:09.045537Z","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":"2026-08-14T04:24:09.067894Z","title":"Durieux, A","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":66,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:09.067894Z"},"links":{"cited_paper":"/paper/1907.10619","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:93bb14f0e150b189f51b9c62c543c48ee9a887f61a4d83bb134c551a902de6a4","observation_id":"5cb69c3b-f332-4223-b910-ad9cb94f956c","resolution":{"observed_at":"2026-08-14T04:24:09.067894Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2003.05432","last_updated":"2021-01-04T16:07:12Z","snapshot_observed_at":"2026-08-14T00:18:59.505783Z","submitted_at":"2020-03-11T17:48:14Z","title":"The impact of flavour data on global fits of the MFV SMEFT","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2003.05432","snapshot_observed_at":"2026-08-14T04:24:09.081474Z","title":"Aoude, T","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":67,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:09.081474Z"},"links":{"cited_paper":"/paper/2003.05432","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:7bb4b43509787d2e223e90baf512083f84b79874bba97b1cbcc4984a294a879b","observation_id":"afe03f4f-559a-466a-b3c8-eea8953c6a5f","resolution":{"observed_at":"2026-08-14T04:24:09.081474Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2012.10456","last_updated":"2021-05-25T17:55:17Z","snapshot_observed_at":"2026-08-11T20:45:58.568940Z","submitted_at":"2020-12-18T19:00:02Z","title":"Top and Beauty synergies in SMEFT-fits at present and future colliders","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2012.10456","snapshot_observed_at":"2026-08-14T04:24:09.091685Z","title":"Bißmann, C","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":68,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:09.091685Z"},"links":{"cited_paper":"/paper/2012.10456","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:064e3b28a42da95b56c825f3558a91c77a536f82754032164bdff0ceba8ce870","observation_id":"0f31e32e-6e2a-4c08-8870-b448ad2ed2da","resolution":{"observed_at":"2026-08-14T04:24:09.091685Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2212.02532","last_updated":"2022-12-05T19:00:09Z","snapshot_observed_at":"2026-08-13T13:27:53.079709Z","submitted_at":"2022-12-05T19:00:09Z","title":"Resolving the Flavor Structure in the MFV-SMEFT","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2212.02532","snapshot_observed_at":"2026-08-14T04:24:09.124942Z","title":"Bruggisser, D","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":69,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:09.124942Z"},"links":{"cited_paper":"/paper/2212.02532","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:5366a896226e24968b25de8b6bbcfaa7d11ff3086529e09277059bac4ef8f762","observation_id":"44051997-9290-4ab5-adcf-2084939456da","resolution":{"observed_at":"2026-08-14T04:24:09.124942Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2304.12837","last_updated":"2023-11-23T10:56:37Z","snapshot_observed_at":"2026-08-13T11:55:27.643713Z","submitted_at":"2023-04-25T14:10:14Z","title":"More Synergies from Beauty, Top, $Z$ and Drell-Yan Measurements in SMEFT","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2304.12837","snapshot_observed_at":"2026-08-14T04:24:09.144846Z","title":"Grunwald, G","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":70,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:09.144846Z"},"links":{"cited_paper":"/paper/2304.12837","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:f1ac6f6c570a3b5dfcad0b3c72d4d8ac13647e12142ab6070f617b0946c79a7f","observation_id":"3275ce54-afc5-4679-af50-62e6cb70defe","resolution":{"observed_at":"2026-08-14T04:24:09.144846Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2310.00047","last_updated":"2024-02-18T17:34:12Z","snapshot_observed_at":"2026-08-14T13:40:51.046843Z","submitted_at":"2023-09-29T18:00:02Z","title":"Indirect constraints on top quark operators from a global SMEFT analysis","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2310.00047","snapshot_observed_at":"2026-08-14T04:24:09.164870Z","title":"Garosi, D","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":71,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:09.164870Z"},"links":{"cited_paper":"/paper/2310.00047","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:a73a06fa809469ed724a401ba0132ce99ba66d295e3fb085abddd78120efae74","observation_id":"fe45e591-d16a-4802-8f00-77efb27f90c5","resolution":{"observed_at":"2026-08-14T04:24:09.164870Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2302.11584","last_updated":"2025-08-07T16:14:42Z","snapshot_observed_at":"2026-08-13T12:39:18.993793Z","submitted_at":"2023-02-22T19:00:01Z","title":"Third-Family Quark-Lepton Unification and Electroweak Precision Tests","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2302.11584","snapshot_observed_at":"2026-08-14T04:24:09.191628Z","title":"Allwicher, G","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":72,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:09.191628Z"},"links":{"cited_paper":"/paper/2302.11584","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:431c2ce5bd5c40dad5f402557a843164c84af9d6345ef462699efd47100dbaec","observation_id":"a8b79c6f-f21a-4891-b349-f7de5839b9ad","resolution":{"observed_at":"2026-08-14T04:24:09.191628Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2311.00020","last_updated":"2023-12-04T10:54:25Z","snapshot_observed_at":"2026-08-13T05:35:31.255426Z","submitted_at":"2023-10-31T18:00:00Z","title":"New Physics in the Third Generation: A Comprehensive SMEFT Analysis and Future Prospects","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2311.00020","snapshot_observed_at":"2026-08-14T04:24:09.203544Z","title":"Allwicher, C","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":73,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:09.203544Z"},"links":{"cited_paper":"/paper/2311.00020","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:0d15b185b66298e51ee5419a8145246f495bef77b9f87fa8f34e1c28572af95c","observation_id":"efeac996-8d5c-4e61-b57a-2c6db3ffe28c","resolution":{"observed_at":"2026-08-14T04:24:09.203544Z","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":"2026-08-14T04:24:09.219110Z","title":"Haisch, J","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":74,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:09.219110Z"},"links":{"citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:479b4e6cd2c0b60082766e27fe35340e119987d7bdfc2679a1d4f66fd5d1e54d","observation_id":"80700727-4b83-4960-8670-c93fbf297c4d","resolution":{"observed_at":"2026-08-14T04:24:09.219110Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1805.00302","last_updated":"2018-08-11T21:00:21Z","snapshot_observed_at":"2026-08-14T19:20:06.161867Z","submitted_at":"2018-05-01T13:01:24Z","title":"The decay $h\\to \\gamma\\gamma$ in the Standard-Model Effective Field Theory","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1805.00302","snapshot_observed_at":"2026-08-14T04:24:09.229962Z","title":"Dedes, M","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":75,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:09.229962Z"},"links":{"cited_paper":"/paper/1805.00302","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:f924189887910acf25ea126f582b1ea4ddea2368c6af8db7f52d1100c0f35a3c","observation_id":"ecf48aeb-f38a-4930-83eb-862b4a64f714","resolution":{"observed_at":"2026-08-14T04:24:09.229962Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2012.02779","last_updated":"2021-04-08T15:54:25Z","snapshot_observed_at":"2026-08-14T00:04:25.364756Z","submitted_at":"2020-12-04T18:56:23Z","title":"Top, Higgs, Diboson and Electroweak Fit to the Standard Model Effective Field Theory","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2012.02779","snapshot_observed_at":"2026-08-14T04:24:09.233642Z","title":"Ellis, M","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":76,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:09.233642Z"},"links":{"cited_paper":"/paper/2012.02779","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:48b5397e546be1201b8a23496e281a84a36ac838de82d49be540d70b94b5a5d6","observation_id":"7fe4d075-e132-41a8-8778-df681a2df2c9","resolution":{"observed_at":"2026-08-14T04:24:09.233642Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2006.15458","last_updated":"2021-04-07T14:59:59Z","snapshot_observed_at":"2026-07-06T09:33:19.997750Z","submitted_at":"2020-06-27T22:08:24Z","title":"Differential cross-section measurements for the electroweak production of dijets in association with a $Z$ boson in proton-proton collisions at ATLAS","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2006.15458","snapshot_observed_at":"2026-08-14T04:24:09.264779Z","title":"Aadet al.(ATLAS), Eur","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":77,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:09.264779Z"},"links":{"cited_paper":"/paper/2006.15458","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:3c08e01cd7c3a28de6dd4d15b706405c96d31eedb8bca1d763533b90e7dddd89","observation_id":"d32ce4b8-811a-4ac6-880c-7933b906ab1a","resolution":{"observed_at":"2026-08-14T04:24:09.264779Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2101.03180","last_updated":"2021-02-11T19:51:55Z","snapshot_observed_at":"2026-08-13T06:03:01.930031Z","submitted_at":"2021-01-08T19:00:20Z","title":"SMEFT analysis of vector boson scattering and diboson data from the LHC Run II","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2101.03180","snapshot_observed_at":"2026-08-14T04:24:09.271846Z","title":null,"venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":78,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:09.271846Z"},"links":{"cited_paper":"/paper/2101.03180","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:b89cdd8d23172b525dc701d1858226d6e5e22091632d6f60a4cccd55f0a750ee","observation_id":"5847b5f8-f3e7-4fe9-865a-da1b844c395f","resolution":{"observed_at":"2026-08-14T04:24:09.271846Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2111.13948","last_updated":"2022-03-10T15:34:51Z","snapshot_observed_at":"2026-08-13T17:26:54.951662Z","submitted_at":"2021-11-27T17:24:28Z","title":"Measurement of W$^\\pm\\gamma$ differential cross sections in proton-proton collisions at $\\sqrt{s}$ = 13 TeV and effective field theory constraints","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2111.13948","snapshot_observed_at":"2026-08-14T04:24:09.277416Z","title":"Tumasyanet al.(CMS), Phys","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":79,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:09.277416Z"},"links":{"cited_paper":"/paper/2111.13948","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:44371f1dd65b26c11dd22046970189f675a14190925b03576804fbdb65139d97","observation_id":"2b45f792-7a8f-49df-8af4-5f0b22fa1482","resolution":{"observed_at":"2026-08-14T04:24:09.277416Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2404.12809","last_updated":"2024-10-28T10:02:33Z","snapshot_observed_at":"2026-08-14T13:28:30.866501Z","submitted_at":"2024-04-19T11:43:33Z","title":"Mapping the SMEFT at High-Energy Colliders: from LEP and the (HL-)LHC to the FCC-ee","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2404.12809","snapshot_observed_at":"2026-08-14T04:24:09.282429Z","title":"Celada, T","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":80,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:09.282429Z"},"links":{"cited_paper":"/paper/2404.12809","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:035f29c434b198ff34bccd8d0d1b5f2d6fb790a4224f4eb39959b8c2f8db9976","observation_id":"7ef12b06-2ea7-4dd5-95e4-8603d2b301aa","resolution":{"observed_at":"2026-08-14T04:24:09.282429Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2307.15761","last_updated":"2024-01-03T18:13:47Z","snapshot_observed_at":"2026-08-13T10:45:13.800651Z","submitted_at":"2023-07-28T18:41:08Z","title":"Search for physics beyond the standard model in top quark production with additional leptons in the context of effective field theory","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2307.15761","snapshot_observed_at":"2026-08-14T04:24:09.294184Z","title":"Hayrapetyanet al.(CMS), JHEP12, 068 (2023), arXiv:2307.15761 [hep-ex]","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":81,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:09.294184Z"},"links":{"cited_paper":"/paper/2307.15761","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:70344afc220baae75700c05f51bb3282294d8fcffa75f5e3c8e494787f39a581","observation_id":"8a6bce05-1691-4480-ba53-e2cfedaa52ad","resolution":{"observed_at":"2026-08-14T04:24:09.294184Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2207.10714","last_updated":"2023-03-17T09:37:05Z","snapshot_observed_at":"2026-08-13T14:59:13.004777Z","submitted_at":"2022-07-21T19:06:31Z","title":"Drell-Yan Tails Beyond the Standard Model","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2207.10714","snapshot_observed_at":"2026-08-14T04:24:09.309023Z","title":"Allwicher, D","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":82,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:09.309023Z"},"links":{"cited_paper":"/paper/2207.10714","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:d130f1ee04be820bc997547898b74d4951655e7ba6a1a4101764ed7802ac2e62","observation_id":"0449ec84-8f7e-4c40-8659-254e05007e8e","resolution":{"observed_at":"2026-08-14T04:24:09.309023Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1507.00757","last_updated":"2015-11-16T21:16:10Z","snapshot_observed_at":"2026-07-06T04:22:44.355065Z","submitted_at":"2015-07-02T20:36:22Z","title":"Renormalization Group Constraints on New Top Interactions from Electroweak Precision Data","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1507.00757","snapshot_observed_at":"2026-08-14T04:24:09.344943Z","title":"de Blas, M","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":83,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:09.344943Z"},"links":{"cited_paper":"/paper/1507.00757","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:4bebe9dd97b7472bc532708c1b53d8d86f6c1fc68997f6bd0690f2ca21adbc46","observation_id":"8ce15d1a-cb32-4454-9cb1-0d83c0469c73","resolution":{"observed_at":"2026-08-14T04:24:09.344943Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2411.02485","last_updated":"2024-11-15T09:11:39Z","snapshot_observed_at":"2026-08-12T22:07:56.790476Z","submitted_at":"2024-11-04T19:00:00Z","title":"New Physics Through Flavor Tagging at FCC-ee","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2411.02485","snapshot_observed_at":"2026-08-14T04:24:09.353739Z","title":"Greljo, H","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":84,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:09.353739Z"},"links":{"cited_paper":"/paper/2411.02485","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:3697fe388f4ccb3c6cb295fc1a317e63f158d3af228ca1c352a1f3f67ccd3406","observation_id":"50d6fd75-539e-422a-b784-faca6e700753","resolution":{"observed_at":"2026-08-14T04:24:09.353739Z","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":"2026-08-14T04:24:09.371452Z","title":"Jiang, Y","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":85,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:09.371452Z"},"links":{"citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:109f645257600107f0d171be619195de1751c7a715147768b41612cc8cf6d0a8","observation_id":"49b244ff-3710-4a9b-a537-3aa3fb3a34f1","resolution":{"observed_at":"2026-08-14T04:24:09.371452Z","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":"2026-08-14T04:24:09.389891Z","title":"Cao and F","venue":null,"work_id":null,"year":2026},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":86,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:09.389891Z"},"links":{"citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:22b6ba59fb52ba65235516bfddc96bfc58ac0164a2c20dc0764503506123ec3d","observation_id":"095061aa-d577-45e1-b2cb-9c285546e590","resolution":{"observed_at":"2026-08-14T04:24:09.389891Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2512.06916","last_updated":"2026-07-27T14:44:48Z","snapshot_observed_at":"2026-08-14T07:44:57.750865Z","submitted_at":"2025-12-07T16:51:58Z","title":"Could electron-top interactions spoil the measurement of the Higgs trilinear? -A quantitative estimate at future lepton colliders-","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2512.06916","snapshot_observed_at":"2026-08-14T04:24:09.401363Z","title":"Allwicher, C","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":87,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:09.401363Z"},"links":{"cited_paper":"/paper/2512.06916","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:24ac17236bce913365f2c3280c0b8df0df0a2380b981939dfe4efbfc15bd9ac1","observation_id":"76c5eba7-c6ef-42b9-b13e-5684f9ba680e","resolution":{"observed_at":"2026-08-14T04:24:09.401363Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2503.17019","last_updated":"2025-03-21T10:27:18Z","snapshot_observed_at":"2026-08-07T16:46:58.618501Z","submitted_at":"2025-03-21T10:27:18Z","title":"Flavored Circular Collider: cornering New Physics at FCC-ee via flavor-changing processes","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2503.17019","snapshot_observed_at":"2026-08-14T04:24:09.424573Z","title":"Allwicher, G","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":88,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:09.424573Z"},"links":{"cited_paper":"/paper/2503.17019","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:d895232e688f8590e38ca288e5d3179f5cda4cad17d13c2f54b00caaa1e381ae","observation_id":"567d36bd-c571-4594-9bb2-0332c3f6bb46","resolution":{"observed_at":"2026-08-14T04:24:09.424573Z","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":"2026-08-14T04:24:09.437409Z","title":"Bellafronte, S","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":89,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:09.437409Z"},"links":{"citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:383465bb561f02001515b16a07941fc80c10d1c8a612d5925b4971b2644dbb88","observation_id":"77257b8a-a6bf-428e-9499-371129bfe603","resolution":{"observed_at":"2026-08-14T04:24:09.437409Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1603.08911","last_updated":"2016-07-20T21:24:14Z","snapshot_observed_at":"2026-08-14T14:31:59.937244Z","submitted_at":"2016-03-29T19:49:48Z","title":"Pinning down electroweak dipole operators of the top quark","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1603.08911","snapshot_observed_at":"2026-08-14T04:24:09.446415Z","title":"Schulze and Y","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":90,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:09.446415Z"},"links":{"cited_paper":"/paper/1603.08911","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:5b50497b5b9c8c5a5071a2b3084b9ca5a63ab6b13922c2e62234ebe827f48b1b","observation_id":"62879ff5-6186-49de-a4b5-601d72ef2406","resolution":{"observed_at":"2026-08-14T04:24:09.446415Z","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":"2026-08-14T04:24:09.450428Z","title":"Brivio, S","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":91,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:09.450428Z"},"links":{"cited_paper":"/paper/1910.03606","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:761bebf04cee3166a064e665fa10b027d9f883b61494e8629b2cb4207f05744b","observation_id":"72336a01-1829-4186-aebf-25eb40822814","resolution":{"observed_at":"2026-08-14T04:24:09.450428Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2105.00006","last_updated":"2021-10-31T16:08:27Z","snapshot_observed_at":"2026-08-13T19:30:27.970445Z","submitted_at":"2021-04-30T18:00:01Z","title":"Combined SMEFT interpretation of Higgs, diboson, and top quark data from the LHC","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2105.00006","snapshot_observed_at":"2026-08-14T04:24:09.455586Z","title":null,"venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":92,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:09.455586Z"},"links":{"cited_paper":"/paper/2105.00006","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:6096c6e7e54ffe6f87dfd320a3e1278990f32c78214f3bec40af5b7abf3b942f","observation_id":"16651b43-3660-42a9-9f1d-4d3bfbbd939b","resolution":{"observed_at":"2026-08-14T04:24:09.455586Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2208.04962","last_updated":"2022-10-26T09:18:30Z","snapshot_observed_at":"2026-08-13T14:48:08.686550Z","submitted_at":"2022-08-09T18:00:02Z","title":"Complete SMEFT predictions for four top quark production at hadron colliders","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2208.04962","snapshot_observed_at":"2026-08-14T04:24:09.459798Z","title":"Aoude, H","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":93,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:09.459798Z"},"links":{"cited_paper":"/paper/2208.04962","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:cacd6d57870d7e01ddc0a6bbc3d2de491ade894506f0a54e611aa99a3b77b50b","observation_id":"e6c4031d-58ac-4013-bad0-a5946a5f610e","resolution":{"observed_at":"2026-08-14T04:24:09.459798Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2512.02256","last_updated":"2026-05-05T21:16:26Z","snapshot_observed_at":"2026-08-14T01:02:40.482289Z","submitted_at":"2025-12-01T22:57:09Z","title":"Impact of Higgs-boson measurements on SMEFT fits","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2512.02256","snapshot_observed_at":"2026-08-14T04:24:09.463825Z","title":"de Blas, A","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":94,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:09.463825Z"},"links":{"cited_paper":"/paper/2512.02256","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:e60356cff00b0e244db484add05339e0fb177989bb19a844740ca083bc0e0489","observation_id":"0cb96b70-be6c-4f0c-9379-8b4a1545628f","resolution":{"observed_at":"2026-08-14T04:24:09.463825Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1104.3122","last_updated":"2011-05-26T17:47:43Z","snapshot_observed_at":"2026-07-06T02:26:24.616868Z","submitted_at":"2011-04-15T18:51:19Z","title":"Effective Field Theory for Nonstandard Top Quark Couplings","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1104.3122","snapshot_observed_at":"2026-08-14T04:24:09.486876Z","title":"Greiner, S","venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":95,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:09.486876Z"},"links":{"cited_paper":"/paper/1104.3122","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:dee1f2769579022b67c6ea3b47948cdf1621ca70c9aa8349b4b03f68aef87b67","observation_id":"f809de82-c6cd-48a4-acee-29a0d53923a9","resolution":{"observed_at":"2026-08-14T04:24:09.486876Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1505.02646","last_updated":"2017-07-11T12:19:45Z","snapshot_observed_at":"2026-08-14T08:09:12.005573Z","submitted_at":"2015-05-11T14:47:22Z","title":"On one-loop corrections in the standard model effective field theory; the $\\Gamma(h \\rightarrow \\gamma \\, \\gamma)$ case","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1505.02646","snapshot_observed_at":"2026-08-14T04:24:09.528536Z","title":"Hartmann and M","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":96,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:09.528536Z"},"links":{"cited_paper":"/paper/1505.02646","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:bdef6c4ca7dc82df50653c6edf4f52ae6bcb1f1039f7b96214ef1f4b553a1819","observation_id":"6a8c50ae-05cd-4b15-be75-e8f08849abb7","resolution":{"observed_at":"2026-08-14T04:24:09.528536Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1507.03568","last_updated":"2018-05-07T08:25:44Z","snapshot_observed_at":"2026-08-04T05:48:29.459336Z","submitted_at":"2015-07-13T19:47:17Z","title":"Higgs decay to two photons at one-loop in the SMEFT","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1507.03568","snapshot_observed_at":"2026-08-14T04:24:09.574753Z","title":"Hartmann and M","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":97,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:09.574753Z"},"links":{"cited_paper":"/paper/1507.03568","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:1d3b2ea24a25e9f262b5407d0c00da3c51eaf4c39f90495f64b5fab32a9eadb9","observation_id":"cc59ccde-9b50-4651-9dcd-63af1eb20f49","resolution":{"observed_at":"2026-08-14T04:24:09.574753Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1909.13632","last_updated":"2020-01-28T13:43:58Z","snapshot_observed_at":"2026-08-13T19:29:54.404751Z","submitted_at":"2019-09-30T12:37:45Z","title":"Constraining top-quark couplings combining top-quark and $\\boldsymbol{B}$ decay observables","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1909.13632","snapshot_observed_at":"2026-08-14T04:24:09.608610Z","title":"Bißmann, J","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":98,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:09.608610Z"},"links":{"cited_paper":"/paper/1909.13632","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:81a75e158b6cb947b08c912530f2126b0ccf5e3fb7b0e545b30bf31e504765d3","observation_id":"0c5a66d5-00bd-442a-bf3a-82e21882b5b1","resolution":{"observed_at":"2026-08-14T04:24:09.608610Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2101.07273","last_updated":"2021-01-18T19:00:01Z","snapshot_observed_at":"2026-08-14T03:37:52.091886Z","submitted_at":"2021-01-18T19:00:01Z","title":"The Flavor of UV Physics","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2101.07273","snapshot_observed_at":"2026-08-14T04:24:09.644865Z","title":"Bruggisser, R","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":99,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:09.644865Z"},"links":{"cited_paper":"/paper/2101.07273","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:5f91b2c160111202272a1ede23cc0c3dc48db6e5a008dd6b7096defe39ba30f2","observation_id":"0f3fcf3a-b097-49f8-a9e3-ad7f771f0e7b","resolution":{"observed_at":"2026-08-14T04:24:09.644865Z","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":"2026-08-14T04:24:09.674745Z","title":null,"venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":100,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:09.674745Z"},"links":{"cited_paper":"/paper/1901.05965","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:c9433e2bb58f6fe823dd91dee2261f3d0f7c0aad8b51d672882ef1d7aa5f06d7","observation_id":"5252700b-b5c5-4477-b812-507ad45095f7","resolution":{"observed_at":"2026-08-14T04:24:09.674745Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","latest_version":1,"primary_category":"hep-ph","snapshot_observed_at":"2026-08-14T19:11:01.480209Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT"},"reference_resolution":{"displayed":100,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":100,"verified_exact":0,"verified_fuzzy":0},"total_outbound_references":245},"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 14 August 2026, this Paper Citation Record lists 100 of 245 outbound references and 0 inbound Pith citation observations for arXiv:2608.10064."}