{"as_of":"2026-08-13T05:16:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:bbace54541d5a20f77e6d59cfcb853b3e4bf4c9c5d85a76ec084dbbb5d7f8926","coverage":[{"denominator":89,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":89,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-12T05:35:38.027810Z","state":"measured"},{"denominator":91,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":91,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-12T06:34:41.77262+00:00","state":"measured"},{"denominator":2,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":2,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-01T00:42:30.474467Z","state":"measured"},{"denominator":1,"lane":"external_citation_measurements","note":"A source-named dated measurement, never combined with another source.","records_observed":0,"source":"arxiv_reference","source_observed_at":"2026-05-17T04:21:31.065408Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"cited_work":{"arxiv_id":"2412.00355","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2412.00355","snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Song and X","venue":null,"work_id":"b126fad0-9d9a-4973-8a8c-08c2dc97965d","year":2025},"citing_paper":{"arxiv_id":"2511.23410","last_updated":"2026-04-29T09:34:34Z","snapshot_observed_at":"2026-07-06T22:37:16.933664Z","submitted_at":"2025-11-28T18:04:40Z","title":"The Art of Counting: a reappraisal of the HEFT expansion","version":2},"reference_index":67,"source":"pdf_text","source_observed_at":"2026-05-17T04:19:01.842577Z"},"links":{"cited_paper":"/paper/2412.00355","citing_paper":"/paper/2511.23410"},"observation_digest":"sha256:ec73da9c982311e403d4d7eec044035f3bae35fa927a96364d782f8f8dafe611","observation_id":"46483b29-7d08-4444-977e-576fca42241e","resolution":{"observed_at":"2026-05-17T04:21:31.067168Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-12T06:34:41.77262+00:00","source":"crossref"},{"observed_at":"2026-08-12T06:34:36.333875+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2412.00355","snapshot_observed_at":"2026-08-01T00:42:30.474467Z","title":"Song and X","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2607.26184","last_updated":"2026-08-04T09:02:54Z","snapshot_observed_at":"2026-08-07T23:09:38.347879Z","submitted_at":"2026-07-28T18:45:03Z","title":"A HEFT Perspective on the Type-II Seesaw Model and the Complete Basis of Lepton-Number-Violating Operators","version":1},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-08-01T00:42:30.474467Z"},"links":{"cited_paper":"/paper/2412.00355","citing_paper":"/paper/2607.26184"},"observation_digest":"sha256:05b8d62773b51f935d38c4434efe769c8479f36a4bddc984dae209d0d8579cf6","observation_id":"3ae43e85-a863-4a66-9d8e-2c53564ad6fc","resolution":{"observed_at":"2026-08-01T00:42:30.474467Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"links":{"evidence":"/evidence","html":"/paper/2412.00355/citation-record","integrity":"/paper/2412.00355/integrity","json":"/paper/2412.00355/citation-record.json","paper":"/paper/2412.00355"},"outbound":[{"citation":{"cited_paper":{"arxiv_id":"1207.7235","last_updated":"2013-01-28T10:46:38Z","snapshot_observed_at":"2026-08-12T13:24:07.072161Z","submitted_at":"2012-07-31T13:27:18Z","title":"Observation of a new boson at a mass of 125 GeV with the CMS experiment at the LHC","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1207.7235","snapshot_observed_at":"2026-08-12T05:35:37.740524Z","title":"Chatrchyan et al.,Observation of a New Boson at a Mass of 125 GeV with the CMS Experiment at the LHC, Phys","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.740524Z"},"links":{"cited_paper":"/paper/1207.7235","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:c18987414b62ece3e75f60c7e2726369782f9cc77ee71878301c97584c818c33","observation_id":"f74df42e-ac49-448f-aad1-9335c1354f16","resolution":{"observed_at":"2026-08-12T05:35:37.740524Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1207.7214","last_updated":"2012-08-31T19:29:54Z","snapshot_observed_at":"2026-08-12T13:22:06.792849Z","submitted_at":"2012-07-31T11:59:59Z","title":"Observation of a new particle in the search for the Standard Model Higgs boson with the ATLAS detector at the LHC","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1207.7214","snapshot_observed_at":"2026-08-12T05:35:37.744650Z","title":"Aad et al.,Observation of a new particle in the search for the Standard Model Higgs boson with the ATLAS detector at the LHC, Phys","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.744650Z"},"links":{"cited_paper":"/paper/1207.7214","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:1af073c902cc2ff70ba1faff9171c7e3fbf90dc533992d3ebaf21224ce92fb53","observation_id":"9d9e6d36-40b5-45d1-81b9-2d66661ff293","resolution":{"observed_at":"2026-08-12T05:35:37.744650Z","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":"2026-07-06T02:11:23.670680Z","submitted_at":"2017-06-27T17:17:52Z","title":"The Standard Model as an Effective Field Theory","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1706.08945","snapshot_observed_at":"2026-08-12T05:35:37.748325Z","title":"Brivio and M","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.748325Z"},"links":{"cited_paper":"/paper/1706.08945","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:94707180b405142f90c1e58830b8896755b64c99dd90b32dec20ab1adc3923b0","observation_id":"7715c0b4-f2ff-4085-a76b-9d5c66410a8c","resolution":{"observed_at":"2026-08-12T05:35:37.748325Z","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":"2026-08-12T05:35:37.751731Z","title":"Appelquist and C","venue":null,"work_id":null,"year":1980},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.751731Z"},"links":{"citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:7645735be9b4dae2c8f2e1c844ab827b754b2d5258baa11d4afcb26f06f11138","observation_id":"1132c6ed-ba97-494f-89c8-9de25c2542f2","resolution":{"observed_at":"2026-08-12T05:35:37.751731Z","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":"2026-08-12T05:35:37.755052Z","title":null,"venue":null,"work_id":null,"year":1980},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.755052Z"},"links":{"citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:5266d834469b19ba6711c20f27a61e0c04a3b56c3ec871c16e5d5cd867f760e8","observation_id":"7b5d3f58-f4bb-4d9f-b2fd-fbc228410f0b","resolution":{"observed_at":"2026-08-12T05:35:37.755052Z","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":"2026-08-12T05:35:37.758485Z","title":null,"venue":null,"work_id":null,"year":1981},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.758485Z"},"links":{"citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:d63e208ae88de3233f68cd7dcc18ef3b305991570e5e8dee39629065ec3da41e","observation_id":"4346fb56-12c7-49bb-9442-01a5e582f288","resolution":{"observed_at":"2026-08-12T05:35:37.758485Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9301281","last_updated":"1993-01-27T10:19:53Z","snapshot_observed_at":"2026-08-09T19:32:45.277590Z","submitted_at":"1993-01-27T10:19:53Z","title":"The Chiral Approach to the Electroweak Interactions","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9301281","snapshot_observed_at":"2026-08-12T05:35:37.762030Z","title":"Feruglio,The Chiral approach to the electroweak interactions, Int","venue":null,"work_id":null,"year":1993},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.762030Z"},"links":{"cited_paper":"/paper/hep-ph/9301281","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:f9cdbd3869065d8e236488d158c4d0c7749d8a755fef07c81b8db68bcf5dd59c","observation_id":"f91d953d-f09a-4e92-88eb-4c171de58330","resolution":{"observed_at":"2026-08-12T05:35:37.762030Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9308276","last_updated":"1993-08-14T01:18:00Z","snapshot_observed_at":"2026-07-07T04:15:51.144057Z","submitted_at":"1993-08-14T01:18:00Z","title":"The Electroweak Chiral Lagrangian for the Standard Model with a Heavy Higgs","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9308276","snapshot_observed_at":"2026-08-12T05:35:37.765459Z","title":null,"venue":null,"work_id":null,"year":1994},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.765459Z"},"links":{"cited_paper":"/paper/hep-ph/9308276","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:ab74859a094a39f86db966a4ce9137b8aa2cc6764585306b465f77119e3ce4d6","observation_id":"37c110c4-b770-47f1-a0cb-75fdad650efb","resolution":{"observed_at":"2026-08-12T05:35:37.765459Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9411207","last_updated":"1994-11-30T12:13:07Z","snapshot_observed_at":"2026-08-10T08:33:32.616121Z","submitted_at":"1994-10-31T21:05:33Z","title":"Non-decoupling effects of the Standard Model Higgs boson to one loop","version":3},"cited_work":{"arxiv_id":"hep-ph/9411207","doi":null,"metadata_source":"pith","pith_arxiv_id":"hep-ph/9411207","snapshot_observed_at":"2026-08-12T05:35:38.724743Z","title":"Non-decoupling effects of the Standard Model Higgs boson to one loop","venue":"hep-ph","work_id":"97adb7fb-2a8f-44bf-a552-272caed5e95a","year":1994},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.769448Z"},"links":{"cited_paper":"/paper/hep-ph/9411207","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:605611ef26514bb5f4b215a4e441b57cc507eddfacc775bc51d0d209b3b1d221","observation_id":"ed03e27f-5ae4-4d73-b247-8fc631b5a4d2","resolution":{"observed_at":"2026-08-12T05:35:38.728790Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-12T06:34:41.77262+00:00","source":"crossref"},{"observed_at":"2026-08-12T06:34:36.333875+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"0704.1505","last_updated":"2007-09-06T03:27:12Z","snapshot_observed_at":"2026-07-06T01:26:04.345345Z","submitted_at":"2007-04-11T23:23:26Z","title":"A Higgs-Higgs bound state due to New Physics at a TeV","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0704.1505","snapshot_observed_at":"2026-08-12T05:35:37.772626Z","title":"Grinstein and M","venue":null,"work_id":null,"year":2007},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.772626Z"},"links":{"cited_paper":"/paper/0704.1505","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:be784cd8638b9cd12a1a8dfcc7f081098d81e143b026f5d6ae176384943d3a2a","observation_id":"27afae0c-d281-4763-bd95-b05c3785954b","resolution":{"observed_at":"2026-08-12T05:35:37.772626Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1203.6510","last_updated":"2012-08-23T12:59:13Z","snapshot_observed_at":"2026-08-07T07:53:19.401360Z","submitted_at":"2012-03-29T12:58:00Z","title":"Effective Theory of a Dynamically Broken Electroweak Standard Model at NLO","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1203.6510","snapshot_observed_at":"2026-08-12T05:35:37.776052Z","title":"Buchalla and O","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.776052Z"},"links":{"cited_paper":"/paper/1203.6510","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:c5968f3234276c59d7732477e76d992423f3bb1325b658795b0b21bb28dbdc35","observation_id":"25aeff94-adaf-4b6a-9540-826c8c8a9ea0","resolution":{"observed_at":"2026-08-12T05:35:37.776052Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1212.3305","last_updated":"2013-11-18T18:18:33Z","snapshot_observed_at":"2026-07-06T03:02:00.289526Z","submitted_at":"2012-12-13T20:27:58Z","title":"The Effective Chiral Lagrangian for a Light Dynamical \"Higgs Particle\"","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1212.3305","snapshot_observed_at":"2026-08-12T05:35:37.779421Z","title":"Alonso, M","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.779421Z"},"links":{"cited_paper":"/paper/1212.3305","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:f57110a7f1394430ae6a4f0e0b8cdac0089af5c3c8c8ea8b595eaf97d69f0169","observation_id":"a9262f6c-88af-400a-a039-1a0c6f333756","resolution":{"observed_at":"2026-08-12T05:35:37.779421Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1307.5017","last_updated":"2015-12-07T20:23:19Z","snapshot_observed_at":"2026-07-06T03:18:35.692259Z","submitted_at":"2013-07-18T17:20:38Z","title":"Complete Electroweak Chiral Lagrangian with a Light Higgs at NLO","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1307.5017","snapshot_observed_at":"2026-08-12T05:35:37.782872Z","title":"Buchalla, O","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.782872Z"},"links":{"cited_paper":"/paper/1307.5017","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:63463d5f7f5cdf7ce3655bb9372e648de9aabdabfb0191fcc206b3afbc276f1e","observation_id":"752ee3f4-cdbf-4eb6-99e5-de9157ede119","resolution":{"observed_at":"2026-08-12T05:35:37.782872Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1311.1823","last_updated":"2014-02-27T14:20:59Z","snapshot_observed_at":"2026-08-10T07:57:09.352369Z","submitted_at":"2013-11-07T21:00:33Z","title":"Disentangling a dynamical Higgs","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1311.1823","snapshot_observed_at":"2026-08-12T05:35:37.785999Z","title":"Brivio, T","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.785999Z"},"links":{"cited_paper":"/paper/1311.1823","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:15edc9a21976af2cb7ba40cc384fa91fcf741bab19ac2b3480bbb1350a47d29e","observation_id":"d3a298a4-a88b-4fb3-8f5d-dd15bcaf0776","resolution":{"observed_at":"2026-08-12T05:35:37.785999Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1312.5624","last_updated":"2013-12-19T16:32:26Z","snapshot_observed_at":"2026-07-06T03:31:23.521122Z","submitted_at":"2013-12-19T16:32:26Z","title":"On the Power Counting in Effective Field Theories","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1312.5624","snapshot_observed_at":"2026-08-12T05:35:37.789346Z","title":"Buchalla, O","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.789346Z"},"links":{"cited_paper":"/paper/1312.5624","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:a823d5128222ee2dc5325f9f674f2f66e4787718e09771f61eae0a65a910808a","observation_id":"b00e3eee-5fed-4b29-bd75-bb072696d63a","resolution":{"observed_at":"2026-08-12T05:35:37.789346Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1406.6367","last_updated":"2014-10-10T14:51:14Z","snapshot_observed_at":"2026-08-07T21:22:21.574907Z","submitted_at":"2014-06-24T20:00:19Z","title":"CP violation with a dynamical Higgs","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1406.6367","snapshot_observed_at":"2026-08-12T05:35:37.792595Z","title":null,"venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.792595Z"},"links":{"cited_paper":"/paper/1406.6367","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:48a600d3ceb19114174b1a68b1dc9045fefced979991a484db6971d3f07b0fe5","observation_id":"b236def0-0cb4-4ad1-a4a8-c169ddbea960","resolution":{"observed_at":"2026-08-12T05:35:37.792595Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1510.03114","last_updated":"2016-03-22T09:20:07Z","snapshot_observed_at":"2026-07-31T05:21:07.457115Z","submitted_at":"2015-10-12T00:05:38Z","title":"Low-energy signals of strongly-coupled electroweak symmetry-breaking scenarios","version":2},"cited_work":{"arxiv_id":"1510.03114","doi":null,"metadata_source":"pith","pith_arxiv_id":"1510.03114","snapshot_observed_at":"2026-08-12T05:35:38.653428Z","title":"Low-energy signals of strongly-coupled electroweak symmetry-breaking scenarios","venue":"hep-ph","work_id":"47b87787-0a79-4ade-bb27-91c6711416cc","year":2015},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.795713Z"},"links":{"cited_paper":"/paper/1510.03114","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:3b3981e386d345667dd93dfd22319bd59ebdeb623f45c17a11913d0774bff78b","observation_id":"28110199-5363-4da3-aaf5-57b1bd396f3f","resolution":{"observed_at":"2026-08-12T05:35:38.656872Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-12T06:34:41.77262+00:00","source":"crossref"},{"observed_at":"2026-08-12T06:34:36.333875+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1511.00724","last_updated":"2016-02-03T10:52:02Z","snapshot_observed_at":"2026-08-09T13:24:32.212669Z","submitted_at":"2015-11-02T22:00:30Z","title":"A Geometric Formulation of Higgs Effective Field Theory: Measuring the Curvature of Scalar Field Space","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1511.00724","snapshot_observed_at":"2026-08-12T05:35:37.799009Z","title":"Alonso, E","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.799009Z"},"links":{"cited_paper":"/paper/1511.00724","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:c04a15b63e4bbd4f763d6a26b1aa530745f2ce5e0c8e606be3dee84f14e1c917","observation_id":"bd8f9a64-5d7d-4da8-bcbe-eb1cbd8f0f80","resolution":{"observed_at":"2026-08-12T05:35:37.799009Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1604.06801","last_updated":"2018-01-22T10:16:05Z","snapshot_observed_at":"2026-08-09T04:23:34.540270Z","submitted_at":"2016-04-22T20:00:02Z","title":"The complete HEFT Lagrangian after the LHC Run I","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1604.06801","snapshot_observed_at":"2026-08-12T05:35:37.802120Z","title":"Brivio, J","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.802120Z"},"links":{"cited_paper":"/paper/1604.06801","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:d2d2d8dba4fcb3873ee08163386b0b53912fa1e2077eae58657bebf941717a9a","observation_id":"fb94f047-c479-4093-a03d-c2ddabba90dc","resolution":{"observed_at":"2026-08-12T05:35:37.802120Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1605.03602","last_updated":"2016-05-11T20:06:23Z","snapshot_observed_at":"2026-08-01T16:22:27.403415Z","submitted_at":"2016-05-11T20:06:23Z","title":"Geometry of the Scalar Sector","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1605.03602","snapshot_observed_at":"2026-08-12T05:35:37.805110Z","title":"Alonso, E","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.805110Z"},"links":{"cited_paper":"/paper/1605.03602","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:43526032c383d8c89431983810bdc27e8f90477267e447762316f2a12bf80998","observation_id":"c15056c1-d411-4e46-b27d-af15e14bb92e","resolution":{"observed_at":"2026-08-12T05:35:37.805110Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1609.06659","last_updated":"2017-07-21T17:36:51Z","snapshot_observed_at":"2026-08-02T09:47:08.594110Z","submitted_at":"2016-09-21T18:17:20Z","title":"Fingerprints of heavy scales in electroweak effective Lagrangians","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1609.06659","snapshot_observed_at":"2026-08-12T05:35:37.808308Z","title":null,"venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.808308Z"},"links":{"cited_paper":"/paper/1609.06659","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:20d262a1297c0b39f9412e7a795da0cf0e1f5136ba5d401f3c1c288a32beddd8","observation_id":"ee816dad-f3fc-4457-99da-3eb4197b1e12","resolution":{"observed_at":"2026-08-12T05:35:37.808308Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1612.04832","last_updated":"2017-03-22T14:07:41Z","snapshot_observed_at":"2026-07-06T05:22:46.074568Z","submitted_at":"2016-12-14T21:00:15Z","title":"Baryon Non-Invariant Couplings in Higgs Effective Field Theory","version":2},"cited_work":{"arxiv_id":"1612.04832","doi":null,"metadata_source":"pith","pith_arxiv_id":"1612.04832","snapshot_observed_at":"2026-08-12T05:35:38.608705Z","title":"Baryon Non-Invariant Couplings in Higgs Effective Field Theory","venue":"hep-ph","work_id":"7206d3c0-205c-4df6-8f31-e97968d39fd8","year":2016},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.811396Z"},"links":{"cited_paper":"/paper/1612.04832","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:43db2b4bdff05227d8e98666463987502f1749921efd01fd1085be17fe4a3dab","observation_id":"250f244b-4e40-43c6-9b2f-68a683fca28e","resolution":{"observed_at":"2026-08-12T05:35:38.612009Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-12T06:34:41.77262+00:00","source":"crossref"},{"observed_at":"2026-08-12T06:34:36.333875+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1804.05664","last_updated":"2020-01-25T19:54:12Z","snapshot_observed_at":"2026-08-02T20:32:56.878259Z","submitted_at":"2018-04-16T13:37:01Z","title":"Effective Field Theory with Nambu-Goldstone Modes","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1804.05664","snapshot_observed_at":"2026-08-12T05:35:37.815050Z","title":"Pich,Effective Field Theory with Nambu-Goldstone Modes, arXiv:1804.05664","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.815050Z"},"links":{"cited_paper":"/paper/1804.05664","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:1931c30a4f59505fd63d6f24b231ad99bbafc4646bf9b7d11e2dc7f66b7c8e64","observation_id":"4d5e4b11-e81c-4c3d-9dac-d3162d484c9a","resolution":{"observed_at":"2026-08-12T05:35:37.815050Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1810.10544","last_updated":"2019-05-25T03:31:46Z","snapshot_observed_at":"2026-07-06T07:10:23.130494Z","submitted_at":"2018-10-24T18:00:02Z","title":"Colorful Imprints of Heavy States in the Electroweak Effective Theory","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1810.10544","snapshot_observed_at":"2026-08-12T05:35:37.818480Z","title":"Krause, A","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.818480Z"},"links":{"cited_paper":"/paper/1810.10544","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:7fefd691d11ea9a0e11fc423e96e1eb0dafd931ceaef75a0c9bcc50b88f60518","observation_id":"6dbf53d1-fa8c-4439-8fb0-7dfcdee15f48","resolution":{"observed_at":"2026-08-12T05:35:37.818480Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2206.07722","last_updated":"2022-12-05T11:55:49Z","snapshot_observed_at":"2026-08-10T23:00:38.596725Z","submitted_at":"2022-06-15T18:00:02Z","title":"Complete NLO Operators in the Higgs Effective Field Theory","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2206.07722","snapshot_observed_at":"2026-08-12T05:35:37.821502Z","title":"Sun, M.-L","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.821502Z"},"links":{"cited_paper":"/paper/2206.07722","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:2aeb1ab41d672718abb1db3be5ffe994e8522650f591959c5d0f3adbdcd49de6","observation_id":"7216e1c2-9a82-420a-978d-40b3b69c1010","resolution":{"observed_at":"2026-08-12T05:35:37.821502Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2210.14939","last_updated":"2022-10-26T18:00:07Z","snapshot_observed_at":"2026-07-06T14:10:51.793831Z","submitted_at":"2022-10-26T18:00:07Z","title":"Complete NNLO Operator Bases in Higgs Effective Field Theory","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2210.14939","snapshot_observed_at":"2026-08-12T05:35:37.824764Z","title":"Sun, M.-L","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.824764Z"},"links":{"cited_paper":"/paper/2210.14939","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:8c88790b2989ea2d2a8e2b03a60fd8822fca9f863c39d05bfd98538a4de875f5","observation_id":"f14dce1f-deb3-48e7-8a70-b18568869873","resolution":{"observed_at":"2026-08-12T05:35:37.824764Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2211.06275","last_updated":"2022-11-11T15:32:47Z","snapshot_observed_at":"2026-08-10T14:00:45.769316Z","submitted_at":"2022-11-11T15:32:47Z","title":"Hilbert Series, the Higgs Mechanism, and HEFT","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2211.06275","snapshot_observed_at":"2026-08-12T05:35:37.827824Z","title":null,"venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.827824Z"},"links":{"cited_paper":"/paper/2211.06275","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:2f9f619b9be512dc3cb55cfa25225af17e6d7824e9653ea2700c691ba65d91fa","observation_id":"33910d45-0731-4b68-b513-411ce3f39229","resolution":{"observed_at":"2026-08-12T05:35:37.827824Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2207.09848","last_updated":"2023-09-19T12:50:35Z","snapshot_observed_at":"2026-08-10T18:21:04.701486Z","submitted_at":"2022-07-20T12:27:06Z","title":"SMEFT is falsifiable through multi-Higgs measurements (even in the absence of new light particles)","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2207.09848","snapshot_observed_at":"2026-08-12T05:35:37.830739Z","title":"Gómez-Ambrosio, F","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.830739Z"},"links":{"cited_paper":"/paper/2207.09848","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:bc060027ab1009f5c6d420bcf1863e31173a67b47f7c42030e231bc4f72991b8","observation_id":"add8a874-44ad-4029-b382-4d20604ed35f","resolution":{"observed_at":"2026-08-12T05:35:37.830739Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2204.01763","last_updated":"2022-04-04T18:02:23Z","snapshot_observed_at":"2026-08-03T15:47:51.888785Z","submitted_at":"2022-04-04T18:02:23Z","title":"The flair of Higgsflare: Distinguishing electroweak EFTs with $W_LW_L \\to n\\times h$","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2204.01763","snapshot_observed_at":"2026-08-12T05:35:37.834103Z","title":"Gómez-Ambrosio, F","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":29,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.834103Z"},"links":{"cited_paper":"/paper/2204.01763","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:6def87eea96e1e512042442e983360260d95df5ce4eee1d134a98e2494acf9cd","observation_id":"1d3242e2-c34d-4bee-bd0d-3760697e24b6","resolution":{"observed_at":"2026-08-12T05:35:37.834103Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2109.13290","last_updated":"2022-08-10T15:43:52Z","snapshot_observed_at":"2026-08-10T09:52:02.797891Z","submitted_at":"2021-09-27T18:25:23Z","title":"On the road(s) to the Standard Model","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2109.13290","snapshot_observed_at":"2026-08-12T05:35:37.837375Z","title":"Alonso and M","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.837375Z"},"links":{"cited_paper":"/paper/2109.13290","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:28c0b055886a18472ce8f21284cdf1e517b281dda75b85a8b593ac14a9a51696","observation_id":"715b9085-59c5-4bf5-b06c-714e173311ad","resolution":{"observed_at":"2026-08-12T05:35:37.837375Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2109.02673","last_updated":"2021-12-21T12:41:54Z","snapshot_observed_at":"2026-07-06T11:45:01.268963Z","submitted_at":"2021-09-06T18:00:06Z","title":"Introducing tools to test Higgs interactions via $WW$ scattering I: one-loop calculations and renormalization in the HEFT","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2109.02673","snapshot_observed_at":"2026-08-12T05:35:37.840785Z","title":null,"venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.840785Z"},"links":{"cited_paper":"/paper/2109.02673","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:8dc640b3feb1bde11b98ead91f6a780d5ba04dbd08055b0dc7e8ad0b539bd549","observation_id":"47bbe7a0-e8f2-4bfc-baed-f92fcb4a16cb","resolution":{"observed_at":"2026-08-12T05:35:37.840785Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2108.03240","last_updated":"2021-12-01T16:36:52Z","snapshot_observed_at":"2026-08-10T23:28:26.942065Z","submitted_at":"2021-08-06T18:00:00Z","title":"Unitarity Violation and the Geometry of Higgs EFTs","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2108.03240","snapshot_observed_at":"2026-08-12T05:35:37.843904Z","title":"Cohen, N","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":32,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.843904Z"},"links":{"cited_paper":"/paper/2108.03240","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:46fca4cbb46214d63fc9d2a9cf24affbef3d99831bd38a7118393216afe58511","observation_id":"f58d3e4b-2890-4e0b-81d2-276e75eb745a","resolution":{"observed_at":"2026-08-12T05:35:37.843904Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2107.07890","last_updated":"2021-10-20T19:07:20Z","snapshot_observed_at":"2026-08-10T22:26:41.826033Z","submitted_at":"2021-07-16T13:23:05Z","title":"One-loop renormalization of VBS with the electroweak chiral Lagrangian in covariant gauges","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2107.07890","snapshot_observed_at":"2026-08-12T05:35:37.847148Z","title":null,"venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.847148Z"},"links":{"cited_paper":"/paper/2107.07890","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:6a2bebaaf16d30283e7086ade0a432a8acab0bb91a722ab5da018447257b76b2","observation_id":"03b5cf6a-e33a-4ee9-a785-1e8ac5d31839","resolution":{"observed_at":"2026-08-12T05:35:37.847148Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2208.05900","last_updated":"2024-05-09T20:15:39Z","snapshot_observed_at":"2026-08-10T07:55:29.691471Z","submitted_at":"2022-08-11T15:59:15Z","title":"One-loop corrections for WW to HH in HEFT with the electroweak chiral Lagrangian","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2208.05900","snapshot_observed_at":"2026-08-12T05:35:37.850349Z","title":null,"venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":34,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.850349Z"},"links":{"cited_paper":"/paper/2208.05900","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:e8b9a31b75848d3c76df697cc0ace42aa1162eb604d62391cc3b9666b511c292","observation_id":"46479ec3-df17-4f2d-9d18-fea6b34b1089","resolution":{"observed_at":"2026-08-12T05:35:37.850349Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1412.1837","last_updated":"2015-07-08T20:01:17Z","snapshot_observed_at":"2026-08-02T22:27:45.850491Z","submitted_at":"2014-12-04T21:03:25Z","title":"How to use the Standard Model effective field theory","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1412.1837","snapshot_observed_at":"2026-08-12T05:35:37.853468Z","title":"Henning, X","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.853468Z"},"links":{"cited_paper":"/paper/1412.1837","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:830bd9e2951d38dc1a158b28454d7b547ee50d07983d49d5d5237d5e2905958b","observation_id":"34c1c9fb-4faa-4b9c-83a9-65bb6771f25d","resolution":{"observed_at":"2026-08-12T05:35:37.853468Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1504.02409","last_updated":"2016-02-10T18:07:42Z","snapshot_observed_at":"2026-08-09T03:34:10.363417Z","submitted_at":"2015-04-09T18:17:50Z","title":"Comparing EFT and Exact One-Loop Analyses of Non-Degenerate Stops","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1504.02409","snapshot_observed_at":"2026-08-12T05:35:37.856682Z","title":"Drozd, J","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":36,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.856682Z"},"links":{"cited_paper":"/paper/1504.02409","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:9ac82ef381f3d202ee07ce9f9679d74e50592e08b998a58852d78b4856b7bb6f","observation_id":"035d0b7e-861b-4407-9e8c-4ef352d3df97","resolution":{"observed_at":"2026-08-12T05:35:37.856682Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1505.06334","last_updated":"2015-08-13T02:34:42Z","snapshot_observed_at":"2026-08-09T06:34:32.224585Z","submitted_at":"2015-05-23T14:07:01Z","title":"Standard Model Effective Field Theory: Integrating out a Generic Scalar","version":2},"cited_work":{"arxiv_id":"1505.06334","doi":null,"metadata_source":"pith","pith_arxiv_id":"1505.06334","snapshot_observed_at":"2026-08-12T05:35:38.489561Z","title":"Standard Model Effective Field Theory: Integrating out a Generic Scalar","venue":"hep-ph","work_id":"ea5eb831-fdd3-41ed-8dc5-6487c91f8130","year":2015},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":37,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.859839Z"},"links":{"cited_paper":"/paper/1505.06334","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:37e3f49bc33cddf153adf2002dc8f4fb8a7c7ffd5d73527cf972ebbe4ded865c","observation_id":"dedea4cc-df16-40ad-8976-8053ae8412aa","resolution":{"observed_at":"2026-08-12T05:35:38.493317Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-12T06:34:41.77262+00:00","source":"crossref"},{"observed_at":"2026-08-12T06:34:36.333875+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1506.00840","last_updated":"2015-09-08T08:15:31Z","snapshot_observed_at":"2026-07-06T04:19:39.091162Z","submitted_at":"2015-06-02T11:12:44Z","title":"Standard Model Effective Field Theory: Integrating out Vector-Like Fermions","version":2},"cited_work":{"arxiv_id":"1506.00840","doi":null,"metadata_source":"pith","pith_arxiv_id":"1506.00840","snapshot_observed_at":"2026-08-12T05:35:38.477134Z","title":"Standard Model Effective Field Theory: Integrating out Vector-Like Fermions","venue":"hep-ph","work_id":"7180df2a-4193-4f83-b8f5-3cea2a6148cd","year":2015},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":38,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.862909Z"},"links":{"cited_paper":"/paper/1506.00840","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:a80a50b962b8c37e663e6adf52842faa28221b070e04379fa3f1abd50523b508","observation_id":"2bc531ba-f6c7-47b5-9b2a-cfc3bdaae981","resolution":{"observed_at":"2026-08-12T05:35:38.480771Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-12T06:34:41.77262+00:00","source":"crossref"},{"observed_at":"2026-08-12T06:34:36.333875+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1509.05942","last_updated":"2018-04-24T03:01:39Z","snapshot_observed_at":"2026-07-06T04:30:27.083173Z","submitted_at":"2015-09-19T22:12:45Z","title":"Effective Field Theory of Integrating out Sfermions in the MSSM: Complete One-Loop Analysis","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1509.05942","snapshot_observed_at":"2026-08-12T05:35:37.866308Z","title":"Huo,Effective Field Theory of Integrating out Sfermions in the MSSM: Complete One-Loop Analysis, Phys","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":39,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.866308Z"},"links":{"cited_paper":"/paper/1509.05942","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:365c53f97a2167a5b61fd2f45496aa9376b5467b9a610e4191f0fe80a8d093a8","observation_id":"ad27f4e0-d8b7-4788-a3c5-c2a7cb19c315","resolution":{"observed_at":"2026-08-12T05:35:37.866308Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1510.03443","last_updated":"2016-01-27T21:06:15Z","snapshot_observed_at":"2026-07-06T04:32:50.206977Z","submitted_at":"2015-10-12T20:15:07Z","title":"Pushing Higgs Effective Theory to its Limits","version":2},"cited_work":{"arxiv_id":"1510.03443","doi":null,"metadata_source":"pith","pith_arxiv_id":"1510.03443","snapshot_observed_at":"2026-08-12T05:35:38.457693Z","title":"Pushing Higgs Effective Theory to its Limits","venue":"hep-ph","work_id":"82a19496-43b5-40dd-85e3-e7442d13d071","year":2015},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":40,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.869445Z"},"links":{"cited_paper":"/paper/1510.03443","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:fa243bdf78d68a5bff4631f33094e7c00dba6c4fa7797fcf53d4cef2c55cbac8","observation_id":"1799cac2-0b54-4e0a-9a47-ddec9bf8ff80","resolution":{"observed_at":"2026-08-12T05:35:38.461224Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-12T06:34:41.77262+00:00","source":"crossref"},{"observed_at":"2026-08-12T06:34:36.333875+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1608.00975","last_updated":"2020-03-30T15:27:03Z","snapshot_observed_at":"2026-08-05T13:57:41.985768Z","submitted_at":"2016-08-02T20:00:04Z","title":"Effective Field Theory with Two Higgs Doublets","version":2},"cited_work":{"arxiv_id":"1608.00975","doi":null,"metadata_source":"pith","pith_arxiv_id":"1608.00975","snapshot_observed_at":"2026-08-12T05:35:38.444270Z","title":"Effective Field Theory with Two Higgs Doublets","venue":"hep-ph","work_id":"c69865a1-b575-4bf5-93cd-a2292e282c5a","year":2016},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":41,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.872799Z"},"links":{"cited_paper":"/paper/1608.00975","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:abb6cc804fa6e2791a03bacd637cd6d7c4cc634e8e3a01383fe2d0661d22806a","observation_id":"cae7b490-49b7-49fe-b324-1fe4bde1a0b3","resolution":{"observed_at":"2026-08-12T05:35:38.447807Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-12T06:34:41.77262+00:00","source":"crossref"},{"observed_at":"2026-08-12T06:34:36.333875+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1611.01112","last_updated":"2016-11-03T17:59:49Z","snapshot_observed_at":"2026-07-06T05:17:16.626374Z","submitted_at":"2016-11-03T17:59:49Z","title":"Higgs EFT for 2HDM and beyond","version":1},"cited_work":{"arxiv_id":"1611.01112","doi":null,"metadata_source":"pith","pith_arxiv_id":"1611.01112","snapshot_observed_at":"2026-08-12T05:35:38.432208Z","title":"Higgs EFT for 2HDM and beyond","venue":"hep-ph","work_id":"3ce72f89-0756-43ef-bd71-eea47761ebe1","year":2016},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":42,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.875896Z"},"links":{"cited_paper":"/paper/1611.01112","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:7959e1d2b36c11080552eabbfd2b5b9300bb48a9be677b89dfc7a35dc6fce96f","observation_id":"c7c0a12d-36ff-4837-8d74-fe65533cc104","resolution":{"observed_at":"2026-08-12T05:35:38.435567Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-12T06:34:41.77262+00:00","source":"crossref"},{"observed_at":"2026-08-12T06:34:36.333875+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1704.07851","last_updated":"2017-07-27T18:39:53Z","snapshot_observed_at":"2026-07-06T05:39:18.366653Z","submitted_at":"2017-04-25T18:12:32Z","title":"Standard Model EFT and Extended Scalar Sectors","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1704.07851","snapshot_observed_at":"2026-08-12T05:35:37.880349Z","title":"Dawson and C","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":43,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.880349Z"},"links":{"cited_paper":"/paper/1704.07851","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:c26b7b9d53ebb6a623f87f0c904df041147f6746344ce1c44791d9c696e8245b","observation_id":"64b62582-1359-408d-954b-4a62b90c3b95","resolution":{"observed_at":"2026-08-12T05:35:37.880349Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1705.02551","last_updated":"2019-07-04T12:32:45Z","snapshot_observed_at":"2026-08-06T10:22:12.252192Z","submitted_at":"2017-05-07T02:37:55Z","title":"Exploring Extended Scalar Sectors with Di-Higgs Signals: A Higgs EFT Perspective","version":3},"cited_work":{"arxiv_id":"1705.02551","doi":null,"metadata_source":"pith","pith_arxiv_id":"1705.02551","snapshot_observed_at":"2026-08-12T05:35:38.411039Z","title":"Exploring Extended Scalar Sectors with Di-Higgs Signals: A Higgs EFT Perspective","venue":"hep-ph","work_id":"6c2dc591-ef6e-4f12-b2b1-e0e4b8d8d546","year":2017},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":44,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.883508Z"},"links":{"cited_paper":"/paper/1705.02551","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:dc53786dc940e45cedbc46bfe9d3193734c2b36af9f6e0c1adba2a3b15027d87","observation_id":"039e10c5-fa8f-400e-803e-e59c9582c090","resolution":{"observed_at":"2026-08-12T05:35:38.414683Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-12T06:34:41.77262+00:00","source":"crossref"},{"observed_at":"2026-08-12T06:34:36.333875+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1711.10391","last_updated":"2018-08-08T15:37:34Z","snapshot_observed_at":"2026-07-06T02:11:23.670680Z","submitted_at":"2017-11-28T16:46:04Z","title":"Effective description of general extensions of the Standard Model: the complete tree-level dictionary","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1711.10391","snapshot_observed_at":"2026-08-12T05:35:37.887008Z","title":"de Blas, J","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":45,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.887008Z"},"links":{"cited_paper":"/paper/1711.10391","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:123b3a2dae0448e9b7e603be54f8deb5e22a4f6f8c4427f04a6c7b2a880612e1","observation_id":"923c7192-7561-4ce7-aba6-dd5c05513ee9","resolution":{"observed_at":"2026-08-12T05:35:37.887008Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1712.07825","last_updated":"2018-05-05T02:21:11Z","snapshot_observed_at":"2026-07-06T06:15:29.485540Z","submitted_at":"2017-12-21T08:19:48Z","title":"Standard Model Effective Field Theory: Integrating out Neutralinos and Charginos in the MSSM","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1712.07825","snapshot_observed_at":"2026-08-12T05:35:37.890591Z","title":null,"venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":46,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.890591Z"},"links":{"cited_paper":"/paper/1712.07825","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:6fa7a6f6655850e5c1d8762451e5d05bcbd4b49c94f2bcdabffa97b2039025b3","observation_id":"7d47b282-8716-4b1b-9c08-d2702d754940","resolution":{"observed_at":"2026-08-12T05:35:37.890591Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1811.08878","last_updated":"2018-11-21T18:50:15Z","snapshot_observed_at":"2026-07-06T07:16:20.519144Z","submitted_at":"2018-11-21T18:50:15Z","title":"Complete One-Loop Matching for a Singlet Scalar in the Standard Model EFT","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1811.08878","snapshot_observed_at":"2026-08-12T05:35:37.894334Z","title":"Jiang, N","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":47,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.894334Z"},"links":{"cited_paper":"/paper/1811.08878","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:5d531e1310ba7acdef3a7b201de0cb4ede2510389111bf303f9737c6d05bd981","observation_id":"c19150fc-b329-414c-83a4-c6de5e3e8b28","resolution":{"observed_at":"2026-08-12T05:35:37.894334Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2001.00017","last_updated":"2019-12-31T19:00:00Z","snapshot_observed_at":"2026-08-11T02:35:40.584321Z","submitted_at":"2019-12-31T19:00:00Z","title":"Loops and trees in generic EFTs","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2001.00017","snapshot_observed_at":"2026-08-12T05:35:37.897538Z","title":"Craig, M","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":48,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.897538Z"},"links":{"cited_paper":"/paper/2001.00017","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:45d47ba52f19bdfdd0ce38add3d6e5b954fc3f73de2743cc7d4fafc1acc3ad85","observation_id":"8f3d550f-e4b6-4660-8be3-624dda124a86","resolution":{"observed_at":"2026-08-12T05:35:37.897538Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2003.05936","last_updated":"2020-06-17T17:00:36Z","snapshot_observed_at":"2026-08-11T07:37:47.995966Z","submitted_at":"2020-03-12T17:59:26Z","title":"Singlet night in Feynman-ville: one-loop matching of a real scalar","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2003.05936","snapshot_observed_at":"2026-08-12T05:35:37.900734Z","title":"Haisch, M","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":49,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.900734Z"},"links":{"cited_paper":"/paper/2003.05936","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:9126883cfaa0b2e0de5177e9cd139fdb719cfb84d21279473cd33111ac4b2079","observation_id":"e27a8d60-1f28-45ae-a484-d3a0d291c33f","resolution":{"observed_at":"2026-08-12T05:35:37.900734Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2003.12525","last_updated":"2021-11-16T14:26:13Z","snapshot_observed_at":"2026-08-04T21:53:16.055999Z","submitted_at":"2020-03-27T16:41:49Z","title":"Matching scalar leptoquarks to the SMEFT at one loop","version":5},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2003.12525","snapshot_observed_at":"2026-08-12T05:35:37.904478Z","title":"Gherardi, D","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":50,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.904478Z"},"links":{"cited_paper":"/paper/2003.12525","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:938d7e4aaba1921a0b304721b65e8388ef294d1cd6a4dbc007c009294b3b7bfe","observation_id":"73cc1284-45b9-478b-9e1c-352b365ae907","resolution":{"observed_at":"2026-08-12T05:35:37.904478Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2007.01296","last_updated":"2021-04-26T17:21:58Z","snapshot_observed_at":"2026-08-06T12:28:20.462111Z","submitted_at":"2020-07-02T17:59:55Z","title":"Putting SMEFT Fits to Work","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2007.01296","snapshot_observed_at":"2026-08-12T05:35:37.907807Z","title":"Dawson, S","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":51,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.907807Z"},"links":{"cited_paper":"/paper/2007.01296","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:926fc70951c828ea1efcbaf6817c6cf2b55119c6ce8b2161ccd44a9b496152c2","observation_id":"24e6d0e7-62f3-48c4-a8c8-06bb61206d13","resolution":{"observed_at":"2026-08-12T05:35:37.907807Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2009.01249","last_updated":"2020-09-02T18:00:02Z","snapshot_observed_at":"2026-08-06T10:34:15.834321Z","submitted_at":"2020-09-02T18:00:02Z","title":"BSM Benchmarks for Effective Field Theories in Higgs and Electroweak Physics","version":1},"cited_work":{"arxiv_id":"2009.01249","doi":null,"metadata_source":"pith","pith_arxiv_id":"2009.01249","snapshot_observed_at":"2026-08-12T05:35:38.345676Z","title":"BSM Benchmarks for Effective Field Theories in Higgs and Electroweak Physics","venue":"hep-ph","work_id":"582b771a-3625-413a-a518-8ca3c90e1912","year":2020},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":52,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.910800Z"},"links":{"cited_paper":"/paper/2009.01249","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:aa8fe23643f28f54c3022dcd3b22b3bdcea12b8e2d59502f7af2c9ada73ff650","observation_id":"83fdf70d-f6bf-45d3-935e-8ab6bd166c72","resolution":{"observed_at":"2026-08-12T05:35:38.349189Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-12T06:34:41.77262+00:00","source":"crossref"},{"observed_at":"2026-08-12T06:34:36.333875+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2102.02819","last_updated":"2021-06-22T15:47:38Z","snapshot_observed_at":"2026-08-11T09:47:56.699406Z","submitted_at":"2021-02-04T19:00:00Z","title":"EWPD in the SMEFT to dimension eight","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2102.02819","snapshot_observed_at":"2026-08-12T05:35:37.913967Z","title":"Corbett, A","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":53,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.913967Z"},"links":{"cited_paper":"/paper/2102.02819","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:bac2e73d8823e0209f79e99c16f75c9903ab427c8bdf7736cbb80f31c72d8faa","observation_id":"2fdcf1b0-b355-4c23-b0f5-61e43e353afd","resolution":{"observed_at":"2026-08-12T05:35:37.913967Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2102.04954","last_updated":"2021-06-30T02:57:12Z","snapshot_observed_at":"2026-08-12T16:57:22.365693Z","submitted_at":"2021-02-09T17:09:55Z","title":"Radiative Decays of Charged Leptons in the Seesaw Effective Field Theory with One-loop Matching","version":3},"cited_work":{"arxiv_id":"2102.04954","doi":null,"metadata_source":"pith","pith_arxiv_id":"2102.04954","snapshot_observed_at":"2026-08-12T05:35:38.325054Z","title":"Radiative Decays of Charged Leptons in the Seesaw Effective Field Theory with One-loop Matching","venue":"hep-ph","work_id":"b23f7a9f-c2c3-4e49-ab9e-6bdfa650365c","year":2021},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":54,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.917246Z"},"links":{"cited_paper":"/paper/2102.04954","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:da0c5d6fcf8ee9ff270067aa0347008167be577ad8ee4527b1352e48977e6525","observation_id":"9bfb193f-9e62-499c-b672-950f16548fe9","resolution":{"observed_at":"2026-08-12T05:35:38.329043Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-12T06:34:41.77262+00:00","source":"crossref"},{"observed_at":"2026-08-12T06:34:36.333875+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2107.12133","last_updated":"2022-01-20T13:20:40Z","snapshot_observed_at":"2026-08-08T16:40:29.710429Z","submitted_at":"2021-07-26T12:05:34Z","title":"Complete One-loop Matching of the Type-I Seesaw Model onto the Standard Model Effective Field Theory","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2107.12133","snapshot_observed_at":"2026-08-12T05:35:37.921259Z","title":"Zhang and S","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":55,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.921259Z"},"links":{"cited_paper":"/paper/2107.12133","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:14d6099ecc6e056bbf37ccee4095dc6968b30d963e90a5cc3229af3eab6c94d6","observation_id":"630ae172-6bc8-4bdf-91af-e8ea5563ceec","resolution":{"observed_at":"2026-08-12T05:35:37.921259Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2108.01094","last_updated":"2021-08-02T18:00:07Z","snapshot_observed_at":"2026-08-02T16:34:30.031061Z","submitted_at":"2021-08-02T18:00:07Z","title":"From Models to SMEFT and Back?","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2108.01094","snapshot_observed_at":"2026-08-12T05:35:37.924283Z","title":"Brivio, S","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":56,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.924283Z"},"links":{"cited_paper":"/paper/2108.01094","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:7af3b5e84e71459aea6e7719cec30428755d02527a099886ab4595331ba515c9","observation_id":"8fc0ace7-36b9-4adf-9ca0-b479c7130c29","resolution":{"observed_at":"2026-08-12T05:35:37.924283Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2108.10055","last_updated":"2021-11-12T07:28:13Z","snapshot_observed_at":"2026-07-06T11:40:40.005168Z","submitted_at":"2021-08-23T10:46:08Z","title":"Universal Scalar Leptoquark Action for Matching","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2108.10055","snapshot_observed_at":"2026-08-12T05:35:37.927360Z","title":"Dedes and K","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":57,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.927360Z"},"links":{"cited_paper":"/paper/2108.10055","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:3310e98c415e57da15e7e76049ad2c2ea8c8b57d5f4b5149ea839d7bb1b7c892","observation_id":"2f4dcbee-4001-4487-8741-389756b91454","resolution":{"observed_at":"2026-08-12T05:35:37.927360Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2110.06929","last_updated":"2021-11-12T13:45:00Z","snapshot_observed_at":"2026-08-10T02:38:25.583364Z","submitted_at":"2021-10-13T18:00:00Z","title":"The Impact of Dimension-8 SMEFT Contributions: A Case Study","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2110.06929","snapshot_observed_at":"2026-08-12T05:35:37.930598Z","title":"Dawson, S","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":58,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.930598Z"},"links":{"cited_paper":"/paper/2110.06929","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:1710838b67b551c5f4d54573d7cb50c83bd7513a6a679adb2cb65e4157682633","observation_id":"4f985405-47da-4597-a4e8-2b5118852937","resolution":{"observed_at":"2026-08-12T05:35:37.930598Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2201.04646","last_updated":"2022-06-28T07:07:50Z","snapshot_observed_at":"2026-08-09T15:51:20.587281Z","submitted_at":"2022-01-12T19:00:07Z","title":"Neutrino seesaw models at one-loop matching: Discrimination by effective operators","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2201.04646","snapshot_observed_at":"2026-08-12T05:35:37.933589Z","title":"Du, X.-X","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":59,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.933589Z"},"links":{"cited_paper":"/paper/2201.04646","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:f5f6ca924d4e59cb2de5fae8c53c80d373f4e8858bc63813fcc7cc3ca33c520b","observation_id":"83e04142-29b7-4a2f-ab4d-7ee0cb213aa7","resolution":{"observed_at":"2026-08-12T05:35:37.933589Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2201.05082","last_updated":"2022-03-22T12:37:24Z","snapshot_observed_at":"2026-08-09T22:44:54.373739Z","submitted_at":"2022-01-13T17:07:48Z","title":"One-loop Matching of the Type-II Seesaw Model onto the Standard Model Effective Field Theory","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2201.05082","snapshot_observed_at":"2026-08-12T05:35:37.936723Z","title":null,"venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":60,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.936723Z"},"links":{"cited_paper":"/paper/2201.05082","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:09918faecbbc06c9f1e818b0f390fb9c2255bfb8d9621aad9612f72b1b0c804f","observation_id":"8d006684-7e28-49e8-88c1-f7aae4fa4480","resolution":{"observed_at":"2026-08-12T05:35:37.936723Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2205.01561","last_updated":"2023-05-11T13:40:27Z","snapshot_observed_at":"2026-08-06T16:40:06.493187Z","submitted_at":"2022-05-03T15:27:03Z","title":"Role of dimension-eight operators in an EFT for the 2HDM","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2205.01561","snapshot_observed_at":"2026-08-12T05:35:37.939858Z","title":"Dawson, D","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":61,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.939858Z"},"links":{"cited_paper":"/paper/2205.01561","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:61b66272588e344a345358422f5c9858de15e49db7fad72dba194010a10727c1","observation_id":"15814c4b-87e2-48e5-9aaa-a08bd5c39fa6","resolution":{"observed_at":"2026-08-12T05:35:37.939858Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2208.07869","last_updated":"2023-03-28T14:57:52Z","snapshot_observed_at":"2026-07-06T13:42:24.750714Z","submitted_at":"2022-08-16T17:53:46Z","title":"Complete One-loop Structure of the Type-(I+II) Seesaw Effective Field Theory","version":2},"cited_work":{"arxiv_id":"2208.07869","doi":null,"metadata_source":"pith","pith_arxiv_id":"2208.07869","snapshot_observed_at":"2026-08-12T05:35:38.259762Z","title":"Complete One-loop Structure of the Type-(I+II) Seesaw Effective Field Theory","venue":"hep-ph","work_id":"3e23fa38-b242-49aa-a748-cdacc528496b","year":2022},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":62,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.942841Z"},"links":{"cited_paper":"/paper/2208.07869","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:26c485c6fd920ed32267a5bcfb7ee5005130d55fdc116ff7bf0c8b677e09928d","observation_id":"67e2372d-f095-4a89-b2d5-c94d6c31a41e","resolution":{"observed_at":"2026-08-12T05:35:38.263117Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-12T06:34:41.77262+00:00","source":"crossref"},{"observed_at":"2026-08-12T06:34:36.333875+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2210.04270","last_updated":"2022-12-03T02:38:52Z","snapshot_observed_at":"2026-08-10T03:58:54.473178Z","submitted_at":"2022-10-09T14:05:17Z","title":"One-loop Matching of Scotogenic Model onto Standard Model Effective Field Theory up to Dimension 7","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2210.04270","snapshot_observed_at":"2026-08-12T05:35:37.946059Z","title":"Liao and X.-D","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":63,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.946059Z"},"links":{"cited_paper":"/paper/2210.04270","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:d19a1e295ad62b2363b89eeb12c5d3fd2c53d3b217492472f6c35468e944b179","observation_id":"324ccdbe-1809-4580-914b-ef8334c8bca7","resolution":{"observed_at":"2026-08-12T05:35:37.946059Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2304.06663","last_updated":"2023-04-13T16:51:11Z","snapshot_observed_at":"2026-08-09T04:01:36.111137Z","submitted_at":"2023-04-13T16:51:11Z","title":"Dimension-8 SMEFT Analysis of Minimal Scalar Field Extensions of the Standard Model","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2304.06663","snapshot_observed_at":"2026-08-12T05:35:37.949362Z","title":"Ellis, K","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":64,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.949362Z"},"links":{"cited_paper":"/paper/2304.06663","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:4fbfdc499e1d8de13022442bfc6d184596471c80986d1dd4eb2196c902b6a681","observation_id":"6345f780-c1d6-46b5-ace5-b4ab572a32b3","resolution":{"observed_at":"2026-08-12T05:35:37.949362Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2305.07689","last_updated":"2023-09-11T13:10:12Z","snapshot_observed_at":"2026-07-06T15:26:38.838948Z","submitted_at":"2023-05-12T18:00:00Z","title":"Matching the 2HDM to the HEFT and the SMEFT: Decoupling and Perturbativity","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2305.07689","snapshot_observed_at":"2026-08-12T05:35:37.952216Z","title":"Dawson, D","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":65,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.952216Z"},"links":{"cited_paper":"/paper/2305.07689","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:423084ef50069b9c19199c8fc1163bb496084d9de744bbb8246b3639e7e51f4a","observation_id":"6139b2ff-3065-4107-b3e5-537de87152a5","resolution":{"observed_at":"2026-08-12T05:35:37.952216Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2307.10380","last_updated":"2023-07-19T18:00:06Z","snapshot_observed_at":"2026-08-05T21:10:55.372933Z","submitted_at":"2023-07-19T18:00:06Z","title":"A complete tree-level dictionary between simplified BSM models and SMEFT (d $\\leq$ 7) operators","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2307.10380","snapshot_observed_at":"2026-08-12T05:35:37.955364Z","title":null,"venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":66,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.955364Z"},"links":{"cited_paper":"/paper/2307.10380","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:17b54ba989deebce80974529286a7d2417aaddc53a4cae8b9df8d1adebe3f915","observation_id":"03e9300c-2dc8-4684-af3f-ac0c5e6a211d","resolution":{"observed_at":"2026-08-12T05:35:37.955364Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2309.14702","last_updated":"2023-09-26T06:41:07Z","snapshot_observed_at":"2026-07-06T16:23:41.780696Z","submitted_at":"2023-09-26T06:41:07Z","title":"One-loop Matching of the Type-III Seesaw Model onto the Standard Model Effective Field Theory","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2309.14702","snapshot_observed_at":"2026-08-12T05:35:37.958476Z","title":"Li and S","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":67,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.958476Z"},"links":{"cited_paper":"/paper/2309.14702","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:c57e8e88609cc5a3baf8c82f2010ea8b6d5673498ce357e0bfc7b6b9ada3903b","observation_id":"adf7fd47-5631-41b6-940f-8e5c7e127432","resolution":{"observed_at":"2026-08-12T05:35:37.958476Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2401.12279","last_updated":"2024-04-12T14:15:03Z","snapshot_observed_at":"2026-08-13T04:37:30.173411Z","submitted_at":"2024-01-22T19:00:00Z","title":"Relevance of one-loop SMEFT matching in the 2HDM","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2401.12279","snapshot_observed_at":"2026-08-12T05:35:37.961605Z","title":"Das Bakshi, S","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":68,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.961605Z"},"links":{"cited_paper":"/paper/2401.12279","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:74e309c5620729091d777ad31090c3decf8427cdadd98ed6dc2645610447acdb","observation_id":"3e0e9165-bc4f-4987-8ec9-1bde15073cca","resolution":{"observed_at":"2026-08-12T05:35:37.961605Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2404.01375","last_updated":"2024-07-24T16:10:48Z","snapshot_observed_at":"2026-08-13T00:39:53.846124Z","submitted_at":"2024-04-01T18:00:01Z","title":"SMEFT Matching to $Z^\\prime$ Models at Dimension-8","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2404.01375","snapshot_observed_at":"2026-08-12T05:35:37.964731Z","title":"Dawson, M","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":69,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.964731Z"},"links":{"cited_paper":"/paper/2404.01375","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:c7d3ed2eafd752c4bf8bc73b7f97be4f913902916eeb159f38ab39db82e657bc","observation_id":"b83ad200-9fbd-4bf0-ba7e-9a19195c1b51","resolution":{"observed_at":"2026-08-12T05:35:37.964731Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1710.06445","last_updated":"2018-08-08T12:49:38Z","snapshot_observed_at":"2026-08-08T09:07:32.559590Z","submitted_at":"2017-10-17T18:00:34Z","title":"MatchingTools: a Python library for symbolic effective field theory calculations","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1710.06445","snapshot_observed_at":"2026-08-12T05:35:37.967988Z","title":null,"venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":70,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.967988Z"},"links":{"cited_paper":"/paper/1710.06445","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:a844925b81cba6cbef3365c37400f37b90b7fe506bc77cf087e36a17b9b04525","observation_id":"414c83d8-9bff-4782-a462-9023633f36e3","resolution":{"observed_at":"2026-08-12T05:35:37.967988Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1808.04403","last_updated":"2018-08-16T19:03:50Z","snapshot_observed_at":"2026-07-06T06:55:27.331336Z","submitted_at":"2018-08-13T18:55:00Z","title":"CoDEx: Wilson coefficient calculator connecting SMEFT to UV theory","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1808.04403","snapshot_observed_at":"2026-08-12T05:35:37.971082Z","title":"Das Bakshi, J","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":71,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.971082Z"},"links":{"cited_paper":"/paper/1808.04403","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:3d8a69822c746057f84fd56409aa213ef1f8e25227a34d357bdceb13d55e997d","observation_id":"50011037-f27d-4ed2-b5f2-0743e536d16d","resolution":{"observed_at":"2026-08-12T05:35:37.971082Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2212.04510","last_updated":"2023-07-28T15:45:48Z","snapshot_observed_at":"2026-08-10T12:44:28.515858Z","submitted_at":"2022-12-08T19:00:01Z","title":"A Proof of Concept for Matchete: An Automated Tool for Matching Effective Theories","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2212.04510","snapshot_observed_at":"2026-08-12T05:35:37.974265Z","title":"Fuentes-Martín, M","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":72,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.974265Z"},"links":{"cited_paper":"/paper/2212.04510","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:021b5e668d8f11b7a882578341db04d5d012c2e9518aead2062c96774d9ea26e","observation_id":"0edaab02-d73b-4277-895b-71a73776d05b","resolution":{"observed_at":"2026-08-12T05:35:37.974265Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2112.10787","last_updated":"2021-12-20T19:00:01Z","snapshot_observed_at":"2026-08-10T09:23:43.874801Z","submitted_at":"2021-12-20T19:00:01Z","title":"Matchmakereft: automated tree-level and one-loop matching","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2112.10787","snapshot_observed_at":"2026-08-12T05:35:37.977417Z","title":"Carmona, A","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":73,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.977417Z"},"links":{"cited_paper":"/paper/2112.10787","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:e1e9f562373bac71acfaf297601377bd6ef6460fbb3c0033b6f319790e0dec30","observation_id":"57ca465b-d1fd-462d-84fc-98a09f0189e8","resolution":{"observed_at":"2026-08-12T05:35:37.977417Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1306.4655","last_updated":"2013-11-04T10:51:42Z","snapshot_observed_at":"2026-07-06T03:16:20.483507Z","submitted_at":"2013-06-19T19:34:59Z","title":"Light top partners and precision physics","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1306.4655","snapshot_observed_at":"2026-08-12T05:35:37.980379Z","title":"Grojean, O","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":74,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.980379Z"},"links":{"cited_paper":"/paper/1306.4655","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:60480898098ad0f9b05942412e7a9cf56ca89eb9e26c1230039e4a98c1a4c9e5","observation_id":"c1fb50de-ee6c-464c-852b-0ef089b54393","resolution":{"observed_at":"2026-08-12T05:35:37.980379Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1409.1589","last_updated":"2014-12-14T19:32:36Z","snapshot_observed_at":"2026-07-06T03:53:32.549552Z","submitted_at":"2014-09-04T20:02:39Z","title":"Sigma Decomposition","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1409.1589","snapshot_observed_at":"2026-08-12T05:35:37.983658Z","title":"Alonso, I","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":75,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.983658Z"},"links":{"cited_paper":"/paper/1409.1589","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:620881062e9cc912421397ace24e2e6bdf484b50cad7c5deda552b092e1942cc","observation_id":"51f78100-0170-41db-9e8f-7bad6035a44b","resolution":{"observed_at":"2026-08-12T05:35:37.983658Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1510.07899","last_updated":"2016-04-01T16:05:49Z","snapshot_observed_at":"2026-07-06T04:34:24.209561Z","submitted_at":"2015-10-27T13:33:55Z","title":"Sigma Decomposition: The CP-Odd Lagrangian","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1510.07899","snapshot_observed_at":"2026-08-12T05:35:37.986726Z","title":null,"venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":76,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.986726Z"},"links":{"cited_paper":"/paper/1510.07899","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:73c687f2c1d78518e7986a9b3d7731d385dc03b2a64f853f08476634b512060f","observation_id":"b09303b4-f919-4f17-aff9-2a906c91af0f","resolution":{"observed_at":"2026-08-12T05:35:37.986726Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1610.08083","last_updated":"2016-10-25T20:28:19Z","snapshot_observed_at":"2026-07-06T05:16:01.203345Z","submitted_at":"2016-10-25T20:28:19Z","title":"The linear-non-linear frontier for the Goldstone Higgs","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1610.08083","snapshot_observed_at":"2026-08-12T05:35:37.990073Z","title":null,"venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":77,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.990073Z"},"links":{"cited_paper":"/paper/1610.08083","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:ebc5a065b3b3c05d1adb6b068eedf27ed82ac041b64562ee431fafb8bbcd76ba","observation_id":"95a9e5ab-131b-4a76-b08a-efaf768f250e","resolution":{"observed_at":"2026-08-12T05:35:37.990073Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1912.13058","last_updated":"2019-12-30T19:00:04Z","snapshot_observed_at":"2026-07-06T08:47:39.805429Z","submitted_at":"2019-12-30T19:00:04Z","title":"Effective Field Theory Perspective on Next-to-Minimal Composite Higgs","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1912.13058","snapshot_observed_at":"2026-08-12T05:35:37.993109Z","title":"Qi, J.-H","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":78,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.993109Z"},"links":{"cited_paper":"/paper/1912.13058","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:77a39d61808c400b7acf9f1d966ae794d9ce5d009a4b203d858c82f4f3700bf2","observation_id":"208cf91f-7968-46aa-915d-878b6660d093","resolution":{"observed_at":"2026-08-12T05:35:37.993109Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2201.05122","last_updated":"2022-04-17T20:32:39Z","snapshot_observed_at":"2026-08-12T22:24:16.087584Z","submitted_at":"2022-01-13T18:27:13Z","title":"Matching to Higgs-Compositeness and Renormalization of the Higgs-Electroweak Chiral Lagrangian extended by a Scalar Singlet","version":2},"cited_work":{"arxiv_id":"2201.05122","doi":null,"metadata_source":"pith","pith_arxiv_id":"2201.05122","snapshot_observed_at":"2026-08-12T05:35:38.127708Z","title":"Matching to Higgs-Compositeness and Renormalization of the Higgs-Electroweak Chiral Lagrangian extended by a Scalar Singlet","venue":"hep-ph","work_id":"424cb69c-61c2-4fe1-80e4-91f18347ae08","year":2022},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":79,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.996288Z"},"links":{"cited_paper":"/paper/2201.05122","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:76f698b6ebbbe049f92dc88a61316ffb535ebda5b9bbfef693f7bd07076fcc07","observation_id":"bf8653de-5352-42d8-81d7-beb436303b97","resolution":{"observed_at":"2026-08-12T05:35:38.131106Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-12T06:34:41.77262+00:00","source":"crossref"},{"observed_at":"2026-08-12T06:34:36.333875+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1608.03564","last_updated":"2016-08-11T18:41:04Z","snapshot_observed_at":"2026-08-13T01:34:50.014386Z","submitted_at":"2016-08-11T18:41:04Z","title":"Standard Model Extended by a Heavy Singlet: Linear vs. Nonlinear EFT","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1608.03564","snapshot_observed_at":"2026-08-12T05:35:37.999560Z","title":"Buchalla, O","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":80,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:37.999560Z"},"links":{"cited_paper":"/paper/1608.03564","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:33e0034405a3de84f8e690897a40b7c4242bf41a90a3b9898a52fb2170bb7ef5","observation_id":"0a2b4526-c5f7-4caf-9d49-9a7ada8cfebf","resolution":{"observed_at":"2026-08-12T05:35:37.999560Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2311.16897","last_updated":"2024-02-27T19:55:11Z","snapshot_observed_at":"2026-08-13T05:15:17.762425Z","submitted_at":"2023-11-28T15:50:32Z","title":"Is the HEFT matching unique?","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2311.16897","snapshot_observed_at":"2026-08-12T05:35:38.002833Z","title":"Dawson, D","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":81,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:38.002833Z"},"links":{"cited_paper":"/paper/2311.16897","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:13d62c72939dc26264943a2d76fd532880c6165d74ef02e13cc79c40556cae69","observation_id":"058c26d6-171d-40c8-add4-2a13a5ce8196","resolution":{"observed_at":"2026-08-12T05:35:38.002833Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2304.09884","last_updated":"2023-04-19T18:00:01Z","snapshot_observed_at":"2026-08-11T12:59:32.469150Z","submitted_at":"2023-04-19T18:00:01Z","title":"Effective Field Theory of the Two Higgs Doublet Model","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2304.09884","snapshot_observed_at":"2026-08-12T05:35:38.005962Z","title":"Banta, T","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":82,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:38.005962Z"},"links":{"cited_paper":"/paper/2304.09884","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:fe93656ec06640d18756ddf2241e75012d1779d86b60b4b6af849978fc81b8f9","observation_id":"45d5a916-cbdc-4595-9c21-193dcbcc445c","resolution":{"observed_at":"2026-08-12T05:35:38.005962Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2307.15693","last_updated":"2023-07-28T17:38:49Z","snapshot_observed_at":"2026-07-06T15:59:56.179560Z","submitted_at":"2023-07-28T17:38:49Z","title":"Non-decoupling effects from heavy Higgs bosons by matching 2HDM to HEFT amplitudes","version":1},"cited_work":{"arxiv_id":"2307.15693","doi":null,"metadata_source":"pith","pith_arxiv_id":"2307.15693","snapshot_observed_at":"2026-08-12T05:35:38.090605Z","title":"Non-decoupling effects from heavy Higgs bosons by matching 2HDM to HEFT amplitudes","venue":"hep-ph","work_id":"27b5470c-bfd2-424b-a8d3-87f40eb2bbae","year":2023},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":83,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:38.009063Z"},"links":{"cited_paper":"/paper/2307.15693","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:dd2233baeeecb24307b70f6184a3d9461a74dce385a960686f6d53608a7c5642","observation_id":"5d169ae2-c45a-409d-b09a-5e7cebd72377","resolution":{"observed_at":"2026-08-12T05:35:38.095986Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-12T06:34:41.77262+00:00","source":"crossref"},{"observed_at":"2026-08-12T06:34:36.333875+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2312.13885","last_updated":"2024-09-11T15:35:29Z","snapshot_observed_at":"2026-08-13T04:56:45.556448Z","submitted_at":"2023-12-21T14:29:18Z","title":"Two-Higgs Doublet Model Matched to Nonlinear Effective Theory","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2312.13885","snapshot_observed_at":"2026-08-12T05:35:38.012187Z","title":"Buchalla, F","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":84,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:38.012187Z"},"links":{"cited_paper":"/paper/2312.13885","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:611083ae9cf0c4b31bbce1a6906877768b880ab5fe4645db4905b2bf08289fe9","observation_id":"f3fe6fbd-e55f-4e94-8690-652c6d6da104","resolution":{"observed_at":"2026-08-12T05:35:38.012187Z","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":"2026-08-12T05:35:38.015362Z","title":null,"venue":null,"work_id":null,"year":1969},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":85,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:38.015362Z"},"links":{"citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:c4ad42ff17e22eed42a29785b2c7258a459ca86637fcb2eeaa9083d24b7afb84","observation_id":"9c9b3ddb-564b-4690-bc46-65272c007ad3","resolution":{"observed_at":"2026-08-12T05:35:38.015362Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2402.06746","last_updated":"2024-06-06T15:43:23Z","snapshot_observed_at":"2026-08-13T04:22:18.312562Z","submitted_at":"2024-02-09T19:21:48Z","title":"Higgs boson off-shell measurements probe non-linearities","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2402.06746","snapshot_observed_at":"2026-08-12T05:35:38.018164Z","title":"Englert, R","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":86,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:38.018164Z"},"links":{"cited_paper":"/paper/2402.06746","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:1de14dbe46b4003d616b7dba62bb1d3a5c8d35aa6a983fa377ecd4a72ccf985b","observation_id":"ea9d2ef3-5404-4703-972f-d1745750797f","resolution":{"observed_at":"2026-08-12T05:35:38.018164Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2208.06760","last_updated":"2023-02-20T11:27:50Z","snapshot_observed_at":"2026-08-10T01:29:56.286812Z","submitted_at":"2022-08-14T02:40:49Z","title":"Electroweak precision tests for triplet scalars","version":5},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2208.06760","snapshot_observed_at":"2026-08-12T05:35:38.021440Z","title":"Cheng, X.-G","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":87,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:38.021440Z"},"links":{"cited_paper":"/paper/2208.06760","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:ebac3b731690c4be96472e660c5fac139e66e168845ab8eae7f4935e96835a5e","observation_id":"1b75118e-3710-4bee-a646-8901e23ecf3a","resolution":{"observed_at":"2026-08-12T05:35:38.021440Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1810.09450","last_updated":"2018-10-22T18:00:00Z","snapshot_observed_at":"2026-07-06T07:09:51.109116Z","submitted_at":"2018-10-22T18:00:00Z","title":"Type-II Seesaw Scalar Triplet Model at a 100 TeV $pp$ Collider: Discovery and Higgs Portal Coupling Determination","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1810.09450","snapshot_observed_at":"2026-08-12T05:35:38.024631Z","title":null,"venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":88,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:38.024631Z"},"links":{"cited_paper":"/paper/1810.09450","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:2fa14b13d35bf896fcb99896df864955f6673cefa630520b35ff5087c38c3277","observation_id":"7d4b709c-6d81-4a8f-a1f7-ed7c3e8f8fa0","resolution":{"observed_at":"2026-08-12T05:35:38.024631Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2206.01479","last_updated":"2023-08-15T15:35:16Z","snapshot_observed_at":"2026-07-06T13:17:04.885030Z","submitted_at":"2022-06-03T10:08:45Z","title":"Electroweak renormalization based on gauge-invariant vacuum expectation values of non-linear Higgs representations: 2. extended Higgs sectors","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2206.01479","snapshot_observed_at":"2026-08-12T05:35:38.027810Z","title":"Dittmaier and H","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching","version":1},"reference_index":89,"source":"pdf_text","source_observed_at":"2026-08-12T05:35:38.027810Z"},"links":{"cited_paper":"/paper/2206.01479","citing_paper":"/paper/2412.00355"},"observation_digest":"sha256:34d6e5cc4840491a5add7cfe7e35947b63ee75461b832b51ff6c8bddf86972eb","observation_id":"d4f3fd4e-5b6d-4c75-abce-31c17c1cae08","resolution":{"observed_at":"2026-08-12T05:35:38.027810Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"paper":{"arxiv_id":"2412.00355","last_updated":"2024-11-30T04:30:36Z","latest_version":1,"primary_category":"hep-ph","snapshot_observed_at":"2026-08-13T02:13:25.371282Z","submitted_at":"2024-11-30T04:30:36Z","title":"A Non-linear Representation of General Scalar Extensions of the Standard Model for HEFT Matching"},"reference_resolution":{"displayed":89,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":75,"verified_exact":14,"verified_fuzzy":0},"total_outbound_references":89},"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":"2026-08-12T06:34:41.77262+00:00","source":"crossref"},{"observed_at":"2026-08-12T06:34:36.333875+00:00","source":"retraction_watch"}],"thesis":"As of 13 August 2026, this Paper Citation Record lists 89 of 89 outbound references and 2 inbound Pith citation observations for arXiv:2412.00355."}