{"as_of":"2026-08-13T18:05:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:a73aceecb90b6c24199efb5656a1d6dcaa379c48dbae03759ceaa8e9f2af7c88","coverage":[{"denominator":122,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":100,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-12T12:51:25.728284Z","state":"measured"},{"denominator":101,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":101,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-13T06:32:02.005865+00:00","state":"measured"},{"denominator":1,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":1,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-12T04:24:21.013722Z","state":"measured"},{"denominator":1,"lane":"external_citation_measurements","note":"A source-named dated measurement, never combined with another source.","records_observed":0,"source":"pith","source_observed_at":"2026-08-12T04:24:23.020238Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"cited_work":{"arxiv_id":"2411.16907","doi":null,"metadata_source":"pith","pith_arxiv_id":"2411.16907","snapshot_observed_at":"2026-08-12T04:24:23.020238Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","venue":"hep-ex","work_id":"b8c11ceb-53e3-44ad-821c-36e83f05bb0f","year":2024},"citing_paper":{"arxiv_id":"2412.01548","last_updated":"2025-05-22T07:37:21Z","snapshot_observed_at":"2026-08-12T13:24:37.057539Z","submitted_at":"2024-12-02T14:36:58Z","title":"Measurement of off-shell Higgs boson production in the $H^*\\rightarrow ZZ\\rightarrow 4\\ell$ decay channel using a neural simulation-based inference technique in 13 TeV $pp$ collisions with the ATLAS detector","version":2},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-08-12T04:24:21.013722Z"},"links":{"cited_paper":"/paper/2411.16907","citing_paper":"/paper/2412.01548"},"observation_digest":"sha256:457247bb7be0766769f187a76e831bd1d42764bfcd1faff814e0ef6b032b9a4f","observation_id":"c5c5f216-9f68-4082-a871-a09a8e0a7cfd","resolution":{"observed_at":"2026-08-12T04:24:23.025748Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}}],"links":{"evidence":"/evidence","html":"/paper/2411.16907/citation-record","integrity":"/paper/2411.16907/integrity","json":"/paper/2411.16907/citation-record.json","paper":"/paper/2411.16907"},"outbound":[{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-12T12:51:25.325321Z","title":"Broken symmetry and the mass of gauge vector mesons","venue":null,"work_id":null,"year":1964},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.325321Z"},"links":{"citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:179f1a18f1f7828cb8dd7846b6fe8b0b9c09b86d5126035feb9a0dfb9c1378cb","observation_id":"24648bce-8df7-4fdb-99f6-219f268ce1d4","resolution":{"observed_at":"2026-08-12T12:51:25.325321Z","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":"2026-08-12T12:51:25.330084Z","title":"Broken symmetries, massless particles and gauge fields","venue":null,"work_id":null,"year":1964},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.330084Z"},"links":{"citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:2282b9f6e7e70b356be71b78e2903c0352e5f3f9dbfa76467994e3347938edf4","observation_id":"317db6d4-3f1c-4d7b-aa9c-eb1c4c4ddab4","resolution":{"observed_at":"2026-08-12T12:51:25.330084Z","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":"2026-08-12T12:51:25.334302Z","title":"Broken symmetries and the masses of gauge bosons","venue":null,"work_id":null,"year":1964},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.334302Z"},"links":{"citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:f42e9c96ceb9d8f2f219b03ca16e7e389cfd9c5c4fe26c7b98d326e6c1453b4a","observation_id":"5dd8c231-9c5f-4c8c-bcc1-118ba883c304","resolution":{"observed_at":"2026-08-12T12:51:25.334302Z","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":"2026-08-12T12:51:25.338325Z","title":"Global conservation laws and massless particles","venue":null,"work_id":null,"year":1964},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.338325Z"},"links":{"citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:599f3fa4c32b839ed6c91a6440f2cf245cc363323658823a59a171cf2f21663b","observation_id":"7e2d3906-0418-4388-8c41-931659ea8da1","resolution":{"observed_at":"2026-08-12T12:51:25.338325Z","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":"2026-08-12T12:51:25.342446Z","title":"Observation of a new particle in the search for the Standard Model Higgs boson with the ATLAS detector at the LHC","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.342446Z"},"links":{"cited_paper":"/paper/1207.7214","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:acbb18b16deb14c33545095a86e7f5ea4341851bb282df648525b33073439438","observation_id":"a7973cbc-253e-4d80-b42f-27a6802ad64e","resolution":{"observed_at":"2026-08-12T12:51:25.342446Z","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":"2026-08-12T13:24:07.072161Z","submitted_at":"2012-07-31T13:27:18Z","title":"Observation of a new boson at a mass of 125 GeV with the CMS experiment at the LHC","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1207.7235","snapshot_observed_at":"2026-08-12T12:51:25.346803Z","title":"Observation of a new boson at a mass of 125 GeV with the CMS experiment at the LHC","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.346803Z"},"links":{"cited_paper":"/paper/1207.7235","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:a4b3cf40de2f10809ef332334daac657303c02ccb8b19349ccc325ae33fab78d","observation_id":"7ee4aeba-f635-4ede-b524-b1254ee2726c","resolution":{"observed_at":"2026-08-12T12:51:25.346803Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1303.4571","last_updated":"2013-07-04T09:09:28Z","snapshot_observed_at":"2026-08-12T13:24:07.569546Z","submitted_at":"2013-03-19T12:44:19Z","title":"Observation of a new boson with mass near 125 GeV in pp collisions at sqrt(s) = 7 and 8 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1303.4571","snapshot_observed_at":"2026-08-12T12:51:25.351699Z","title":"Observation of a new boson with mass near 125 GeV in pp collisions at √s = 7 and 8 TeV","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.351699Z"},"links":{"cited_paper":"/paper/1303.4571","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:9e05dda78efd13d4d3911e0e6557657de058f3007b0263dd6bf220c23215492a","observation_id":"172ed109-f651-4282-a98e-32b0edca9b3f","resolution":{"observed_at":"2026-08-12T12:51:25.351699Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1808.08238","last_updated":"2018-09-29T09:50:27Z","snapshot_observed_at":"2026-07-06T06:57:19.091760Z","submitted_at":"2018-08-24T18:00:43Z","title":"Observation of $H \\rightarrow b\\bar{b}$ decays and $VH$ production with the ATLAS detector","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1808.08238","snapshot_observed_at":"2026-08-12T12:51:25.355956Z","title":"Observation of H → bb decays and VH production with the ATLAS detector","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.355956Z"},"links":{"cited_paper":"/paper/1808.08238","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:b269fe54100609411aa2c2610226ded19f0e9acbba59fd3b50d9a8df2d5ca320","observation_id":"8d274296-b955-48c1-9e6a-04c0fb3ee46b","resolution":{"observed_at":"2026-08-12T12:51:25.355956Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1808.08242","last_updated":"2018-09-19T01:50:24Z","snapshot_observed_at":"2026-08-06T03:15:14.049289Z","submitted_at":"2018-08-24T18:04:40Z","title":"Observation of Higgs boson decay to bottom quarks","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1808.08242","snapshot_observed_at":"2026-08-12T12:51:25.360129Z","title":"Observation of Higgs boson decay to bottom quarks","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.360129Z"},"links":{"cited_paper":"/paper/1808.08242","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:c67bc40a07bc242acb487f04272aed3f8a330d9aa44cff2fc11f276f18a04799","observation_id":"94f6fdfe-0f4e-4623-b803-4fdcc3bedaca","resolution":{"observed_at":"2026-08-12T12:51:25.360129Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2410.19611","last_updated":"2025-05-21T14:15:41Z","snapshot_observed_at":"2026-08-12T22:15:04.009817Z","submitted_at":"2024-10-25T15:03:36Z","title":"Measurements of $WH$ and $ZH$ production with Higgs boson decays into bottom quarks and direct constraints on the charm Yukawa coupling in $13\\,\\mathrm{TeV}$ $pp$ collisions with the ATLAS detector","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2410.19611","snapshot_observed_at":"2026-08-12T12:51:25.364075Z","title":"Measurements of WH and ZH production with Higgs boson decays into bottom quarks and direct constraints on the charm Yukawa coupling in 13 TeV pp collisions with the ATLAS detector","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.364075Z"},"links":{"cited_paper":"/paper/2410.19611","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:cbfcd9e6119456bf7ee575a34596aa357a6c33bf5ead3e6f8ca9bd8291e22725","observation_id":"abcd211c-9842-498d-82eb-ced80dfae625","resolution":{"observed_at":"2026-08-12T12:51:25.364075Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2312.07562","last_updated":"2024-05-30T16:47:48Z","snapshot_observed_at":"2026-08-13T05:05:58.058428Z","submitted_at":"2023-12-09T20:13:30Z","title":"Measurement of simplified template cross sections of the Higgs boson produced in association with W or Z bosons in the H $\\to$ $\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2312.07562","snapshot_observed_at":"2026-08-12T12:51:25.368246Z","title":null,"venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.368246Z"},"links":{"cited_paper":"/paper/2312.07562","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:eb804506bf21347af148b9c4f85d85616fc0fc01747b0dd86e1ff6c863abae63","observation_id":"4c211a24-79f9-41dc-8a43-f3a4f6513f1a","resolution":{"observed_at":"2026-08-12T12:51:25.368246Z","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":"2026-08-12T12:51:25.372106Z","title":"Effective Lagrangian analysis of new interactions and flavor conservation","venue":null,"work_id":null,"year":1986},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.372106Z"},"links":{"citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:001fe85eea6c039bf0162bd37fa83ee01fd30b28854b38e6baa3f1b321509115","observation_id":"622b0dc2-ca31-4cc0-8e8c-4388d312fda2","resolution":{"observed_at":"2026-08-12T12:51:25.372106Z","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(91)90061-t","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-12T12:51:25.928541Z","title":"Operator analysis for precision electroweak physics","venue":null,"work_id":"81e15fe9-8fe0-4f4b-a00c-710a021762d0","year":1991},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.376046Z"},"links":{"citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:fca153eda0668cef9e160313b6ded3204b804b9f4362638cbd30b3d363b728eb","observation_id":"60fffde3-e7e2-428d-b758-8860b90ecfd4","resolution":{"observed_at":"2026-08-12T12:51:25.933334Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"0712.0396","last_updated":"2007-12-03T21:34:47Z","snapshot_observed_at":"2026-07-06T01:35:51.899163Z","submitted_at":"2007-12-03T21:34:47Z","title":"Electroweak Corrections in High Energy Processes using Effective Field Theory","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0712.0396","snapshot_observed_at":"2026-08-12T12:51:25.379913Z","title":"Electroweak corrections in high energy processes using effective field theory","venue":null,"work_id":null,"year":2008},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.379913Z"},"links":{"cited_paper":"/paper/0712.0396","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:da2c80fe485a2ae8b69312cd45ef4bfea0f5e54a6bf74b2fef698464472dc28b","observation_id":"e6599e86-e6ed-4332-9772-c80635753091","resolution":{"observed_at":"2026-08-12T12:51:25.379913Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1205.4231","last_updated":"2012-05-18T19:58:08Z","snapshot_observed_at":"2026-07-06T02:11:23.670680Z","submitted_at":"2012-05-18T19:58:08Z","title":"Effective Field Theory: A Modern Approach to Anomalous Couplings","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1205.4231","snapshot_observed_at":"2026-08-12T12:51:25.384238Z","title":"Effective field theory: A modern approach to anomalous couplings","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.384238Z"},"links":{"cited_paper":"/paper/1205.4231","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:0ef843a4f8d59fbd6c3a166e60f8616a0e0e618e7e1e1cec6924d05f0b0bda70","observation_id":"b6f1464a-3352-47cd-b0cb-6e61d2f851df","resolution":{"observed_at":"2026-08-12T12:51:25.384238Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1308.2627","last_updated":"2020-07-15T12:41:06Z","snapshot_observed_at":"2026-08-07T19:35:43.779739Z","submitted_at":"2013-08-12T17:21:12Z","title":"Renormalization Group Evolution of the Standard Model Dimension Six Operators I: Formalism and lambda Dependence","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1308.2627","snapshot_observed_at":"2026-08-12T12:51:25.388225Z","title":"Renormalization group evolution of the standard model dimension six operators I: formalism and lambda dependence","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.388225Z"},"links":{"cited_paper":"/paper/1308.2627","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:c6c2c8f36906d8a89c92cccb2e27ea5b324a0be558f6fea278ed4e3cffe965bd","observation_id":"dc75a5c5-74f2-4883-b097-4c8a8b3b0eef","resolution":{"observed_at":"2026-08-12T12:51:25.388225Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1312.2014","last_updated":"2024-06-13T16:23:18Z","snapshot_observed_at":"2026-08-12T21:44:49.413147Z","submitted_at":"2013-12-06T21:09:00Z","title":"Renormalization Group Evolution of the Standard Model Dimension Six Operators III: Gauge Coupling Dependence and Phenomenology","version":5},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1312.2014","snapshot_observed_at":"2026-08-12T12:51:25.392314Z","title":"Renormalization group evolution of the standard model dimension six operators III: gauge coupling dependence and phenomenology","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.392314Z"},"links":{"cited_paper":"/paper/1312.2014","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:ae303b90193b91b6366d2753b26ed5cd6cfb34f86925b09825601b522d9bde03","observation_id":"89879e19-0985-4859-b524-f5757d3f448a","resolution":{"observed_at":"2026-08-12T12:51:25.392314Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1310.4838","last_updated":"2020-07-15T12:41:18Z","snapshot_observed_at":"2026-08-06T19:18:12.176848Z","submitted_at":"2013-10-17T20:07:48Z","title":"Renormalization Group Evolution of the Standard Model Dimension Six Operators II: Yukawa Dependence","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1310.4838","snapshot_observed_at":"2026-08-12T12:51:25.396421Z","title":"Renormalization group evolution of the standard model dimension six operators II: Yukawa dependence","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.396421Z"},"links":{"cited_paper":"/paper/1310.4838","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:53f40fc28d1754563faa44b3d1f91cd291aa21c54281574096c825dce4df514e","observation_id":"aa4ef536-c12f-4da0-a8f4-7216a343107e","resolution":{"observed_at":"2026-08-12T12:51:25.396421Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1408.5147","last_updated":"2014-12-05T14:25:48Z","snapshot_observed_at":"2026-08-01T12:30:57.535301Z","submitted_at":"2014-08-21T20:08:40Z","title":"Effective Theories and Measurements at Colliders","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1408.5147","snapshot_observed_at":"2026-08-12T12:51:25.400520Z","title":"Effective theories and measurements at colliders","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.400520Z"},"links":{"cited_paper":"/paper/1408.5147","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:7a571f70ec9de85660199b39bd967ad132ff825d112441199df893453469d797","observation_id":"46fe706f-ef3b-493e-8d23-53e080373c97","resolution":{"observed_at":"2026-08-12T12:51:25.400520Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1706.08945","last_updated":"2018-11-12T14:43:11Z","snapshot_observed_at":"2026-08-13T06:43:55.862289Z","submitted_at":"2017-06-27T17:17:52Z","title":"The Standard Model as an Effective Field Theory","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1706.08945","snapshot_observed_at":"2026-08-12T12:51:25.404733Z","title":"The standard model as an effective field theory","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.404733Z"},"links":{"cited_paper":"/paper/1706.08945","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:26939fcb320ff450fa64d65c2b4c584d7b7b76f4354983925a666d707118d328","observation_id":"8b0ea555-57e8-4b95-8272-b20923f71379","resolution":{"observed_at":"2026-08-12T12:51:25.404733Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2303.16922","last_updated":"2023-10-04T08:29:30Z","snapshot_observed_at":"2026-08-13T12:13:50.609284Z","submitted_at":"2023-03-29T18:00:00Z","title":"The Standard Model effective field theory at work","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2303.16922","snapshot_observed_at":"2026-08-12T12:51:25.408793Z","title":"The standard model effective field theory at work","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.408793Z"},"links":{"cited_paper":"/paper/2303.16922","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:4c177aef74027a9eedd5f4bdaecf6fb32d4956bf6e1ec31ae23894ebc64f4eac","observation_id":"d8692a59-5eb6-47a1-a0a8-3f730ceb8205","resolution":{"observed_at":"2026-08-12T12:51:25.408793Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2104.12152","last_updated":"2021-09-18T23:24:59Z","snapshot_observed_at":"2026-08-09T18:32:42.620749Z","submitted_at":"2021-04-25T13:16:27Z","title":"Constraints on anomalous Higgs boson couplings to vector bosons and fermions in its production and decay using the four-lepton final state","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2104.12152","snapshot_observed_at":"2026-08-12T12:51:25.412758Z","title":"Constraints on anomalous Higgs boson couplings to vector bosons and fermions in its production and decay using the four-lepton final state","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.412758Z"},"links":{"cited_paper":"/paper/2104.12152","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:77b22be88d6ef54e7a325c7e320df443d37d4a1c44e1cdbf7ec99d9cadc5107e","observation_id":"c9781527-fcd5-44ce-b3d3-0789b4a8666e","resolution":{"observed_at":"2026-08-12T12:51:25.412758Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2403.00657","last_updated":"2024-08-19T14:06:29Z","snapshot_observed_at":"2026-08-13T04:05:27.506027Z","submitted_at":"2024-03-01T16:37:44Z","title":"Constraints on anomalous Higgs boson couplings from its production and decay using the WW channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2403.00657","snapshot_observed_at":"2026-08-12T12:51:25.416852Z","title":"Constraints on anomalous Higgs boson couplings from its production and decay using the WW channel in proton–proton collisions at√s = 13 TeV","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.416852Z"},"links":{"cited_paper":"/paper/2403.00657","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:ab52c18509e8f2487d55045ee9c192d2ba422f424b81b349d4cf1f3e936c586f","observation_id":"9867f90a-fdc6-48e6-967b-ab0ad4db1394","resolution":{"observed_at":"2026-08-12T12:51:25.416852Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2205.05120","last_updated":"2023-08-17T13:50:41Z","snapshot_observed_at":"2026-08-13T15:46:52.756732Z","submitted_at":"2022-05-10T18:49:51Z","title":"Constraints on anomalous Higgs boson couplings to vector bosons and fermions from the production of Higgs bosons using the $\\tau\\tau$ final state","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2205.05120","snapshot_observed_at":"2026-08-12T12:51:25.420918Z","title":"Constraints on anomalous Higgs boson couplings to vector bosons and fermions from the production of Higgs bosons using the ττ final state","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.420918Z"},"links":{"cited_paper":"/paper/2205.05120","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:59291584b57958419d6a2f18394fe25b2b1f8dd31c169620b1f076a9be2b305e","observation_id":"47cea12f-5883-4570-b3e0-d30f18f24539","resolution":{"observed_at":"2026-08-12T12:51:25.420918Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1001.3396","last_updated":"2010-03-22T15:05:55Z","snapshot_observed_at":"2026-08-09T02:36:23.329917Z","submitted_at":"2010-01-19T19:59:31Z","title":"Spin determination of single-produced resonances at hadron colliders","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1001.3396","snapshot_observed_at":"2026-08-12T12:51:25.424858Z","title":"Spin determination of single-produced resonances at hadron colliders","venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.424858Z"},"links":{"cited_paper":"/paper/1001.3396","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:2ec47378a4cc43f9e7686b071efc918f52b8fe667a076534f5fc8b22c002e364","observation_id":"44c726fb-5bcd-4361-ac38-0d4844d99c53","resolution":{"observed_at":"2026-08-12T12:51:25.424858Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1208.4018","last_updated":"2014-02-18T14:45:02Z","snapshot_observed_at":"2026-08-08T18:43:04.893187Z","submitted_at":"2012-08-20T14:10:32Z","title":"On the spin and parity of a single-produced resonance at the LHC","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1208.4018","snapshot_observed_at":"2026-08-12T12:51:25.428678Z","title":"On the spin and parity of a single-produced resonance at the LHC","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.428678Z"},"links":{"cited_paper":"/paper/1208.4018","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:52db4bc59499b15fa8cbdaa5a011feeb15d463f76883f99a902bddf9e737dcd4","observation_id":"680289de-21dc-4d9d-8806-7bb19da99447","resolution":{"observed_at":"2026-08-12T12:51:25.428678Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1309.4819","last_updated":"2014-02-18T14:18:53Z","snapshot_observed_at":"2026-07-06T03:23:24.779854Z","submitted_at":"2013-09-18T23:12:30Z","title":"Constraining anomalous HVV interactions at proton and lepton colliders","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1309.4819","snapshot_observed_at":"2026-08-12T12:51:25.432566Z","title":"Constraining anomalous HVV interactions at proton and lepton colliders","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.432566Z"},"links":{"cited_paper":"/paper/1309.4819","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:bef0115346030e0fe705904dba9906949bbfd07a870250dc258ded68548ea320","observation_id":"2c450d8a-b4d1-44b9-91c6-3a4743cfd503","resolution":{"observed_at":"2026-08-12T12:51:25.432566Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1903.04618","last_updated":"2019-07-08T10:01:04Z","snapshot_observed_at":"2026-07-06T07:38:33.968966Z","submitted_at":"2019-03-11T21:46:53Z","title":"Measurement of $VH$, $H\\to b\\bar{b}$ production as a function of the vector-boson transverse momentum in 13 TeV $pp$ collisions with the ATLAS detector","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1903.04618","snapshot_observed_at":"2026-08-12T12:51:25.436588Z","title":"Measurement of VH, H → bb production as a function of the vector-boson transverse momentum in 13 TeV pp collisions with the ATLAS detector","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.436588Z"},"links":{"cited_paper":"/paper/1903.04618","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:4a7e583c62d15d0a501e4525beca38b34b1ce2c18d3e5b8339876cf5647dedff","observation_id":"60e4f9cd-138b-4d2d-8181-13d67e76ade9","resolution":{"observed_at":"2026-08-12T12:51:25.436588Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2007.02873","last_updated":"2021-03-08T11:29:38Z","snapshot_observed_at":"2026-08-10T01:49:01.766501Z","submitted_at":"2020-07-06T16:36:23Z","title":"Measurements of $WH$ and $ZH$ production in the $H \\rightarrow b\\bar{b}$ decay channel in $pp$ collisions at 13 TeV with the ATLAS detector","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2007.02873","snapshot_observed_at":"2026-08-12T12:51:25.440560Z","title":"Measurements of WH and ZH production in the H → bb decay channel in pp collisions at 13 TeV with the ATLAS detector","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":29,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.440560Z"},"links":{"cited_paper":"/paper/2007.02873","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:13167ddfe06cf7052d8db19a243f2f7542fe867c588fbf74cb40dc529d27bd4a","observation_id":"167c7db3-893e-48aa-b6c5-109cf80542b3","resolution":{"observed_at":"2026-08-12T12:51:25.440560Z","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":"2026-08-12T12:51:25.444503Z","title":"Combined Higgs boson production and decay measurements with up to 137 fb−1 of proton-proton collision data at √s = 13 TeV","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.444503Z"},"links":{"citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:3483906b2604cfb823e5bfb3d07c0ab06377d1ccfa41b5fa3f7b14b71b382e68","observation_id":"7f2f8e00-9b02-45d7-b882-def67ed5a6bd","resolution":{"observed_at":"2026-08-12T12:51:25.444503Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2012.02779","last_updated":"2021-04-08T15:54:25Z","snapshot_observed_at":"2026-07-06T10:20:52.839902Z","submitted_at":"2020-12-04T18:56:23Z","title":"Top, Higgs, Diboson and Electroweak Fit to the Standard Model Effective Field Theory","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2012.02779","snapshot_observed_at":"2026-08-12T12:51:25.448404Z","title":"Top, higgs, diboson and electroweak fit to the standard model effective field theory","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.448404Z"},"links":{"cited_paper":"/paper/2012.02779","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:e4839c2ba88c2c0d6ffc81a2384b4a35e793bac5afebb00b5c1f3ec1e70af239","observation_id":"a82e4248-6edf-442c-b375-b30f913d9f6f","resolution":{"observed_at":"2026-08-12T12:51:25.448404Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2105.00006","last_updated":"2021-10-31T16:08:27Z","snapshot_observed_at":"2026-08-09T12:33:54.696381Z","submitted_at":"2021-04-30T18:00:01Z","title":"Combined SMEFT interpretation of Higgs, diboson, and top quark data from the LHC","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2105.00006","snapshot_observed_at":"2026-08-12T12:51:25.452454Z","title":"Combined SMEFT interpretation of Higgs, diboson, and top quark data from the LHC","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":32,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.452454Z"},"links":{"cited_paper":"/paper/2105.00006","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:1a852790d7d242d77964b3f6ad7ae8cfe964ee05d5cc909d8dbf4e39ab36d48b","observation_id":"79525673-d1d9-44f0-b975-0f308ebf807c","resolution":{"observed_at":"2026-08-12T12:51:25.452454Z","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":"10.17182/hepdata.155497","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-12T12:51:25.915466Z","title":"HEPData record for this analysis","venue":null,"work_id":"57a2dae4-e07a-43b1-9008-98e50d41b032","year":2024},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.456489Z"},"links":{"citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:e903a1ab8a026ce99ca2a9387a256ae9138d1fe0822fa5dc7a3763685e1514ac","observation_id":"d8ce29d3-ab69-4a8e-93fd-ea6acfc08e01","resolution":{"observed_at":"2026-08-12T12:51:25.919478Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+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":"2026-08-12T12:51:25.460275Z","title":"Baryon- and lepton-nonconserving processes","venue":null,"work_id":null,"year":1979},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":34,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.460275Z"},"links":{"citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:06797d14e63a687136b958de142c50a0312930719b59fae8f87ee17924cb2756","observation_id":"43242ae6-ebbd-4747-9f02-28d9b07ac11e","resolution":{"observed_at":"2026-08-12T12:51:25.460275Z","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":"2026-08-12T12:51:25.464087Z","title":"Dimension-six terms in the standard model Lagrangian","venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.464087Z"},"links":{"cited_paper":"/paper/1008.4884","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:9980b25142a6e0188e05caf547803707f07c008473a0f08797e55cfdc590f1bd","observation_id":"149353f5-9dbb-4585-8f89-0718a7ce54f1","resolution":{"observed_at":"2026-08-12T12:51:25.464087Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1411.0669","last_updated":"2015-02-05T18:10:43Z","snapshot_observed_at":"2026-07-06T03:59:25.234938Z","submitted_at":"2014-11-03T21:00:04Z","title":"Model-independent precision constraints on dimension-6 operators","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1411.0669","snapshot_observed_at":"2026-08-12T12:51:25.468151Z","title":"Model-independent precision constraints on dimension-6 operators","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":36,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.468151Z"},"links":{"cited_paper":"/paper/1411.0669","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:79eefa9a0cedbf4ea311a9c74c8077c754d41feccfd196c847a7c5a9dd1b5453","observation_id":"aec8df24-07e5-492e-b320-71bf0888f310","resolution":{"observed_at":"2026-08-12T12:51:25.468151Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1807.01796","last_updated":"2018-10-29T20:18:07Z","snapshot_observed_at":"2026-08-05T03:57:41.548803Z","submitted_at":"2018-07-04T21:43:45Z","title":"Probing Electroweak Precision Physics via boosted Higgs-strahlung at the LHC","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1807.01796","snapshot_observed_at":"2026-08-12T12:51:25.472140Z","title":"Probing electroweak precision physics via boosted Higgs-strahlung at the LHC","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":37,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.472140Z"},"links":{"cited_paper":"/paper/1807.01796","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:3dda017daa273839832a3cde4ef210783da9b93582591b14be9d3d43463c134c","observation_id":"6d9972d3-46d5-43a8-81b0-ed852c50be66","resolution":{"observed_at":"2026-08-12T12:51:25.472140Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1912.07628","last_updated":"2020-11-11T11:23:43Z","snapshot_observed_at":"2026-08-11T17:50:36.681777Z","submitted_at":"2019-12-16T19:00:13Z","title":"Towards the ultimate differential SMEFT analysis","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1912.07628","snapshot_observed_at":"2026-08-12T12:51:25.476088Z","title":"Towards the ultimate differential SMEFT analysis","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":38,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.476088Z"},"links":{"cited_paper":"/paper/1912.07628","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:c06850707cdf48377d3076a7e8a0d67d51a2a4c6ab1560529f1d114278b63035","observation_id":"2464381e-1c41-46e3-8d45-297395512e5c","resolution":{"observed_at":"2026-08-12T12:51:25.476088Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1805.00013","last_updated":"2018-07-26T19:00:29Z","snapshot_observed_at":"2026-07-06T06:36:31.526822Z","submitted_at":"2018-04-30T18:00:00Z","title":"Constraining Effective Field Theories with Machine Learning","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1805.00013","snapshot_observed_at":"2026-08-12T12:51:25.480095Z","title":"Constraining effective field theories with machine learning","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":39,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.480095Z"},"links":{"cited_paper":"/paper/1805.00013","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:24b2ef7e7cba63aafe9470271633ada47e00dd06f9a34ab12be1b378b506f318","observation_id":"d3712dd5-93ad-4dff-9021-a1250cb9bb78","resolution":{"observed_at":"2026-08-12T12:51:25.480095Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1805.12244","last_updated":"2019-08-05T14:02:58Z","snapshot_observed_at":"2026-08-10T07:24:46.700192Z","submitted_at":"2018-05-30T22:14:20Z","title":"Mining gold from implicit models to improve likelihood-free inference","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1805.12244","snapshot_observed_at":"2026-08-12T12:51:25.484234Z","title":"Mining gold from implicit models to improve likelihood-free inference","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":40,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.484234Z"},"links":{"cited_paper":"/paper/1805.12244","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:5b53ebfdb60e34901414c1680da1ac766fa5ddd56835af7011e7ef0e9b5cfedc","observation_id":"ad8a1468-d91b-4667-8a98-658c293dca97","resolution":{"observed_at":"2026-08-12T12:51:25.484234Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2007.10356","last_updated":"2020-09-18T14:45:33Z","snapshot_observed_at":"2026-08-13T07:31:49.503777Z","submitted_at":"2020-07-20T18:00:04Z","title":"Parametrized classifiers for optimal EFT sensitivity","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2007.10356","snapshot_observed_at":"2026-08-12T12:51:25.488203Z","title":"Parametrized classifiers for optimal EFT sensitivity","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":41,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.488203Z"},"links":{"cited_paper":"/paper/2007.10356","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:5a080dce76adfd580ad3b35eafdbb874cbd0848f8745aabe4a13a4334726d7fe","observation_id":"45bbe9fb-7a49-46a2-a6a6-fcd42454c8f4","resolution":{"observed_at":"2026-08-12T12:51:25.488203Z","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":"2026-08-12T12:51:25.492236Z","title":"Tree boosting for learning EFT parameters","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":42,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.492236Z"},"links":{"citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:cda3b9b96ee13d946ad60bb1386cd5966e667dbafec05180dccfdd19db2e257c","observation_id":"a3c511ac-2364-4865-9013-762be87e7c6f","resolution":{"observed_at":"2026-08-12T12:51:25.492236Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2205.12976","last_updated":"2022-05-25T18:00:03Z","snapshot_observed_at":"2026-08-13T15:36:24.826287Z","submitted_at":"2022-05-25T18:00:03Z","title":"Learning the EFT likelihood with tree boosting","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2205.12976","snapshot_observed_at":"2026-08-12T12:51:25.496017Z","title":"Learning the EFT likelihood with tree boosting","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":43,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.496017Z"},"links":{"cited_paper":"/paper/2205.12976","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:7093ff90ef062ed399627f5e07eda40bfa72c1a71b2b3b3efcb66e0b1ff1baa8","observation_id":"ff455f9a-b096-4ca2-a697-072e848330df","resolution":{"observed_at":"2026-08-12T12:51:25.496017Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2211.02058","last_updated":"2023-05-23T15:19:42Z","snapshot_observed_at":"2026-08-13T13:49:52.526966Z","submitted_at":"2022-11-03T18:00:02Z","title":"Unbinned multivariate observables for global SMEFT analyses from machine learning","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2211.02058","snapshot_observed_at":"2026-08-12T12:51:25.500152Z","title":"Unbinned multivariate observables for global SMEFT analyses from machine learning","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":44,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.500152Z"},"links":{"cited_paper":"/paper/2211.02058","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:943a6d2de080961da2ea4d0513781a87187830fb55769c9000ccc540bc155877","observation_id":"8b391a2a-8197-437c-9f3d-3b87e712e276","resolution":{"observed_at":"2026-08-12T12:51:25.500152Z","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":"2026-08-09T05:25:17.126955Z","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":"2026-08-12T12:51:25.504136Z","title":"Handbook of LHC Higgs cross sections: 4. Deciphering the nature of the Higgs sector","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":45,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.504136Z"},"links":{"cited_paper":"/paper/1610.07922","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:0036947b8959dc8bc4cdd73ec34ad2c2dd25c8210c95d970460ea0f3357553c7","observation_id":"277a3e3f-6907-4d8e-8d48-a4f4dee80935","resolution":{"observed_at":"2026-08-12T12:51:25.504136Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2109.13363","last_updated":"2022-05-15T05:11:18Z","snapshot_observed_at":"2026-08-13T18:03:58.571307Z","submitted_at":"2021-09-27T21:58:45Z","title":"Constraining anomalous Higgs boson couplings to virtual photons","version":3},"cited_work":{"arxiv_id":"2109.13363","doi":null,"metadata_source":"pith","pith_arxiv_id":"2109.13363","snapshot_observed_at":"2026-08-12T12:51:26.809932Z","title":"Constraining anomalous Higgs boson couplings to virtual photons","venue":"hep-ph","work_id":"f1f173dc-7faa-486d-9221-d68ebd66da4b","year":2021},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":46,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.508265Z"},"links":{"cited_paper":"/paper/2109.13363","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:54abb72550e3c30889da76f5d1c55ce54719deeff03d3e8166a69c02201e2ae8","observation_id":"999de85a-4345-4665-a92a-c624f56ed5b3","resolution":{"observed_at":"2026-08-12T12:51:26.814410Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2306.09963","last_updated":"2024-11-07T15:06:21Z","snapshot_observed_at":"2026-08-13T11:15:08.717921Z","submitted_at":"2023-06-16T16:45:13Z","title":"Diboson production in the SMEFT from gluon fusion","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2306.09963","snapshot_observed_at":"2026-08-12T12:51:25.512564Z","title":"Diboson production in the SMEFT from gluon fusion","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":47,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.512564Z"},"links":{"cited_paper":"/paper/2306.09963","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:4cdd44b9c8d47795f31f800cfb7386e6626bcc70be718f961bae8e778a45bc33","observation_id":"40eb8026-8093-4ef1-9032-416149170830","resolution":{"observed_at":"2026-08-12T12:51:25.512564Z","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":"2026-08-12T12:51:25.516862Z","title":"The CMS experiment at the CERN LHC","venue":null,"work_id":null,"year":2008},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":48,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.516862Z"},"links":{"citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:1135296b72e9b22149bf4a215459914be8c6b46e8ae6a4e34a5c79f08315fff9","observation_id":"57ba8af4-14e5-459b-8492-118010a47b92","resolution":{"observed_at":"2026-08-12T12:51:25.516862Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2309.05466","last_updated":"2024-05-30T20:06:18Z","snapshot_observed_at":"2026-08-13T11:17:27.420331Z","submitted_at":"2023-09-11T14:08:49Z","title":"Development of the CMS detector for the CERN LHC Run 3","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2309.05466","snapshot_observed_at":"2026-08-12T12:51:25.520886Z","title":"Development of the CMS detector for the CERN LHC Run 3","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":49,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.520886Z"},"links":{"cited_paper":"/paper/2309.05466","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:5b595db7b87e689bd51436b17c33dcf4731d81516f3ba0b7d99ffe9c32269cbe","observation_id":"06d70011-9236-4896-9b3a-a610056e0d5d","resolution":{"observed_at":"2026-08-12T12:51:25.520886Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1405.6569","last_updated":"2014-10-28T15:10:15Z","snapshot_observed_at":"2026-07-06T02:11:23.670680Z","submitted_at":"2014-05-26T13:38:11Z","title":"Description and performance of track and primary-vertex reconstruction with the CMS tracker","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1405.6569","snapshot_observed_at":"2026-08-12T12:51:25.524892Z","title":"Description and performance of track and primary-vertex reconstruction with the CMS tracker","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":50,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.524892Z"},"links":{"cited_paper":"/paper/1405.6569","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:13c67b6262003e95d40f1ccd58b8848c7fdba9fd050bd85c35e648630ebe460f","observation_id":"37bbfafb-6722-4f7c-9201-9cab15e797fd","resolution":{"observed_at":"2026-08-12T12:51:25.524892Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2012.14304","last_updated":"2020-12-22T16:28:59Z","snapshot_observed_at":"2026-08-08T22:50:04.478622Z","submitted_at":"2020-12-22T16:28:59Z","title":"The CMS Phase-1 Pixel Detector Upgrade","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2012.14304","snapshot_observed_at":"2026-08-12T12:51:25.528881Z","title":"The CMS phase-1 pixel detector upgrade","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":51,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.528881Z"},"links":{"cited_paper":"/paper/2012.14304","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:01f928ab15d03e654a36daf4d641453d823f37e59671bb63374a7be7d209aeb3","observation_id":"de224cf6-156c-4fc2-ad92-b77bddd29218","resolution":{"observed_at":"2026-08-12T12:51:25.528881Z","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":"2026-08-12T12:51:25.532851Z","title":"Track impact parameter resolution for the full pseudo rapidity coverage in the 2017 dataset with the CMS phase-1 pixel detector","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":52,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.532851Z"},"links":{"citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:54688174a6338ab64281ffbe4c140049d5c17318c93513eb9c1212c9ea6360ad","observation_id":"cc5ea783-06ea-44c2-8830-fbe13274cba5","resolution":{"observed_at":"2026-08-12T12:51:25.532851Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1706.04965","last_updated":"2017-10-09T17:28:30Z","snapshot_observed_at":"2026-07-06T02:11:23.670680Z","submitted_at":"2017-06-15T17:02:16Z","title":"Particle-flow reconstruction and global event description with the CMS detector","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1706.04965","snapshot_observed_at":"2026-08-12T12:51:25.536664Z","title":"Particle-flow reconstruction and global event description with the CMS detector","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":53,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.536664Z"},"links":{"cited_paper":"/paper/1706.04965","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:f96df87387f78deb7b942ce9341144791693db61697d6203e49579d6e564d602","observation_id":"67a17d32-ecc3-45ec-b351-b7be068f6013","resolution":{"observed_at":"2026-08-12T12:51:25.536664Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2006.10165","last_updated":"2020-10-19T20:23:25Z","snapshot_observed_at":"2026-08-13T15:26:13.804191Z","submitted_at":"2020-06-17T21:21:21Z","title":"Performance of the CMS Level-1 trigger in proton-proton collisions at $\\sqrt{s} =$ 13 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2006.10165","snapshot_observed_at":"2026-08-12T12:51:25.540576Z","title":"Performance of the CMS Level-1 trigger in proton-proton collisions at √s = 13 TeV","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":54,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.540576Z"},"links":{"cited_paper":"/paper/2006.10165","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:d50ad9d7e2283a35d657ca41dc5293d2ec77ca9d095f20ba02c176681b33d947","observation_id":"eda2300e-fff0-46be-b71c-7c8936886952","resolution":{"observed_at":"2026-08-12T12:51:25.540576Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1609.02366","last_updated":"2017-01-25T15:35:04Z","snapshot_observed_at":"2026-07-06T02:11:23.670680Z","submitted_at":"2016-09-08T10:11:43Z","title":"The CMS trigger system","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1609.02366","snapshot_observed_at":"2026-08-12T12:51:25.544910Z","title":"The CMS trigger system","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":55,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.544910Z"},"links":{"cited_paper":"/paper/1609.02366","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:8021c17f9c9eb40a1b7c8f1932ae1f94fd6b59cca963506fc4598abc295cb005","observation_id":"253e1273-6fa2-4d69-854c-a3c1ecce5d91","resolution":{"observed_at":"2026-08-12T12:51:25.544910Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2102.04790","last_updated":"2021-07-04T12:06:24Z","snapshot_observed_at":"2026-08-12T17:45:48.810231Z","submitted_at":"2021-02-09T12:12:33Z","title":"Performance of the CMS muon trigger system in proton-proton collisions at $\\sqrt{s} =$ 13 TeV","version":2},"cited_work":{"arxiv_id":"2102.04790","doi":null,"metadata_source":"pith","pith_arxiv_id":"2102.04790","snapshot_observed_at":"2026-08-12T12:51:26.697093Z","title":"Performance of the CMS muon trigger system in proton-proton collisions at $\\sqrt{s} =$ 13 TeV","venue":"hep-ex","work_id":"a13cd042-2c80-44da-aefb-ce0e05f1bfe4","year":2021},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":56,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.548927Z"},"links":{"cited_paper":"/paper/2102.04790","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:1c0670a894c29d06ebb98a19c918e22d31cc2b225e5ae764be7995d5f0138092","observation_id":"8ece9f84-ce0b-4a55-8faf-d52f6f7bca84","resolution":{"observed_at":"2026-08-12T12:51:26.701944Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0409146","last_updated":"2004-09-13T15:09:18Z","snapshot_observed_at":"2026-07-06T02:11:23.670680Z","submitted_at":"2004-09-13T15:09:18Z","title":"A New Method for Combining NLO QCD with Shower Monte Carlo Algorithms","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0409146","snapshot_observed_at":"2026-08-12T12:51:25.552952Z","title":"A New method for combining NLO QCD with shower Monte Carlo algorithms","venue":null,"work_id":null,"year":2004},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":57,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.552952Z"},"links":{"cited_paper":"/paper/hep-ph/0409146","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:e9343ce88bc9f667a39dd5912dd289e24ac96660bfddc42b20d59f23331db42f","observation_id":"6029c302-0a27-45e7-9063-c0a5dd1f4a4c","resolution":{"observed_at":"2026-08-12T12:51:25.552952Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0709.2092","last_updated":"2007-09-13T17:49:16Z","snapshot_observed_at":"2026-08-07T18:07:31.311870Z","submitted_at":"2007-09-13T17:49:16Z","title":"Matching NLO QCD computations with Parton Shower simulations: the POWHEG method","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0709.2092","snapshot_observed_at":"2026-08-12T12:51:25.556941Z","title":"Matching NLO QCD computations with parton shower simulations: the POWHEG method","venue":null,"work_id":null,"year":2007},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":58,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.556941Z"},"links":{"cited_paper":"/paper/0709.2092","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:0f06744604d96bdb2978388453186e7f1239042a24f3f5a854b4663bbec64ddf","observation_id":"9d08ccc0-4d89-4f08-873a-3d7757e349c7","resolution":{"observed_at":"2026-08-12T12:51:25.556941Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1002.2581","last_updated":"2010-02-12T16:07:27Z","snapshot_observed_at":"2026-07-06T02:06:43.898500Z","submitted_at":"2010-02-12T16:07:27Z","title":"A general framework for implementing NLO calculations in shower Monte Carlo programs: the POWHEG BOX","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1002.2581","snapshot_observed_at":"2026-08-12T12:51:25.560840Z","title":"A general framework for implementing NLO calculations in shower Monte Carlo programs: the POWHEG BOX","venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":59,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.560840Z"},"links":{"cited_paper":"/paper/1002.2581","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:e1d7a12ac3bc57c4046acb3fb3b398d27a96dc21691de8d35826df82dcf24f92","observation_id":"c7735930-f072-44c2-951a-84c44e61aa8c","resolution":{"observed_at":"2026-08-12T12:51:25.560840Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0707.3088","last_updated":"2007-09-22T14:46:39Z","snapshot_observed_at":"2026-07-06T01:29:38.477605Z","submitted_at":"2007-07-20T15:04:38Z","title":"A Positive-Weight Next-to-Leading-Order Monte Carlo for Heavy Flavour Hadroproduction","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0707.3088","snapshot_observed_at":"2026-08-12T12:51:25.564924Z","title":"A positive-weight next-to-leading-order Monte Carlo for heavy flavour hadroproduction","venue":null,"work_id":null,"year":2007},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":60,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.564924Z"},"links":{"cited_paper":"/paper/0707.3088","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:0b618c57e2289f744cfac3b25f04233e725b25807846a2c3a907cc4621f82da9","observation_id":"7d5131bb-0c48-4f06-9be0-02a902fb88c2","resolution":{"observed_at":"2026-08-12T12:51:25.564924Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1112.5675","last_updated":"2013-03-27T17:28:42Z","snapshot_observed_at":"2026-08-03T00:06:09.978819Z","submitted_at":"2011-12-23T23:40:35Z","title":"Top++: a program for the calculation of the top-pair cross-section at hadron colliders","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1112.5675","snapshot_observed_at":"2026-08-12T12:51:25.568891Z","title":"Top++: a program for the calculation of the top-pair cross-section at hadron colliders","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":61,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.568891Z"},"links":{"cited_paper":"/paper/1112.5675","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:fd637b7ea3649798808406a9c640269854cccd23e5d5722e8b8078f5efaa2a75","observation_id":"29d7155a-d883-47a9-98a0-4a17b32a1db0","resolution":{"observed_at":"2026-08-12T12:51:25.568891Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1207.5391","last_updated":"2012-10-02T15:17:47Z","snapshot_observed_at":"2026-08-02T02:59:59.833887Z","submitted_at":"2012-07-23T13:45:41Z","title":"Single-top t-channel hadroproduction in the four-flavour scheme with POWHEG and aMC@NLO","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1207.5391","snapshot_observed_at":"2026-08-12T12:51:25.572786Z","title":"Single-topt-channel hadroproduction in the four-flavour scheme with POWHEG and aMC@NLO","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":62,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.572786Z"},"links":{"cited_paper":"/paper/1207.5391","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:5e8f0571d15d826443b70b330de6b557a9614ae40a25b317d0d3e77b4cfd6985","observation_id":"c5ed2f08-cc23-4de8-ae45-a42174b40ff2","resolution":{"observed_at":"2026-08-12T12:51:25.572786Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1009.2450","last_updated":"2010-09-13T17:00:38Z","snapshot_observed_at":"2026-08-04T12:34:37.080715Z","submitted_at":"2010-09-13T17:00:38Z","title":"Single-top Wt-channel production matched with parton showers using the POWHEG method","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1009.2450","snapshot_observed_at":"2026-08-12T12:51:25.577001Z","title":"Single-top Wt-channel production matched with parton showers using the POWHEG method","venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":63,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.577001Z"},"links":{"cited_paper":"/paper/1009.2450","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:9246d2514c40aab3d0a4d42541023a3ad385b49f45d1a5808c24b72bf169b14d","observation_id":"2414a6e5-6120-4737-a29f-4cc862e95de7","resolution":{"observed_at":"2026-08-12T12:51:25.577001Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1405.0301","last_updated":"2014-07-21T09:46:15Z","snapshot_observed_at":"2026-07-06T02:11:23.670680Z","submitted_at":"2014-05-01T20:24:46Z","title":"The automated computation of tree-level and next-to-leading order differential cross sections, and their matching to parton shower simulations","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1405.0301","snapshot_observed_at":"2026-08-12T12:51:25.581010Z","title":"The automated computation of tree-level and next-to-leading order differential cross sections, and their matching to parton shower simulations","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":64,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.581010Z"},"links":{"cited_paper":"/paper/1405.0301","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:309958cb8a85cb6013cb0ff9acd2b4b9bd445da62b5d142a689f292012ffeaf5","observation_id":"9251fdb7-6acd-4f83-9220-501d0d528442","resolution":{"observed_at":"2026-08-12T12:51:25.581010Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1212.3460","last_updated":"2013-03-11T08:31:32Z","snapshot_observed_at":"2026-08-10T09:10:10.262171Z","submitted_at":"2012-12-14T12:57:29Z","title":"Automatic spin-entangled decays of heavy resonances in Monte Carlo simulations","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1212.3460","snapshot_observed_at":"2026-08-12T12:51:25.585050Z","title":"Automatic spin-entangled decays of heavy resonances in Monte Carlo simulations","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":65,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.585050Z"},"links":{"cited_paper":"/paper/1212.3460","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:b6201839a766b6148d87f177d234468ef5e9ae52dda5faa62a635ab0c4ede387","observation_id":"928ddd00-b57f-4a4a-b545-a60048b74f74","resolution":{"observed_at":"2026-08-12T12:51:25.585050Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0706.2569","last_updated":"2008-01-16T17:24:24Z","snapshot_observed_at":"2026-08-06T19:41:15.386949Z","submitted_at":"2007-06-18T10:31:19Z","title":"Comparative study of various algorithms for the merging of parton showers and matrix elements in hadronic collisions","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0706.2569","snapshot_observed_at":"2026-08-12T12:51:25.589090Z","title":"Comparative study of various algorithms for the merging of parton showers and matrix elements in hadronic collisions","venue":null,"work_id":null,"year":2008},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":66,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.589090Z"},"links":{"cited_paper":"/paper/0706.2569","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:f24ab267e99ea9fccd9e712e6cb70cfd52ea5e736d5e7575472079ca86aa12ec","observation_id":"508d615a-a553-4948-ad35-035868f215d8","resolution":{"observed_at":"2026-08-12T12:51:25.589090Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1209.6215","last_updated":"2012-09-27T13:10:53Z","snapshot_observed_at":"2026-07-06T02:11:23.670680Z","submitted_at":"2012-09-27T13:10:53Z","title":"Merging meets matching in MC@NLO","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1209.6215","snapshot_observed_at":"2026-08-12T12:51:25.592896Z","title":"Merging meets matching in MC@NLO","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":67,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.592896Z"},"links":{"cited_paper":"/paper/1209.6215","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:ce6fa30f7fdb199183349c707138289d8f1a422aef7f75ae5abbede89ac6ceb5","observation_id":"c0bbc782-dc69-469b-9da9-df7c14210bff","resolution":{"observed_at":"2026-08-12T12:51:25.592896Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2406.14620","last_updated":"2024-12-04T10:15:39Z","snapshot_observed_at":"2026-08-12T23:38:05.549424Z","submitted_at":"2024-06-20T18:00:03Z","title":"LHC EFT WG Note: SMEFT predictions, event reweighting, and simulation","version":5},"cited_work":{"arxiv_id":"2406.14620","doi":null,"metadata_source":"pith","pith_arxiv_id":"2406.14620","snapshot_observed_at":"2026-08-12T12:51:26.542496Z","title":"LHC EFT WG Note: SMEFT predictions, event reweighting, and simulation","venue":"hep-ph","work_id":"ca07d097-4cc2-426e-be06-142b88d980b0","year":2024},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":68,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.597145Z"},"links":{"cited_paper":"/paper/2406.14620","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:6fcfb0c5c716a021f3206909992bdfc585bbddfa45fee20aced2d345942129ef","observation_id":"6ef4bcec-585e-484b-a137-fb13123dd80f","resolution":{"observed_at":"2026-08-12T12:51:26.547095Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1206.3572","last_updated":"2012-06-15T20:00:03Z","snapshot_observed_at":"2026-08-10T07:40:10.562901Z","submitted_at":"2012-06-15T20:00:03Z","title":"MINLO: Multi-scale improved NLO","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1206.3572","snapshot_observed_at":"2026-08-12T12:51:25.601225Z","title":"MINLO: multi-scale improved NLO","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":69,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.601225Z"},"links":{"cited_paper":"/paper/1206.3572","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:5eca602ef67605ebb344d737ca78edbed6464f21d7478e32b6367a7ed286d0c4","observation_id":"8083f07a-0e2f-48a0-b248-0b5faab61b4d","resolution":{"observed_at":"2026-08-12T12:51:25.601225Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1306.2542","last_updated":"2013-10-01T10:50:21Z","snapshot_observed_at":"2026-07-06T03:15:35.443617Z","submitted_at":"2013-06-11T14:51:41Z","title":"HW/HZ + 0 and 1 jet at NLO with the POWHEG BOX interfaced to GoSam and their merging within MiNLO","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1306.2542","snapshot_observed_at":"2026-08-12T12:51:25.605196Z","title":"HW/HZ + 0 and 1 jet at NLO with the POWHEG BOX interfaced to GoSam and their merging within MiNLO","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":70,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.605196Z"},"links":{"cited_paper":"/paper/1306.2542","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:43db2380897e7e81085e55c22c22e0279a52522041c7fc3b5c38eaaa25741f68","observation_id":"746706df-f665-44c3-baef-bd131fc9a745","resolution":{"observed_at":"2026-08-12T12:51:25.605196Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1709.06492","last_updated":"2017-12-20T12:59:55Z","snapshot_observed_at":"2026-08-12T01:38:51.666875Z","submitted_at":"2017-09-19T15:51:50Z","title":"The SMEFTsim package, theory and tools","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1709.06492","snapshot_observed_at":"2026-08-12T12:51:25.609576Z","title":"The SMEFTsim package, theory and tools","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":71,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.609576Z"},"links":{"cited_paper":"/paper/1709.06492","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:3f84290cc82d31cd847f590b9bf7c07c8eb35a0bef5e3073d1951cc20947ffc8","observation_id":"54df2860-1935-4feb-a6d0-a0bda07a4850","resolution":{"observed_at":"2026-08-12T12:51:25.609576Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2012.11343","last_updated":"2021-08-18T08:49:26Z","snapshot_observed_at":"2026-08-10T05:21:01.695651Z","submitted_at":"2020-12-21T13:47:03Z","title":"SMEFTsim 3.0 -- a practical guide","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2012.11343","snapshot_observed_at":"2026-08-12T12:51:25.613632Z","title":"SMEFTsim 3.0 — a practical guide","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":72,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.613632Z"},"links":{"cited_paper":"/paper/2012.11343","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:c3fc0283fb57ac1c781ed5f49110108bf04a1d50168813645bd4766a5cd0945b","observation_id":"c5f954b7-420d-43e4-857f-27812cc7f3cc","resolution":{"observed_at":"2026-08-12T12:51:25.613632Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1906.06949","last_updated":"2019-10-09T09:12:32Z","snapshot_observed_at":"2026-08-10T23:24:23.178715Z","submitted_at":"2019-06-17T11:05:30Z","title":"The Higgs width in the SMEFT","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1906.06949","snapshot_observed_at":"2026-08-12T12:51:25.617636Z","title":"The Higgs width in the SMEFT","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":73,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.617636Z"},"links":{"cited_paper":"/paper/1906.06949","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:f37ead6551a0961a87d9cede042f79fac3327ef71b6d09d0eb4265acef182842","observation_id":"9287c498-8b4d-49c9-9d7c-e8387ae8d55d","resolution":{"observed_at":"2026-08-12T12:51:25.617636Z","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":"10.22323/1.073.0025","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-12T12:51:25.879277Z","title":"MadWeight: automatic event reweighting with matrix elements","venue":null,"work_id":"5425248a-0cf2-4f56-9f00-a1f23d15dbda","year":2008},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":74,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.621740Z"},"links":{"citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:b00d2695e7e9562c7d97b00d2212947dfd0f304a9298942194f06825e5403ea3","observation_id":"2eebce88-4fd3-4068-a310-06f3985c978c","resolution":{"observed_at":"2026-08-12T12:51:25.885104Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1706.00428","last_updated":"2017-09-22T16:31:07Z","snapshot_observed_at":"2026-07-06T02:11:23.670680Z","submitted_at":"2017-06-01T18:00:01Z","title":"Parton distributions from high-precision collider data","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1706.00428","snapshot_observed_at":"2026-08-12T12:51:25.625572Z","title":"Parton distributions from high-precision collider data","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":75,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.625572Z"},"links":{"cited_paper":"/paper/1706.00428","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:de6b642a9095281c86a5f1acfd1b24b2536e9e1a67ce87e11d5a3a1175631c2d","observation_id":"ba890bea-7a9e-4c17-bfa0-19fa8f7f805c","resolution":{"observed_at":"2026-08-12T12:51:25.625572Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1903.12179","last_updated":"2020-01-05T21:49:38Z","snapshot_observed_at":"2026-08-05T21:36:34.054502Z","submitted_at":"2019-03-28T16:29:09Z","title":"Extraction and validation of a new set of CMS PYTHIA8 tunes from underlying-event measurements","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1903.12179","snapshot_observed_at":"2026-08-12T12:51:25.629437Z","title":"Extraction and validation of a new set of CMS PYTHIA8 tunes from underlying-event measurements","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":76,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.629437Z"},"links":{"cited_paper":"/paper/1903.12179","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:57f58829453b987af5f0b836740bef0375f7749e1237196452b9acab22678239","observation_id":"3bcfead3-29d8-422f-ab6b-45e8688205d5","resolution":{"observed_at":"2026-08-12T12:51:25.629437Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1802.02613","last_updated":"2018-08-08T16:56:23Z","snapshot_observed_at":"2026-07-06T06:22:17.424495Z","submitted_at":"2018-02-07T19:39:40Z","title":"Measurement of the inelastic proton-proton cross section at $\\sqrt{s}=$ 13 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1802.02613","snapshot_observed_at":"2026-08-12T12:51:25.633454Z","title":"Measurement of the inelastic proton-proton cross section at√s = 13 TeV","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":77,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.633454Z"},"links":{"cited_paper":"/paper/1802.02613","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:7a6c2a27d8790aa8554123d84ee55e8df4dae0321d7e9590ce755d5e57dd64af","observation_id":"f8ac973e-39e3-4e66-87ed-63b655bcf4d3","resolution":{"observed_at":"2026-08-12T12:51:25.633454Z","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":"2026-08-12T12:51:25.637537Z","title":"G EANT 4—a simulation toolkit","venue":null,"work_id":null,"year":2003},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":78,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.637537Z"},"links":{"citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:0d1a4f2dee0a1340f59c75b146851a8e46e652d307073c154b76bdc824cb073c","observation_id":"acea65bc-9bdf-4bf1-92ff-ce649f7cf7b2","resolution":{"observed_at":"2026-08-12T12:51:25.637537Z","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":"2026-08-12T12:51:25.641675Z","title":"Technical proposal for the Phase-II upgrade of the Compact Muon Solenoid","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":79,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.641675Z"},"links":{"citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:a27809c794a666d7290c90b867d96cf042f83c324f55a4eab1c7e2e0b5e8f6e1","observation_id":"a686b3b5-4b2f-45fd-94a9-6cefe80bcb6f","resolution":{"observed_at":"2026-08-12T12:51:25.641675Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2012.06888","last_updated":"2021-05-17T23:09:51Z","snapshot_observed_at":"2026-07-06T10:23:49.697086Z","submitted_at":"2020-12-12T19:08:13Z","title":"Electron and photon reconstruction and identification with the CMS experiment at the CERN LHC","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2012.06888","snapshot_observed_at":"2026-08-12T12:51:25.645521Z","title":"Electron and photon reconstruction and identification with the CMS experiment at the CERN LHC","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":80,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.645521Z"},"links":{"cited_paper":"/paper/2012.06888","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:1076aebac3743b7b6727efdae3b0aba3c34c9c395db6f411509fc0204f9623b1","observation_id":"ebadfdd9-4b14-4179-aa32-2dfccd43b135","resolution":{"observed_at":"2026-08-12T12:51:25.645521Z","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":"2026-08-12T12:51:25.649762Z","title":"ECAL 2016 refined calibration and Run2 summary plots","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":81,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.649762Z"},"links":{"citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:b49197808b197c7236bf0cf1442ce4a15d107b66b29a03adf5af6c2179cb0917","observation_id":"99622ed5-cc5e-4489-9d40-45392a132796","resolution":{"observed_at":"2026-08-12T12:51:25.649762Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1804.04528","last_updated":"2018-06-20T09:58:05Z","snapshot_observed_at":"2026-08-13T15:01:53.705880Z","submitted_at":"2018-04-12T14:19:59Z","title":"Performance of the CMS muon detector and muon reconstruction with proton-proton collisions at $\\sqrt{s}=$ 13 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1804.04528","snapshot_observed_at":"2026-08-12T12:51:25.653528Z","title":"Performance of the CMS muon detector and muon reconstruction with proton-proton collisions at √s = 13 TeV","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":82,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.653528Z"},"links":{"cited_paper":"/paper/1804.04528","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:12b42fa83b2535fd164db1340b477757d0b6e87ad3b62f0cf0d15fa54a4120dc","observation_id":"f78faf82-c45f-44df-a985-ea03787828e6","resolution":{"observed_at":"2026-08-12T12:51:25.653528Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0802.1189","last_updated":"2008-04-21T21:44:17Z","snapshot_observed_at":"2026-07-06T01:34:46.001237Z","submitted_at":"2008-02-08T18:17:17Z","title":"The anti-k_t jet clustering algorithm","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0802.1189","snapshot_observed_at":"2026-08-12T12:51:25.657701Z","title":"The anti-kT jet clustering algorithm","venue":null,"work_id":null,"year":2008},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":83,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.657701Z"},"links":{"cited_paper":"/paper/0802.1189","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:0f751a5db388299972d5dfa75ac25595ba7e3c0f63ab05b65d544874250ef794","observation_id":"0e508e3d-f974-44ff-9a1d-901320fa4d49","resolution":{"observed_at":"2026-08-12T12:51:25.657701Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1111.6097","last_updated":"2011-11-25T20:37:47Z","snapshot_observed_at":"2026-08-02T19:23:48.927074Z","submitted_at":"2011-11-25T20:37:47Z","title":"FastJet user manual","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1111.6097","snapshot_observed_at":"2026-08-12T12:51:25.661688Z","title":"FastJet user manual","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":84,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.661688Z"},"links":{"cited_paper":"/paper/1111.6097","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:d72b5ffb1e8ee455c32aca79c172fc11a5be4096c8f5c0326318c8b6fac10105","observation_id":"609d34ff-5184-4b66-a5ad-827810e61904","resolution":{"observed_at":"2026-08-12T12:51:25.661688Z","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":"2026-08-12T12:51:25.666737Z","title":"Jet energy scale and resolution measurement with Run 2 legacy data collected by CMS at 13 TeV","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":85,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.666737Z"},"links":{"citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:d4611617894e54b66bfbf03cddb8b23b2ab659b63bcb42f7accaa72401fb3792","observation_id":"2cb95a73-5393-45d1-8c43-85962513884c","resolution":{"observed_at":"2026-08-12T12:51:25.666737Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0707.1378","last_updated":"2008-01-09T08:27:05Z","snapshot_observed_at":"2026-08-10T10:53:54.386519Z","submitted_at":"2007-07-10T13:53:09Z","title":"Pileup subtraction using jet areas","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0707.1378","snapshot_observed_at":"2026-08-12T12:51:25.670534Z","title":"Pileup subtraction using jet areas","venue":null,"work_id":null,"year":2008},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":86,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.670534Z"},"links":{"cited_paper":"/paper/0707.1378","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:602e67ddd079b07a42e083882f160ba57838d888099188abf40f3a1ca6fd6d1e","observation_id":"914bfbd8-baba-4c19-a1c5-6d83f502aba2","resolution":{"observed_at":"2026-08-12T12:51:25.670534Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1607.03663","last_updated":"2017-02-26T16:27:23Z","snapshot_observed_at":"2026-08-10T09:14:31.164299Z","submitted_at":"2016-07-13T10:00:10Z","title":"Jet energy scale and resolution in the CMS experiment in pp collisions at 8 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1607.03663","snapshot_observed_at":"2026-08-12T12:51:25.675658Z","title":"Jet energy scale and resolution in the CMS experiment in pp collisions at 8 TeV","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":87,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.675658Z"},"links":{"cited_paper":"/paper/1607.03663","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:ff911c99f64d44d56a99467004b72301127f66fcb36dd6448f5bf6c4ad9c7df1","observation_id":"21b99878-5060-4850-925b-61a75394d1b9","resolution":{"observed_at":"2026-08-12T12:51:25.675658Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1407.6013","last_updated":"2014-09-30T00:58:29Z","snapshot_observed_at":"2026-08-13T12:00:05.716625Z","submitted_at":"2014-07-22T20:00:30Z","title":"Pileup Per Particle Identification","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1407.6013","snapshot_observed_at":"2026-08-12T12:51:25.679658Z","title":"Pileup per particle identification","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":88,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.679658Z"},"links":{"cited_paper":"/paper/1407.6013","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:9479699cb21b83afdb240532d5332509e0a54cc86a2193b4efa4c17e8859ac64","observation_id":"b76ee133-79ac-4c8f-a447-8b510b62ca76","resolution":{"observed_at":"2026-08-12T12:51:25.679658Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2003.00503","last_updated":"2020-09-17T14:24:07Z","snapshot_observed_at":"2026-08-11T00:36:00.125055Z","submitted_at":"2020-03-01T15:30:21Z","title":"Pileup mitigation at CMS in 13 TeV data","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2003.00503","snapshot_observed_at":"2026-08-12T12:51:25.683547Z","title":"Pileup mitigation at CMS in 13 TeV data","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":89,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.683547Z"},"links":{"cited_paper":"/paper/2003.00503","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:79b935633fa71cb419b3b955d0e66f625319e21dc408272c5b4105a37023d543","observation_id":"06f6eb44-9801-4c01-8011-7d2636dda1af","resolution":{"observed_at":"2026-08-12T12:51:25.683547Z","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":"2026-08-12T12:51:25.687673Z","title":"Jet algorithms performance in 13 TeV data","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":90,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.687673Z"},"links":{"citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:72aca1c1ed603ecf749730d06a8dc3a35061f9fccfa22a645d1e772599d6bf57","observation_id":"ebe8f308-9178-40c4-8905-5a1dc57f58a3","resolution":{"observed_at":"2026-08-12T12:51:25.687673Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2008.10519","last_updated":"2020-10-27T21:39:30Z","snapshot_observed_at":"2026-08-06T10:58:22.456881Z","submitted_at":"2020-08-24T15:42:36Z","title":"Jet Flavour Classification Using DeepJet","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2008.10519","snapshot_observed_at":"2026-08-12T12:51:25.691462Z","title":"Jet flavour classification using DeepJet","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":91,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.691462Z"},"links":{"cited_paper":"/paper/2008.10519","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:ed46ebd053d344445c8d7a559bf5d21d6ae51528ef574151999c1b42093c5344","observation_id":"8c03d374-b8db-4d54-bad5-429f139aca5d","resolution":{"observed_at":"2026-08-12T12:51:25.691462Z","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":"2026-08-12T12:51:25.695479Z","title":"Performance summary of AK4 jet b tagging with data from proton-proton collisions at 13 TeV","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":92,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.695479Z"},"links":{"citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:189cae08013541d8dce70a73a83a9a2e4a813e2789229b80e3160ae3a8937300","observation_id":"9145f5c9-c2eb-4d60-ad22-0cc1e45ae2e5","resolution":{"observed_at":"2026-08-12T12:51:25.695479Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1912.06046","last_updated":"2020-11-05T19:27:38Z","snapshot_observed_at":"2026-07-06T08:44:06.481703Z","submitted_at":"2019-12-12T15:50:03Z","title":"A deep neural network for simultaneous estimation of b jet energy and resolution","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1912.06046","snapshot_observed_at":"2026-08-12T12:51:25.699319Z","title":"A deep neural network for simultaneous estimation of b jet energy and resolution","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":93,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.699319Z"},"links":{"cited_paper":"/paper/1912.06046","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:5529911aa02cdea903332d35183883efa023afab8818b1f9a9bf4060a32a75eb","observation_id":"9168e4c8-0621-4888-8215-23bd375eaadb","resolution":{"observed_at":"2026-08-12T12:51:25.699319Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1902.08570","last_updated":"2020-03-30T15:57:41Z","snapshot_observed_at":"2026-08-08T07:02:39.109312Z","submitted_at":"2019-02-22T17:26:39Z","title":"ParticleNet: Jet Tagging via Particle Clouds","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1902.08570","snapshot_observed_at":"2026-08-12T12:51:25.703304Z","title":"Jet tagging via particle clouds","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":94,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.703304Z"},"links":{"cited_paper":"/paper/1902.08570","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:8b4aecfc2af635069915f13e85ace2720a9073f3bc16ec318a5735060e907c1d","observation_id":"3a3c5987-a5ad-4c0b-867c-da440dd20265","resolution":{"observed_at":"2026-08-12T12:51:25.703304Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0802.2470","last_updated":"2008-06-19T09:05:18Z","snapshot_observed_at":"2026-07-06T01:35:39.772283Z","submitted_at":"2008-02-18T19:57:19Z","title":"Jet substructure as a new Higgs search channel at the LHC","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0802.2470","snapshot_observed_at":"2026-08-12T12:51:25.707877Z","title":"Jet substructure as a new Higgs search channel at the LHC","venue":null,"work_id":null,"year":2008},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":95,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.707877Z"},"links":{"cited_paper":"/paper/0802.2470","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:cdeb1b96662f012d5a19440782322a7e4fe5dcccdc3237eb1c779a8e208bc7b2","observation_id":"eba4e7a0-fb3d-46a4-963c-a64fcb779289","resolution":{"observed_at":"2026-08-12T12:51:25.707877Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1307.0007","last_updated":"2013-09-05T07:53:00Z","snapshot_observed_at":"2026-08-10T07:11:47.571566Z","submitted_at":"2013-06-28T20:00:02Z","title":"Towards an understanding of jet substructure","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1307.0007","snapshot_observed_at":"2026-08-12T12:51:25.712102Z","title":"Towards an understanding of jet substructure","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":96,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.712102Z"},"links":{"cited_paper":"/paper/1307.0007","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:17da5f7c45208e74b264934367c90f440fafbbad24526b87b65ddb1e913ae01f","observation_id":"8457ce52-8193-4161-ba88-e930266eb195","resolution":{"observed_at":"2026-08-12T12:51:25.712102Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1402.2657","last_updated":"2014-05-13T07:41:29Z","snapshot_observed_at":"2026-07-06T03:35:44.240652Z","submitted_at":"2014-02-11T21:00:11Z","title":"Soft Drop","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1402.2657","snapshot_observed_at":"2026-08-12T12:51:25.716004Z","title":"Soft Drop","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":97,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.716004Z"},"links":{"cited_paper":"/paper/1402.2657","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:d9995b89fa414bc88da2f7b969210f25c62c92974bcb41862613fa65ae7a8334","observation_id":"77e79783-b97b-41ad-872f-afe959950b7d","resolution":{"observed_at":"2026-08-12T12:51:25.716004Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9707323","last_updated":"1997-08-23T10:15:05Z","snapshot_observed_at":"2026-07-07T04:26:19.861370Z","submitted_at":"1997-07-11T13:56:31Z","title":"Better Jet Clustering Algorithms","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9707323","snapshot_observed_at":"2026-08-12T12:51:25.719922Z","title":"Better jet clustering algorithms","venue":null,"work_id":null,"year":1997},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":98,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.719922Z"},"links":{"cited_paper":"/paper/hep-ph/9707323","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:49a43f38397c7c3ec5ae47285fd8b41bd2f99c66ac0ef6d7f6abbccc726f01dd","observation_id":"7c89cf3b-5b75-4ffd-8d2a-bc8e3aa2de23","resolution":{"observed_at":"2026-08-12T12:51:25.719922Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9907280","last_updated":"1999-07-08T16:22:59Z","snapshot_observed_at":"2026-07-07T04:33:42.809220Z","submitted_at":"1999-07-08T16:22:59Z","title":"Hadronization Corrections to Jet Cross Sections in Deep-Inelastic Scattering","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9907280","snapshot_observed_at":"2026-08-12T12:51:25.724113Z","title":"Hadronization corrections to jet cross-sections in deep inelastic scattering","venue":null,"work_id":null,"year":1998},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":99,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.724113Z"},"links":{"cited_paper":"/paper/hep-ph/9907280","citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:8aac06b7b1eb94ac1d799ba920c66ab759ab586cfdb959949da88fddb39b575c","observation_id":"0d7d65f7-2a24-404b-a32c-f703a29ecb08","resolution":{"observed_at":"2026-08-12T12:51:25.724113Z","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":"2026-08-12T12:51:25.728284Z","title":"Identification of highly Lorentz-boosted heavy particles using graph neural networks and new mass decorrelation techniques","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":100,"source":"pdf_text","source_observed_at":"2026-08-12T12:51:25.728284Z"},"links":{"citing_paper":"/paper/2411.16907"},"observation_digest":"sha256:3ccc7b46dab4bde8206c82d27d667337d53488d44406ee6c82d96a76d0347956","observation_id":"c45b26ea-a2a9-4f89-8f19-90432daf5a48","resolution":{"observed_at":"2026-08-12T12:51:25.728284Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"paper":{"arxiv_id":"2411.16907","last_updated":"2025-03-21T16:52:01Z","latest_version":2,"primary_category":"hep-ex","snapshot_observed_at":"2026-08-13T06:32:09.702854Z","submitted_at":"2024-11-25T20:17:20Z","title":"Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\\to\\mathrm{b\\bar{b}}$ decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV"},"reference_resolution":{"displayed":100,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":94,"verified_exact":6,"verified_fuzzy":0},"total_outbound_references":122},"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":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"thesis":"As of 13 August 2026, this Paper Citation Record lists 100 of 122 outbound references and 1 inbound Pith citation observation for arXiv:2411.16907."}