{"as_of":"2026-08-15T15:49:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:e3ee299d8cd123d0b16ba737c2fff1609117946c379375ac98223c08d8ce5e81","coverage":[{"denominator":138,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":100,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-14T12:20:59.971408Z","state":"measured"},{"denominator":100,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":100,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-15T06:32:42.880941+00:00","state":"measured"},{"denominator":0,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":0,"source":"paper_references, paper_reference_links","source_observed_at":null,"state":"measured"},{"denominator":1,"lane":"external_citation_measurements","note":"A source-named dated measurement, never combined with another source.","records_observed":0,"source":"cited_works","source_observed_at":null,"state":"measured"}],"external_citation_measurements":[],"inbound":[],"links":{"evidence":"/evidence","html":"/paper/1908.07596/citation-record","integrity":"/paper/1908.07596/integrity","json":"/paper/1908.07596/citation-record.json","paper":"/paper/1908.07596"},"outbound":[{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T12:20:58.759732Z","title":null,"venue":null,"work_id":null,"year":1961},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:58.759732Z"},"links":{"citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:4eb0f35693c3afe424b13bf4ce8b1ab63d72974deff08a3e8186d90993df64f4","observation_id":"8c275f68-d8f8-4a1f-b4fc-531f27e49827","resolution":{"observed_at":"2026-08-14T12:20:58.759732Z","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":"2026-08-14T12:20:58.776351Z","title":"Weinberg, Phys","venue":null,"work_id":null,"year":1967},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:58.776351Z"},"links":{"citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:c665602bdd1723e8e9876de72a16d2db047764954d92f4bed2f0a04f5e7981de","observation_id":"441992a0-8280-49ef-8d58-2abe24b1f69e","resolution":{"observed_at":"2026-08-14T12:20:58.776351Z","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":"2026-08-14T12:20:58.789774Z","title":"Salam, Conf","venue":null,"work_id":null,"year":1968},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:58.789774Z"},"links":{"citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:de02c10a3cb7c4a30da1df844302478372d52e779c16477735308996d825773e","observation_id":"ba510a75-10ec-4d6e-a0e8-8e4077f95ccd","resolution":{"observed_at":"2026-08-14T12:20:58.789774Z","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":"2026-08-14T12:20:58.799238Z","title":"’t Hooft and M","venue":null,"work_id":null,"year":1972},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:58.799238Z"},"links":{"citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:e5020e4ca3f596ed8278371b1bf5e58d860b36e975c8ca2be2718c636dff0a87","observation_id":"695a4555-a4b6-47f6-abd1-e47b23aa8a23","resolution":{"observed_at":"2026-08-14T12:20:58.799238Z","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":"2026-08-14T12:20:58.808727Z","title":"Englert and R","venue":null,"work_id":null,"year":1964},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:58.808727Z"},"links":{"citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:735711cfcd40512249043c80444ee89cf9f6f1bfe460ad6f683bd604cf6a8365","observation_id":"a21e4611-2d42-4568-90c0-2cf413d2b5c0","resolution":{"observed_at":"2026-08-14T12:20:58.808727Z","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":"2026-08-14T12:20:58.818708Z","title":null,"venue":null,"work_id":null,"year":1964},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:58.818708Z"},"links":{"citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:07fec6bddd5df7be12968a9aec533492dcb88cb2a52594497df4d14f19526127","observation_id":"3bea6a5d-a4e9-415d-b449-756805c8a568","resolution":{"observed_at":"2026-08-14T12:20:58.818708Z","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":"2026-08-14T12:20:58.830440Z","title":null,"venue":null,"work_id":null,"year":1964},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:58.830440Z"},"links":{"citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:b88a89e8d75ad86e865475940554be834414a0781cfa8de79661d563089a3d83","observation_id":"0e073530-ae57-4890-8f00-574464ce876f","resolution":{"observed_at":"2026-08-14T12:20:58.830440Z","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":"2026-08-14T12:20:58.840300Z","title":null,"venue":null,"work_id":null,"year":1964},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:58.840300Z"},"links":{"citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:c4cdb713caea50accc84a1011928d0485eb6fcf6e328779754a735d4289e546d","observation_id":"c6a6dc81-bb0a-4e2c-af2d-4b245eb0d8a0","resolution":{"observed_at":"2026-08-14T12:20:58.840300Z","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":"2026-08-14T12:20:58.850237Z","title":null,"venue":null,"work_id":null,"year":1966},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:58.850237Z"},"links":{"citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:4597e33ec1143956fc63ea67049f0c91b3ea725fbffd90fa16597df292c88558","observation_id":"300ba303-74f3-42fc-b57d-ef73682de0b7","resolution":{"observed_at":"2026-08-14T12:20:58.850237Z","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":"2026-08-14T12:20:58.857233Z","title":null,"venue":null,"work_id":null,"year":1967},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:58.857233Z"},"links":{"citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:87e476c43d16c2eef4aeb8610b449a125b109d341e1313f28836f4a8d9183252","observation_id":"8e144c4d-d79b-4e62-a037-7fd98093d68c","resolution":{"observed_at":"2026-08-14T12:20:58.857233Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1804.05863","last_updated":"2018-04-16T18:01:13Z","snapshot_observed_at":"2026-08-14T19:25:25.923614Z","submitted_at":"2018-04-16T18:01:13Z","title":"Introduction to Effective Field Theories","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1804.05863","snapshot_observed_at":"2026-08-14T12:20:58.871487Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:58.871487Z"},"links":{"cited_paper":"/paper/1804.05863","citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:6b160f5ebd4f8566c817f4055bb575cc76e14b8ea8c5e0e476ecea728e80ebf1","observation_id":"303f71e2-5d9c-49b1-9705-1b42ca29ae9e","resolution":{"observed_at":"2026-08-14T12:20:58.871487Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1512.08749","last_updated":"2015-12-29T18:38:24Z","snapshot_observed_at":"2026-08-14T22:16:38.461180Z","submitted_at":"2015-12-29T18:38:24Z","title":"Electroweak Symmetry Breaking and the Higgs Boson","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1512.08749","snapshot_observed_at":"2026-08-14T12:20:58.883303Z","title":"Pich, Acta Phys","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:58.883303Z"},"links":{"cited_paper":"/paper/1512.08749","citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:c9f8f8e9fc3d59ae0cabbfc3025964b20092754a8d6e25f812963935895c9379","observation_id":"a0e24ba0-624b-4c7a-b4f1-2062bd686b9f","resolution":{"observed_at":"2026-08-14T12:20:58.883303Z","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":"2026-08-14T12:20:58.890693Z","title":"Buchmuller and D","venue":null,"work_id":null,"year":1986},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:58.890693Z"},"links":{"citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:0802c3486e3062a9682a15ff6cdc2ad3a095f86eee8d9cc4c1d7050e014a2662","observation_id":"d5f67eb0-62f3-481e-8bed-0fd4d0af6f2d","resolution":{"observed_at":"2026-08-14T12:20:58.890693Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1008.4884","last_updated":"2017-01-15T20:19:22Z","snapshot_observed_at":"2026-08-12T14:13:27.638436Z","submitted_at":"2010-08-28T19:19:07Z","title":"Dimension-Six Terms in the Standard Model Lagrangian","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1008.4884","snapshot_observed_at":"2026-08-14T12:20:58.897843Z","title":"Grzadkowski, M","venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:58.897843Z"},"links":{"cited_paper":"/paper/1008.4884","citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:e291668168615424b8d79e3bda5fbb965883cc3d223438a5a1fd5b3f25ed105c","observation_id":"a363bbcd-7c37-4379-a1b3-95c10e7dd153","resolution":{"observed_at":"2026-08-14T12:20:58.897843Z","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":"2026-08-14T12:20:58.903636Z","title":"Feruglio, Int","venue":null,"work_id":null,"year":1993},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:58.903636Z"},"links":{"cited_paper":"/paper/hep-ph/9301281","citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:f8578505e0d92d5e0fb2243542fa08f0b649e29761e6a9f0d410875da7e5826a","observation_id":"003fbb7b-3186-4ce2-a140-f1670e456359","resolution":{"observed_at":"2026-08-14T12:20:58.903636Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0704.1505","last_updated":"2007-09-06T03:27:12Z","snapshot_observed_at":"2026-08-15T10:42:51.920666Z","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":"2026-08-14T12:20:58.912853Z","title":"Grinstein and M","venue":null,"work_id":null,"year":2007},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:58.912853Z"},"links":{"cited_paper":"/paper/0704.1505","citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:c7b7292ebd291df011db75e677bc99fa02d298e27469e0421214ecf10fd76e00","observation_id":"c18ff75d-5d1c-4e11-a4ec-66f20be4dfec","resolution":{"observed_at":"2026-08-14T12:20:58.912853Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1002.1011","last_updated":"2010-05-24T20:04:26Z","snapshot_observed_at":"2026-08-15T05:27:22.513426Z","submitted_at":"2010-02-04T15:07:36Z","title":"Strong Double Higgs Production at the LHC","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1002.1011","snapshot_observed_at":"2026-08-14T12:20:58.923089Z","title":"Contino, C","venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:58.923089Z"},"links":{"cited_paper":"/paper/1002.1011","citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:cd01576d7a7e11a0770b7e2eea85f616b9b4a4827bc2736ee219525558de21ea","observation_id":"a44e387b-689f-4854-8101-ad341cfcc610","resolution":{"observed_at":"2026-08-14T12:20:58.923089Z","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":"2026-08-15T00:35:47.869181Z","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":"2026-08-14T12:20:58.939124Z","title":"Alonso, M","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:58.939124Z"},"links":{"cited_paper":"/paper/1212.3305","citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:895503e449a8de143fe13227af12ef8c19d8a439cce84ba8237e606a166bae0f","observation_id":"a255b2bd-1974-4f08-b452-924a79728f29","resolution":{"observed_at":"2026-08-14T12:20:58.939124Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1212.3307","last_updated":"2013-09-19T14:54:53Z","snapshot_observed_at":"2026-08-15T00:35:47.726484Z","submitted_at":"2012-12-13T20:28:44Z","title":"Flavour with a Light Dynamical \"Higgs Particle\"","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1212.3307","snapshot_observed_at":"2026-08-14T12:20:58.952328Z","title":"Alonso, M","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:58.952328Z"},"links":{"cited_paper":"/paper/1212.3307","citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:049b0a4bbd7fd2b49779dbd5409e917efb00c187bd0a10d9c2066b7e0eb1c8ce","observation_id":"2f7bcf3b-b0a0-4202-87d5-76e446bd5603","resolution":{"observed_at":"2026-08-14T12:20:58.952328Z","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":"2026-08-15T00:09:52.760166Z","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":"2026-08-14T12:20:58.961305Z","title":"Buchalla, O","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:58.961305Z"},"links":{"cited_paper":"/paper/1307.5017","citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:3ebc6d70c01da8808ff52ff113b809842911101450f2e3dc2838fa284132b969","observation_id":"a66dbf91-8af3-431f-b89e-75fad3eaa336","resolution":{"observed_at":"2026-08-14T12:20:58.961305Z","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":"2026-08-14T23:56:03.620165Z","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":"2026-08-14T12:20:58.972239Z","title":"Brivio, T","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:58.972239Z"},"links":{"cited_paper":"/paper/1311.1823","citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:2863ffc6b6e8c621f466dcebefc4041491df6ace7e9f7862537fd4bd96cc1d5c","observation_id":"6b837a4a-3b02-47ba-bfbd-b92a76798727","resolution":{"observed_at":"2026-08-14T12:20:58.972239Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1405.5412","last_updated":"2014-12-04T10:54:09Z","snapshot_observed_at":"2026-08-14T23:33:14.117672Z","submitted_at":"2014-05-21T13:26:44Z","title":"Higgs ultraviolet softening","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1405.5412","snapshot_observed_at":"2026-08-14T12:20:58.979484Z","title":"Brivio, O","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:58.979484Z"},"links":{"cited_paper":"/paper/1405.5412","citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:bf46af3eb2569e721c04a0577fb2176101c130bde3dc1fa3aada84ec72c2a1df","observation_id":"f79d81ed-63c9-43c3-8d6b-dab14c75bd47","resolution":{"observed_at":"2026-08-14T12:20:58.979484Z","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":"2026-08-14T23:29:12.534661Z","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":"2026-08-14T12:20:58.988522Z","title":null,"venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:58.988522Z"},"links":{"cited_paper":"/paper/1406.6367","citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:491e7997075344d4996142f02e86e5efd7a9749255739a4f0428808fce70a35d","observation_id":"05f03473-6ff7-430d-9bfa-30d8c075cb67","resolution":{"observed_at":"2026-08-14T12:20:58.988522Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1409.1571","last_updated":"2014-09-04T20:00:02Z","snapshot_observed_at":"2026-08-14T23:20:42.318493Z","submitted_at":"2014-09-04T20:00:02Z","title":"On the renormalization of the electroweak chiral Lagrangian with a Higgs","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1409.1571","snapshot_observed_at":"2026-08-14T12:20:58.998756Z","title":null,"venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:58.998756Z"},"links":{"cited_paper":"/paper/1409.1571","citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:7ef9ae6a283be7c97312b7ec868cfd37ee99f0b6b5b83deca13669c991870954","observation_id":"592b2ddc-59f1-41e9-ba9a-8f38e4744c1e","resolution":{"observed_at":"2026-08-14T12:20:58.998756Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1604.03555","last_updated":"2016-04-12T20:00:06Z","snapshot_observed_at":"2026-08-14T22:01:57.812399Z","submitted_at":"2016-04-12T20:00:06Z","title":"Mapping the genuine bosonic quartic couplings","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1604.03555","snapshot_observed_at":"2026-08-14T12:20:59.010649Z","title":null,"venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.010649Z"},"links":{"cited_paper":"/paper/1604.03555","citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:e8e7ced0181c2bb49b22f02c2102f6424d11836a257e7eec7a7b0d21c39f6c91","observation_id":"3f5cb5df-f043-424f-b77e-9201cb12459f","resolution":{"observed_at":"2026-08-14T12:20:59.010649Z","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":"2026-08-14T22:00:27.856919Z","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":"2026-08-14T12:20:59.019151Z","title":"Brivio, J","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.019151Z"},"links":{"cited_paper":"/paper/1604.06801","citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:62fe8fa67cdbe11c0dde875952cf66e362ef40458e4a8b484d36751acc1d44f8","observation_id":"c82614a8-7ad9-4931-8c82-98e4d967a6fe","resolution":{"observed_at":"2026-08-14T12:20:59.019151Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1610.07922","last_updated":"2017-05-15T16:42:19Z","snapshot_observed_at":"2026-08-14T21:33:38.030583Z","submitted_at":"2016-10-25T15:30:43Z","title":"Handbook of LHC Higgs Cross Sections: 4. Deciphering the Nature of the Higgs Sector","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1610.07922","snapshot_observed_at":"2026-08-14T12:20:59.029687Z","title":"de Florianet","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.029687Z"},"links":{"cited_paper":"/paper/1610.07922","citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:bd37abd2edb5926e3cff3e828d5952e588246bd889d67fe321561a8c89d85488","observation_id":"aa00879e-ab48-4e66-b3f8-b58fcd86aa57","resolution":{"observed_at":"2026-08-14T12:20:59.029687Z","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":"2026-08-14T21:25:25.859632Z","submitted_at":"2016-12-14T21:00:15Z","title":"Baryon Non-Invariant Couplings in Higgs Effective Field Theory","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1612.04832","snapshot_observed_at":"2026-08-14T12:20:59.040386Z","title":"Merlo, S","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.040386Z"},"links":{"cited_paper":"/paper/1612.04832","citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:8b5e8c5ee6218df35cb9c2981403bd2dac928036ed59f3f2fbd85f898b47b766","observation_id":"0a7fcd22-7fed-4eee-8559-88cfb22482aa","resolution":{"observed_at":"2026-08-14T12:20:59.040386Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1710.06412","last_updated":"2018-01-31T16:55:39Z","snapshot_observed_at":"2026-08-14T20:22:49.520887Z","submitted_at":"2017-10-17T17:42:33Z","title":"Complete One-Loop Renormalization of the Higgs-Electroweak Chiral Lagrangian","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1710.06412","snapshot_observed_at":"2026-08-14T12:20:59.053061Z","title":"Buchalla, O","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":29,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.053061Z"},"links":{"cited_paper":"/paper/1710.06412","citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:25eb5cd91c002bd7615a12329e36646acca1c9592c18eab8f96823e6c18645d5","observation_id":"17034c53-a964-48eb-8f5f-177ad7eb03f9","resolution":{"observed_at":"2026-08-14T12:20:59.053061Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1710.06848","last_updated":"2017-10-18T17:57:08Z","snapshot_observed_at":"2026-08-14T20:22:27.247364Z","submitted_at":"2017-10-18T17:57:08Z","title":"Renormalization group evolution of Higgs effective field theory","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1710.06848","snapshot_observed_at":"2026-08-14T12:20:59.066117Z","title":"Alonso, K","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.066117Z"},"links":{"cited_paper":"/paper/1710.06848","citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:731adc8aedd5822c3c771195cee115d45e5dd4daa73318332e354c234e95dc2f","observation_id":"ee2cd4ad-4f1d-4bb5-8306-4aa62f8850e1","resolution":{"observed_at":"2026-08-14T12:20:59.066117Z","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":"2026-08-14T22:28:21.515441Z","submitted_at":"2015-10-12T00:05:38Z","title":"Low-energy signals of strongly-coupled electroweak symmetry-breaking scenarios","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1510.03114","snapshot_observed_at":"2026-08-14T12:20:59.079987Z","title":null,"venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.079987Z"},"links":{"cited_paper":"/paper/1510.03114","citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:59ffa0e634fd3a427a3503aa23615181111481b8bec2a5ab2022782702874019","observation_id":"a5ede393-990b-4883-944b-567db8d9c068","resolution":{"observed_at":"2026-08-14T12:20:59.079987Z","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":"2026-08-14T21:38:48.014033Z","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":"2026-08-14T12:20:59.095117Z","title":null,"venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":32,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.095117Z"},"links":{"cited_paper":"/paper/1609.06659","citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:69eb3314016dfca5cbb906514561c87379f705f9b5ccbaa63ed9bbb0d15f90b6","observation_id":"e3c9ebb1-0827-4223-aba2-a0ca54229039","resolution":{"observed_at":"2026-08-14T12:20:59.095117Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0812.1594","last_updated":"2022-05-24T09:22:41Z","snapshot_observed_at":"2026-08-15T05:59:41.925592Z","submitted_at":"2008-12-09T20:49:40Z","title":"Two-component spinor techniques and Feynman rules for quantum field theory and supersymmetry","version":6},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0812.1594","snapshot_observed_at":"2026-08-14T12:20:59.101664Z","title":null,"venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.101664Z"},"links":{"cited_paper":"/paper/0812.1594","citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:ccec16f78aaa83b9ae83d61636fadcf03fe4757b941365dd166971e0dc3497f7","observation_id":"46a0d6e9-b0b0-4403-b616-ed651dd0278d","resolution":{"observed_at":"2026-08-14T12:20:59.101664Z","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":"2026-08-14T12:20:59.109742Z","title":"Goldstone, Nuovo Cim.19, 154 (1961)","venue":null,"work_id":null,"year":1961},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":34,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.109742Z"},"links":{"citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:8eb693c4f71dc520bef82f451ffbf770997e84ec45eef53da183305148ec0b3d","observation_id":"44187d24-8be6-4ec5-b3a0-45cd4e9c882b","resolution":{"observed_at":"2026-08-14T12:20:59.109742Z","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":"2026-08-14T12:20:59.118229Z","title":"Nakamuraet al","venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.118229Z"},"links":{"citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:1a108d15873a01f797f68395648b4fb793eaa2e91b3b77789a2c6e437e8ef12f","observation_id":"337420ef-e2ad-4b0e-9f3a-26a0571d2c87","resolution":{"observed_at":"2026-08-14T12:20:59.118229Z","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":"2026-08-14T12:20:59.143617Z","title":"Nir, ”The Standard Model and Flavor Physics”, available at http://indico.ictp.it/event/7968/ (under ”The SM and Flavor”)","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":36,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.143617Z"},"links":{"citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:e9ba1ce82ae33199424888ec3f18768f968fe22193acf90176873d52d2d37567","observation_id":"a1def28c-5440-4608-9b1a-5d24ee5321b0","resolution":{"observed_at":"2026-08-14T12:20:59.143617Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1711.03624","last_updated":"2017-11-09T22:16:28Z","snapshot_observed_at":"2026-08-14T20:15:07.740040Z","submitted_at":"2017-11-09T22:16:28Z","title":"Just a Taste: Lectures on Flavor Physics","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1711.03624","snapshot_observed_at":"2026-08-14T12:20:59.158919Z","title":"Grossman and P","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":37,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.158919Z"},"links":{"cited_paper":"/paper/1711.03624","citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:2a48b8efe755e412dfc207382e9aac610fa206ce3fd4be84d5da169a6425b0b6","observation_id":"88b9f842-167f-4385-80c8-abc9daab64c5","resolution":{"observed_at":"2026-08-14T12:20:59.158919Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1201.0537","last_updated":"2012-01-02T21:26:31Z","snapshot_observed_at":"2026-08-15T04:23:59.791822Z","submitted_at":"2012-01-02T21:26:31Z","title":"The Standard Model of Electroweak Interactions","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1201.0537","snapshot_observed_at":"2026-08-14T12:20:59.170359Z","title":"Pich, arXiv:1201.0537 [hep-ph]","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":38,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.170359Z"},"links":{"cited_paper":"/paper/1201.0537","citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:ae15c4f16f63e9514b903ad1f48ced34eba01cbecb2e93dcf0d96de6084abc30","observation_id":"827ed067-536e-43b2-a848-7676a583f868","resolution":{"observed_at":"2026-08-14T12:20:59.170359Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0801.1134","last_updated":"2010-03-12T21:26:59Z","snapshot_observed_at":"2026-08-15T10:24:06.071178Z","submitted_at":"2008-01-07T23:30:23Z","title":"New Measurement of the Electron Magnetic Moment and the Fine Structure Constant","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0801.1134","snapshot_observed_at":"2026-08-14T12:20:59.184354Z","title":"Hanneke, S","venue":null,"work_id":null,"year":2008},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":39,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.184354Z"},"links":{"cited_paper":"/paper/0801.1134","citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:b5b98d8bf5251f23d3f8be479e2893004f05ad24e9e5802d7de98205ce09cca0","observation_id":"52d0c69b-c7af-4845-9252-85e505259214","resolution":{"observed_at":"2026-08-14T12:20:59.184354Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1110.0016","last_updated":"2011-10-22T16:04:37Z","snapshot_observed_at":"2026-08-15T04:33:35.045861Z","submitted_at":"2011-09-30T20:35:12Z","title":"Workshop on Precision Measurements of alphas","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1110.0016","snapshot_observed_at":"2026-08-14T12:20:59.190702Z","title":"Bethke et al., arXiv:1110.0016 [hep-ph]","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":40,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.190702Z"},"links":{"cited_paper":"/paper/1110.0016","citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:6f607eabcd6af920a01598b5a74b4e80889d0544c6b12a6ceb19943ebf64291e","observation_id":"e3679f5c-9ece-46dc-bcaa-eaa7b90eef5a","resolution":{"observed_at":"2026-08-14T12:20:59.190702Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1012.2367","last_updated":"2011-01-11T13:31:54Z","snapshot_observed_at":"2026-08-15T05:00:20.099876Z","submitted_at":"2010-12-10T20:11:15Z","title":"Precision Electroweak Measurements and Constraints on the Standard Model","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1012.2367","snapshot_observed_at":"2026-08-14T12:20:59.199984Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":41,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.199984Z"},"links":{"cited_paper":"/paper/1012.2367","citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:a535c9ef770792bf3279e85b8a53ee86657c3d9589d0835708484741ac8f2de5","observation_id":"c562cbb0-497f-488a-a792-593157c6d0a2","resolution":{"observed_at":"2026-08-14T12:20:59.199984Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1107.5255","last_updated":"2011-09-08T02:47:31Z","snapshot_observed_at":"2026-08-15T04:39:53.748701Z","submitted_at":"2011-07-26T16:18:13Z","title":"Combination of CDF and DO results on the mass of the top quark using up to 5.8~fb-1 of data","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1107.5255","snapshot_observed_at":"2026-08-14T12:20:59.210324Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":42,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.210324Z"},"links":{"cited_paper":"/paper/1107.5255","citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:8ff245a6b02be026d97b0d68ca2448c06a1a8b031fcac16ed337270222603f9b","observation_id":"ac75b70e-3aad-4992-b31b-fd55cd933eff","resolution":{"observed_at":"2026-08-14T12:20:59.210324Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1107.0975","last_updated":"2012-09-11T14:18:50Z","snapshot_observed_at":"2026-08-15T04:41:56.085997Z","submitted_at":"2011-07-05T20:00:05Z","title":"Updated Status of the Global Electroweak Fit and Constraints on New Physics","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1107.0975","snapshot_observed_at":"2026-08-14T12:20:59.219139Z","title":null,"venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":43,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.219139Z"},"links":{"cited_paper":"/paper/1107.0975","citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:6c2b053fb7fc754a0fed433a895b0a31f6d81dffcc1fb348d4a81ecf32d5661c","observation_id":"dab55414-2c5f-4962-a686-d7d7c7e3fb32","resolution":{"observed_at":"2026-08-14T12:20:59.219139Z","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":"2026-08-14T12:20:59.235249Z","title":"Aad et al","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":44,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.235249Z"},"links":{"cited_paper":"/paper/1207.7214","citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:23f6cbca02976210ab915ea9289f7dd3cf372ad05c8e6114281547f7de2d4743","observation_id":"fd0df7a9-1d43-40aa-94ec-3d72e8814c20","resolution":{"observed_at":"2026-08-14T12:20:59.235249Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1207.7235","last_updated":"2013-01-28T10:46:38Z","snapshot_observed_at":"2026-08-15T00:51:31.889320Z","submitted_at":"2012-07-31T13:27:18Z","title":"Observation of a new boson at a mass of 125 GeV with the CMS experiment at the LHC","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1207.7235","snapshot_observed_at":"2026-08-14T12:20:59.250018Z","title":"Chatrchyanet al","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":45,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.250018Z"},"links":{"cited_paper":"/paper/1207.7235","citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:4fcae7291460db228e77967e741c27ef728108f73e0b9ced4ee292661d0eed3e","observation_id":"9613ae9c-32ca-4884-ae18-c26393b2517f","resolution":{"observed_at":"2026-08-14T12:20:59.250018Z","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":"2026-08-14T12:20:59.279490Z","title":"Aad et al","venue":null,"work_id":null,"year":2008},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":46,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.279490Z"},"links":{"citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:736f327ad5ee4f66c4a5efe369402bc3b82752c405aad0da4c1ae3426b2f4d7f","observation_id":"9e258f67-c980-426e-b12a-52cf932dde0c","resolution":{"observed_at":"2026-08-14T12:20:59.279490Z","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":"2026-08-14T12:20:59.288683Z","title":"Chatrchyanet al","venue":null,"work_id":null,"year":2008},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":47,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.288683Z"},"links":{"citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:f8308be7fdb72bfc750999f11d7a027302d5b8b650f95c09b1cfa79e28e3fbe0","observation_id":"ec77a9d0-2ea0-4ac7-bd02-f93174d7dabd","resolution":{"observed_at":"2026-08-14T12:20:59.288683Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1503.07589","last_updated":"2015-03-26T00:44:34Z","snapshot_observed_at":"2026-08-14T22:54:52.954714Z","submitted_at":"2015-03-26T00:44:34Z","title":"Combined Measurement of the Higgs Boson Mass in $pp$ Collisions at $\\sqrt{s}=7$ and 8 TeV with the ATLAS and CMS Experiments","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1503.07589","snapshot_observed_at":"2026-08-14T12:20:59.298093Z","title":"Aad et al","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":48,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.298093Z"},"links":{"cited_paper":"/paper/1503.07589","citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:1d7ca6b2e123ffc676050e75d350e007c267fd891115dde2050df0ab2bc86bc0","observation_id":"f2b58e9a-540d-4d0a-9e5a-bd232cada24b","resolution":{"observed_at":"2026-08-14T12:20:59.298093Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1506.05669","last_updated":"2015-10-23T14:12:14Z","snapshot_observed_at":"2026-08-14T22:43:54.350790Z","submitted_at":"2015-06-18T13:25:31Z","title":"Study of the spin and parity of the Higgs boson in diboson decays with the ATLAS detector","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1506.05669","snapshot_observed_at":"2026-08-14T12:20:59.313391Z","title":"Aad et al","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":49,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.313391Z"},"links":{"cited_paper":"/paper/1506.05669","citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:b460a152cdd3f1d49e6b46f305a74ee42be8eacd111f58e5bbd067f3edf273a7","observation_id":"46f03a8a-56ba-4db8-9048-4f6d719789f0","resolution":{"observed_at":"2026-08-14T12:20:59.313391Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1411.3441","last_updated":"2015-07-16T17:42:26Z","snapshot_observed_at":"2026-08-14T23:11:49.859045Z","submitted_at":"2014-11-13T04:03:58Z","title":"Constraints on the spin-parity and anomalous HVV couplings of the Higgs boson in proton collisions at 7 and 8 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1411.3441","snapshot_observed_at":"2026-08-14T12:20:59.323958Z","title":"Khachatryan et al","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":50,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.323958Z"},"links":{"cited_paper":"/paper/1411.3441","citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:e9a5b3c6781c40075af4212ebe1dbae8a7c40ea70fa14326eb2a4ead2143dd75","observation_id":"0598a78b-01ab-4068-bd8b-355958288d66","resolution":{"observed_at":"2026-08-14T12:20:59.323958Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1606.02266","last_updated":"2016-09-15T09:40:30Z","snapshot_observed_at":"2026-08-14T21:53:47.636040Z","submitted_at":"2016-06-07T19:04:06Z","title":"Measurements of the Higgs boson production and decay rates and constraints on its couplings from a combined ATLAS and CMS analysis of the LHC $pp$ collision data at $\\sqrt{s}=$ 7 and 8 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1606.02266","snapshot_observed_at":"2026-08-14T12:20:59.332704Z","title":"Aad et al","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":51,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.332704Z"},"links":{"cited_paper":"/paper/1606.02266","citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:e6036ed87d8052a60e99a33e21dc1b3cb48566806e8f4ccccbc6ae9105e4e98f","observation_id":"a63874b7-efce-494f-8b4f-68aa895f8f76","resolution":{"observed_at":"2026-08-14T12:20:59.332704Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1509.06047","last_updated":"2015-12-22T03:21:00Z","snapshot_observed_at":"2026-08-14T22:31:37.013133Z","submitted_at":"2015-09-20T19:40:12Z","title":"Search for flavour-changing neutral current top quark decays $t\\to Hq$ in $pp$ collisions at $\\sqrt{s}=8$ TeV with the ATLAS detector","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1509.06047","snapshot_observed_at":"2026-08-14T12:20:59.343860Z","title":"Aad et al","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":52,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.343860Z"},"links":{"cited_paper":"/paper/1509.06047","citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:039a1ef3c45008682e603c355823dd057fdfc090b325a4653f8007781df074aa","observation_id":"2242665e-68c9-457d-9e6c-8e48555de06b","resolution":{"observed_at":"2026-08-14T12:20:59.343860Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1604.07730","last_updated":"2017-03-07T18:06:23Z","snapshot_observed_at":"2026-08-15T15:39:55.282612Z","submitted_at":"2016-04-26T16:03:01Z","title":"Search for lepton-flavour-violating decays of the Higgs and $Z$ bosons with the ATLAS detector","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1604.07730","snapshot_observed_at":"2026-08-14T12:20:59.358773Z","title":"Aad et al","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":53,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.358773Z"},"links":{"cited_paper":"/paper/1604.07730","citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:6ecb3481842dfb5b188aed05e4399bc169345bf0636b43bc94d6d3f2ed24a6e6","observation_id":"6df437b1-535c-4428-abc1-d4b8ad474ca8","resolution":{"observed_at":"2026-08-14T12:20:59.358773Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0502132","last_updated":"2005-02-14T18:58:06Z","snapshot_observed_at":"2026-08-11T01:04:20.315237Z","submitted_at":"2005-02-14T18:58:06Z","title":"Phenomenological guide to physics beyond the Standard Model","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0502132","snapshot_observed_at":"2026-08-14T12:20:59.373202Z","title":"Pokorski, doi:10.1007/1-4020-3733-3_9 hep-ph/0502132","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":54,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.373202Z"},"links":{"cited_paper":"/paper/hep-ph/0502132","citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:b162ad0063fbf7e68657ac75b8720249a223c34133bb687f978b7873c64d8906","observation_id":"2afcb086-e838-4399-9019-2f5d53810383","resolution":{"observed_at":"2026-08-14T12:20:59.373202Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1203.2654","last_updated":"2012-04-02T10:07:49Z","snapshot_observed_at":"2026-08-15T04:16:32.887231Z","submitted_at":"2012-03-12T21:17:27Z","title":"On the B to D* tau nu Sensitivity to New Physics","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1203.2654","snapshot_observed_at":"2026-08-14T12:20:59.390468Z","title":"Fajfer, J","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":55,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.390468Z"},"links":{"cited_paper":"/paper/1203.2654","citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:d5c792c358af8c24261d3a40c78a4376a8241e417e8c47277d26126118e00a08","observation_id":"f1f21dc3-80f8-43f1-9d33-c169468f5f5a","resolution":{"observed_at":"2026-08-14T12:20:59.390468Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1308.2803","last_updated":"2014-01-28T14:15:43Z","snapshot_observed_at":"2026-08-15T00:06:59.508460Z","submitted_at":"2013-08-13T09:51:35Z","title":"Towards the Ultimate SM Fit to Close in on Higgs Physics","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1308.2803","snapshot_observed_at":"2026-08-14T12:20:59.409229Z","title":"Pomarol and F","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":56,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.409229Z"},"links":{"cited_paper":"/paper/1308.2803","citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:e1f4f017da2b7a47a9219c9d12236997ea8af6f7e1cb8de285dbeab7326500dd","observation_id":"b7bdb85e-798c-44c5-927c-9c9cec57e64c","resolution":{"observed_at":"2026-08-14T12:20:59.409229Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1408.6207","last_updated":"2016-03-14T18:46:47Z","snapshot_observed_at":"2026-08-14T23:21:50.360096Z","submitted_at":"2014-08-26T18:46:34Z","title":"High-Energy Vector Boson Scattering after the Higgs Discovery","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1408.6207","snapshot_observed_at":"2026-08-14T12:20:59.425466Z","title":"Kilian, T","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":57,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.425466Z"},"links":{"cited_paper":"/paper/1408.6207","citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:d75a55a4b36c0b79a09105ab0765e8addbbcac641cc660ac799aa3f7ae44202b","observation_id":"4634c86a-6dfc-4252-a188-8d83f9b96335","resolution":{"observed_at":"2026-08-14T12:20:59.425466Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1807.02512","last_updated":"2018-07-06T17:58:37Z","snapshot_observed_at":"2026-08-14T18:54:51.878220Z","submitted_at":"2018-07-06T17:58:37Z","title":"Transversal Modes and Higgs Bosons in Electroweak Vector-Boson Scattering at the LHC","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1807.02512","snapshot_observed_at":"2026-08-14T12:20:59.435302Z","title":"Brass, C","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":58,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.435302Z"},"links":{"cited_paper":"/paper/1807.02512","citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:1d259a9e39c1e14d63cebc7de3ad1e58de3f4c6477f407cef889bd19d2c88e57","observation_id":"d9a67707-3b97-48a3-84c5-9705ae0702ab","resolution":{"observed_at":"2026-08-14T12:20:59.435302Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1809.04189","last_updated":"2018-10-04T16:22:18Z","snapshot_observed_at":"2026-08-14T18:29:43.974933Z","submitted_at":"2018-09-11T22:45:05Z","title":"Studies of Dimension-Six EFT effects in Vector Boson Scattering","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1809.04189","snapshot_observed_at":"2026-08-14T12:20:59.446322Z","title":"Gómez-Ambrosio, [arXiv:1809.04189]","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":59,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.446322Z"},"links":{"cited_paper":"/paper/1809.04189","citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:ed9d57dd8ab3bc625e6f28a8ec6d55e820d18f4dcb128a25ac828b012bdec27b","observation_id":"f67bfcdb-a78c-4e50-9694-371e591000c2","resolution":{"observed_at":"2026-08-14T12:20:59.446322Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1212.4158","last_updated":"2013-04-19T13:01:16Z","snapshot_observed_at":"2026-08-15T00:35:24.274426Z","submitted_at":"2012-12-17T21:00:38Z","title":"Longitudinal WW scattering in light of the \"Higgs\" discovery","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1212.4158","snapshot_observed_at":"2026-08-14T12:20:59.456067Z","title":"Espriu and B","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":60,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.456067Z"},"links":{"cited_paper":"/paper/1212.4158","citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:22989db2387f61825aada37812f62b67990344dde95cecab738d65dcca5c39b8","observation_id":"ef95e447-b8bd-4e49-be55-d7aff067d3b9","resolution":{"observed_at":"2026-08-14T12:20:59.456067Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1307.2400","last_updated":"2013-09-12T12:11:18Z","snapshot_observed_at":"2026-08-15T00:11:17.303023Z","submitted_at":"2013-07-09T11:03:34Z","title":"Radiative corrections to WL WL scattering in composite Higgs models","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1307.2400","snapshot_observed_at":"2026-08-14T12:20:59.467736Z","title":"Espriu, F","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":61,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.467736Z"},"links":{"cited_paper":"/paper/1307.2400","citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:4e0c7bc46033cb774a316cdc22d074ed819bcd3910ca989a3be56e6d40c0107e","observation_id":"86812bef-12d6-4cc0-8d26-7cb44c917332","resolution":{"observed_at":"2026-08-14T12:20:59.467736Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1308.1629","last_updated":"2013-11-18T10:56:34Z","snapshot_observed_at":"2026-08-15T07:11:59.628359Z","submitted_at":"2013-08-07T16:44:39Z","title":"Light \"Higgs\", yet strong interactions","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1308.1629","snapshot_observed_at":"2026-08-14T12:20:59.478214Z","title":null,"venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":62,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.478214Z"},"links":{"cited_paper":"/paper/1308.1629","citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:52ea5458e5ae0ff34b99aa118e739b7fd50bf2357c03f9abc30f0c118da18ede","observation_id":"f775baef-4a43-4324-b70d-c8cf98aeed5c","resolution":{"observed_at":"2026-08-14T12:20:59.478214Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1311.5993","last_updated":"2014-01-30T11:59:28Z","snapshot_observed_at":"2026-08-14T23:54:12.029459Z","submitted_at":"2013-11-23T12:55:13Z","title":"One-loop $W_L W_L$ and $Z_L Z_L$ scattering from the Electroweak Chiral Lagrangian with a light Higgs-like scalar","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1311.5993","snapshot_observed_at":"2026-08-14T12:20:59.489179Z","title":null,"venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":63,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.489179Z"},"links":{"cited_paper":"/paper/1311.5993","citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:254bee7955e5aef4b83b79c6573420fe23e549a3c6b29ee988662d41f9cf0c98","observation_id":"2177e4d8-1906-4e37-9c99-6ff88af7906e","resolution":{"observed_at":"2026-08-14T12:20:59.489179Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1403.7386","last_updated":"2014-07-30T13:51:21Z","snapshot_observed_at":"2026-08-14T23:39:34.645474Z","submitted_at":"2014-03-28T14:25:29Z","title":"Unitarity and causality constraints in composite Higgs models","version":2},"cited_work":{"arxiv_id":"1403.7386","doi":null,"metadata_source":"pith","pith_arxiv_id":"1403.7386","snapshot_observed_at":"2026-08-14T12:21:04.625787Z","title":"Unitarity and causality constraints in composite Higgs models","venue":"hep-ph","work_id":"ee7ec635-dcf6-4761-99eb-c9c59f132d20","year":2014},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":64,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.503529Z"},"links":{"cited_paper":"/paper/1403.7386","citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:2b0f17b6e9fad4ce0b7422e5aa67c11a66e7d08ea209dacd60e6251585fe5ee8","observation_id":"a0094f5f-a30d-4a81-b067-b4a9a41a5a97","resolution":{"observed_at":"2026-08-14T12:21:04.655764Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1404.2866","last_updated":"2014-08-26T12:55:16Z","snapshot_observed_at":"2026-08-14T23:37:55.362421Z","submitted_at":"2014-04-10T16:17:36Z","title":"One-loop $\\gamma\\gamma\\to W^+_L W^-_L$ and $\\gamma\\gamma\\to Z_L Z_L$ from the Electroweak Chiral Lagrangian with a light Higgs-like scalar","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1404.2866","snapshot_observed_at":"2026-08-14T12:20:59.512771Z","title":null,"venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":65,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.512771Z"},"links":{"cited_paper":"/paper/1404.2866","citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:de888025e0dd4f4b6c169f8ae135cd6988cf88679038994f4a13dae0f7be97b3","observation_id":"ce62dab1-005e-46ed-aa35-8e66f5c7fda6","resolution":{"observed_at":"2026-08-14T12:20:59.512771Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1707.04580","last_updated":"2017-11-14T16:54:11Z","snapshot_observed_at":"2026-08-14T20:47:35.061231Z","submitted_at":"2017-07-14T17:55:48Z","title":"Production of vector resonances at the LHC via WZ-scattering: a unitarized EChL analysis","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1707.04580","snapshot_observed_at":"2026-08-14T12:20:59.522821Z","title":null,"venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":66,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.522821Z"},"links":{"cited_paper":"/paper/1707.04580","citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:a1b756485dddedfe167029537eceb837f6bba3277d4195035bb24c829a543585","observation_id":"088067a0-e206-4cc7-a60b-3351de38eab1","resolution":{"observed_at":"2026-08-14T12:20:59.522821Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1405.6241","last_updated":"2014-10-21T13:00:31Z","snapshot_observed_at":"2026-08-14T23:32:53.132872Z","submitted_at":"2014-05-23T21:54:55Z","title":"Evidence for Electroweak Production of $W^{\\pm}W^{\\pm}jj$ in $pp$ Collisions at $\\sqrt{s}=8$ TeV with the ATLAS Detector","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1405.6241","snapshot_observed_at":"2026-08-14T12:20:59.533228Z","title":"Aad et al","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":67,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.533228Z"},"links":{"cited_paper":"/paper/1405.6241","citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:d635ae8403cfaf5929c0b215007a83dfbfa311143205d9978786a09fa1615a23","observation_id":"e90762f8-d55c-4a8b-a49f-8b854327c9d2","resolution":{"observed_at":"2026-08-14T12:20:59.533228Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1410.6315","last_updated":"2015-02-03T16:19:23Z","snapshot_observed_at":"2026-08-14T23:14:35.215375Z","submitted_at":"2014-10-23T10:39:22Z","title":"Study of vector boson scattering and search for new physics in events with two same-sign leptons and two jets","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1410.6315","snapshot_observed_at":"2026-08-14T12:20:59.541463Z","title":"Khachatryan et al","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":68,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.541463Z"},"links":{"cited_paper":"/paper/1410.6315","citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:9333f681d494b4615bab1f2ad987d9c3d975180fba2ffea506da8684de253b58","observation_id":"bad13713-e12f-4add-8835-a67ddae7fa1b","resolution":{"observed_at":"2026-08-14T12:20:59.541463Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1709.05822","last_updated":"2018-03-11T15:18:52Z","snapshot_observed_at":"2026-08-14T20:32:16.622660Z","submitted_at":"2017-09-18T08:50:32Z","title":"Observation of electroweak production of same-sign W boson pairs in the two jet and two same-sign lepton final state in proton-proton collisions at $\\sqrt{s} = $ 13 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1709.05822","snapshot_observed_at":"2026-08-14T12:20:59.552287Z","title":null,"venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":69,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.552287Z"},"links":{"cited_paper":"/paper/1709.05822","citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:508c8f50b15cfbbcbf9f77f61959306f4f9be7bf69b034b9c1f9461abb88af0d","observation_id":"0828ed46-c65f-43d3-9fc9-a6f5d12d8b96","resolution":{"observed_at":"2026-08-14T12:20:59.552287Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1603.02151","last_updated":"2016-03-07T16:52:13Z","snapshot_observed_at":"2026-08-14T22:07:10.669423Z","submitted_at":"2016-03-07T16:52:13Z","title":"Measurements of $W^\\pm Z$ production cross sections in $pp$ collisions at $\\sqrt{s} = 8$ TeV with the ATLAS detector and limits on anomalous gauge boson self-couplings","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1603.02151","snapshot_observed_at":"2026-08-14T12:20:59.565513Z","title":"Aad et al","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":70,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.565513Z"},"links":{"cited_paper":"/paper/1603.02151","citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:7e9a1e2dd90eb39bd25881d1fd2130c8c9d74acf51b63aa727761a534317bfe5","observation_id":"271c01f9-fe44-4d9d-97ba-a111a1f4377e","resolution":{"observed_at":"2026-08-14T12:20:59.565513Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1708.02812","last_updated":"2017-11-17T14:22:21Z","snapshot_observed_at":"2026-08-14T20:42:22.129558Z","submitted_at":"2017-08-09T12:33:11Z","title":"Measurement of vector boson scattering and constraints on anomalous quartic couplings from events with four leptons and two jets in proton-proton collisions at sqrt(s) = 13 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1708.02812","snapshot_observed_at":"2026-08-14T12:20:59.584119Z","title":null,"venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":71,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.584119Z"},"links":{"cited_paper":"/paper/1708.02812","citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:e65beb441b14c2476cfe996d91d307f25cb522f2cf0a569f43c4bbfb19f042dc","observation_id":"b14ac9a1-7fd5-49ce-81f1-d8d306af4ff2","resolution":{"observed_at":"2026-08-14T12:20:59.584119Z","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":"2026-08-14T12:20:59.606516Z","title":null,"venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":72,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.606516Z"},"links":{"citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:08eab3538d5fd6ebfaf12117270eb574bb36ee5d916240f796e8622e54a52835","observation_id":"c689dd76-2ae0-483a-b3b9-6b4cd11f2fd0","resolution":{"observed_at":"2026-08-14T12:20:59.606516Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1208.1390","last_updated":"2012-10-04T09:31:27Z","snapshot_observed_at":"2026-08-15T00:50:36.989787Z","submitted_at":"2012-08-07T10:33:20Z","title":"Measurement of WZ production in proton-proton collisions at sqrt(s) = 7 TeV with the ATLAS detector","version":3},"cited_work":{"arxiv_id":"1208.1390","doi":null,"metadata_source":"pith","pith_arxiv_id":"1208.1390","snapshot_observed_at":"2026-08-14T12:21:04.202730Z","title":"Measurement of WZ production in proton-proton collisions at sqrt(s) = 7 TeV with the ATLAS detector","venue":"hep-ex","work_id":"86f6210e-e2eb-4b09-be2a-c4edfeefa3b5","year":2012},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":73,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.613196Z"},"links":{"cited_paper":"/paper/1208.1390","citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:43f5b81d689132d8d8f0b68bbe6fe6126563a3d09b32245dad9225288f743636","observation_id":"4ae4f282-ad76-45e3-a180-c3dc354a1c1c","resolution":{"observed_at":"2026-08-14T12:21:04.216836Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1609.05721","last_updated":"2017-05-12T18:43:31Z","snapshot_observed_at":"2026-08-15T03:36:52.486994Z","submitted_at":"2016-09-19T13:33:45Z","title":"Measurement of the WZ production cross section in pp collisions at sqrt{s} = 7 and 8 TeV and search for anomalous triple gauge couplings at sqrt{s} = 8 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1609.05721","snapshot_observed_at":"2026-08-14T12:20:59.637647Z","title":"Khachatryan et al","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":74,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.637647Z"},"links":{"cited_paper":"/paper/1609.05721","citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:fd3e2bc87724a359f5a6b87abaa357d9ccd8701c1a2d60f7f458d05c4f2b2b99","observation_id":"f9620d54-ed6a-47e3-b437-110eb2e20ea5","resolution":{"observed_at":"2026-08-14T12:20:59.637647Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1607.06943","last_updated":"2017-01-25T17:20:59Z","snapshot_observed_at":"2026-08-14T21:47:07.715897Z","submitted_at":"2016-07-23T14:34:31Z","title":"Measurement of the WZ production cross section in pp collisions at sqrt(s) = 13 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1607.06943","snapshot_observed_at":"2026-08-14T12:20:59.654700Z","title":"Khachatryan et al","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":75,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.654700Z"},"links":{"cited_paper":"/paper/1607.06943","citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:9fcf68f3f694dd6a9fb93fcaf92928a6dd0a8aedcf4c297820e52c6d9f9abc11","observation_id":"1a732c68-d10a-4272-9fd2-91877620e491","resolution":{"observed_at":"2026-08-14T12:20:59.654700Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1610.07572","last_updated":"2017-09-21T11:57:03Z","snapshot_observed_at":"2026-08-14T21:33:48.065056Z","submitted_at":"2016-10-24T19:37:06Z","title":"Multi-Boson Interactions at the LHC","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1610.07572","snapshot_observed_at":"2026-08-14T12:20:59.663366Z","title":null,"venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":76,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.663366Z"},"links":{"cited_paper":"/paper/1610.07572","citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:fc9f30ff3f677e805d3957123928a3d25383c767a022bcf7d1997a83fa3dc550","observation_id":"6973345e-0386-4318-974c-2ae2c8b259d0","resolution":{"observed_at":"2026-08-14T12:20:59.663366Z","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":"2026-08-14T12:20:59.677948Z","title":"Chankowski, lecture notes available at https://www.fuw.edu.pl/ chank/qftoei.html","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":77,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.677948Z"},"links":{"citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:33d9971aedfc04ae594f22c31685f7f6d2aebdec58a9befb5e9a1bf10d8ac524","observation_id":"c4ec15d2-6270-4bb2-aa29-3aa57b92322d","resolution":{"observed_at":"2026-08-14T12:20:59.677948Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1706.02712","last_updated":"2017-08-15T14:57:49Z","snapshot_observed_at":"2026-08-14T20:55:13.203576Z","submitted_at":"2017-06-08T18:00:10Z","title":"UV complete me: Positivity Bounds for Particles with Spin","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1706.02712","snapshot_observed_at":"2026-08-14T12:20:59.692520Z","title":"de Rham, S","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":78,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.692520Z"},"links":{"cited_paper":"/paper/1706.02712","citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:742149e99602a25f24ed2ef4db974029e2838f595ffd33cb7cc0e497c86efca9","observation_id":"c19171c1-8ae1-41a4-aef4-f6d3d7cc1c7f","resolution":{"observed_at":"2026-08-14T12:20:59.692520Z","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":"2026-08-14T12:20:59.703375Z","title":null,"venue":null,"work_id":null,"year":1974},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":79,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.703375Z"},"links":{"citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:4db65b8358d4ad49e2586184b2c5ffd94f65c1a9f38a65baee84c590c51b4945","observation_id":"1e219188-fff5-46f1-a7ab-5add009fc834","resolution":{"observed_at":"2026-08-14T12:20:59.703375Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1016/0370-2693(73)90692-8","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T12:21:00.819934Z","title":null,"venue":null,"work_id":"6005420a-80a1-4ba6-96b3-052d7ac13b0a","year":1973},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":80,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.708856Z"},"links":{"citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:ff4b40821941de3a53fa8b559cce832aa6bf7b08da7b5e82de88b91dc8c6dc40","observation_id":"a4846599-2e92-4cd5-8195-dbf59529a7ec","resolution":{"observed_at":"2026-08-14T12:21:00.842668Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T12:20:59.719200Z","title":"Fermi, Ric","venue":null,"work_id":null,"year":1933},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":81,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.719200Z"},"links":{"citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:dc2c1687957988dc7cf9089783a4b4245b5a065abc6d8c09bed1cca58be6cf45","observation_id":"b8f2c42c-a9f8-4ae8-bcb6-eeff07d66287","resolution":{"observed_at":"2026-08-14T12:20:59.719200Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1508.05895","last_updated":"2015-12-07T14:40:38Z","snapshot_observed_at":"2026-08-14T22:35:25.463721Z","submitted_at":"2015-08-24T18:00:57Z","title":"Rosetta: an operator basis translator for Standard Model effective field theory","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1508.05895","snapshot_observed_at":"2026-08-14T12:20:59.733957Z","title":"Falkowski, B","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":82,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.733957Z"},"links":{"cited_paper":"/paper/1508.05895","citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:891815b5608dea9f6576d98bc7b565c63451d59a0953aa76fc0507a12dc2c91e","observation_id":"1be8cf6c-88ed-4577-8adf-bee9b7545366","resolution":{"observed_at":"2026-08-14T12:20:59.733957Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9806303","last_updated":"1998-06-08T12:53:54Z","snapshot_observed_at":"2026-07-07T04:29:43.370671Z","submitted_at":"1998-06-08T12:53:54Z","title":"Effective Field Theory","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9806303","snapshot_observed_at":"2026-08-14T12:20:59.744913Z","title":"Pich, hep-ph/9806303","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":83,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.744913Z"},"links":{"cited_paper":"/paper/hep-ph/9806303","citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:d80c26954423235e14d7631f1ba601d8369fc329b5b99661d710e3717a620f7c","observation_id":"cea4b062-367b-4e10-ae42-ffb9e24ec5b2","resolution":{"observed_at":"2026-08-14T12:20:59.744913Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9502366","last_updated":"1995-02-22T14:19:34Z","snapshot_observed_at":"2026-07-07T04:19:12.848381Z","submitted_at":"1995-02-22T14:19:34Z","title":"Chiral Perturbation Theory","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9502366","snapshot_observed_at":"2026-08-14T12:20:59.756084Z","title":"Pich, Rept","venue":null,"work_id":null,"year":1995},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":84,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.756084Z"},"links":{"cited_paper":"/paper/hep-ph/9502366","citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:290c5b24b8027133cdddb20da4ac6dfab9ba5e62d2584a9e93906b93fd72316d","observation_id":"ce562c15-f699-4a47-8098-2563c26989c7","resolution":{"observed_at":"2026-08-14T12:20:59.756084Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1804.05664","last_updated":"2020-01-25T19:54:12Z","snapshot_observed_at":"2026-08-14T19:25:35.684745Z","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":"2026-08-14T12:20:59.778225Z","title":"Pich, arXiv:1804.05664 [hep-ph]","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":85,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.778225Z"},"links":{"cited_paper":"/paper/1804.05664","citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:05ab3be52255146b09985fc4cb9604e83d23c3944406af79a5ac0f856ad78266","observation_id":"75aaed33-7ad3-4464-98b0-e9325f34901a","resolution":{"observed_at":"2026-08-14T12:20:59.778225Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0505265","last_updated":"2005-05-31T09:13:05Z","snapshot_observed_at":"2026-08-14T10:32:35.068561Z","submitted_at":"2005-05-31T09:13:05Z","title":"A Chiral Perturbation Theory Primer","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0505265","snapshot_observed_at":"2026-08-14T12:20:59.785987Z","title":"Scherer and M","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":86,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.785987Z"},"links":{"cited_paper":"/paper/hep-ph/0505265","citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:0cd7ff7e0de96cf4f64a5063ec85591c5e00ca13b9abda15b673867d4c164b91","observation_id":"e2e644ef-51d9-4590-8b24-73f0764b9863","resolution":{"observed_at":"2026-08-14T12:20:59.785987Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1811.09413","last_updated":"2019-09-20T13:00:51Z","snapshot_observed_at":"2026-08-14T17:54:47.501683Z","submitted_at":"2018-11-23T10:11:08Z","title":"Field redefinitions in effective theories at higher orders","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1811.09413","snapshot_observed_at":"2026-08-14T12:20:59.795263Z","title":null,"venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":87,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.795263Z"},"links":{"cited_paper":"/paper/1811.09413","citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:2a0a9efb15a1a1f2cd97e35fe4330bff834a8cfdad1dc84246ccf9b79b965a3f","observation_id":"1af84f1c-c67e-437c-8232-eda537cb83ac","resolution":{"observed_at":"2026-08-14T12:20:59.795263Z","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":"2026-08-14T12:20:59.804038Z","title":null,"venue":null,"work_id":null,"year":1969},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":88,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.804038Z"},"links":{"citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:ca5923434296a2cb1aef25b6ee5dcfee782458d3165004f12bc665099d59c2ec","observation_id":"acee1317-0d5a-4f53-83ea-66bbdae5abbd","resolution":{"observed_at":"2026-08-14T12:20:59.804038Z","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":"2026-08-14T12:20:59.815976Z","title":null,"venue":null,"work_id":null,"year":1969},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":89,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.815976Z"},"links":{"citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:76ed71ab6c9ed79e9787a4b262604add2741b99bf6a30ee5e04654d5ae9f0dcc","observation_id":"6634be50-9a79-46be-a75b-678095de5d0e","resolution":{"observed_at":"2026-08-14T12:20:59.815976Z","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":"2026-08-14T12:20:59.824288Z","title":"Weinberg, Physica A96, no","venue":null,"work_id":null,"year":1979},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":90,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.824288Z"},"links":{"citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:45323bd352bf6feeaf72bf2af07ae87ccae83f9ef05c0cdf4a1940c6192039cf","observation_id":"866771eb-612d-48ad-838d-4f5208a6eb4e","resolution":{"observed_at":"2026-08-14T12:20:59.824288Z","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":"2026-08-14T12:20:59.830349Z","title":"Gasser and H","venue":null,"work_id":null,"year":1984},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":91,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.830349Z"},"links":{"citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:c4644ae1be1dea24cb31a346d9a6485330e8c66039e492ed388b8bb1c7b1ad3d","observation_id":"cf29258f-67da-4a80-ada8-d5acee067145","resolution":{"observed_at":"2026-08-14T12:20:59.830349Z","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":"2026-08-14T12:20:59.843134Z","title":"Gasser and H","venue":null,"work_id":null,"year":1985},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":92,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.843134Z"},"links":{"citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:df7dba1f44074682ba65c8e070f95f5ac80e30ed8053efb2b9c04228b272302e","observation_id":"315a6af8-7327-4ca4-ae95-a6829c392c27","resolution":{"observed_at":"2026-08-14T12:20:59.843134Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9902437","last_updated":"1999-04-09T12:03:00Z","snapshot_observed_at":"2026-07-07T04:32:18.341447Z","submitted_at":"1999-02-23T08:08:28Z","title":"The Mesonic Chiral Lagrangian of Order $p^6$","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9902437","snapshot_observed_at":"2026-08-14T12:20:59.864110Z","title":"Bijnens, G","venue":null,"work_id":null,"year":1999},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":93,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.864110Z"},"links":{"cited_paper":"/paper/hep-ph/9902437","citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:2e17431e57eab2735202b8268ac86a5b21e4ab7cec4622d7f4fb8d6a034e7fdd","observation_id":"0cb3b2d2-19f3-4af3-a408-b26a9e89eb35","resolution":{"observed_at":"2026-08-14T12:20:59.864110Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0705.0576","last_updated":"2007-05-04T09:28:35Z","snapshot_observed_at":"2026-08-15T10:41:36.729958Z","submitted_at":"2007-05-04T09:28:35Z","title":"On the mesonic Lagrangian of order p^6 in chiral SU(2)","version":1},"cited_work":{"arxiv_id":"0705.0576","doi":null,"metadata_source":"pith","pith_arxiv_id":"0705.0576","snapshot_observed_at":"2026-08-14T12:21:03.476870Z","title":"On the mesonic Lagrangian of order p^6 in chiral SU(2)","venue":"hep-ph","work_id":"8d9a90f5-3877-4cf3-b171-ce27b3bf04ec","year":2007},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":94,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.884836Z"},"links":{"cited_paper":"/paper/0705.0576","citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:7a5cd992cfa92166161978eb989155f6f22fac646cbc12b0f91b9fd4e9d00644","observation_id":"28f503e2-b65b-4b3a-ae7b-19e96506be75","resolution":{"observed_at":"2026-08-14T12:21:03.496997Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0110400","last_updated":"2005-10-26T14:06:17Z","snapshot_observed_at":"2026-07-07T03:54:04.623665Z","submitted_at":"2001-10-31T12:27:03Z","title":"The anomalous chiral Lagrangian of order $p^6$","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0110400","snapshot_observed_at":"2026-08-14T12:20:59.898024Z","title":"Bijnens, L","venue":null,"work_id":null,"year":2002},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":95,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.898024Z"},"links":{"cited_paper":"/paper/hep-ph/0110400","citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:b021c4d60472132964c3a9871b2ba0212478cf7d65b6bd7b1c70565fd4c33d87","observation_id":"43b0c8c4-efc7-49b3-b838-4522e55d804b","resolution":{"observed_at":"2026-08-14T12:20:59.898024Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0110261","last_updated":"2001-10-18T18:47:12Z","snapshot_observed_at":"2026-07-07T03:53:54.908138Z","submitted_at":"2001-10-18T18:47:12Z","title":"The anomalous chiral perturbation theory meson Lagrangian to order $p^6$ revisited","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0110261","snapshot_observed_at":"2026-08-14T12:20:59.913885Z","title":"Ebertshauser, H","venue":null,"work_id":null,"year":2002},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":96,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.913885Z"},"links":{"cited_paper":"/paper/hep-ph/0110261","citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:c296a70249a99813568af2a0c78a9622a43ff7002d1e6d1b237d327ffd064ae5","observation_id":"e17efd82-1a55-4317-8506-989c708ca55a","resolution":{"observed_at":"2026-08-14T12:20:59.913885Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1601.07551","last_updated":"2016-09-09T10:28:58Z","snapshot_observed_at":"2026-08-14T22:12:48.861536Z","submitted_at":"2016-01-27T21:00:01Z","title":"Analysis of General Power Counting Rules in Effective Field Theory","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1601.07551","snapshot_observed_at":"2026-08-14T12:20:59.932197Z","title":null,"venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":97,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.932197Z"},"links":{"cited_paper":"/paper/1601.07551","citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:a1ace32411d411ddcd19c0a30fbe57a91ec338c1423646be7709a128ec8235eb","observation_id":"dfddfb46-6d6b-4d33-a31b-4d10121613ce","resolution":{"observed_at":"2026-08-14T12:20:59.932197Z","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":"2026-08-14T12:20:59.943332Z","title":"Appelquist and C","venue":null,"work_id":null,"year":1980},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":98,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.943332Z"},"links":{"citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:4497d53a749afa8c128e91d9c4d31504f45ef94667d348f52b72563e64b18404","observation_id":"dd74fd9d-5513-4c3b-9729-f817046276fc","resolution":{"observed_at":"2026-08-14T12:20:59.943332Z","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":"2026-08-14T12:20:59.957223Z","title":"Dobado and M","venue":null,"work_id":null,"year":1989},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":99,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.957223Z"},"links":{"citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:2e01e8947dbafdce52335260fc13efe0c128862dc3c0728788b1f626e41bd029","observation_id":"d6910391-eb2a-4843-b25b-e45af39d4145","resolution":{"observed_at":"2026-08-14T12:20:59.957223Z","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":"2026-08-14T12:20:59.971408Z","title":"Dobado and M","venue":null,"work_id":null,"year":1989},"citing_paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach","version":1},"reference_index":100,"source":"pdf_text","source_observed_at":"2026-08-14T12:20:59.971408Z"},"links":{"citing_paper":"/paper/1908.07596"},"observation_digest":"sha256:97fa205e6ab74781e4268d276c6c73bf1ffdf779d5a6b515cc72c1619065fc67","observation_id":"27eafdeb-6bad-4a1f-bb9d-9e572192452e","resolution":{"observed_at":"2026-08-14T12:20:59.971408Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"paper":{"arxiv_id":"1908.07596","last_updated":"2019-08-20T20:22:51Z","latest_version":1,"primary_category":"hep-ph","snapshot_observed_at":"2026-08-15T07:31:54.192089Z","submitted_at":"2019-08-20T20:22:51Z","title":"The W and Z scattering as a probe of physics beyond the Standard Model: Effective Field Theory approach"},"reference_resolution":{"displayed":100,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":96,"verified_exact":4,"verified_fuzzy":0},"total_outbound_references":138},"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":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"thesis":"As of 15 August 2026, this Paper Citation Record lists 100 of 138 outbound references and 0 inbound Pith citation observations for arXiv:1908.07596."}