{"as_of":"2026-08-05T18:46:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:0845152f8fab7dddfc284362f92a1df0a83e9dfb61fa6f4349a5783538f39d6c","coverage":[{"denominator":100,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":100,"source":"paper_references, paper_reference_links","source_observed_at":"2026-07-12T02:47:06.419343Z","state":"measured"},{"denominator":100,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":100,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-05T06:32:48.257954+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/2607.03398/citation-record","integrity":"/paper/2607.03398/integrity","json":"/paper/2607.03398/citation-record.json","paper":"/paper/2607.03398"},"outbound":[{"citation":{"cited_paper":{"arxiv_id":"2511.15381","last_updated":"2026-05-11T16:23:12Z","snapshot_observed_at":"2026-07-06T22:36:24.466921Z","submitted_at":"2025-11-19T12:16:15Z","title":"New algorithms for Feynman integral reduction and $\\varepsilon$-factorised differential equations","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2511.15381","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":"Breeet al., (2025), arXiv:2511.15381","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/2511.15381","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:05bbe9b52cf6b258f873641a5be0cc0c8699a644fe061f61862cc26b446a3228","observation_id":"5bb99bc2-67d8-4364-a0f1-52ce894466f2","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","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":"2026-07-12T02:47:06.419343Z","title":null,"venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:683eb647ac72dbea641096c30da9a3b7fae2607a5248de2cbff9b1e18d60df51","observation_id":"57783909-5bbc-46f5-8f90-057df95f5577","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2203.01469","last_updated":"2022-11-15T02:34:35Z","snapshot_observed_at":"2026-08-04T17:08:56.495123Z","submitted_at":"2022-03-03T00:52:42Z","title":"The $Higgs\\to b\\bar{b}, c\\bar{c}, gg$ measurement at CEPC","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2203.01469","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":null,"venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/2203.01469","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:236c3ba6507ee8d36de26b20805e3db1999a18b9dc96f3db738f139bf9da4513","observation_id":"7ee3fa4a-2869-4d95-929c-a1bf486c2013","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2205.08553","last_updated":"2024-04-08T14:14:50Z","snapshot_observed_at":"2026-07-06T13:10:56.430851Z","submitted_at":"2022-05-17T18:00:05Z","title":"The Physics potential of the CEPC. Prepared for the US Snowmass Community Planning Exercise (Snowmass 2021)","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2205.08553","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":"Chenget al., The Physics potential of the CEPC","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/2205.08553","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:0dfa05a2ee6daa3f17b9bffbc60e7cb283c71a18a5033448ffe931c664638134","observation_id":"fd9771f0-d11d-47a0-8068-f2571d19b03e","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","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":"2026-07-12T02:47:06.419343Z","title":"Altmannet al.,ECF A Higgs, electroweak, and top Factory Study, CERN Yellow Reports: Monographs V ol","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:d1d02fc27153743d08d31d8863d9a9710324997b1efc68dabddbd05d806f33dd","observation_id":"34c36584-9051-469a-b580-765f685bd582","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","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":"2026-07-12T02:47:06.419343Z","title":"Braaten and J","venue":null,"work_id":null,"year":1980},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:2ac8987e0f9d5a589e9b8682b30429efa7a9023fcac8cac0d970e0f597355d81","observation_id":"d87c653a-9d25-4554-9ca6-459b362d5b28","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","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":"2026-07-12T02:47:06.419343Z","title":"Sakai, Phys","venue":null,"work_id":null,"year":1980},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:293c8b0efd4dac61f01cbf8b2f2f7b072a69346ae7bbd3d8c0ab7d4ef955ea2e","observation_id":"bd5b4c4b-3716-4620-8151-cd1842741a39","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9505358","last_updated":"1995-05-23T01:59:31Z","snapshot_observed_at":"2026-07-07T04:19:57.456626Z","submitted_at":"1995-05-23T01:59:31Z","title":"Second Order QCD Corrections to Scalar and Pseudoscalar Higgs Decays into Massive Bottom Quarks","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9505358","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":null,"venue":null,"work_id":null,"year":1996},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/hep-ph/9505358","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:776a5179115829eab12ec46ae91c2ba61b0e8016f151e561521390b221065367","observation_id":"fce6b269-bfe9-4a4d-be6f-13d4e4257eb1","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0511063","last_updated":"2005-12-19T13:05:59Z","snapshot_observed_at":"2026-07-07T04:09:11.749528Z","submitted_at":"2005-11-07T11:13:59Z","title":"Scalar Correlator at O(alpha_s^4), Higgs Decay into b-quarks and Bounds on the Light Quark Masses","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0511063","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":null,"venue":null,"work_id":null,"year":2006},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/hep-ph/0511063","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:42a43f1e250c5861f45838f88f6baf3016265e2a9ec64bd9f78b76724102f08b","observation_id":"1f8b6ca6-e30a-467e-b72f-301d31eae42a","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1707.01044","last_updated":"2017-10-05T17:04:45Z","snapshot_observed_at":"2026-07-06T05:49:43.427852Z","submitted_at":"2017-07-04T15:49:31Z","title":"On Higgs decays to hadrons and the R-ratio at N^4LO","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1707.01044","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":"Herzog, B","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/1707.01044","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:e812f23db618518200703064cec51b15b0c09f1716ded22ec260fb6dd43f79fa","observation_id":"3ce08a24-9046-450f-87b1-e4de212447c7","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1703.02988","last_updated":"2017-03-08T19:00:28Z","snapshot_observed_at":"2026-07-06T05:32:56.174403Z","submitted_at":"2017-03-08T19:00:28Z","title":"Completing the hadronic Higgs boson decay at order $\\alpha_s^4$","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1703.02988","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":"Davies, M","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/1703.02988","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:7580caee4c52b2cfd7617d5fa37e196c2f7f8cd3f9a1b2a046c4b2a5025f1ea3","observation_id":"0ecbaeb0-82d8-4cc9-8dd6-8d091cfa2fcf","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1812.07811","last_updated":"2018-12-19T08:40:24Z","snapshot_observed_at":"2026-07-06T07:22:10.393846Z","submitted_at":"2018-12-19T08:40:24Z","title":"Exact Top Yukawa corrections to Higgs boson decay into bottom quarks","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1812.07811","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":"Primo, G","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/1812.07811","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:bf1fdf3246e22c6594e739ff4696508b3a0250a301e5a6503a6a42a37ed8e08b","observation_id":"18625fd7-88a7-446f-9511-fa65248c596f","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2006.03563","last_updated":"2020-06-05T17:15:08Z","snapshot_observed_at":"2026-08-03T17:07:23.843487Z","submitted_at":"2020-06-05T17:15:08Z","title":"Top-induced contributions to $H\\rightarrow b\\bar{b}$ and $H\\rightarrow c\\bar{c}$ at $\\mathcal{O}(\\alpha_s^3)$","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2006.03563","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":"Mondini, U","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/2006.03563","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:6c638d20805f33d70ec445b6ee3306902601ff6225fe98c41092ce7406d6ea23","observation_id":"710bd9b2-50e5-411a-9600-e141e82be408","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2411.07493","last_updated":"2025-03-24T14:13:07Z","snapshot_observed_at":"2026-07-06T19:48:49.553384Z","submitted_at":"2024-11-12T02:44:01Z","title":"Analytic decay width of the Higgs boson to massive bottom quarks at order $\\alpha_s^3$","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2411.07493","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":null,"venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/2411.07493","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:589582985c1c2ce2f41ef6a141769dacf822da927de6ae14d89bb875d0626d76","observation_id":"6d1d46ff-d214-438e-ae48-6489112b563f","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","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":"2026-07-12T02:47:06.419343Z","title":null,"venue":null,"work_id":null,"year":2026},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:204b86d3bd986174b4b132796b17461c877d7c7d5fc79733893f73db19b6da3c","observation_id":"48ef04de-617c-4805-a93e-0e962cedea67","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","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":"2026-07-12T02:47:06.419343Z","title":null,"venue":null,"work_id":null,"year":1981},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:02affbd6920fcb5ffae488c9232b7da8422bb1d36f0d086ce47a147f856b48f8","observation_id":"a06dc15f-c51c-44ed-9d18-54a0bb06a197","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","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":"2026-07-12T02:47:06.419343Z","title":null,"venue":null,"work_id":null,"year":1981},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:7b509a7f5bbb13663f023a1b1667e6a9fb876306490bc12433d1e4a4a0ae3396","observation_id":"6cbd7f33-6836-4055-83f4-428ca7185843","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1310.1145","last_updated":"2013-10-04T01:43:34Z","snapshot_observed_at":"2026-08-03T05:12:51.116171Z","submitted_at":"2013-10-04T01:43:34Z","title":"LiteRed 1.4: a powerful tool for the reduction of the multiloop integrals","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1310.1145","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":null,"venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/1310.1145","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:aed0fa53622c2b3c8a0a1a663196e48d0a00d0797f162d05e88dea841510acbe","observation_id":"98d91c6b-386c-4b27-b0ad-e5cd5d9c9784","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1201.4330","last_updated":"2012-01-20T16:22:46Z","snapshot_observed_at":"2026-07-06T02:41:28.989809Z","submitted_at":"2012-01-20T16:22:46Z","title":"Reduze 2 - Distributed Feynman Integral Reduction","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1201.4330","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":"von Manteuffel and C","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/1201.4330","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:93caa2a690e0a83cfbced25b711d9df70090dbeabae06f3dd9443c937ffc2ba6","observation_id":"c060c3b7-928e-4d0e-bfff-74e3d19087ba","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1705.05610","last_updated":"2018-04-26T13:54:46Z","snapshot_observed_at":"2026-07-06T05:42:48.879600Z","submitted_at":"2017-05-16T09:31:16Z","title":"Kira - A Feynman Integral Reduction Program","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1705.05610","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":"Maierhöfer, J","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/1705.05610","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:93cb8230279a89419c758b0fa71594651daab997dd3b11e29fb3a2b68e0f9234","observation_id":"3b32f7f2-f1a6-4f18-9ea2-35a8a7259e5f","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1901.07808","last_updated":"2019-02-10T16:44:50Z","snapshot_observed_at":"2026-07-06T07:28:25.420986Z","submitted_at":"2019-01-23T10:41:16Z","title":"FIRE6: Feynman Integral REduction with Modular Arithmetic","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1901.07808","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":null,"venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/1901.07808","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:66dafb6b5df0cbba647f1039216fe4e19f156743acbc29ac0586869511b40121","observation_id":"78192071-5c1f-4dd0-a94e-5ce78b082bba","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2008.06494","last_updated":"2023-02-22T22:51:09Z","snapshot_observed_at":"2026-07-06T09:47:16.564697Z","submitted_at":"2020-08-14T17:58:33Z","title":"Integral Reduction with Kira 2.0 and Finite Field Methods","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2008.06494","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":"Klappert, F","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/2008.06494","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:183e3bb1150be7c5451686276c1cd5537cbf1ac9ab418488e4c2beab868faf47","observation_id":"80e4b458-a5e6-464c-946e-ccb7004c38a4","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1905.08019","last_updated":"2019-07-17T10:17:15Z","snapshot_observed_at":"2026-08-04T21:37:56.686306Z","submitted_at":"2019-05-20T12:07:06Z","title":"FiniteFlow: multivariate functional reconstruction using finite fields and dataflow graphs","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1905.08019","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":"Peraro, JHEP07, 031 (2019), arXiv:1905.08019","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/1905.08019","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:64ac221d8a3a32ae0a71900099c760090c7f78f15e7782d30127263a9c13f4e5","observation_id":"6b754ca7-cc88-4c96-84ad-b88d337850ad","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2305.08783","last_updated":"2024-10-24T08:12:25Z","snapshot_observed_at":"2026-08-04T12:06:41.351658Z","submitted_at":"2023-05-15T16:43:50Z","title":"NeatIBP 1.0, A package generating small-size integration-by-parts relations for Feynman integrals","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2305.08783","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":null,"venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/2305.08783","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:29dfb1105bce40f6dfeacc9919c16f38a0acdbc125e6c5ea5842b8e37f644f7e","observation_id":"3661a275-a357-4283-8cdb-eeab1854bd32","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2405.14621","last_updated":"2025-02-06T02:04:35Z","snapshot_observed_at":"2026-08-03T00:40:10.812718Z","submitted_at":"2024-05-23T14:29:31Z","title":"Blade: A package for block-triangular form improved Feynman integrals decomposition","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2405.14621","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":null,"venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/2405.14621","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:dd3ce34101f047935cd2ca6989f5c0e88798eadf3e8ba0b1e8438348526eb4cb","observation_id":"4b2cab48-354e-4f7b-a7fd-ecaf7d0e3d60","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0102033","last_updated":"2001-02-03T11:42:35Z","snapshot_observed_at":"2026-07-07T03:51:21.780507Z","submitted_at":"2001-02-03T11:42:35Z","title":"High-precision calculation of multi-loop Feynman integrals by difference equations","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0102033","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":"Laporta, Int","venue":null,"work_id":null,"year":2000},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/hep-ph/0102033","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:effe53f67834e87497625cf765a275aeae248bb21f819b36d32e2e6c5a201ed4","observation_id":"6c04341e-6ee3-4674-bc78-946c42d178e8","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2412.15962","last_updated":"2026-04-29T11:38:13Z","snapshot_observed_at":"2026-07-06T20:10:56.727212Z","submitted_at":"2024-12-20T14:57:51Z","title":"Feynman Integral Reduction without Integration-By-Parts","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2412.15962","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":"Wang and L","venue":null,"work_id":null,"year":2026},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/2412.15962","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:ec34371826a90c619c90d7c899e17b92d6554d784276fb45964d02db2c812b94","observation_id":"59a580a8-07bc-4529-8074-b46271e6f289","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","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":"2026-07-12T02:47:06.419343Z","title":null,"venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:12cffb07b6fba88d9d6dd0c9989b801e9a44bd3d52859c1973cdc8f0bf688e25","observation_id":"7f67b044-1fd1-449a-9571-c9e97dbae4ba","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","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":"2026-07-12T02:47:06.419343Z","title":"de la Cruz and D","venue":null,"work_id":null,"year":2026},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":29,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:e414a178fd412dccfab2c026533cf8953a3e05657529fce80d2363af8dc59ddd","observation_id":"e43a6ea8-391e-417d-9f9f-e809cbd35744","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","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":"2026-07-12T02:47:06.419343Z","title":"Smith and M","venue":null,"work_id":null,"year":2026},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:bc86b36a4e06db004517f6705e6158f9411bd829a810f24ab7a8f934fc72a537","observation_id":"af6370fc-b662-438d-9efb-1ac821020393","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2604.25916","last_updated":"2026-04-28T17:59:10Z","snapshot_observed_at":"2026-07-06T23:11:39.318906Z","submitted_at":"2026-04-28T17:59:10Z","title":"Nonlocal-in-time tail effects in gravitational scattering to fifth Post-Minkowskian and tenth self-force orders","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2604.25916","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":"Dlapa, G","venue":null,"work_id":null,"year":2026},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/2604.25916","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:e5092eb8ee5b35fa8fcc4c14c8c5823ab68c4c146b002fef83463735e34baa11","observation_id":"78e9199d-c1e4-4dc9-bbb4-313daf58bee8","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2605.09541","last_updated":"2026-05-10T13:53:34Z","snapshot_observed_at":"2026-07-06T23:21:35.327066Z","submitted_at":"2026-05-10T13:53:34Z","title":"An Algorithm for the Symbolic Reduction of Multi-loop Feynman Integrals via Generating Functions","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2605.09541","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":null,"venue":null,"work_id":null,"year":2026},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":32,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/2605.09541","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:242dd0d8a5313bde71f6dd30b28dc2c64f15ef67cef7e71746b52f0dcf533a9b","observation_id":"32b34f60-026b-411e-969d-226b41ac0caf","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","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":"2026-07-12T02:47:06.419343Z","title":null,"venue":null,"work_id":null,"year":1991},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:10ca44d685919fb066709c2a2ed525d09ee213b73f464d8094476844bd70ef04","observation_id":"b7cbc934-fb85-4f18-a1a3-c494dddeee7d","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/9711188","last_updated":"1997-12-11T15:42:49Z","snapshot_observed_at":"2026-07-07T05:15:17.255729Z","submitted_at":"1997-11-26T11:57:35Z","title":"Differential Equations for Feynman Graph Amplitudes","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/9711188","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":"Remiddi, Nuovo Cim","venue":null,"work_id":null,"year":1997},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":34,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/hep-th/9711188","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:7d7fc7634d9c7499083fa30d96e3399b7f820202b884d292d20b9fb0135f7442","observation_id":"8c9d2533-9b98-4c48-ab4d-4ab7f45e42cf","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9912329","last_updated":"2000-04-27T09:19:33Z","snapshot_observed_at":"2026-07-07T04:35:22.917311Z","submitted_at":"1999-12-14T08:54:32Z","title":"Differential Equations for Two-Loop Four-Point Functions","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9912329","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":"Gehrmann and E","venue":null,"work_id":null,"year":2000},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/hep-ph/9912329","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:e771160ecb3e3dbde2e1b6c613a99bb1c784ecd5e40481c6bc89cd5f069668d7","observation_id":"a454b0ca-4d88-4d39-b2cf-9146b7cd79a1","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2006.05510","last_updated":"2020-11-29T23:47:37Z","snapshot_observed_at":"2026-08-01T02:18:13.147527Z","submitted_at":"2020-06-09T21:07:54Z","title":"DiffExp, a Mathematica package for computing Feynman integrals in terms of one-dimensional series expansions","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2006.05510","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":"Hidding, Comput","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":36,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/2006.05510","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:0b9ec26e2c6ab4c5341804d11e936df7c4600005be969033fbe8441c7c51e45b","observation_id":"f06d03a1-eecb-48bc-a287-db92306089f2","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1711.09572","last_updated":"2018-02-27T07:48:35Z","snapshot_observed_at":"2026-07-06T06:11:17.645784Z","submitted_at":"2017-11-27T08:09:54Z","title":"A Systematic and Efficient Method to Compute Multi-loop Master Integrals","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1711.09572","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":"Liu, Y .-Q","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":37,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/1711.09572","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:9bc97defebcb34584a5046706621f71a0eee2fabf5a71f0603352dd54b40e199","observation_id":"98702f90-08b2-4512-84a1-cb7e5ff6c378","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2201.11669","last_updated":"2022-10-27T12:29:10Z","snapshot_observed_at":"2026-08-03T16:31:05.674748Z","submitted_at":"2022-01-27T17:15:37Z","title":"AMFlow: a Mathematica package for Feynman integrals computation via Auxiliary Mass Flow","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2201.11669","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":"Liu and Y .-Q","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":38,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/2201.11669","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:d7b29415d31a5af16a9808e4972170669a31f23e4df52801fba00fa6a0c80a28","observation_id":"ec800890-8d6b-495b-942f-ab0c42fc5f75","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2205.03345","last_updated":"2022-10-21T13:07:01Z","snapshot_observed_at":"2026-08-04T15:55:08.939152Z","submitted_at":"2022-05-06T16:25:21Z","title":"Evaluation of Feynman integrals with arbitrary complex masses via series expansions","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2205.03345","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":"Armadillo, R","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":39,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/2205.03345","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:e6c63cc1d0dac39776f887d32f39dce5c359741207195d4264fa6fccf0895060","observation_id":"0551ce8e-19e9-4b00-ae83-1e7558e8c431","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2408.06426","last_updated":"2025-04-11T13:00:53Z","snapshot_observed_at":"2026-07-06T18:59:51.988540Z","submitted_at":"2024-08-12T18:07:28Z","title":"Semi-automatic Calculations of Multi-loop Feynman Amplitudes with AmpRed","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2408.06426","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":"Chen, Comput","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":40,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/2408.06426","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:6228d48a5b4797cda612a5a640a418232d8e843c7221f0e93216b49a979cc7b4","observation_id":"8938b6d1-59e8-45cb-8c84-4dde0bbca5be","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2501.01943","last_updated":"2025-01-03T18:50:38Z","snapshot_observed_at":"2026-07-06T20:16:18.023949Z","submitted_at":"2025-01-03T18:50:38Z","title":"LINE: Loop Integrals Numerical Evaluation","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2501.01943","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":null,"venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":41,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/2501.01943","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:e8099cfe556d94a0a99c133a14945c20a2c8d9bd1bfa35d98e9bddd548737781","observation_id":"49e07aaa-4c60-41bf-b90c-c9b3512c61f4","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2606.26691","last_updated":"2026-06-25T07:22:04Z","snapshot_observed_at":"2026-07-07T00:01:01.437499Z","submitted_at":"2026-06-25T07:22:04Z","title":"CHESS: CHEbyshev pSeudo-Spectral transport for Feynman integral differential equations","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2606.26691","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":"Liu and Y","venue":null,"work_id":null,"year":2026},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":42,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/2606.26691","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:7a7ba3fb420bedfdd1d6d402d012088d6f701304db5917421e2af308047e5518","observation_id":"55d49437-cb7b-4a6c-9648-f3ba0a3fc299","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2606.30354","last_updated":"2026-06-29T14:23:37Z","snapshot_observed_at":"2026-07-07T00:04:15.048683Z","submitted_at":"2026-06-29T14:23:37Z","title":"Solution of Canonical Differential Equations for Integrals on Arbitrary Geometries","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2606.30354","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":"Czakon and L","venue":null,"work_id":null,"year":2026},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":43,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/2606.30354","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:34dbd9081907321186b39fb74b180afc61300c2ddd1dc05c1718741dededf560","observation_id":"b76c6a1a-371d-433d-9e9b-6e08764c0ffe","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1304.1806","last_updated":"2013-05-31T15:05:36Z","snapshot_observed_at":"2026-07-06T03:10:29.622191Z","submitted_at":"2013-04-05T20:00:03Z","title":"Multiloop integrals in dimensional regularization made simple","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1304.1806","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":null,"venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":44,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/1304.1806","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:57b00b2f0d6aa0aba181f5d4e74c7eda4a59ba6ab400dda1a709d173ddc664a8","observation_id":"737cfae1-28c7-4ab7-ab37-8284b19aeb60","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","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":"2026-07-12T02:47:06.419343Z","title":"Chen, Bull","venue":null,"work_id":null,"year":1977},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":45,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:19a3b07b287a8b55830e7f028b4284011c5a4222023ed6ebead44f4836b1d513","observation_id":"d0757d85-a85e-4916-83e8-ceae2694d141","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9905237","last_updated":"1999-05-04T13:03:18Z","snapshot_observed_at":"2026-07-07T04:32:57.370560Z","submitted_at":"1999-05-04T13:03:18Z","title":"Harmonic Polylogarithms","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9905237","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":"Remiddi and J","venue":null,"work_id":null,"year":2000},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":46,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/hep-ph/9905237","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:92d8285b40bf5e409a21054d3169a13dcfd03d4714ecfd68b91e408c00fc680e","observation_id":"a163638c-9812-4c28-ada6-4704992eaa34","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1105.2076","last_updated":"2011-05-10T23:59:56Z","snapshot_observed_at":"2026-07-31T02:20:36.972172Z","submitted_at":"2011-05-10T23:59:56Z","title":"Multiple polylogarithms, cyclotomy and modular complexes","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1105.2076","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":null,"venue":null,"work_id":null,"year":1998},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":47,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/1105.2076","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:b356653a88c497ea37df27fef640ac61b4cd8768453b94091e7b239f032d937f","observation_id":"2768ad8b-56a6-4ca4-af2f-266530af7432","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1006.5703","last_updated":"2010-10-07T18:04:24Z","snapshot_observed_at":"2026-07-06T02:12:17.652140Z","submitted_at":"2010-06-29T19:03:36Z","title":"Classical Polylogarithms for Amplitudes and Wilson Loops","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1006.5703","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":null,"venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":48,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/1006.5703","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:20cd3d4ef76690b18e3c9f0083cc8d69dd66b9755527e10bc4a66ddc6c9c1b86","observation_id":"12a75644-f1de-441e-bc9c-d3502b6c526f","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1110.0458","last_updated":"2011-10-03T19:54:07Z","snapshot_observed_at":"2026-08-05T04:23:25.078670Z","submitted_at":"2011-10-03T19:54:07Z","title":"From polygons and symbols to polylogarithmic functions","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1110.0458","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":null,"venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":49,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/1110.0458","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:a055914897a59f7fce9701853b1a86ddbd1d592b76085fed459ae1f4b908d448","observation_id":"cfd802c7-ff57-47d8-85cd-f5440ef0a93b","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1203.0454","last_updated":"2012-03-02T13:31:22Z","snapshot_observed_at":"2026-08-05T10:31:04.623567Z","submitted_at":"2012-03-02T13:31:22Z","title":"Hopf algebras, coproducts and symbols: an application to Higgs boson amplitudes","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1203.0454","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":"Duhr, JHEP08, 043 (2012), arXiv:1203.0454","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":50,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/1203.0454","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:440efd3c932cc20235723e2f8a0c32c4c2946dd32e2f47518db9a34086c661cf","observation_id":"eceb2899-08b2-460b-b4ec-0a2a9ae04be6","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1012.6032","last_updated":"2010-12-29T20:47:33Z","snapshot_observed_at":"2026-08-05T15:57:57.241786Z","submitted_at":"2010-12-29T20:47:33Z","title":"Local Integrals for Planar Scattering Amplitudes","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1012.6032","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":"Arkani-Hamed, J","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":51,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/1012.6032","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:2f9be5b435419d4415c6ef9d02f4241a1a2902d70afdc5f37c7a0f674a374c59","observation_id":"1681c95b-96ed-47a6-bd03-1c2b311c0324","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1411.0911","last_updated":"2015-04-21T10:15:37Z","snapshot_observed_at":"2026-08-01T19:28:07.876962Z","submitted_at":"2014-11-04T13:56:11Z","title":"Reducing differential equations for multiloop master integrals","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1411.0911","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":null,"venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":52,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/1411.0911","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:3f05135a8dc44711fd77c99c157f46a8460c4b7cbab77e26ba5a8781d41a38d1","observation_id":"01529026-0876-440d-99d8-deec975c44d5","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1701.00725","last_updated":"2017-06-28T09:53:30Z","snapshot_observed_at":"2026-07-06T05:24:54.988450Z","submitted_at":"2017-01-03T15:36:18Z","title":"epsilon: A tool to find a canonical basis of master integrals","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1701.00725","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":"Prausa, Comput","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":53,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/1701.00725","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:ce785ad326d6ecf145c76dd4a2da4dd530c83f56038e02aa3f39ae8d4caea77a","observation_id":"69f5792f-0b34-4170-beed-fbd7b55418be","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1701.04269","last_updated":"2017-01-16T12:52:27Z","snapshot_observed_at":"2026-07-06T05:26:19.801141Z","submitted_at":"2017-01-16T12:52:27Z","title":"Fuchsia: a tool for reducing differential equations for Feynman master integrals to epsilon form","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1701.04269","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":"Gituliar and V","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":54,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/1701.04269","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:f2e6ba1e81c4b86616296b91a83beb2ba2089c60107e8fea90a7ec632a722d4c","observation_id":"7cb0841c-2c00-43b5-8176-001e75b07bce","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1705.06252","last_updated":"2017-11-29T13:54:59Z","snapshot_observed_at":"2026-07-06T05:43:04.302843Z","submitted_at":"2017-05-17T16:35:45Z","title":"Algorithmic transformation of multi-loop master integrals to a canonical basis with CANONICA","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1705.06252","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":"Meyer, Comput","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":55,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/1705.06252","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:c3373e3673c35434f1a6c3b07f177349ed4e3215914e3ace5e73c078272be2bf","observation_id":"54bdd19e-dccf-4bd6-9517-1728210511c5","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2012.00279","last_updated":"2020-12-01T05:36:00Z","snapshot_observed_at":"2026-07-06T10:19:22.004464Z","submitted_at":"2020-12-01T05:36:00Z","title":"Libra: a package for transformation of differential systems for multiloop integrals","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2012.00279","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":null,"venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":56,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/2012.00279","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:b51f42942a8b173976a6db994a89e5f1d4a2cf315e14f9e761a6d9b2641effd3","observation_id":"2fb1748a-235d-48ab-ad55-338734ec96b3","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2002.02340","last_updated":"2020-02-06T16:39:28Z","snapshot_observed_at":"2026-08-04T14:10:04.340330Z","submitted_at":"2020-02-06T16:39:28Z","title":"Deriving canonical differential equations for Feynman integrals from a single uniform weight integral","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2002.02340","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":"Dlapa, J","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":57,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/2002.02340","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:510565f8fd6f0ed3174b5a63849be18af76883d4df5ccc6b86cee5842ec944e2","observation_id":"85600cc5-1e49-498e-9d24-8c357160efcd","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2002.09492","last_updated":"2020-03-05T18:06:40Z","snapshot_observed_at":"2026-07-06T08:59:13.242196Z","submitted_at":"2020-02-21T19:00:00Z","title":"Constructing d-log integrands and computing master integrals for three-loop four-particle scattering","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2002.09492","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":null,"venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":58,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/2002.09492","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:7315dcd9ddb711d694226ec81f0a5e541b179e3dd3298cbbbc473fc44faba382","observation_id":"457304a5-5389-49f1-9bee-db7f0318aae2","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0406160","last_updated":"2004-10-07T12:17:55Z","snapshot_observed_at":"2026-07-07T04:03:58.130205Z","submitted_at":"2004-06-15T12:36:54Z","title":"Analytic treatment of the two loop equal mass sunrise graph","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0406160","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":"Laporta and E","venue":null,"work_id":null,"year":2005},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":59,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/hep-ph/0406160","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:23bff2571af0bd66df1d57e890263d4c44c0e474184cfa3fc2e410ebcd07115a","observation_id":"4c2822fa-4850-4a06-88fa-eeebb76f8231","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1309.5865","last_updated":"2014-10-24T17:42:43Z","snapshot_observed_at":"2026-08-04T18:03:32.834752Z","submitted_at":"2013-09-23T16:24:01Z","title":"The elliptic dilogarithm for the sunset graph","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1309.5865","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":"Bloch and P","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":60,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/1309.5865","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:4947c50780824091a9d239198b0ce6c5d0485a9be0640ff090346226bd7bc019","observation_id":"e90eaecc-cefa-4809-98ff-041250e84069","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1302.7004","last_updated":"2013-02-27T21:07:32Z","snapshot_observed_at":"2026-08-03T12:11:09.159599Z","submitted_at":"2013-02-27T21:07:32Z","title":"The two-loop sunrise graph with arbitrary masses","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1302.7004","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":"Adams, C","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":61,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/1302.7004","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:4b575408c6fc786dd08bdb7a4b6247fb9926a73a42272df80a224d3021be9b2a","observation_id":"413e0f36-c081-46b4-aecf-8c3c567311a9","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1504.03255","last_updated":"2015-04-13T16:57:04Z","snapshot_observed_at":"2026-07-06T04:14:51.310119Z","submitted_at":"2015-04-13T16:57:04Z","title":"The two-loop sunrise integral around four space-time dimensions and generalisations of the Clausen and Glaisher functions towards the elliptic case","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1504.03255","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":"Adams, C","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":62,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/1504.03255","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:3624e40b3a81be44911a9786e34f5af6c77fa8db9acbb907e37ffb133c9d0857","observation_id":"bf4593d1-1542-4194-9c5f-fa4527b95d28","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1607.01571","last_updated":"2016-11-14T19:20:16Z","snapshot_observed_at":"2026-07-06T05:02:33.207110Z","submitted_at":"2016-07-06T11:30:02Z","title":"The kite integral to all orders in terms of elliptic polylogarithms","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1607.01571","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":"Adams, C","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":63,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/1607.01571","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:a7e22541da849ddb9bd5a86456eb8f1a8b6e6840a38f00591ed932fec2143125","observation_id":"3aa961d1-531d-43c6-9ffd-190c3477ea3f","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1709.03622","last_updated":"2017-10-10T09:08:15Z","snapshot_observed_at":"2026-07-06T05:59:11.248495Z","submitted_at":"2017-09-11T23:14:11Z","title":"An Elliptic Generalization of Multiple Polylogarithms","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1709.03622","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":"Remiddi and L","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":64,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/1709.03622","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:62513d037cbcf5cc7280ddb11d21cd3e490aee1c4e1748036db4c06b9f0d95c5","observation_id":"c6478fc9-d092-443f-840b-22f8f1da926b","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1712.07089","last_updated":"2017-12-19T18:19:05Z","snapshot_observed_at":"2026-08-02T21:51:12.497978Z","submitted_at":"2017-12-19T18:19:05Z","title":"Elliptic polylogarithms and iterated integrals on elliptic curves I: general formalism","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1712.07089","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":"Broedel, C","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":65,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/1712.07089","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:225c09df681225726997d1f236508a1085c1238efb4f4f303ccca9c97a079b64","observation_id":"bafa3d39-eb7b-4688-9294-ecee5659d130","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1803.10256","last_updated":"2018-03-27T18:05:43Z","snapshot_observed_at":"2026-08-04T19:21:51.154156Z","submitted_at":"2018-03-27T18:05:43Z","title":"Elliptic symbol calculus: from elliptic polylogarithms to iterated integrals of Eisenstein series","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1803.10256","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":"Broedel, C","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":66,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/1803.10256","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:c2a716feca08ea3077b92887bb58dc1572cec1e8a06ae2f6358b4b8652735b09","observation_id":"d7a2b123-2902-43de-98dd-2121f038e5a4","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1809.10698","last_updated":"2018-09-27T18:02:20Z","snapshot_observed_at":"2026-08-03T21:41:59.984045Z","submitted_at":"2018-09-27T18:02:20Z","title":"Elliptic Feynman integrals and pure functions","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1809.10698","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":"Broedel, C","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":67,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/1809.10698","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:20ddebffcbd3e999649dfc64b6b1214241312929b0182b59a5295323127f2cdb","observation_id":"661e76cf-ac83-446f-a8b7-3f281cf271db","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2201.03593","last_updated":"2022-06-13T19:01:27Z","snapshot_observed_at":"2026-08-05T15:56:44.455688Z","submitted_at":"2022-01-10T19:03:01Z","title":"Feynman Integrals","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2201.03593","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":"Weinzierl,Feynman Integrals","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":68,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/2201.03593","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:5e09e08f557a0eb1e80d83a6a6ec50e15a78349e91cc02514de8db482361cdad","observation_id":"8f7469d3-26c7-4f9d-aa21-0c7df619ebf1","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1802.05020","last_updated":"2018-04-02T20:34:43Z","snapshot_observed_at":"2026-07-06T06:23:21.453011Z","submitted_at":"2018-02-14T10:16:47Z","title":"The $\\varepsilon$-form of the differential equations for Feynman integrals in the elliptic case","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1802.05020","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":"Adams and S","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":69,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/1802.05020","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:ebc20205038bf3a278a43261dc7840dfd28e51a8390a7edfad50c7c17daf2ea8","observation_id":"44c0564e-c620-4825-abec-998ec2f3ab81","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2311.06385","last_updated":"2023-11-10T20:26:49Z","snapshot_observed_at":"2026-07-06T16:45:55.261144Z","submitted_at":"2023-11-10T20:26:49Z","title":"Two-loop QED corrections to the scattering of four massive leptons","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2311.06385","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":"Delto, C","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":70,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/2311.06385","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:b58e4161675e9dbb1a3dd0e3b3d41e84cc8ea5897c03964216b0702b92d919a0","observation_id":"8617b4be-e5d9-435a-890e-6fa67d96caed","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","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":"2026-07-12T02:47:06.419343Z","title":"Marzucca, A","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":71,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:f9a2d98e456bf448589abaad10a4fb1051283ecb4f4df7d32f0b89f1df3baa42","observation_id":"064f21e4-7701-40ec-a62e-04e42358a877","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2503.03603","last_updated":"2025-08-21T14:24:05Z","snapshot_observed_at":"2026-07-06T20:47:14.977471Z","submitted_at":"2025-03-05T15:38:19Z","title":"Canonical differential equations for the elliptic two-loop five-point integral family relevant to $t\\bar t +$jet production at leading colour","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2503.03603","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":"Becchetti, C","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":72,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/2503.03603","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:0e4e20768d6ffb3e990eb39c4f8fb0399859f7d762c64a6fbbd23f459b04a6ad","observation_id":"37600697-514e-4425-b928-9b30f7b6606b","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2412.07522","last_updated":"2025-05-12T12:18:45Z","snapshot_observed_at":"2026-07-06T20:04:39.240950Z","submitted_at":"2024-12-10T13:59:44Z","title":"Electroweak double-box integrals for Moller scattering","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2412.07522","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":"Schwanemann and S","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":73,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/2412.07522","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:c7d24ab838c8999e521952b9149f49675e10be9ed608b6c9192158148dd5bd71","observation_id":"3fa3678c-4f72-45b3-9d9a-84598c89e90a","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1912.06201","last_updated":"2020-01-14T16:07:11Z","snapshot_observed_at":"2026-07-06T08:44:12.200272Z","submitted_at":"2019-12-12T20:44:54Z","title":"The $l$-loop Banana Amplitude from GKZ Systems and relative Calabi-Yau Periods","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1912.06201","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":"Klemm, C","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":74,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/1912.06201","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:c7310ce8bd02259f116200dff19f1872c7e3df9e9f13d0e0e0cf91fd22910692","observation_id":"34807961-40dd-4f23-a5dc-4de572b2a584","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2008.10574","last_updated":"2021-05-14T13:56:14Z","snapshot_observed_at":"2026-08-05T16:38:19.088220Z","submitted_at":"2020-08-24T17:25:17Z","title":"Analytic Structure of all Loop Banana Amplitudes","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2008.10574","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":"Bönisch, F","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":75,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/2008.10574","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:e9eabda784df0b780de7b9629a59ea0869b3f2fbcc477568c66f40b5a6df9c98","observation_id":"d85360ff-9404-4343-af6a-c6c7a4fa2b63","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1704.05465","last_updated":"2018-11-23T06:52:23Z","snapshot_observed_at":"2026-07-06T05:38:18.248922Z","submitted_at":"2017-04-18T18:00:03Z","title":"Maximal cuts and differential equations for Feynman integrals. An application to the three-loop massive banana graph","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1704.05465","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":"Primo and L","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":76,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/1704.05465","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:14298be1738904959f49ad2abb60ca0cf464062a8a0d8730cfc58508dfc38f25","observation_id":"e1abd958-de13-4426-a2f7-32fe7a98d201","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2207.12893","last_updated":"2022-08-12T07:22:46Z","snapshot_observed_at":"2026-07-06T13:35:29.958339Z","submitted_at":"2022-07-26T13:42:59Z","title":"The three-loop equal-mass banana integral in $\\varepsilon$-factorised form with meromorphic modular forms","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2207.12893","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":"Pögel, X","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":77,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/2207.12893","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:341a5a20a2a3d70e648f0b49a0b7fa02387859f66b2c1f72d953a18a5229c883","observation_id":"8cf2a5f6-912e-4746-8183-16532642c69b","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2211.04292","last_updated":"2023-02-07T18:31:56Z","snapshot_observed_at":"2026-08-05T17:14:08.515451Z","submitted_at":"2022-11-08T14:59:40Z","title":"Taming Calabi-Yau Feynman integrals: The four-loop equal-mass banana integral","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2211.04292","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":"Pögel, X","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":78,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/2211.04292","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:1e37003d98ce5b0a5efed94c2cafbde70aaa2acb2f3e5382b76524c1484ec8c3","observation_id":"11e33e4a-23e0-4d01-9268-6880dbdd1183","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2212.08908","last_updated":"2023-04-10T12:09:36Z","snapshot_observed_at":"2026-07-06T14:32:03.511072Z","submitted_at":"2022-12-17T15:52:23Z","title":"Bananas of equal mass: any loop, any order in the dimensional regularisation parameter","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2212.08908","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":"Pögel, X","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":79,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/2212.08908","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:e71ef774823b00f6983247a08c5ed740e62bc97d7bc73bb04eee55c44d8857b6","observation_id":"ef68bd3e-9f6a-4bdc-b2e1-0854b981272a","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1805.09326","last_updated":"2018-08-09T16:10:40Z","snapshot_observed_at":"2026-08-01T23:13:44.001806Z","submitted_at":"2018-05-23T18:00:00Z","title":"Traintracks Through Calabi-Yaus: Amplitudes Beyond Elliptic Polylogarithms","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1805.09326","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":null,"venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":80,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/1805.09326","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:a743b7247def4c59a6be6d380aa7462766e67efb5c059697cd5968e82f5ed662","observation_id":"99dff743-7dc2-4b2d-9ce6-d941f9d7a1ca","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1810.07689","last_updated":"2019-01-28T11:16:47Z","snapshot_observed_at":"2026-07-06T07:08:59.218192Z","submitted_at":"2018-10-17T17:59:59Z","title":"A (Bounded) Bestiary of Feynman Integral Calabi-Yau Geometries","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1810.07689","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":null,"venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":81,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/1810.07689","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:3739084070e732fe3d1abff04ef84f2e8273bfdd0bfd8dc4e27fe9dfa283fe37","observation_id":"1e739f41-3bdd-4581-9815-536eb8e8d60c","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2212.09550","last_updated":"2022-12-19T15:42:34Z","snapshot_observed_at":"2026-08-03T22:51:01.511466Z","submitted_at":"2022-12-19T15:42:34Z","title":"The ice cone family and iterated integrals for Calabi-Yau varieties","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2212.09550","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":null,"venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":82,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/2212.09550","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:74639b7ab6976653e3251a348f325baf8945cd528d056dbfda1596a9ed619d42","observation_id":"a6b61fa7-b394-401c-8f03-13d4737b0eb5","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2209.05291","last_updated":"2022-09-12T14:50:03Z","snapshot_observed_at":"2026-07-06T13:51:16.413902Z","submitted_at":"2022-09-12T14:50:03Z","title":"Yangian-invariant fishnet integrals in 2 dimensions as volumes of Calabi-Yau varieties","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2209.05291","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":null,"venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":83,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/2209.05291","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:791543cdd76f794c6e62d1adf8f9ad7ce1843bdbb962a939320e5464372e2caf","observation_id":"8053ca23-0254-4312-bc08-6ecbb0203fb3","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2408.05154","last_updated":"2024-11-06T19:10:26Z","snapshot_observed_at":"2026-07-06T18:58:56.504337Z","submitted_at":"2024-08-09T16:18:13Z","title":"On the electron self-energy to three loops in QED","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2408.05154","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":null,"venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":84,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/2408.05154","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:c142968969d0dec4f39c912bbd1659b1dc6d6250918a14392efe54b30d488808","observation_id":"7e718962-8de8-4184-ba70-aba992d87850","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","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":"2026-07-12T02:47:06.419343Z","title":"Forner, C","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":85,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:92f5563e72250baa53cf97b4d5eb94a8f6f2f0ae593a8d2a87061f3cde0e7b38","observation_id":"5a99ac49-ef6f-4550-bf7f-3f179ec09e5c","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2411.11846","last_updated":"2025-03-19T13:39:55Z","snapshot_observed_at":"2026-07-06T19:52:07.342252Z","submitted_at":"2024-11-18T18:59:58Z","title":"Emergence of Calabi-Yau manifolds in high-precision black hole scattering","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2411.11846","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":"Driesseet al., Nature641, 603 (2025), arXiv:2411.11846","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":86,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/2411.11846","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:412637cfe0c12ffb331fed22e7d477f3532c08f7915d9066d24a8819a31949e2","observation_id":"581118bf-f011-4364-99c1-c919cc70d59f","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2503.20655","last_updated":"2025-03-26T15:52:08Z","snapshot_observed_at":"2026-07-06T20:59:04.804570Z","submitted_at":"2025-03-26T15:52:08Z","title":"Aspects of canonical differential equations for Calabi-Yau geometries and beyond","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2503.20655","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":"Duhret al., JHEP06, 128 (2025), arXiv:2503.20655","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":87,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/2503.20655","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:123fd4f1350ac2fb1a298515d9feebed0e50027b9cd08e73a1b9eebbf468bd39","observation_id":"95bccd69-7c39-4a48-bb94-49e46f717a22","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2512.13794","last_updated":"2026-05-11T15:09:48Z","snapshot_observed_at":"2026-07-06T22:39:04.164003Z","submitted_at":"2025-12-15T19:00:02Z","title":"The spectrum of Feynman-integral geometries at two loops","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2512.13794","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":"Bargielaet al., JHEP05, 057 (2026), arXiv:2512.13794","venue":null,"work_id":null,"year":2026},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":88,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/2512.13794","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:21ccb9cd32b99a1c490eecaf0a1bd9f3b15d80c116b6ac37c456c2a654e91026","observation_id":"6e3189ca-75da-4dab-8787-28b33b1505d1","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","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":"2026-07-12T02:47:06.419343Z","title":"Brammer, H","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":89,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:4f962224af8312bda12195f4e3610e7db502876dcc42358d5e9c7102526f53de","observation_id":"a5062695-ba26-4e12-8030-5d097a94fa0f","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","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":"2026-07-12T02:47:06.419343Z","title":"Lellouch, A","venue":null,"work_id":null,"year":2026},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":90,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:1253cd9bcd89b0a82967a53be3b5f19d7f464937529dc4fe344d9979cb6a8ffd","observation_id":"8c2521d9-060b-4b3a-89cb-56aa7f84d9a5","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","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":"2026-07-12T02:47:06.419343Z","title":"Duhret al., Canonical differential equations beyond polylogs, 2026, arXiv:2602.04371","venue":null,"work_id":null,"year":2026},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":91,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:6022577584ce72abafd5b9adc487a7adbb5fecc0089e627ce11360c72976e9c0","observation_id":"0454bad5-4728-4c44-b1c6-ddee73a170d7","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2605.07729","last_updated":"2026-05-08T13:35:27Z","snapshot_observed_at":"2026-07-06T23:20:06.574823Z","submitted_at":"2026-05-08T13:35:27Z","title":"Genus drop involving non-hyperelliptic curves in Feynman integrals","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2605.07729","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":null,"venue":null,"work_id":null,"year":2026},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":92,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/2605.07729","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:c8e89e393b10787085e04078a97e6e4a7485b4bf30cd9d9a31e2f00238c61443","observation_id":"91c89d44-626b-4ecd-8d91-2b0cdf1bec32","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2305.14090","last_updated":"2023-05-23T14:14:59Z","snapshot_observed_at":"2026-07-06T15:31:28.888752Z","submitted_at":"2023-05-23T14:14:59Z","title":"On a procedure to derive $\\epsilon$-factorised differential equations beyond polylogarithms","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2305.14090","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":"Görges, C","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":93,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/2305.14090","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:74f1f9c9e65b61008e9e31058294dc5396f95e5d49a85becf56927b3cd9d2f13","observation_id":"f2e4494f-e41e-45e2-9192-35c8532a70bc","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","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":"2026-07-12T02:47:06.419343Z","title":null,"venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":94,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:6c44e1c18b089edd7bcc3c29a7adb657f84b8bee8f18000fbbaf04769f2bdddd","observation_id":"379bef85-16a5-4fc0-a948-ca8ba57c4751","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2412.12057","last_updated":"2025-04-06T20:54:34Z","snapshot_observed_at":"2026-08-03T14:57:12.178790Z","submitted_at":"2024-12-16T18:32:32Z","title":"Calabi-Yau Feynman integrals in gravity: $\\varepsilon$-factorized form for apparent singularities","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2412.12057","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":"Frellesvig, R","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":95,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/2412.12057","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:df6906fb7098281a4b32e262c7a302a961d10d8156d1d57b8180fe5abe77b992","observation_id":"cc785087-3dd3-4845-9c98-a9a7ce0e7cb6","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","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":"2026-07-12T02:47:06.419343Z","title":"Pögel, T","venue":null,"work_id":null,"year":2026},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":96,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:acea188d72e0e76943b5aaed8c08b399cde18b50f695cbd1c06ea56dc0afbf82","observation_id":"9278bcd8-cc33-4fe7-a43a-6f203a09fb84","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2305.13951","last_updated":"2023-09-11T07:53:17Z","snapshot_observed_at":"2026-07-06T15:31:23.076745Z","submitted_at":"2023-05-23T11:25:49Z","title":"$\\varepsilon$-factorized differential equations for two-loop non-planar triangle Feynman integrals with elliptic curves","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2305.13951","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":"Jiang, X","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":97,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/2305.13951","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:ab648b1485dd4aef42c94d0dd2b1980fdcf76fb7d99461610fb6e0558c7f33e4","observation_id":"e58be786-07dd-435e-943d-4d8404eea1ca","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1807.00842","last_updated":"2018-07-02T18:02:51Z","snapshot_observed_at":"2026-07-06T06:48:01.186635Z","submitted_at":"2018-07-02T18:02:51Z","title":"From modular forms to differential equations for Feynman integrals","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1807.00842","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":"Broedel, C","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":98,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/1807.00842","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:a9456ed630788b4bebb6145fff501648970ca288f615603004049cfb71a0722f","observation_id":"e08b1d32-6388-4803-af22-e54b8821a199","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2407.08799","last_updated":"2025-06-24T14:07:00Z","snapshot_observed_at":"2026-07-06T18:45:01.801741Z","submitted_at":"2024-07-11T18:18:23Z","title":"Self-dualities and Galois symmetries in Feynman integrals","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2407.08799","snapshot_observed_at":"2026-07-12T02:47:06.419343Z","title":"Pögel, X","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":99,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"cited_paper":"/paper/2407.08799","citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:f6af947a64169d646df428abc92da358674d38603294a14a6eaf4f764e7de759","observation_id":"eb8a5baa-23c7-4b11-97ff-430d88b5efac","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","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":"2026-07-12T02:47:06.419343Z","title":null,"venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks","version":1},"reference_index":100,"source":"pdf_text","source_observed_at":"2026-07-12T02:47:06.419343Z"},"links":{"citing_paper":"/paper/2607.03398"},"observation_digest":"sha256:d2ece58651afd5c4766b88a9e90d41c0372eb778600c65b583ad10851577156e","observation_id":"5d587c6f-b735-4a92-98a9-6be5587cd56f","resolution":{"observed_at":"2026-07-12T02:47:06.419343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"paper":{"arxiv_id":"2607.03398","last_updated":"2026-07-03T14:59:14Z","latest_version":1,"primary_category":"hep-ph","snapshot_observed_at":"2026-07-12T02:47:05.735748Z","submitted_at":"2026-07-03T14:59:14Z","title":"Analytic result of a three-loop integral family in the Higgs decay to four massive bottom quarks"},"reference_resolution":{"displayed":100,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":100,"verified_exact":0,"verified_fuzzy":0},"total_outbound_references":100},"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":"2026-08-05T06:32:48.257954+00:00","source":"crossref"},{"observed_at":"2026-08-05T06:32:44.755628+00:00","source":"retraction_watch"}],"thesis":"As of 5 August 2026, this Paper Citation Record lists 100 of 100 outbound references and 0 inbound Pith citation observations for arXiv:2607.03398."}