{"as_of":"2026-08-14T08:32:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:5b5286e8646236018bbe188937825418ca05ea3d165958721dd76b6fb3370e2c","coverage":[{"denominator":75,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":75,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-12T21:24:47.245564Z","state":"measured"},{"denominator":75,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":75,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-14T06:32:32.682623+00:00","state":"measured"},{"denominator":0,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":0,"source":"paper_references, paper_reference_links","source_observed_at":null,"state":"measured"},{"denominator":1,"lane":"external_citation_measurements","note":"A source-named dated measurement, never combined with another source.","records_observed":0,"source":"cited_works","source_observed_at":null,"state":"measured"}],"external_citation_measurements":[],"inbound":[],"links":{"evidence":"/evidence","html":"/paper/2411.08802/citation-record","integrity":"/paper/2411.08802/integrity","json":"/paper/2411.08802/citation-record.json","paper":"/paper/2411.08802"},"outbound":[{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-12T21:24:48.391862Z","title":"7, we have checked that it removed all poles from virtual amplitudes for each process","venue":null,"work_id":"cf571558-e013-4d3c-baba-57096fe302e1","year":null},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:46.895563Z"},"links":{"citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:06284fce2e8565e7ca437b9187975139d2f691ae43a0670dd4b3a70f8a1107c4","observation_id":"bb3d76b2-9105-4f72-b7de-dd931b106887","resolution":{"observed_at":"2026-08-12T21:24:48.396860Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-12T21:24:48.377214Z","title":"Two numerical numbers corresponding to real and dipole terms are large in the singular re- gion, but their subtraction lies in the regular region","venue":null,"work_id":"96c2cdcd-9bf8-4217-85f4-2ba37dbd370e","year":null},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:46.901134Z"},"links":{"citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:66b114ba25f0728c19f259db22a5a949536a521d847e038a6c49fe75a1787be2","observation_id":"72f368bd-bb02-4d94-a5a9-0d30b725249e","resolution":{"observed_at":"2026-08-12T21:24:48.382141Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-12T21:24:48.363134Z","title":"By varyingα ∈ (0,1], we see consistent results for all processes within statistical uncertainties","venue":null,"work_id":"432cfbd2-7650-4de0-814a-747a906bcdbd","year":null},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:46.905946Z"},"links":{"citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:b6219095f76c9d8e6fa082f4754f395b6fbb1aecfd0c43260e48b8f80bd6ac9d","observation_id":"827fd670-a972-44f4-8114-b715dac5c4ad","resolution":{"observed_at":"2026-08-12T21:24:48.367843Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-12T21:24:48.349012Z","title":"For all real emission processes, in addition to the photons, there are also gluons in the final state","venue":null,"work_id":"1ada206c-f430-4464-811d-285df2eaddad","year":2000},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:46.910785Z"},"links":{"citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:9fc284ffd1d393671a46668ba9a11a0e451e003c79983193bbff4d9fe5535b8b","observation_id":"557b8ebd-3e42-4b60-84cf-9ffd8307f02f","resolution":{"observed_at":"2026-08-12T21:24:48.353913Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-12T21:24:48.335710Z","title":null,"venue":null,"work_id":"62904fa2-df2f-4c61-ae2e-6e24cd3eaca5","year":2022},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:46.917092Z"},"links":{"citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:922428dbbc2f28525552c95fe889ed9ad86bd34e8ac573456906764dceb79238","observation_id":"5aa6d117-5e89-415b-844d-766acc3e0120","resolution":{"observed_at":"2026-08-12T21:24:48.340106Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ex/0509008","last_updated":"2006-02-27T21:07:09Z","snapshot_observed_at":"2026-08-07T03:48:30.361762Z","submitted_at":"2005-09-07T16:45:02Z","title":"Precision Electroweak Measurements on the Z Resonance","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ex/0509008","snapshot_observed_at":"2026-08-12T21:24:46.921782Z","title":"Schael et al., Precision electroweak measurements on the Z resonance, Phys","venue":null,"work_id":null,"year":2006},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:46.921782Z"},"links":{"cited_paper":"/paper/hep-ex/0509008","citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:0b543fcb6f2e659e5f89003ce5ce49ee0c768b892b2a65c7b45be01956a56e84","observation_id":"8f2f5c42-ed75-4982-85a8-fab07e2f8540","resolution":{"observed_at":"2026-08-12T21:24:46.921782Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1809.01830","last_updated":"2019-09-20T09:52:22Z","snapshot_observed_at":"2026-08-13T18:28:37.894508Z","submitted_at":"2018-09-06T05:39:12Z","title":"Standard Model Theory for the FCC-ee Tera-Z stage","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1809.01830","snapshot_observed_at":"2026-08-12T21:24:46.926975Z","title":"Blondel et al., Standard model theory for the FCC-ee Tera-Z stage, in Mini Workshop on Precision EW and QCD Calculations for the FCC Studies : Methods and Techniques, vol","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:46.926975Z"},"links":{"cited_paper":"/paper/1809.01830","citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:11d72c6fd08df529ccacbef6dfaff6f09f375561f894c7c8d9c1054ea752eff5","observation_id":"dcaa5571-1bf4-47b6-9464-d368faa83cd5","resolution":{"observed_at":"2026-08-12T21:24:46.926975Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1804.10236","last_updated":"2018-04-26T18:33:56Z","snapshot_observed_at":"2026-07-06T06:35:43.204577Z","submitted_at":"2018-04-26T18:33:56Z","title":"Complete electroweak two-loop corrections to Z boson production and decay","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1804.10236","snapshot_observed_at":"2026-08-12T21:24:46.931997Z","title":"Dubovyk, A","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:46.931997Z"},"links":{"cited_paper":"/paper/1804.10236","citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:b1a83ad176bba24d92f1429e524571e26281959bebeb8db90b92f9f4531195dc","observation_id":"d7d07e64-1725-46bc-b555-5d98ba93016c","resolution":{"observed_at":"2026-08-12T21:24:46.931997Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2203.06520","last_updated":"2022-12-19T15:48:24Z","snapshot_observed_at":"2026-08-09T01:30:31.777074Z","submitted_at":"2022-03-12T21:33:32Z","title":"The Future Circular Collider: a Summary for the US 2021 Snowmass Process","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2203.06520","snapshot_observed_at":"2026-08-12T21:24:46.936927Z","title":"Bernardi et al., The Future Circular Collider: a Summary for the US 2021 Snowmass Process, 2203.06520","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:46.936927Z"},"links":{"cited_paper":"/paper/2203.06520","citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:25c618183b5ea205378212ec19b8a4b35269e495074daeb80dfb02086f289dea","observation_id":"93dfade8-1c03-4ffe-b764-426197f20303","resolution":{"observed_at":"2026-08-12T21:24:46.936927Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1302.3415","last_updated":"2013-09-19T06:57:45Z","snapshot_observed_at":"2026-08-12T21:46:24.089476Z","submitted_at":"2013-02-14T14:48:09Z","title":"Electroweak Measurements in Electron-Positron Collisions at W-Boson-Pair Energies at LEP","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1302.3415","snapshot_observed_at":"2026-08-12T21:24:46.942451Z","title":"Schael et al., Electroweak Measurements in Electron-Positron Collisions at W-Boson-Pair Energies at LEP, Phys","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:46.942451Z"},"links":{"cited_paper":"/paper/1302.3415","citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:bdbb6f5e27f917520a5d48354c660cee9ec97e2c28f7c4f5cbda8b265a6a8226","observation_id":"c24cca18-8d1c-4f83-97e5-178a95521fb8","resolution":{"observed_at":"2026-08-12T21:24:46.942451Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1412.2928","last_updated":"2014-12-09T11:55:37Z","snapshot_observed_at":"2026-08-10T04:42:05.126112Z","submitted_at":"2014-12-09T11:55:37Z","title":"Precision Electroweak Measurements at FCC-ee","version":1},"cited_work":{"arxiv_id":"1412.2928","doi":null,"metadata_source":"pith","pith_arxiv_id":"1412.2928","snapshot_observed_at":"2026-08-12T21:24:47.975538Z","title":"Precision Electroweak Measurements at FCC-ee","venue":"hep-ex","work_id":"59b52020-91fd-4e3e-baa8-1791a55de16d","year":2014},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:46.947032Z"},"links":{"cited_paper":"/paper/1412.2928","citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:dbdab2cf967f42ac0e361cfdab7cc7b117f3f8d13049a8efcfb81c01a1e31d27","observation_id":"3bc0a404-d1cc-4d21-b930-e5d6713ffaa7","resolution":{"observed_at":"2026-08-12T21:24:47.980573Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-12T21:24:48.322005Z","title":"Patrignani et al., Review of Particle Physics, Chin","venue":null,"work_id":"cb58891f-c564-475b-ba28-731c1c57a322","year":2016},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:46.951916Z"},"links":{"citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:06b6560fb58c57060f239aee3f1a2738ee10ceefcb1f9ea8c36cf5230bf3caef","observation_id":"014ce1f6-616b-456d-bdcd-773bb02f2e4f","resolution":{"observed_at":"2026-08-12T21:24:48.326891Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1411.5924","last_updated":"2015-07-10T20:50:02Z","snapshot_observed_at":"2026-07-06T04:01:17.632482Z","submitted_at":"2014-11-21T15:50:30Z","title":"Rare exclusive decays of the Z-boson revisited","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1411.5924","snapshot_observed_at":"2026-08-12T21:24:46.956865Z","title":"Huang and F","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:46.956865Z"},"links":{"cited_paper":"/paper/1411.5924","citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:b8a72c3be975746d8ceb23e27ea4fd197a1c95d7a9ada22cdad9fe49cbe0c2c7","observation_id":"90b01d45-2570-4cfa-8aca-b5f849033671","resolution":{"observed_at":"2026-08-12T21:24:46.956865Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2308.06558","last_updated":"2024-06-04T07:21:38Z","snapshot_observed_at":"2026-08-13T10:35:35.449934Z","submitted_at":"2023-08-12T13:04:02Z","title":"Testing $Z$ boson rare decays $Z\\to H_1 \\gamma, A_1 \\gamma$ with $(g-2)_\\mu$, $M_W$, and $BR(h_{\\rm SM}\\to Z\\gamma)$ in the NMSSM","version":2},"cited_work":{"arxiv_id":"2308.06558","doi":null,"metadata_source":"pith","pith_arxiv_id":"2308.06558","snapshot_observed_at":"2026-08-12T21:24:47.940643Z","title":"Testing $Z$ boson rare decays $Z\\to H_1 \\gamma, A_1 \\gamma$ with $(g-2)_\\mu$, $M_W$, and $BR(h_{\\rm SM}\\to Z\\gamma)$ in the NMSSM","venue":"hep-ph","work_id":"f476de77-6681-475b-bc5f-2ef129d458b2","year":2023},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:46.962076Z"},"links":{"cited_paper":"/paper/2308.06558","citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:87e712faf0ef35633d245bf5ba55f6cc9e5c6b8b5f8976dc99c7ae08ec36ecb2","observation_id":"fd7dea5e-1364-4631-a2ec-c0d0c9bdc341","resolution":{"observed_at":"2026-08-12T21:24:47.945899Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-12T21:24:48.308380Z","title":null,"venue":null,"work_id":"74f2c475-648c-4206-8d61-147491178cb2","year":1986},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:46.966797Z"},"links":{"citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:81126c7ba011464e11cb5493f9f2a1f3d5b9de3d1a9d94fd7be20385bfe37b77","observation_id":"4ddc6839-7065-446c-9295-d30e283d37eb","resolution":{"observed_at":"2026-08-12T21:24:48.312955Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-12T21:24:48.294601Z","title":"Bernabeu, A","venue":null,"work_id":"ff140bba-82e6-4b49-b732-164df99fa920","year":1988},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:46.971032Z"},"links":{"citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:ae0bf845228520db3584d0c867d2e6813812493b601edeea4f00e42e62f5e447","observation_id":"bbbc7b5f-13ac-4593-ba3a-f4e90008d0a3","resolution":{"observed_at":"2026-08-12T21:24:48.299082Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-12T21:24:48.280744Z","title":"Beenakker and W","venue":null,"work_id":"8b012691-97e8-4ffd-9b0a-37be971b47ca","year":1988},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:46.975357Z"},"links":{"citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:8a20bf55e2ed43149e4636a822ace6f627ec81176d8b5bbcb559643897ec5b63","observation_id":"1a376a68-5d0d-4168-8d3f-6686bc1f6a3c","resolution":{"observed_at":"2026-08-12T21:24:48.285127Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1607.08375","last_updated":"2016-09-30T23:58:14Z","snapshot_observed_at":"2026-07-06T05:05:12.809681Z","submitted_at":"2016-07-28T09:37:13Z","title":"The two-loop electroweak bosonic corrections to $\\sin^2\\theta_{\\rm eff}^{\\rm b}$","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1607.08375","snapshot_observed_at":"2026-08-12T21:24:46.980179Z","title":"Dubovyk, A","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:46.980179Z"},"links":{"cited_paper":"/paper/1607.08375","citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:2371a61602d6063faa9bc182962842f547bc49683b70f57a03dbae097435731c","observation_id":"23cdf0e8-0e38-40a4-b129-a7b84887f904","resolution":{"observed_at":"2026-08-12T21:24:46.980179Z","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":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-12T21:24:48.266931Z","title":"Djouadi and C","venue":null,"work_id":"1b8eb70d-aeef-4b4a-b76f-d1ddfe085965","year":1987},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:46.984863Z"},"links":{"citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:3c807c332f365cd30dc237de7fded1b6844d6c4e7ec629a0d727b5a8b681c1fc","observation_id":"3626dd3c-3a8f-446e-bb33-22822f34ad46","resolution":{"observed_at":"2026-08-12T21:24:48.271388Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-12T21:24:48.251023Z","title":"Djouadi, O(alpha alpha-s) Vacuum Polarization Functions of the Standard Model Gauge Bosons, Nuovo Cim","venue":null,"work_id":"fe5d1b3b-fbbd-4208-b3cf-0e838cded209","year":1988},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:46.989391Z"},"links":{"citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:281e60e2133a5ce3432ce3367d5c1543f06db08fca912613965b1406307d8012","observation_id":"77abadb8-96ef-4668-adae-937cc6e4d832","resolution":{"observed_at":"2026-08-12T21:24:48.256621Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-12T21:24:48.235490Z","title":null,"venue":null,"work_id":"51574f34-742b-4d2f-8100-d2cb5e25b36a","year":1990},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:46.993632Z"},"links":{"citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:fc9a8974df64da30cee6cac8a314787f019ee075700da055b14e44a1b2d0b784","observation_id":"0c409098-352b-4d4c-8804-a97e5d5ea966","resolution":{"observed_at":"2026-08-12T21:24:48.240104Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-12T21:24:48.221392Z","title":null,"venue":null,"work_id":"0c4f6613-0474-45fb-9cad-1faf3c704963","year":1992},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:46.997873Z"},"links":{"citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:fb9f1bd6f2fa2d66a11e907a72f84a4fb7957062d11451a35c6b1495d1b3d13f","observation_id":"9a8abc0e-d192-450a-8254-3661e001e558","resolution":{"observed_at":"2026-08-12T21:24:48.225909Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9309298","last_updated":"1993-09-20T21:50:13Z","snapshot_observed_at":"2026-07-07T04:16:01.492229Z","submitted_at":"1993-09-20T21:50:13Z","title":"Electroweak gauge bosons self--energies: complete QCD corrections","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9309298","snapshot_observed_at":"2026-08-12T21:24:47.001818Z","title":"Djouadi and P","venue":null,"work_id":null,"year":1994},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:47.001818Z"},"links":{"cited_paper":"/paper/hep-ph/9309298","citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:d22ec1d16a81c385f5edadf18a5dcf73f02c264298602de4caad762f789fdbe4","observation_id":"49db87e0-34d9-4065-b9f3-3ad02f6fb4ae","resolution":{"observed_at":"2026-08-12T21:24:47.001818Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9205238","last_updated":"1992-05-27T16:28:54Z","snapshot_observed_at":"2026-07-07T04:14:21.840920Z","submitted_at":"1992-05-27T16:28:54Z","title":"Radiative Correction Effects of a Very Heavy Top","version":1},"cited_work":{"arxiv_id":"hep-ph/9205238","doi":null,"metadata_source":"pith","pith_arxiv_id":"hep-ph/9205238","snapshot_observed_at":"2026-08-12T21:24:47.892455Z","title":"Radiative Correction Effects of a Very Heavy Top","venue":"hep-ph","work_id":"a2ba1392-9527-48ba-a12d-aae453901e1b","year":1992},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:47.006275Z"},"links":{"cited_paper":"/paper/hep-ph/9205238","citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:3f82768c4d9c613625f0b785e3e471db9bb9b2bc2115c83c10216bb798f6c718","observation_id":"e4ad33f5-cb03-4426-a481-ca9ed278422c","resolution":{"observed_at":"2026-08-12T21:24:47.897748Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-12T21:24:48.207288Z","title":"Barbieri, M","venue":null,"work_id":"2bc2a1a7-542e-466a-90a4-ed2900105cf1","year":1993},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:47.010773Z"},"links":{"citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:c75b21a3c958c35106bfc49b43ae4aaf745312cbb667b92f293aaa0f12c61f3f","observation_id":"a8168ef6-0e0a-4c25-988b-07738fe80f5a","resolution":{"observed_at":"2026-08-12T21:24:48.211936Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-12T21:24:48.192924Z","title":"Fleischer, O","venue":null,"work_id":"3ee80f92-e0fa-40cf-8a1d-0817e31f356d","year":1993},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:47.015237Z"},"links":{"citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:9a160e77cd5ce788bfcf89f4dbe2f5f4ed1cbfc2d1c4c1a65851973f5616d910","observation_id":"16a73c00-9d78-4054-b4f8-6e1103e3c9d3","resolution":{"observed_at":"2026-08-12T21:24:48.197802Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-12T21:24:48.178012Z","title":"Fleischer, O","venue":null,"work_id":"caa836ef-7327-4624-9b03-207f4c33fede","year":1995},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:47.019568Z"},"links":{"citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:7b8ce87ed9d8ab4102b4f57446ca34ad40d2564deac0fc987d57f7ed719ebd9e","observation_id":"c4129ce7-81b2-4a9a-9524-1705563f85b5","resolution":{"observed_at":"2026-08-12T21:24:48.182884Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9603374","last_updated":"1996-04-05T15:24:12Z","snapshot_observed_at":"2026-07-07T04:22:15.203297Z","submitted_at":"1996-03-21T23:20:48Z","title":"Two-loop heavy top effects on the MZ-MW interdependence","version":2},"cited_work":{"arxiv_id":"hep-ph/9603374","doi":null,"metadata_source":"pith","pith_arxiv_id":"hep-ph/9603374","snapshot_observed_at":"2026-08-12T21:24:47.872124Z","title":"Two-loop heavy top effects on the MZ-MW interdependence","venue":"hep-ph","work_id":"5e5b4416-e1c5-4cb2-bdcb-e09a6167587f","year":1996},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:47.023795Z"},"links":{"cited_paper":"/paper/hep-ph/9603374","citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:be04426000482ef4b5ba1e7c32ef9ee31ce7a1425993457fd26bf7248edf4261","observation_id":"ca615fe5-d1fe-4791-85c8-c97d4b7efdb7","resolution":{"observed_at":"2026-08-12T21:24:47.876968Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9611363","last_updated":"1996-11-19T12:45:33Z","snapshot_observed_at":"2026-07-07T04:24:19.108383Z","submitted_at":"1996-11-19T12:45:33Z","title":"Precise calculation of MW, sin^2 theta_MSbar, and sin^2 theta_eff","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9611363","snapshot_observed_at":"2026-08-12T21:24:47.028465Z","title":"Degrassi, P","venue":null,"work_id":null,"year":1997},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":29,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:47.028465Z"},"links":{"cited_paper":"/paper/hep-ph/9611363","citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:206ff2df1c3a44e032aeb57f32780985ea871e4cecb07806d21a957597d93bcb","observation_id":"4a7c56ac-ea9e-44b2-b954-2a79c923d4e4","resolution":{"observed_at":"2026-08-12T21:24:47.028465Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9905472","last_updated":"1999-11-17T15:09:25Z","snapshot_observed_at":"2026-07-07T04:33:12.291470Z","submitted_at":"1999-05-25T13:47:22Z","title":"Two-loop heavy top corrections to the Z boson partial widths","version":2},"cited_work":{"arxiv_id":"hep-ph/9905472","doi":null,"metadata_source":"pith","pith_arxiv_id":"hep-ph/9905472","snapshot_observed_at":"2026-08-12T21:24:47.836598Z","title":"Two-loop heavy top corrections to the Z boson partial widths","venue":"hep-ph","work_id":"d5cf43dd-ce53-4c49-b7f4-85b16d540ab4","year":1999},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:47.033865Z"},"links":{"cited_paper":"/paper/hep-ph/9905472","citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:7d89a5ed67be08009834f9911db78026563cbfc24627360f4ff956cdfda31cc9","observation_id":"594003ec-6a72-4225-a870-c680363d0847","resolution":{"observed_at":"2026-08-12T21:24:47.841390Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0007091","last_updated":"2003-05-22T14:59:25Z","snapshot_observed_at":"2026-07-07T03:49:07.692348Z","submitted_at":"2000-07-10T23:02:41Z","title":"Complete fermionic two-loop results for the M_W-M_Z interdependence","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0007091","snapshot_observed_at":"2026-08-12T21:24:47.038709Z","title":"Freitas, W","venue":null,"work_id":null,"year":2000},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:47.038709Z"},"links":{"cited_paper":"/paper/hep-ph/0007091","citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:79c475bda39bccefef06c839a7d43e6496f5d32e70685e515a86c71d8cbad764","observation_id":"42f8130d-654c-4e79-b1bb-9b981b72b0ee","resolution":{"observed_at":"2026-08-12T21:24:47.038709Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0202131","last_updated":"2003-05-22T15:16:47Z","snapshot_observed_at":"2026-07-07T03:55:13.495575Z","submitted_at":"2002-02-14T15:18:28Z","title":"Electroweak two-loop corrections to the MW-MZ mass correlation in the Standard Model","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0202131","snapshot_observed_at":"2026-08-12T21:24:47.043416Z","title":"Freitas, W","venue":null,"work_id":null,"year":2002},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":32,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:47.043416Z"},"links":{"cited_paper":"/paper/hep-ph/0202131","citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:853c58754bf8078468b3a7c094047eef3adc0ceff6607997e1b3289992038089","observation_id":"4216f8d7-bee3-4cc1-9f03-0d1917cd8262","resolution":{"observed_at":"2026-08-12T21:24:47.043416Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0407317","last_updated":"2004-07-28T08:51:45Z","snapshot_observed_at":"2026-08-09T13:19:31.799656Z","submitted_at":"2004-07-28T08:51:45Z","title":"Complete Two-Loop Electroweak Fermionic Corrections to sin^2(theta_eff) and Indirect Determination of the Higgs Boson Mass","version":1},"cited_work":{"arxiv_id":"hep-ph/0407317","doi":null,"metadata_source":"pith","pith_arxiv_id":"hep-ph/0407317","snapshot_observed_at":"2026-08-12T21:24:47.788352Z","title":"Complete Two-Loop Electroweak Fermionic Corrections to sin^2(theta_eff) and Indirect Determination of the Higgs Boson Mass","venue":"hep-ph","work_id":"0a067f92-0e57-46ac-bf7b-33503cc4a55f","year":2004},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:47.048132Z"},"links":{"cited_paper":"/paper/hep-ph/0407317","citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:9abcc212de5e82a0a0b1712146ed0c4cb60a52a4142ff78a676f3bb1e7667d02","observation_id":"694ebc72-cf19-4a7a-ba50-411c408ae3d9","resolution":{"observed_at":"2026-08-12T21:24:47.793525Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0507158","last_updated":"2005-10-20T11:49:39Z","snapshot_observed_at":"2026-07-07T04:08:01.708979Z","submitted_at":"2005-07-13T15:34:38Z","title":"The effective electroweak mixing angle $\\sin^2\\theta_{eff}$ with two-loop fermionic contributions","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0507158","snapshot_observed_at":"2026-08-12T21:24:47.053082Z","title":"Hollik, U","venue":null,"work_id":null,"year":2005},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":34,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:47.053082Z"},"links":{"cited_paper":"/paper/hep-ph/0507158","citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:6417aeeda8039de15457f8d640d8af2bec6aa3dd238a5cd744fecc37e610094f","observation_id":"6a536249-1f8c-4b21-92c9-b2832ec80089","resolution":{"observed_at":"2026-08-12T21:24:47.053082Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0811.1364","last_updated":"2009-01-20T15:45:29Z","snapshot_observed_at":"2026-08-02T21:47:02.743657Z","submitted_at":"2008-11-09T20:17:09Z","title":"Two-loop electroweak fermionic corrections to sin^2 theta_{eff}^{b anti-b}","version":2},"cited_work":{"arxiv_id":"0811.1364","doi":null,"metadata_source":"pith","pith_arxiv_id":"0811.1364","snapshot_observed_at":"2026-08-12T21:24:47.754574Z","title":"Two-loop electroweak fermionic corrections to sin^2 theta_{eff}^{b anti-b}","venue":"hep-ph","work_id":"0dd77d54-008a-4b99-8574-da912e60a49e","year":2008},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:47.058994Z"},"links":{"cited_paper":"/paper/0811.1364","citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:e08e609164b3790ad4ce8374ce71a45fd41299d9dcd958f3b12173fedc4f31ce","observation_id":"910db210-fcea-43ab-b15d-91383f18bde7","resolution":{"observed_at":"2026-08-12T21:24:47.759620Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1205.0299","last_updated":"2013-09-13T19:07:23Z","snapshot_observed_at":"2026-08-14T08:10:13.112506Z","submitted_at":"2012-05-02T01:22:08Z","title":"Electroweak two-loop corrections to sin^2{\\theta}(eff,bb) and R(b) using numerical Mellin-Barnes integrals","version":3},"cited_work":{"arxiv_id":"1205.0299","doi":null,"metadata_source":"pith","pith_arxiv_id":"1205.0299","snapshot_observed_at":"2026-08-12T21:24:47.734606Z","title":"Electroweak two-loop corrections to sin^2{\\theta}(eff,bb) and R(b) using numerical Mellin-Barnes integrals","venue":"hep-ph","work_id":"69ac0283-dc60-4abe-8177-14b8c9459f90","year":2012},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":36,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:47.064000Z"},"links":{"cited_paper":"/paper/1205.0299","citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:93ea9c48c92c7f6058a99753cecb047ec45bd7c5f2f82afd6761993d6f7afe94","observation_id":"dc7b603b-3c79-4446-852b-f9eba8054e52","resolution":{"observed_at":"2026-08-12T21:24:47.739645Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1310.2256","last_updated":"2014-01-04T19:13:35Z","snapshot_observed_at":"2026-08-02T02:24:26.001742Z","submitted_at":"2013-10-08T20:02:52Z","title":"Two-loop fermionic electroweak corrections to the Z-boson width and production rate","version":2},"cited_work":{"arxiv_id":"1310.2256","doi":null,"metadata_source":"pith","pith_arxiv_id":"1310.2256","snapshot_observed_at":"2026-08-12T21:24:47.714155Z","title":"Two-loop fermionic electroweak corrections to the Z-boson width and production rate","venue":"hep-ph","work_id":"eafe653d-0986-4f15-a808-fde774873da7","year":2013},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":37,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:47.068722Z"},"links":{"cited_paper":"/paper/1310.2256","citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:6b626df55666b6e2a49f4f3ab1e859230ddda4f56c51f2c056cb9bed8c6e5ed2","observation_id":"41b25da4-79c4-430d-bb32-5cd7592ac3b7","resolution":{"observed_at":"2026-08-12T21:24:47.719195Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1401.2447","last_updated":"2020-12-22T22:09:30Z","snapshot_observed_at":"2026-07-31T17:57:27.902068Z","submitted_at":"2014-01-10T20:37:04Z","title":"Higher-order electroweak corrections to the partial widths and branching ratios of the Z boson","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1401.2447","snapshot_observed_at":"2026-08-12T21:24:47.073162Z","title":"Freitas, Higher-order electroweak corrections to the partial widths and branching ratios of the Z boson, JHEP 04 (2014) 070, [1401.2447]","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":38,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:47.073162Z"},"links":{"cited_paper":"/paper/1401.2447","citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:02eec8c681b554a2de48be9ed5fbe2ac4951e3eb8ee4c222aa5233b2b70a00b9","observation_id":"6c987c33-639c-4c07-b929-4368d2b03e81","resolution":{"observed_at":"2026-08-12T21:24:47.073162Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9406363","last_updated":"1995-02-15T10:04:13Z","snapshot_observed_at":"2026-07-07T04:17:31.341382Z","submitted_at":"1994-06-22T14:48:38Z","title":"$O(\\alpha \\alpha_s^2)$ correction to the electroweak $\\rho$ parameter","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9406363","snapshot_observed_at":"2026-08-12T21:24:47.077597Z","title":"Avdeev, J","venue":null,"work_id":null,"year":1994},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":39,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:47.077597Z"},"links":{"cited_paper":"/paper/hep-ph/9406363","citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:ec256966bb162bb61f9bf81a9c8256918469049f050509605239a31e982f833c","observation_id":"74a3b853-277b-4ba8-adf0-9bbeec2ae30a","resolution":{"observed_at":"2026-08-12T21:24:47.077597Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9502291","last_updated":"1995-02-14T08:17:18Z","snapshot_observed_at":"2026-07-31T08:15:28.964136Z","submitted_at":"1995-02-13T15:51:40Z","title":"Corrections of order ${\\cal O}(G_F M_t^2 \\as^2)$ to the $\\rho$ parameter","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9502291","snapshot_observed_at":"2026-08-12T21:24:47.082532Z","title":null,"venue":null,"work_id":null,"year":1995},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":40,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:47.082532Z"},"links":{"cited_paper":"/paper/hep-ph/9502291","citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:2d961ad4c922519c5748ef746ff1c71e75434460ceace0fde2385013818acadc","observation_id":"970f8b65-bcba-4d38-a432-192b4d2a0bb0","resolution":{"observed_at":"2026-08-12T21:24:47.082532Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0011373","last_updated":"2000-12-19T09:05:39Z","snapshot_observed_at":"2026-07-07T03:50:36.913744Z","submitted_at":"2000-11-29T19:08:29Z","title":"Three-Loop Leading Top Mass Contributions to the rho Parameter","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0011373","snapshot_observed_at":"2026-08-12T21:24:47.087109Z","title":null,"venue":null,"work_id":null,"year":2001},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":41,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:47.087109Z"},"links":{"cited_paper":"/paper/hep-ph/0011373","citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:df596d9e3a4ff92c6963dd53c687dbcbb75dbc45425b9a4a36abf8df08631e96","observation_id":"d2b8ddc8-031e-4c55-9965-791e6c8251c9","resolution":{"observed_at":"2026-08-12T21:24:47.087109Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0302275","last_updated":"2003-04-03T16:39:49Z","snapshot_observed_at":"2026-07-07T03:59:15.396337Z","submitted_at":"2003-02-28T14:24:01Z","title":"Three Loop Top Quark Contributions to the rho Parameter","version":2},"cited_work":{"arxiv_id":"hep-ph/0302275","doi":null,"metadata_source":"pith","pith_arxiv_id":"hep-ph/0302275","snapshot_observed_at":"2026-08-12T21:24:47.634870Z","title":"Three Loop Top Quark Contributions to the rho Parameter","venue":"hep-ph","work_id":"7ba20964-610f-4c48-a8cf-1afcb96d7a74","year":2003},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":42,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:47.092501Z"},"links":{"cited_paper":"/paper/hep-ph/0302275","citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:091f61f6c4da95f2a9a4fa1d1fdc896e1ccab72dd0e2993327cd181aac5e5fd7","observation_id":"22868b7f-7942-4967-b6b2-1469773f64ad","resolution":{"observed_at":"2026-08-12T21:24:47.640409Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0504055","last_updated":"2005-11-11T10:14:24Z","snapshot_observed_at":"2026-07-07T04:07:06.547214Z","submitted_at":"2005-04-07T14:11:31Z","title":"Four-Loop Singlet Contribution to the $\\rho$ Parameter","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0504055","snapshot_observed_at":"2026-08-12T21:24:47.097188Z","title":"Schroder and M","venue":null,"work_id":null,"year":2005},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":43,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:47.097188Z"},"links":{"cited_paper":"/paper/hep-ph/0504055","citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:0c6f8fa1e2b5ca33c8149d2838ad45e718c4e56dd390cae5093683d1515c9fc5","observation_id":"ece6133a-4dbb-41e3-aee4-333d9695a7d4","resolution":{"observed_at":"2026-08-12T21:24:47.097188Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0605201","last_updated":"2006-09-28T16:09:00Z","snapshot_observed_at":"2026-08-01T18:00:54.074044Z","submitted_at":"2006-05-18T19:37:39Z","title":"Four-Loop QCD Corrections to the Rho Parameter","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0605201","snapshot_observed_at":"2026-08-12T21:24:47.102148Z","title":null,"venue":null,"work_id":null,"year":2006},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":44,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:47.102148Z"},"links":{"cited_paper":"/paper/hep-ph/0605201","citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:342bd61eef58f2834fed77290b12fe2ef5f6b1745b50b5dbae1f031d32c80a1e","observation_id":"5d267f68-3f4a-4aa6-9fb1-fa5b52a1f0a0","resolution":{"observed_at":"2026-08-12T21:24:47.102148Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0606232","last_updated":"2006-10-05T11:39:52Z","snapshot_observed_at":"2026-07-07T04:11:23.949703Z","submitted_at":"2006-06-21T15:28:47Z","title":"Single Scale Tadpoles and O(GF mt^2 as^3) Corrections to the rho Parameter","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0606232","snapshot_observed_at":"2026-08-12T21:24:47.106933Z","title":"Boughezal and M","venue":null,"work_id":null,"year":2006},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":45,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:47.106933Z"},"links":{"cited_paper":"/paper/hep-ph/0606232","citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:0f291d611c06b7e4429c37c4ba9581701ab466387b3fb32fd92e30df4a067c3f","observation_id":"f7959e9e-9ca0-45d1-beb0-4fdd74baf663","resolution":{"observed_at":"2026-08-12T21:24:47.106933Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1306.6352","last_updated":"2013-06-26T20:31:40Z","snapshot_observed_at":"2026-08-12T17:39:03.657493Z","submitted_at":"2013-06-26T20:31:40Z","title":"The International Linear Collider Technical Design Report - Volume 2: Physics","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1306.6352","snapshot_observed_at":"2026-08-12T21:24:47.111378Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":46,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:47.111378Z"},"links":{"cited_paper":"/paper/1306.6352","citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:76dfe8a356ea8f4732b73009412017d0ec08eef42ad64b57e7d9a758ea266b73","observation_id":"e8011391-fd1c-4f1d-afaa-6e0146057a65","resolution":{"observed_at":"2026-08-12T21:24:47.111378Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1308.6176","last_updated":"2013-12-11T17:16:06Z","snapshot_observed_at":"2026-08-02T16:21:29.936126Z","submitted_at":"2013-08-28T14:55:58Z","title":"First Look at the Physics Case of TLEP","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1308.6176","snapshot_observed_at":"2026-08-12T21:24:47.116165Z","title":"Bicer et al., First Look at the Physics Case of TLEP, JHEP 01 (2014) 164, [1308.6176]","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":47,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:47.116165Z"},"links":{"cited_paper":"/paper/1308.6176","citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:6bf0f62bfc548274b99ec175c4c74397652fdbdb26eff724392be78f58055d73","observation_id":"8a176a51-2774-49f2-af71-a2e9dd1f8ae1","resolution":{"observed_at":"2026-08-12T21:24:47.116165Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1602.05043","last_updated":"2016-02-17T15:03:47Z","snapshot_observed_at":"2026-07-06T04:46:19.812646Z","submitted_at":"2016-02-16T15:03:19Z","title":"Physics at the FCC-ee","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1602.05043","snapshot_observed_at":"2026-08-12T21:24:47.120762Z","title":"d’Enterria, Physics at the FCC-ee, in 17th Lomonosov Conference on Elementary Particle Physics, pp","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":48,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:47.120762Z"},"links":{"cited_paper":"/paper/1602.05043","citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:0eafa0811f87961fbcde305de301d7311b23f88da5e99e6a8e05a090332a4375","observation_id":"8da50a93-7363-4f21-81ad-c47f1f5bb0dd","resolution":{"observed_at":"2026-08-12T21:24:47.120762Z","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":"2026-08-12T21:24:47.125426Z","title":"Ahmad et al., CEPC-SPPC Preliminary Conceptual Design Report","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":49,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:47.125426Z"},"links":{"citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:1c32a96f3f8822a3840bf1f1d051835ae43453c2a9c5eeb83e090157231af783","observation_id":"9808481f-8612-4c30-ae92-dc4b3880f83e","resolution":{"observed_at":"2026-08-12T21:24:47.125426Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0012260","last_updated":"2001-05-16T16:07:13Z","snapshot_observed_at":"2026-07-07T03:50:56.660518Z","submitted_at":"2000-12-20T19:20:02Z","title":"Generating Feynman Diagrams and Amplitudes with FeynArts 3","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0012260","snapshot_observed_at":"2026-08-12T21:24:47.130193Z","title":"Hahn, Generating Feynman diagrams and amplitudes with FeynArts 3, Comput","venue":null,"work_id":null,"year":2001},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":50,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:47.130193Z"},"links":{"cited_paper":"/paper/hep-ph/0012260","citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:08f7b7292298b5f590658a832b1760de1c76fbb64ed70453df57fe25d861366e","observation_id":"9648d9f5-ff49-496f-aa40-2e063f157f14","resolution":{"observed_at":"2026-08-12T21:24:47.130193Z","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":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-12T21:24:48.152784Z","title":"Kublbeck, M","venue":null,"work_id":"cd42eb87-9a2c-41f5-b25a-b629420db184","year":1990},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":51,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:47.134631Z"},"links":{"citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:9d2055a7f9d807488224e064e7c8f663e136a0e297b1c2bc1bdbcb21ba53f7bf","observation_id":"5e54555c-c9ed-4c79-954d-a97294bf88db","resolution":{"observed_at":"2026-08-12T21:24:48.157274Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1101.2414","last_updated":"2011-01-12T17:40:04Z","snapshot_observed_at":"2026-07-06T02:21:57.688025Z","submitted_at":"2011-01-12T17:40:04Z","title":"Simplifying Multi-Jet QCD Computation","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1101.2414","snapshot_observed_at":"2026-08-12T21:24:47.139056Z","title":null,"venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":52,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:47.139056Z"},"links":{"cited_paper":"/paper/1101.2414","citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:62347b959ab28092ad950ad45b9bdae22884bce53c1835e6155990665f0bfe16","observation_id":"41f90bed-8ee5-48bd-bf0b-b951bed2041b","resolution":{"observed_at":"2026-08-12T21:24:47.139056Z","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":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-12T21:24:48.137338Z","title":"Kleiss and W","venue":null,"work_id":"dff06c56-6af7-4a45-8341-e32b672a94f0","year":1986},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":53,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:47.143595Z"},"links":{"citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:22ecb2f29d5a23222686ae7d995c09066dfc47fc76b7c88c6b7580a1b96a8d98","observation_id":"839f4235-4a1c-47fd-87c0-75a25639565b","resolution":{"observed_at":"2026-08-12T21:24:48.142555Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2409.01264","last_updated":"2024-09-02T13:59:05Z","snapshot_observed_at":"2026-08-12T22:53:01.784990Z","submitted_at":"2024-09-02T13:59:05Z","title":"Probing Anomalous Higgs Boson Couplings at Colliders","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2409.01264","snapshot_observed_at":"2026-08-12T21:24:47.147906Z","title":"Das, Probing Anomalous Higgs Boson Couplings at Colliders","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":54,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:47.147906Z"},"links":{"cited_paper":"/paper/2409.01264","citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:22a5165f247b3d25e65e15380765fdb13581a4eedc162b45210ab3c0830c6f3b","observation_id":"f0809ffb-7659-4bcf-83f8-9f4099e2a9d7","resolution":{"observed_at":"2026-08-12T21:24:47.147906Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9807565","last_updated":"1998-07-31T13:28:21Z","snapshot_observed_at":"2026-07-07T04:30:18.471293Z","submitted_at":"1998-07-31T13:28:21Z","title":"Automatized One-Loop Calculations in 4 and D dimensions","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9807565","snapshot_observed_at":"2026-08-12T21:24:47.152547Z","title":"Hahn and M","venue":null,"work_id":null,"year":1999},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":55,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:47.152547Z"},"links":{"cited_paper":"/paper/hep-ph/9807565","citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:692c06d02ff0709974489d95b45d4c74f886dc386bcbe37221469c46f15d0fda","observation_id":"2e05aecc-1ed7-42e5-8c4a-14357d6f71a4","resolution":{"observed_at":"2026-08-12T21:24:47.152547Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"math-ph/0010025","last_updated":"2000-10-19T23:40:36Z","snapshot_observed_at":"2026-07-07T06:12:35.362030Z","submitted_at":"2000-10-19T13:02:55Z","title":"New features of FORM","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"math-ph/0010025","snapshot_observed_at":"2026-08-12T21:24:47.157424Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":56,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:47.157424Z"},"links":{"cited_paper":"/paper/math-ph/0010025","citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:25148b680d7bc8a01167d487b91193146498e52693b392640e9a8f9de9ebce33","observation_id":"7a47a245-d445-4cd9-af4f-3e4587bfcc7f","resolution":{"observed_at":"2026-08-12T21:24:47.157424Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1207.2927","last_updated":"2012-09-28T09:55:06Z","snapshot_observed_at":"2026-07-06T02:51:43.851040Z","submitted_at":"2012-07-12T11:32:55Z","title":"Di-Vector Boson + Jet Production via Gluon Fusion at Hadron Colliders","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1207.2927","snapshot_observed_at":"2026-08-12T21:24:47.163007Z","title":"Agrawal and A","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":57,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:47.163007Z"},"links":{"cited_paper":"/paper/1207.2927","citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:f17cd2b26c82aa2b2df550101a22ddbf8603c5b4d16f75596b4cc09600e1da78","observation_id":"3f6b5966-5f94-42c5-862b-aaed0c56abad","resolution":{"observed_at":"2026-08-12T21:24:47.163007Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0011346","last_updated":"2000-11-28T14:29:08Z","snapshot_observed_at":"2026-07-07T03:50:36.913744Z","submitted_at":"2000-11-28T14:29:08Z","title":"Production of Two Photons and a Jet Through Gluon Fusion","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0011346","snapshot_observed_at":"2026-08-12T21:24:47.168309Z","title":"Agrawal and G","venue":null,"work_id":null,"year":2001},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":58,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:47.168309Z"},"links":{"cited_paper":"/paper/hep-ph/0011346","citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:f75487dd2f5d2d973e83b0321531a153176c441526f57fac0b2d173b2c5dd8f4","observation_id":"7b7d9984-0e13-4dbd-b51e-62acf1652fe1","resolution":{"observed_at":"2026-08-12T21:24:47.168309Z","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":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-12T21:24:48.122295Z","title":null,"venue":null,"work_id":"c980a192-f039-47ea-a8d4-c62ac6e334d3","year":1990},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":59,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:47.172814Z"},"links":{"citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:55c30f145236c47c75853880ac436eafacfa73f182efd2c885af6e9c01870127","observation_id":"e9e6fef8-274d-4c99-9159-24253632cb2f","resolution":{"observed_at":"2026-08-12T21:24:48.126677Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1007.4716","last_updated":"2010-07-27T13:30:24Z","snapshot_observed_at":"2026-08-12T09:20:10.197860Z","submitted_at":"2010-07-27T13:30:24Z","title":"OneLOop: for the evaluation of one-loop scalar functions","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1007.4716","snapshot_observed_at":"2026-08-12T21:24:47.177378Z","title":"van Hameren, OneLOop: For the evaluation of one-loop scalar functions, Comput","venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":60,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:47.177378Z"},"links":{"cited_paper":"/paper/1007.4716","citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:9915a06676ae648b2d8439c594d7b691c3406b06f9cbfb327c291878cd820945","observation_id":"a7231fe4-654a-42a3-bc87-7e9c8450a33d","resolution":{"observed_at":"2026-08-12T21:24:47.177378Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"physics/9710017","last_updated":"1997-10-17T17:44:36Z","snapshot_observed_at":"2026-08-12T03:31:24.054752Z","submitted_at":"1997-10-17T17:44:36Z","title":"Multidimensional integration in a heterogeneous network environment","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"physics/9710017","snapshot_observed_at":"2026-08-12T21:24:47.182305Z","title":"Veseli, Multidimensional integration in a heterogeneous network environment, Comput","venue":null,"work_id":null,"year":1998},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":61,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:47.182305Z"},"links":{"cited_paper":"/paper/physics/9710017","citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:4c01b68fef15e79b72e2f087a513968a79b5e3fb55c2153e15c4bd636a99be8c","observation_id":"b9cddf88-7ee6-4e84-8674-b0b9ea256d98","resolution":{"observed_at":"2026-08-12T21:24:47.182305Z","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":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-12T21:24:48.108130Z","title":null,"venue":null,"work_id":"c7cc49fd-f6d4-40bf-9dc0-d1a8911dcd8c","year":1978},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":62,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:47.187272Z"},"links":{"citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:343a919881df3616e014fed6f425becf3ba0357d51dfcbea97fc7ea766843161","observation_id":"331bd848-89ea-4287-948f-0153064b5abb","resolution":{"observed_at":"2026-08-12T21:24:48.112417Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-12T21:24:47.191661Z","title":"Geist, A","venue":null,"work_id":null,"year":1994},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":63,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:47.191661Z"},"links":{"citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:9309a7b1f3fd7064d130b6f0a359b615f3118ea03aad09e428b73367c2a41bd2","observation_id":"7b7c846e-975f-45b8-8061-4caf03cd18bf","resolution":{"observed_at":"2026-08-12T21:24:47.191661Z","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":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-12T21:24:48.093832Z","title":"Kleiss, W","venue":null,"work_id":"1e10bf3b-497a-4403-8425-547e905cd04a","year":1986},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":64,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:47.196151Z"},"links":{"citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:52da4ca5eb2f377b021a0b6f1437d3f4b4f1d6fcd914a19a98d9f72f14ba18d3","observation_id":"5acdda56-9005-4b8d-8726-9c183a5c4073","resolution":{"observed_at":"2026-08-12T21:24:48.098513Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.5167/uzh-32633","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-12T21:24:47.277547Z","title":"Greiner, Automation of the dipole substraction method","venue":null,"work_id":"c132ae66-a60a-4014-a65c-8f026c641683","year":2010},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":65,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:47.200369Z"},"links":{"citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:c62506e351a2c4e6ebf18e5ae486cebffb45b04cb5a8b089b96f62f54b9a2750","observation_id":"7d01ffe2-e735-44f1-8164-e79bba7340f8","resolution":{"observed_at":"2026-08-12T21:24:47.284256Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9605323","last_updated":"1997-11-06T11:40:37Z","snapshot_observed_at":"2026-07-07T04:22:39.163372Z","submitted_at":"1996-05-15T19:25:49Z","title":"A General Algorithm for Calculating Jet Cross Sections in NLO QCD","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9605323","snapshot_observed_at":"2026-08-12T21:24:47.205063Z","title":"Catani and M","venue":null,"work_id":null,"year":1997},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":66,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:47.205063Z"},"links":{"cited_paper":"/paper/hep-ph/9605323","citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:75e4d76645d1cb7469161c7a43a67423f776b0c0decb54d8e8b68aba4d2135ce","observation_id":"6e46d48c-08f8-4ced-a00a-56a6b65dca7d","resolution":{"observed_at":"2026-08-12T21:24:47.205063Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2410.17605","last_updated":"2024-10-23T07:00:41Z","snapshot_observed_at":"2026-08-12T22:17:00.632523Z","submitted_at":"2024-10-23T07:00:41Z","title":"New Physics Off the $Z$-Pole: $e^+ e^- \\rightarrow f \\bar f$ at Future Lepton Colliders","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2410.17605","snapshot_observed_at":"2026-08-12T21:24:47.209493Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":67,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:47.209493Z"},"links":{"cited_paper":"/paper/2410.17605","citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:75cfcecb52527308166545927f74f795f28544a78e23076cd323bc303152a4e2","observation_id":"c0fce378-c54f-412c-a6c9-77aca1957907","resolution":{"observed_at":"2026-08-12T21:24:47.209493Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1909.02000","last_updated":"2022-09-26T18:43:01Z","snapshot_observed_at":"2026-08-14T05:01:11.184693Z","submitted_at":"2019-09-04T18:00:00Z","title":"Electroweak and QCD Corrections to $Z$ and $W$ pole observables in the SMEFT","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1909.02000","snapshot_observed_at":"2026-08-12T21:24:47.214502Z","title":"Dawson and P","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":68,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:47.214502Z"},"links":{"cited_paper":"/paper/1909.02000","citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:6a3a5325b3ebc3699914734d81aac8d9bc4e195ca6e7083a847106af208e83c3","observation_id":"fedd4565-46f2-4d64-9280-0671e4ce9fbc","resolution":{"observed_at":"2026-08-12T21:24:47.214502Z","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":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-12T21:24:48.078081Z","title":"Tanabashi et al., Review of Particle Physics, Phys","venue":null,"work_id":"c2a6df82-8d4a-4835-a4ff-ec9d9e404d87","year":2018},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":69,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:47.218903Z"},"links":{"citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:e9db896d8e60d57bb9a729590fec8bc50055ed1b8368ef0a353e27d6d2a8e052","observation_id":"a9b945a8-c6d8-41db-bb21-7448a78f383f","resolution":{"observed_at":"2026-08-12T21:24:48.083040Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9906465","last_updated":"1999-06-24T10:04:25Z","snapshot_observed_at":"2026-07-07T04:33:32.996165Z","submitted_at":"1999-06-23T14:11:17Z","title":"Theory of Z boson decays","version":2},"cited_work":{"arxiv_id":"hep-ph/9906465","doi":null,"metadata_source":"pith","pith_arxiv_id":"hep-ph/9906465","snapshot_observed_at":"2026-08-12T21:24:47.362921Z","title":"Theory of Z boson decays","venue":"hep-ph","work_id":"3076b169-59a6-4e77-8981-0bc52305fc0f","year":1999},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":70,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:47.223278Z"},"links":{"cited_paper":"/paper/hep-ph/9906465","citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:65becf439edbfd972eb5d82c89ae7428a58cc0a1cb3e7b7f8dbc726f60492fd5","observation_id":"1f76bceb-3076-401a-8ef3-f4fe40eb7bb8","resolution":{"observed_at":"2026-08-12T21:24:47.367757Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2111.12515","last_updated":"2021-11-24T14:25:06Z","snapshot_observed_at":"2026-08-13T17:28:25.344817Z","submitted_at":"2021-11-24T14:25:06Z","title":"Electroweak input parameters","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2111.12515","snapshot_observed_at":"2026-08-12T21:24:47.227640Z","title":"Brivio, S","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":71,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:47.227640Z"},"links":{"cited_paper":"/paper/2111.12515","citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:8185ab2dd65bb0eb23ab13682b4e8364a62edf1847b66a7bc4c0b7fd222d8023","observation_id":"69902e30-cca0-47cf-bd66-212fdb2a9021","resolution":{"observed_at":"2026-08-12T21:24:47.227640Z","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":"2026-08-12T21:24:47.232355Z","title":"Cacciari, G","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":72,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:47.232355Z"},"links":{"cited_paper":"/paper/1111.6097","citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:5a3c714347dbb1fa28cbc80a4676328c336d3a5ee272888e6479c5e980fd03ce","observation_id":"df1c4db8-7c5d-455b-8b4c-fde733801fb6","resolution":{"observed_at":"2026-08-12T21:24:47.232355Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0512210","last_updated":"2006-08-17T09:18:49Z","snapshot_observed_at":"2026-08-03T17:23:02.358795Z","submitted_at":"2005-12-16T08:26:46Z","title":"Dispelling the N^3 myth for the Kt jet-finder","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0512210","snapshot_observed_at":"2026-08-12T21:24:47.236672Z","title":"Cacciari and G","venue":null,"work_id":null,"year":2006},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":73,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:47.236672Z"},"links":{"cited_paper":"/paper/hep-ph/0512210","citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:c8a0857c541b5a6bc7308d64dee8723e1348c90d65d0e57426f83c775e768482","observation_id":"1c6a68b3-33ff-454c-af3f-c91361118262","resolution":{"observed_at":"2026-08-12T21:24:47.236672Z","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":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-12T21:24:48.063116Z","title":"Catani, Y","venue":null,"work_id":"fa986954-8b47-4524-9f32-b29cb4d53e95","year":1993},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":74,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:47.241374Z"},"links":{"citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:db11ef953af53a083f266083076741b3ae7838cea628b6059b32a259993fc273","observation_id":"04436d91-07a9-4782-b8a0-e52753889eaf","resolution":{"observed_at":"2026-08-12T21:24:48.068146Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9305266","last_updated":"1993-05-14T01:40:29Z","snapshot_observed_at":"2026-08-11T20:21:20.986182Z","submitted_at":"1993-05-14T01:40:29Z","title":"Successive Combination Jet Algorithm For Hadron Collisions","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9305266","snapshot_observed_at":"2026-08-12T21:24:47.245564Z","title":null,"venue":null,"work_id":null,"year":1993},"citing_paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$","version":1},"reference_index":75,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:47.245564Z"},"links":{"cited_paper":"/paper/hep-ph/9305266","citing_paper":"/paper/2411.08802"},"observation_digest":"sha256:b5dba73f4d6068201fc967a84643420286aca21c621b1d3168650edc2dbe72f3","observation_id":"6fdb9fe7-d8b0-4f15-bec6-23fb6c443074","resolution":{"observed_at":"2026-08-12T21:24:47.245564Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"paper":{"arxiv_id":"2411.08802","last_updated":"2024-11-13T17:29:08Z","latest_version":1,"primary_category":"hep-ph","snapshot_observed_at":"2026-08-13T18:28:54.395011Z","submitted_at":"2024-11-13T17:29:08Z","title":"Next-to-leading order QCD corrections to $Z\\to q\\bar{q}\\gamma$, $q\\bar{q}\\gamma\\gamma$"},"reference_resolution":{"displayed":75,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":46,"verified_exact":12,"verified_fuzzy":17},"total_outbound_references":75},"refusal":"A citation records a reference. It does not transfer a finding from one paper to another.","schema":"pith.paper-citation-record.v1","standing_sources":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"thesis":"As of 14 August 2026, this Paper Citation Record lists 75 of 75 outbound references and 0 inbound Pith citation observations for arXiv:2411.08802."}