{"as_of":"2026-08-09T15:51:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:a4a812add217b34365d0eb8e45074c6bd46c4af4dc8be3eb2c2c814075c2c5cf","coverage":[{"denominator":68,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":68,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-06T18:22:28.672073Z","state":"measured"},{"denominator":72,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":72,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-09T06:31:02.800959+00:00","state":"measured"},{"denominator":4,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":4,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-03T16:10:28.675624Z","state":"measured"},{"denominator":1,"lane":"external_citation_measurements","note":"A source-named dated measurement, never combined with another source.","records_observed":0,"source":"arxiv_reference","source_observed_at":"2026-07-04T20:30:07.477339Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2507.08558","snapshot_observed_at":"2026-08-03T16:10:28.675624Z","title":"Alioli, G","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2512.14823","last_updated":"2025-12-16T19:00:03Z","snapshot_observed_at":"2026-08-05T11:25:37.210778Z","submitted_at":"2025-12-16T19:00:03Z","title":"Higgs-Pair Production via Gluon Fusion: Top-Yukawa- and light-quark-induced electroweak Corrections","version":1},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-08-03T16:10:28.675624Z"},"links":{"cited_paper":"/paper/2507.08558","citing_paper":"/paper/2512.14823"},"observation_digest":"sha256:0afdec190994c0984358ebdf5bd10974d960f6e1198ff7e52994dd96312fbeb7","observation_id":"fb4f2253-7539-4df6-8b12-363b18e29785","resolution":{"observed_at":"2026-08-03T16:10:28.675624Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2507.08558","snapshot_observed_at":"2026-08-03T07:40:49.921974Z","title":"Alioli, G","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2601.19990","last_updated":"2026-06-03T14:31:23Z","snapshot_observed_at":"2026-08-03T07:40:44.788844Z","submitted_at":"2026-01-27T19:00:21Z","title":"Fully differential Higgs boson pair production at N$^3$LO with top quark mass effects","version":2},"reference_index":48,"source":"pdf_text","source_observed_at":"2026-08-03T07:40:49.921974Z"},"links":{"cited_paper":"/paper/2507.08558","citing_paper":"/paper/2601.19990"},"observation_digest":"sha256:206b8f50684f6144ab216b40dede1b99ec97f0779fc9c9679f82a64f3d1b37ce","observation_id":"4d16b6a2-c6ed-42ec-89d0-4b9aa10baf5a","resolution":{"observed_at":"2026-08-03T07:40:49.921974Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"cited_work":{"arxiv_id":"2507.08558","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2507.08558","snapshot_observed_at":"2026-07-04T20:30:07.477339Z","title":"Alioli, G","venue":null,"work_id":"8e927bc5-b935-44b2-8cd5-29e092be615f","year":2025},"citing_paper":{"arxiv_id":"2606.05300","last_updated":"2026-06-03T18:00:11Z","snapshot_observed_at":"2026-08-05T13:55:53.309449Z","submitted_at":"2026-06-03T18:00:11Z","title":"NNLO+PS Higgs-pair production in MiNNLOPS","version":1},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-06-28T05:20:44.481989Z"},"links":{"cited_paper":"/paper/2507.08558","citing_paper":"/paper/2606.05300"},"observation_digest":"sha256:fbbdfb90b9994390f4afb8a7d44d6a656d5ee3f30f1429f9a783e9e0e1bfb9cf","observation_id":"bd4f7742-2356-43df-a2fc-a8038778e026","resolution":{"observed_at":"2026-07-02T09:56:51.792992Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"cited_work":{"arxiv_id":"2507.08558","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2507.08558","snapshot_observed_at":"2026-07-04T20:30:07.477339Z","title":"Alioli, G","venue":null,"work_id":"8e927bc5-b935-44b2-8cd5-29e092be615f","year":2025},"citing_paper":{"arxiv_id":"2606.25928","last_updated":"2026-06-24T15:06:24Z","snapshot_observed_at":"2026-08-05T11:23:26.823743Z","submitted_at":"2026-06-24T15:06:24Z","title":"Electroweak corrections to Higgs boson pair production: The quark channel","version":1},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-06-25T20:07:31.995758Z"},"links":{"cited_paper":"/paper/2507.08558","citing_paper":"/paper/2606.25928"},"observation_digest":"sha256:a843085c4edca8df4c501c2b774efc35b358622519173a210ea4e29a2b4fec7a","observation_id":"05e600bd-a30d-4774-bb1a-a6e020ca92db","resolution":{"observed_at":"2026-07-04T20:30:07.478734Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}}],"links":{"evidence":"/evidence","html":"/paper/2507.08558/citation-record","integrity":"/paper/2507.08558/integrity","json":"/paper/2507.08558/citation-record.json","paper":"/paper/2507.08558"},"outbound":[{"citation":{"cited_paper":{"arxiv_id":"2002.06398","last_updated":"2020-04-21T17:51:35Z","snapshot_observed_at":"2026-07-06T08:57:32.293614Z","submitted_at":"2020-02-15T15:30:34Z","title":"A measurement of the Higgs boson mass in the diphoton decay channel","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2002.06398","snapshot_observed_at":"2026-08-06T18:22:24.369080Z","title":null,"venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-08-06T18:22:24.369080Z"},"links":{"cited_paper":"/paper/2002.06398","citing_paper":"/paper/2507.08558"},"observation_digest":"sha256:eb3e80198ef906897d1679d315845cc39a6b9de3c9f1152807509cbe889e3442","observation_id":"ee6bae0f-4969-4345-a4db-396f7db0a60c","resolution":{"observed_at":"2026-08-06T18:22:24.369080Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2308.07216","last_updated":"2023-12-14T17:25:14Z","snapshot_observed_at":"2026-07-06T16:06:02.777393Z","submitted_at":"2023-08-14T15:37:43Z","title":"Measurement of the Higgs boson mass with $H \\rightarrow \\gamma\\gamma$ decays in 140 fb$^{-1}$ of $\\sqrt{s}=13$ TeV $pp$ collisions with the ATLAS detector","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2308.07216","snapshot_observed_at":"2026-08-06T18:22:24.456461Z","title":null,"venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-08-06T18:22:24.456461Z"},"links":{"cited_paper":"/paper/2308.07216","citing_paper":"/paper/2507.08558"},"observation_digest":"sha256:96be84af69bbb25610d01eccaea1d0f7a482a7e05704841444e10b3a26d84b9a","observation_id":"0bf3e6ea-1a75-40ab-8eb5-c897c68b49b4","resolution":{"observed_at":"2026-08-06T18:22:24.456461Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1506.05669","last_updated":"2015-10-23T14:12:14Z","snapshot_observed_at":"2026-08-01T21:12:56.784743Z","submitted_at":"2015-06-18T13:25:31Z","title":"Study of the spin and parity of the Higgs boson in diboson decays with the ATLAS detector","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1506.05669","snapshot_observed_at":"2026-08-06T18:22:24.506256Z","title":null,"venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-08-06T18:22:24.506256Z"},"links":{"cited_paper":"/paper/1506.05669","citing_paper":"/paper/2507.08558"},"observation_digest":"sha256:1a1ca257451b48ec6d6d8dedbd7ba618d312e42ef2d99cacbf647d8a728bbf16","observation_id":"1bfdc165-ed40-4f09-bfa7-e02c6e4ece1f","resolution":{"observed_at":"2026-08-06T18:22:24.506256Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2406.09971","last_updated":"2024-09-06T14:48:33Z","snapshot_observed_at":"2026-08-09T03:39:19.221409Z","submitted_at":"2024-06-14T12:30:11Z","title":"Combination of searches for Higgs boson pair production in $pp$ collisions at $\\sqrt{s}=13$ TeV with the ATLAS detector","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2406.09971","snapshot_observed_at":"2026-08-06T18:22:24.556897Z","title":null,"venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-06T18:22:24.556897Z"},"links":{"cited_paper":"/paper/2406.09971","citing_paper":"/paper/2507.08558"},"observation_digest":"sha256:c17c05392cbb03c949efd76c3b7fef80fb49aff0ebcd8ba2f56b0f83ebd78bae","observation_id":"57fd231c-908d-4b0d-bbc0-2e24308128e0","resolution":{"observed_at":"2026-08-06T18:22:24.556897Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-06T18:22:31.110833Z","title":null,"venue":null,"work_id":"8ae95a17-e838-4d56-b925-9a8a9d50ab18","year":1988},"citing_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-08-06T18:22:24.654908Z"},"links":{"citing_paper":"/paper/2507.08558"},"observation_digest":"sha256:fb002015c0ca751b2831cf04e6a914f6e91bccab3643c8f0646d26cf55666606","observation_id":"2661c3c0-9e82-4361-96c8-9e1718102799","resolution":{"observed_at":"2026-08-06T18:22:31.232175Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-06T18:22:31.015737Z","title":null,"venue":null,"work_id":"2d2cde95-dbfa-4cb3-99bb-745d2b1ce712","year":1987},"citing_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-06T18:22:24.692658Z"},"links":{"citing_paper":"/paper/2507.08558"},"observation_digest":"sha256:f0c24d387d6f12556c64d5c9f6a8093fa7a80c3631e73dd9b3e0fd02e44b149e","observation_id":"7be1df5d-1bfe-4c3a-bbc3-af3def8f7e97","resolution":{"observed_at":"2026-08-06T18:22:31.034034Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9603205","last_updated":"1996-03-01T14:52:47Z","snapshot_observed_at":"2026-07-07T04:22:04.686235Z","submitted_at":"1996-03-01T14:52:47Z","title":"Pair Production of Neutral Higgs Particles in Gluon--Gluon Collisions","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9603205","snapshot_observed_at":"2026-08-06T18:22:24.768547Z","title":"Plehn, M","venue":null,"work_id":null,"year":1996},"citing_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-06T18:22:24.768547Z"},"links":{"cited_paper":"/paper/hep-ph/9603205","citing_paper":"/paper/2507.08558"},"observation_digest":"sha256:52351ed9562993c2bc2ab298c729410b49b6cea825db7bc6c4fafdd66d69926b","observation_id":"3cd0a6a6-0bb0-4110-80f9-96e5d1156e31","resolution":{"observed_at":"2026-08-06T18:22:24.768547Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1305.5206","last_updated":"2013-06-21T14:00:20Z","snapshot_observed_at":"2026-07-06T03:13:58.490499Z","submitted_at":"2013-05-22T17:40:28Z","title":"Two-loop virtual corrections to Higgs pair production","version":2},"cited_work":{"arxiv_id":"1305.5206","doi":null,"metadata_source":"pith","pith_arxiv_id":"1305.5206","snapshot_observed_at":"2026-08-06T18:22:30.554128Z","title":"Two-loop virtual corrections to Higgs pair production","venue":"hep-ph","work_id":"eadd7d6f-18a2-4abf-aa0c-f3fe7176c966","year":2013},"citing_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-06T18:22:24.835097Z"},"links":{"cited_paper":"/paper/1305.5206","citing_paper":"/paper/2507.08558"},"observation_digest":"sha256:ec0c7753fed7d474d689c47a76d7172a8feb78d993cf4e7682773bf1ecd89234","observation_id":"f9becdfc-5a75-4cb5-8b51-7467f47e73fb","resolution":{"observed_at":"2026-08-06T18:22:30.668193Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1606.09519","last_updated":"2016-06-30T14:48:22Z","snapshot_observed_at":"2026-08-05T11:25:39.992209Z","submitted_at":"2016-06-30T14:48:22Z","title":"Differential Higgs Boson Pair Production at Next-to-Next-to-Leading Order in QCD","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1606.09519","snapshot_observed_at":"2026-08-06T18:22:24.869271Z","title":"de Florian, M","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-06T18:22:24.869271Z"},"links":{"cited_paper":"/paper/1606.09519","citing_paper":"/paper/2507.08558"},"observation_digest":"sha256:2212700e6da78631d682e4286fd3da08bff4d4168c5405587ce948e919875e1d","observation_id":"3f01a593-2232-4fe5-abf6-10c9afe736e7","resolution":{"observed_at":"2026-08-06T18:22:24.869271Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1909.06808","last_updated":"2020-03-02T01:29:36Z","snapshot_observed_at":"2026-08-06T09:54:18.879405Z","submitted_at":"2019-09-15T14:14:33Z","title":"Higgs boson pair production via gluon fusion at N$^3$LO in QCD","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1909.06808","snapshot_observed_at":"2026-08-06T18:22:24.924499Z","title":null,"venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-06T18:22:24.924499Z"},"links":{"cited_paper":"/paper/1909.06808","citing_paper":"/paper/2507.08558"},"observation_digest":"sha256:b8b8107800d351a2328d968e550a82a8ff8279c13dc9833bc3bc17474c3ab465","observation_id":"449c7e6f-889e-4a7a-bdc0-07ab02a565de","resolution":{"observed_at":"2026-08-06T18:22:24.924499Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1604.06447","last_updated":"2016-08-01T16:52:49Z","snapshot_observed_at":"2026-07-06T04:53:41.754642Z","submitted_at":"2016-04-21T19:57:25Z","title":"Higgs boson pair production in gluon fusion at NLO with full top-quark mass dependence","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1604.06447","snapshot_observed_at":"2026-08-06T18:22:24.996250Z","title":"Borowka, N","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-08-06T18:22:24.996250Z"},"links":{"cited_paper":"/paper/1604.06447","citing_paper":"/paper/2507.08558"},"observation_digest":"sha256:a85d1b45b84e007777ac738dff699b545e79f3072f199e2d57e1a26cada61c1c","observation_id":"95c1a3db-9cab-4803-a3e9-e9a76c91d85f","resolution":{"observed_at":"2026-08-06T18:22:24.996250Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1608.04798","last_updated":"2016-08-16T22:30:01Z","snapshot_observed_at":"2026-08-06T22:40:50.047078Z","submitted_at":"2016-08-16T22:30:01Z","title":"Full top quark mass dependence in Higgs boson pair production at NLO","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1608.04798","snapshot_observed_at":"2026-08-06T18:22:25.044177Z","title":"Borowka, N","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-08-06T18:22:25.044177Z"},"links":{"cited_paper":"/paper/1608.04798","citing_paper":"/paper/2507.08558"},"observation_digest":"sha256:f18350f53075cd076b098554133af664f4db68a2102657a874239cc2f5639795","observation_id":"e314b20a-5047-427b-a663-7c9bea96f50f","resolution":{"observed_at":"2026-08-06T18:22:25.044177Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2407.04653","last_updated":"2024-11-15T14:18:23Z","snapshot_observed_at":"2026-07-06T18:42:05.670928Z","submitted_at":"2024-07-05T17:08:59Z","title":"Electroweak corrections to Higgs boson pair production: The top-Yukawa and self-coupling contributions","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2407.04653","snapshot_observed_at":"2026-08-06T18:22:25.140044Z","title":"Heinrich, S","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-06T18:22:25.140044Z"},"links":{"cited_paper":"/paper/2407.04653","citing_paper":"/paper/2507.08558"},"observation_digest":"sha256:778ed87600ea497f1863b769564b2f11c66645c4a5381c7f34dcb3c1c97dc9e8","observation_id":"da5d8997-81b8-44c3-a103-1438d02308b9","resolution":{"observed_at":"2026-08-06T18:22:25.140044Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2503.16620","last_updated":"2025-06-02T09:23:17Z","snapshot_observed_at":"2026-08-07T16:48:16.671305Z","submitted_at":"2025-03-20T18:21:50Z","title":"Two-loop light-quark Electroweak corrections to Higgs boson pair production in gluon fusion","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2503.16620","snapshot_observed_at":"2026-08-06T18:22:25.183459Z","title":"Bonetti, P","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-06T18:22:25.183459Z"},"links":{"cited_paper":"/paper/2503.16620","citing_paper":"/paper/2507.08558"},"observation_digest":"sha256:cc5def6d1787ced3116582049965ca1cea71be893ba73beb0211581989abed5c","observation_id":"b65d95c3-4855-4690-b1c8-ed8be157a780","resolution":{"observed_at":"2026-08-06T18:22:25.183459Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1305.7340","last_updated":"2013-05-31T09:38:11Z","snapshot_observed_at":"2026-07-06T03:14:46.161042Z","submitted_at":"2013-05-31T09:38:11Z","title":"On the Higgs boson pair production at the LHC","version":1},"cited_work":{"arxiv_id":"1305.7340","doi":null,"metadata_source":"pith","pith_arxiv_id":"1305.7340","snapshot_observed_at":"2026-08-06T18:22:30.417782Z","title":"On the Higgs boson pair production at the LHC","venue":"hep-ph","work_id":"36adae32-6b3b-490f-a483-6fed662755ea","year":2013},"citing_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-08-06T18:22:25.218589Z"},"links":{"cited_paper":"/paper/1305.7340","citing_paper":"/paper/2507.08558"},"observation_digest":"sha256:b815afabff2b6e021e7c6df22847d289112dbc3c7ead79c4b187a84d78d80994","observation_id":"59a9a20b-b6d0-4291-b581-f8cf51b43df3","resolution":{"observed_at":"2026-08-06T18:22:30.466483Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1408.2422","last_updated":"2014-08-11T14:33:45Z","snapshot_observed_at":"2026-07-06T03:51:25.839395Z","submitted_at":"2014-08-11T14:33:45Z","title":"Virtual corrections to Higgs boson pair production in the large top quark mass limit","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1408.2422","snapshot_observed_at":"2026-08-06T18:22:25.284280Z","title":"Grigo, K","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-08-06T18:22:25.284280Z"},"links":{"cited_paper":"/paper/1408.2422","citing_paper":"/paper/2507.08558"},"observation_digest":"sha256:dafa3f91e614e074258b0b3fff603aec88e08cf5148f055bcab0527c7ccfcf80","observation_id":"c1788b97-102c-4c6b-97db-db4cf689926b","resolution":{"observed_at":"2026-08-06T18:22:25.284280Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1508.00909","last_updated":"2015-08-04T20:17:19Z","snapshot_observed_at":"2026-07-06T04:25:49.911940Z","submitted_at":"2015-08-04T20:17:19Z","title":"Higgs boson pair production: top quark mass effects at NLO and NNLO","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1508.00909","snapshot_observed_at":"2026-08-06T18:22:25.349888Z","title":"Grigo, J","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-08-06T18:22:25.349888Z"},"links":{"cited_paper":"/paper/1508.00909","citing_paper":"/paper/2507.08558"},"observation_digest":"sha256:ba06e1c92b03e6c830dadc8ba7f0e36309da0e05e129f653111f73908758551c","observation_id":"03410a85-36a6-4f3d-aa99-de82af4fcd8e","resolution":{"observed_at":"2026-08-06T18:22:25.349888Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1401.7340","last_updated":"2014-03-20T16:48:43Z","snapshot_observed_at":"2026-07-06T03:34:35.165632Z","submitted_at":"2014-01-28T21:05:23Z","title":"Higgs pair production at the LHC with NLO and parton-shower effects","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1401.7340","snapshot_observed_at":"2026-08-06T18:22:25.424769Z","title":"Frederix, S","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-08-06T18:22:25.424769Z"},"links":{"cited_paper":"/paper/1401.7340","citing_paper":"/paper/2507.08558"},"observation_digest":"sha256:7670220d32abaf32579a28b2229ff41520459aacd9c9ae0d416acf3d4f4bb8b9","observation_id":"ca0a6e7c-fa90-4f4b-89a8-05675e83e208","resolution":{"observed_at":"2026-08-06T18:22:25.424769Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1408.6542","last_updated":"2014-08-27T20:01:00Z","snapshot_observed_at":"2026-07-06T03:52:48.428145Z","submitted_at":"2014-08-27T20:01:00Z","title":"Top-quark mass effects in double and triple Higgs production in gluon-gluon fusion at NLO","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1408.6542","snapshot_observed_at":"2026-08-06T18:22:25.497688Z","title":"Maltoni, E","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-08-06T18:22:25.497688Z"},"links":{"cited_paper":"/paper/1408.6542","citing_paper":"/paper/2507.08558"},"observation_digest":"sha256:dfad69727ddcedaf70972b34feeb38acf37626d5425a369dc36eea6354d31fb8","observation_id":"4903b297-75df-46dc-a458-7347fe3fea47","resolution":{"observed_at":"2026-08-06T18:22:25.497688Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1401.0007","last_updated":"2014-08-13T15:41:16Z","snapshot_observed_at":"2026-07-06T03:32:13.149972Z","submitted_at":"2013-12-30T21:00:03Z","title":"Higgs Boson pair production merged to one jet","version":2},"cited_work":{"arxiv_id":"1401.0007","doi":null,"metadata_source":"pith","pith_arxiv_id":"1401.0007","snapshot_observed_at":"2026-08-06T18:22:30.216450Z","title":"Higgs Boson pair production merged to one jet","venue":"hep-ph","work_id":"107a6adf-50a1-4e97-910e-aafe30953018","year":2013},"citing_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-08-06T18:22:25.562148Z"},"links":{"cited_paper":"/paper/1401.0007","citing_paper":"/paper/2507.08558"},"observation_digest":"sha256:500444ae7afac0018e913273c6ea36566378e15973dc68d5c9ad0aa68cd16bd0","observation_id":"9a50b587-5bce-49e0-9457-58c866afb93d","resolution":{"observed_at":"2026-08-06T18:22:30.253620Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1703.09252","last_updated":"2017-12-04T17:53:56Z","snapshot_observed_at":"2026-07-06T05:35:24.598806Z","submitted_at":"2017-03-27T18:25:55Z","title":"NLO predictions for Higgs boson pair production with full top quark mass dependence matched to parton showers","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1703.09252","snapshot_observed_at":"2026-08-06T18:22:25.617161Z","title":"Heinrich, S","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-08-06T18:22:25.617161Z"},"links":{"cited_paper":"/paper/1703.09252","citing_paper":"/paper/2507.08558"},"observation_digest":"sha256:dca35da01b20220c24e8aba17d43756f00ea2753d672a1a71d482c29765f4986","observation_id":"bbff63ee-0bbb-4904-81a7-7366cd12c8fe","resolution":{"observed_at":"2026-08-06T18:22:25.617161Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1903.08137","last_updated":"2019-06-24T17:28:52Z","snapshot_observed_at":"2026-08-04T03:55:17.714440Z","submitted_at":"2019-03-19T17:48:02Z","title":"Probing the trilinear Higgs boson coupling in di-Higgs production at NLO QCD including parton shower effects","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1903.08137","snapshot_observed_at":"2026-08-06T18:22:25.696341Z","title":"Heinrich, S","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-08-06T18:22:25.696341Z"},"links":{"cited_paper":"/paper/1903.08137","citing_paper":"/paper/2507.08558"},"observation_digest":"sha256:063198e374b599fe193f41b6ebd74caa1c2e9deb06415011afb827e3372e2840","observation_id":"1b887280-27ef-49e0-826c-81735228d116","resolution":{"observed_at":"2026-08-06T18:22:25.696341Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1711.03319","last_updated":"2018-02-21T02:12:47Z","snapshot_observed_at":"2026-08-07T05:05:00.356264Z","submitted_at":"2017-11-09T11:01:14Z","title":"Parton Shower and NLO-Matching uncertainties in Higgs Boson Pair Production","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1711.03319","snapshot_observed_at":"2026-08-06T18:22:25.776845Z","title":"Jones and S","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-08-06T18:22:25.776845Z"},"links":{"cited_paper":"/paper/1711.03319","citing_paper":"/paper/2507.08558"},"observation_digest":"sha256:6133f3291e4d4be53c62389e08429b941a1f5f1e228b74d8cb1753a9f7c3b861","observation_id":"d52df6a8-c36f-4ac0-8c63-0fe884b3e59a","resolution":{"observed_at":"2026-08-06T18:22:25.776845Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2212.10489","last_updated":"2023-06-30T12:42:21Z","snapshot_observed_at":"2026-07-06T14:33:08.041820Z","submitted_at":"2022-12-20T18:05:06Z","title":"Double Higgs production at NNLO interfaced to parton showers in GENEVA","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2212.10489","snapshot_observed_at":"2026-08-06T18:22:25.840997Z","title":"Alioli, G","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-08-06T18:22:25.840997Z"},"links":{"cited_paper":"/paper/2212.10489","citing_paper":"/paper/2507.08558"},"observation_digest":"sha256:d1b2624d474de6b1c8c44cf86e91d31218413e6fa22542548cbfd169644b88d3","observation_id":"69fad1c7-80b7-4b44-b01d-42cba1d30c15","resolution":{"observed_at":"2026-08-06T18:22:25.840997Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2405.20372","last_updated":"2024-05-30T18:00:01Z","snapshot_observed_at":"2026-07-06T18:22:57.400982Z","submitted_at":"2024-05-30T18:00:01Z","title":"Three-loop corrections to Higgs boson pair production: reducible contribution","version":1},"cited_work":{"arxiv_id":"2405.20372","doi":null,"metadata_source":"pith","pith_arxiv_id":"2405.20372","snapshot_observed_at":"2026-08-06T18:22:30.053652Z","title":"Three-loop corrections to Higgs boson pair production: reducible contribution","venue":"hep-ph","work_id":"5473f87e-ee22-439f-841f-3bbd257a611f","year":2024},"citing_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-08-06T18:22:25.918816Z"},"links":{"cited_paper":"/paper/2405.20372","citing_paper":"/paper/2507.08558"},"observation_digest":"sha256:ea6fd0b5777a081134ede3e9f98d1da24a1f3144e8d70a3c2c5734119a1656f1","observation_id":"acf5b347-8b59-4775-8f05-82b911dbe4a0","resolution":{"observed_at":"2026-08-06T18:22:30.113933Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2503.10051","last_updated":"2025-08-18T06:36:16Z","snapshot_observed_at":"2026-08-07T17:08:08.002532Z","submitted_at":"2025-03-13T05:08:34Z","title":"$gg\\rightarrow HH$ amplitude induced by bottom quarks at two-loop level: planar master integrals","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2503.10051","snapshot_observed_at":"2026-08-06T18:22:25.980973Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-08-06T18:22:25.980973Z"},"links":{"cited_paper":"/paper/2503.10051","citing_paper":"/paper/2507.08558"},"observation_digest":"sha256:ed67c78d53ef9a43be297df91f6626c2c05a4749fce953324309a016115a8ad7","observation_id":"fe6be75b-51d4-4d3f-b910-f17901f3c0ac","resolution":{"observed_at":"2026-08-06T18:22:25.980973Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2503.17449","last_updated":"2025-03-21T18:00:05Z","snapshot_observed_at":"2026-08-08T04:54:47.408632Z","submitted_at":"2025-03-21T18:00:05Z","title":"Three-loop large-$N_c$ virtual corrections to $gg\\to HH$ in the forward limit","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2503.17449","snapshot_observed_at":"2026-08-06T18:22:26.060338Z","title":"Davies, K","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-08-06T18:22:26.060338Z"},"links":{"cited_paper":"/paper/2503.17449","citing_paper":"/paper/2507.08558"},"observation_digest":"sha256:9175f2ac62a5d6fdf1cd7a986e61389ac95e7965a5e8ce6c144b92597ca31646","observation_id":"72e5a44c-8ae7-4787-a894-2fcae460c093","resolution":{"observed_at":"2026-08-06T18:22:26.060338Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1807.03704","last_updated":"2018-07-10T15:22:24Z","snapshot_observed_at":"2026-08-02T01:56:06.874800Z","submitted_at":"2018-07-10T15:22:24Z","title":"Soft gluon resummation for Higgs boson pair production including finite Mt effects","version":1},"cited_work":{"arxiv_id":"1807.03704","doi":null,"metadata_source":"pith","pith_arxiv_id":"1807.03704","snapshot_observed_at":"2026-08-06T18:22:29.943984Z","title":"Soft gluon resummation for Higgs boson pair production including finite Mt effects","venue":"hep-ph","work_id":"6fb16f13-ddb5-4014-acfb-8c33ab3ff49c","year":2018},"citing_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-08-06T18:22:26.132024Z"},"links":{"cited_paper":"/paper/1807.03704","citing_paper":"/paper/2507.08558"},"observation_digest":"sha256:466a2901e37c2135303b7d2c191f4f04b0ce6c6674b64fb581895f028e82619e","observation_id":"995145b9-aaaf-46b3-862b-4a91e260f1c7","resolution":{"observed_at":"2026-08-06T18:22:29.973991Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1803.02463","last_updated":"2018-03-06T22:59:04Z","snapshot_observed_at":"2026-08-06T21:51:14.939387Z","submitted_at":"2018-03-06T22:59:04Z","title":"Higgs boson pair production at NNLO with top quark mass effects","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1803.02463","snapshot_observed_at":"2026-08-06T18:22:26.189262Z","title":"Grazzini, G","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"reference_index":29,"source":"pdf_text","source_observed_at":"2026-08-06T18:22:26.189262Z"},"links":{"cited_paper":"/paper/1803.02463","citing_paper":"/paper/2507.08558"},"observation_digest":"sha256:8120d2fe58d2b9741987a84d050b6596a76fa6cf0a04d9f953e8fda134f9ea7e","observation_id":"f7b2cb46-62c8-4639-8980-510e354d5ef3","resolution":{"observed_at":"2026-08-06T18:22:26.189262Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2304.01968","last_updated":"2024-10-17T17:06:24Z","snapshot_observed_at":"2026-07-06T15:12:11.121128Z","submitted_at":"2023-04-04T17:25:21Z","title":"Effective Field Theory descriptions of Higgs boson pair production","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2304.01968","snapshot_observed_at":"2026-08-06T18:22:26.233201Z","title":"Alasfar et al., Effective Field Theory descriptions of Higgs boson pair production , SciPost Phys","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-08-06T18:22:26.233201Z"},"links":{"cited_paper":"/paper/2304.01968","citing_paper":"/paper/2507.08558"},"observation_digest":"sha256:eead74530e46a5d1a950278a47d0f88e02869967fd91bb8d7cdb810fa1c52c4b","observation_id":"841dfe78-239e-4b6e-ab91-4213c385dfd3","resolution":{"observed_at":"2026-08-06T18:22:26.233201Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2502.20976","last_updated":"2025-08-11T14:19:15Z","snapshot_observed_at":"2026-08-07T17:40:05.280564Z","submitted_at":"2025-02-28T11:41:56Z","title":"Di-Higgs and Effective Field Theory: Signal Reweighting Beyond $m_{hh}$","version":2},"cited_work":{"arxiv_id":"2502.20976","doi":null,"metadata_source":"pith","pith_arxiv_id":"2502.20976","snapshot_observed_at":"2026-08-06T18:22:29.753205Z","title":"Di-Higgs and Effective Field Theory: Signal Reweighting Beyond $m_{hh}$","venue":"hep-ph","work_id":"1cb85237-102c-43dc-849c-10888a3cc4b4","year":2025},"citing_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-08-06T18:22:26.282492Z"},"links":{"cited_paper":"/paper/2502.20976","citing_paper":"/paper/2507.08558"},"observation_digest":"sha256:f961c050e92cdd9e86bd60f7bf37c423150710c2441d0c345588f688eb4d73ac","observation_id":"1538b2f0-be60-4a60-bd56-f4798d099a12","resolution":{"observed_at":"2026-08-06T18:22:29.858524Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2311.16963","last_updated":"2024-06-11T04:32:37Z","snapshot_observed_at":"2026-07-06T16:53:55.269172Z","submitted_at":"2023-11-28T17:10:11Z","title":"Electroweak corrections to double Higgs production at the LHC","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2311.16963","snapshot_observed_at":"2026-08-06T18:22:26.326885Z","title":"Bi, L.-H","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"reference_index":32,"source":"pdf_text","source_observed_at":"2026-08-06T18:22:26.326885Z"},"links":{"cited_paper":"/paper/2311.16963","citing_paper":"/paper/2507.08558"},"observation_digest":"sha256:d14ccd1de4b32a0b16e2077d62622b960ee9926c36cf4c8f71e8cc0792a39c67","observation_id":"f168bfc7-6013-47d2-b12c-ae9791ebfca1","resolution":{"observed_at":"2026-08-06T18:22:26.326885Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2309.10525","last_updated":"2023-09-19T11:10:53Z","snapshot_observed_at":"2026-08-06T17:33:55.197911Z","submitted_at":"2023-09-19T11:10:53Z","title":"Higgs boson pair production at NLO in the POWHEG approach and the top quark mass uncertainties","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2309.10525","snapshot_observed_at":"2026-08-06T18:22:26.377929Z","title":"Bagnaschi, G","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-08-06T18:22:26.377929Z"},"links":{"cited_paper":"/paper/2309.10525","citing_paper":"/paper/2507.08558"},"observation_digest":"sha256:a14c2b612e8164b8fb53713fe608b166eee45a050032a3a9d27a276bbe4350c8","observation_id":"caecabc3-de73-4c65-86dc-93053c841a60","resolution":{"observed_at":"2026-08-06T18:22:26.377929Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1306.4581","last_updated":"2013-09-27T10:17:25Z","snapshot_observed_at":"2026-07-06T03:16:13.248543Z","submitted_at":"2013-06-19T15:29:20Z","title":"Heavy-quark mass effects in Higgs boson production at the LHC","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1306.4581","snapshot_observed_at":"2026-08-06T18:22:26.412001Z","title":"Grazzini and H","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"reference_index":34,"source":"pdf_text","source_observed_at":"2026-08-06T18:22:26.412001Z"},"links":{"cited_paper":"/paper/1306.4581","citing_paper":"/paper/2507.08558"},"observation_digest":"sha256:268069d4c3bf63e9d1ae38b29509e55cff50b41f18201581c4b8bbb591cab810","observation_id":"103b656f-971c-4726-9d37-a807c2ce7291","resolution":{"observed_at":"2026-08-06T18:22:26.412001Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1512.08570","last_updated":"2016-08-07T20:58:06Z","snapshot_observed_at":"2026-08-06T15:56:14.678274Z","submitted_at":"2015-12-29T00:49:20Z","title":"On the computation of finite bottom-quark mass effects in Higgs boson production","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1512.08570","snapshot_observed_at":"2026-08-06T18:22:26.467260Z","title":"Mueller and D","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-08-06T18:22:26.467260Z"},"links":{"cited_paper":"/paper/1512.08570","citing_paper":"/paper/2507.08558"},"observation_digest":"sha256:fdcb5ef803f0cb281c153ac52355c5fd95f935e0c84565088d2e216bd18346bc","observation_id":"efe2597a-12d4-488c-9e74-6fafec55fdb7","resolution":{"observed_at":"2026-08-06T18:22:26.467260Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1504.06577","last_updated":"2015-04-24T17:30:46Z","snapshot_observed_at":"2026-07-06T04:15:59.669933Z","submitted_at":"2015-04-24T17:30:46Z","title":"NLO QCD Corrections to Higgs Pair Production including Dimension-6 Operators","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1504.06577","snapshot_observed_at":"2026-08-06T18:22:26.531018Z","title":"Grober, M","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"reference_index":36,"source":"pdf_text","source_observed_at":"2026-08-06T18:22:26.531018Z"},"links":{"cited_paper":"/paper/1504.06577","citing_paper":"/paper/2507.08558"},"observation_digest":"sha256:ef7db274d3cce7711caa1a3d1f1943ad175e52ec17d4950436d608fe301ad3f3","observation_id":"35875be4-e8e9-4b3f-b70b-a28bdbb47b5c","resolution":{"observed_at":"2026-08-06T18:22:26.531018Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1705.05314","last_updated":"2017-05-15T16:13:49Z","snapshot_observed_at":"2026-07-06T05:42:42.520454Z","submitted_at":"2017-05-15T16:13:49Z","title":"Higgs Pair Production at NLO QCD for CP-violating Higgs Sectors","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1705.05314","snapshot_observed_at":"2026-08-06T18:22:26.554001Z","title":"Grober, M","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"reference_index":37,"source":"pdf_text","source_observed_at":"2026-08-06T18:22:26.554001Z"},"links":{"cited_paper":"/paper/1705.05314","citing_paper":"/paper/2507.08558"},"observation_digest":"sha256:3e358e88e57af70f4ae7d0008b2540edc8e1d50773df1e7ea026cd90afd27f8f","observation_id":"60a01bc3-b582-4d6f-b856-d95a4a03f0fc","resolution":{"observed_at":"2026-08-06T18:22:26.554001Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1704.05700","last_updated":"2017-12-01T14:34:45Z","snapshot_observed_at":"2026-07-06T05:38:22.554675Z","submitted_at":"2017-04-19T11:34:59Z","title":"Higgs boson pair production at NNLO in QCD including dimension 6 operators","version":2},"cited_work":{"arxiv_id":"1704.05700","doi":null,"metadata_source":"pith","pith_arxiv_id":"1704.05700","snapshot_observed_at":"2026-08-06T18:22:29.478654Z","title":"Higgs boson pair production at NNLO in QCD including dimension 6 operators","venue":"hep-ph","work_id":"2f7c78e3-1f8e-4a9f-9b9e-416fe770f017","year":2017},"citing_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"reference_index":38,"source":"pdf_text","source_observed_at":"2026-08-06T18:22:26.612291Z"},"links":{"cited_paper":"/paper/1704.05700","citing_paper":"/paper/2507.08558"},"observation_digest":"sha256:5a15b0fe66900df8eda1ec48ca16133ff2d18c4a8cfdc9991443e34a241f1f7f","observation_id":"50afc091-5c5f-4ebf-b1c7-946aaf37b193","resolution":{"observed_at":"2026-08-06T18:22:29.559937Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1804.07407","last_updated":"2018-08-15T16:10:46Z","snapshot_observed_at":"2026-07-06T06:34:24.166201Z","submitted_at":"2018-04-19T23:44:58Z","title":"NLO QCD corrections to SM-EFT dilepton and electroweak Higgs boson production, matched to parton shower in POWHEG","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1804.07407","snapshot_observed_at":"2026-08-06T18:22:26.668125Z","title":"Alioli, W","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"reference_index":39,"source":"pdf_text","source_observed_at":"2026-08-06T18:22:26.668125Z"},"links":{"cited_paper":"/paper/1804.07407","citing_paper":"/paper/2507.08558"},"observation_digest":"sha256:57b58ec0d8cd729fbe5f7c2dfd03ae9c777b3f4f6e2bc59124e509dcdc1ac931","observation_id":"105ac7d2-fda4-4be4-bc72-6824d85217c2","resolution":{"observed_at":"2026-08-06T18:22:26.668125Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2006.16877","last_updated":"2020-10-13T13:57:37Z","snapshot_observed_at":"2026-07-06T09:34:05.468702Z","submitted_at":"2020-06-30T15:08:38Z","title":"A non-linear EFT description of $gg\\to HH$ at NLO interfaced to POWHEG","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2006.16877","snapshot_observed_at":"2026-08-06T18:22:26.702682Z","title":"Heinrich, S","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"reference_index":40,"source":"pdf_text","source_observed_at":"2026-08-06T18:22:26.702682Z"},"links":{"cited_paper":"/paper/2006.16877","citing_paper":"/paper/2507.08558"},"observation_digest":"sha256:69c9d540b94c610bac72729f174a14886a494b3b6995b2823b73ec171bf8a51a","observation_id":"ee64d44e-95da-429b-bb32-438c62c12945","resolution":{"observed_at":"2026-08-06T18:22:26.702682Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2110.06929","last_updated":"2021-11-12T13:45:00Z","snapshot_observed_at":"2026-07-06T11:57:35.819061Z","submitted_at":"2021-10-13T18:00:00Z","title":"The Impact of Dimension-8 SMEFT Contributions: A Case Study","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2110.06929","snapshot_observed_at":"2026-08-06T18:22:26.765574Z","title":"Dawson, S","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"reference_index":41,"source":"pdf_text","source_observed_at":"2026-08-06T18:22:26.765574Z"},"links":{"cited_paper":"/paper/2110.06929","citing_paper":"/paper/2507.08558"},"observation_digest":"sha256:03c36a417e53c402cafb54de57ba62a753342ab46a974421f39e1017ae461f1f","observation_id":"87bc26be-789b-415e-8d97-e9484f49cdbb","resolution":{"observed_at":"2026-08-06T18:22:26.765574Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2106.14050","last_updated":"2021-09-27T14:39:47Z","snapshot_observed_at":"2026-07-06T11:23:23.417429Z","submitted_at":"2021-06-26T15:51:02Z","title":"Anomalous couplings in Higgs-boson pair production at approximate NNLO QCD","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2106.14050","snapshot_observed_at":"2026-08-06T18:22:26.817318Z","title":"de Florian, I","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"reference_index":42,"source":"pdf_text","source_observed_at":"2026-08-06T18:22:26.817318Z"},"links":{"cited_paper":"/paper/2106.14050","citing_paper":"/paper/2507.08558"},"observation_digest":"sha256:a24594965890f0a157d13980ee671c456eb77772fa695b52585bb5026c7dfa13","observation_id":"b64f8750-11e2-4660-ba6c-90812d45c5e4","resolution":{"observed_at":"2026-08-06T18:22:26.817318Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2204.13045","last_updated":"2023-10-27T07:16:41Z","snapshot_observed_at":"2026-07-06T13:04:23.687710Z","submitted_at":"2022-04-27T16:37:05Z","title":"SMEFT predictions for $gg\\to hh$ at full NLO QCD and truncation uncertainties","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2204.13045","snapshot_observed_at":"2026-08-06T18:22:26.856926Z","title":"Heinrich, J","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"reference_index":43,"source":"pdf_text","source_observed_at":"2026-08-06T18:22:26.856926Z"},"links":{"cited_paper":"/paper/2204.13045","citing_paper":"/paper/2507.08558"},"observation_digest":"sha256:0c4cf07f93b449dc983a0f923e59cec29167dc7c8637cb29d883396f2a35b99d","observation_id":"5febbb07-e6a2-49ab-8771-f26506f224c5","resolution":{"observed_at":"2026-08-06T18:22:26.856926Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2303.16922","last_updated":"2023-10-04T08:29:30Z","snapshot_observed_at":"2026-08-02T22:31:37.261666Z","submitted_at":"2023-03-29T18:00:00Z","title":"The Standard Model effective field theory at work","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2303.16922","snapshot_observed_at":"2026-08-06T18:22:26.899023Z","title":"Isidori, F","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"reference_index":44,"source":"pdf_text","source_observed_at":"2026-08-06T18:22:26.899023Z"},"links":{"cited_paper":"/paper/2303.16922","citing_paper":"/paper/2507.08558"},"observation_digest":"sha256:1c7086bd8e4ce1bbffca109582fb93d13391d333044f0e8ee477b2ceccefd0dd","observation_id":"dedd7eaa-1ca3-40dd-98a5-6e740e2fe347","resolution":{"observed_at":"2026-08-06T18:22:26.899023Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2310.18221","last_updated":"2024-03-25T15:04:48Z","snapshot_observed_at":"2026-07-06T16:39:32.455002Z","submitted_at":"2023-10-27T15:50:31Z","title":"On $\\gamma_5$ schemes and the interplay of SMEFT operators in the Higgs-gluon coupling","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2310.18221","snapshot_observed_at":"2026-08-06T18:22:26.956719Z","title":"Di Noi, R","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"reference_index":45,"source":"pdf_text","source_observed_at":"2026-08-06T18:22:26.956719Z"},"links":{"cited_paper":"/paper/2310.18221","citing_paper":"/paper/2507.08558"},"observation_digest":"sha256:a937bdbb66aca8a05eaf35835867b23b970de6fe49b628028ef830fe2f9136fe","observation_id":"989cebe1-9446-4ef6-80ca-5103b198ce05","resolution":{"observed_at":"2026-08-06T18:22:26.956719Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2311.15004","last_updated":"2024-06-25T16:14:57Z","snapshot_observed_at":"2026-07-06T16:52:15.355330Z","submitted_at":"2023-11-25T11:50:23Z","title":"Combining chromomagnetic and four-fermion operators with leading SMEFT operators for $gg\\to hh$ at NLO QCD","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2311.15004","snapshot_observed_at":"2026-08-06T18:22:26.993058Z","title":"Heinrich and J","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"reference_index":46,"source":"pdf_text","source_observed_at":"2026-08-06T18:22:26.993058Z"},"links":{"cited_paper":"/paper/2311.15004","citing_paper":"/paper/2507.08558"},"observation_digest":"sha256:6f485f9323c57565053ad0a0610766db2f9f617c46f21f32111b9de5a58144df","observation_id":"04644c18-b85b-45f1-9faf-54aad92731cd","resolution":{"observed_at":"2026-08-06T18:22:26.993058Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2409.19578","last_updated":"2024-09-29T06:37:59Z","snapshot_observed_at":"2026-07-06T19:23:58.763033Z","submitted_at":"2024-09-29T06:37:59Z","title":"Renormalisation group effects in SMEFT for di-Higgs production","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2409.19578","snapshot_observed_at":"2026-08-06T18:22:27.032967Z","title":"Heinrich and J","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"reference_index":47,"source":"pdf_text","source_observed_at":"2026-08-06T18:22:27.032967Z"},"links":{"cited_paper":"/paper/2409.19578","citing_paper":"/paper/2507.08558"},"observation_digest":"sha256:92b4f164090c2106bb69c8de210db92c9a633918277c1454d86136928438f375","observation_id":"e26c15ca-e8f0-47ba-854c-a1b1b4a58828","resolution":{"observed_at":"2026-08-06T18:22:27.032967Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1004.2489","last_updated":"2010-08-30T21:11:07Z","snapshot_observed_at":"2026-07-06T02:06:43.432085Z","submitted_at":"2010-04-14T20:00:06Z","title":"N-Jettiness: An Inclusive Event Shape to Veto Jets","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1004.2489","snapshot_observed_at":"2026-08-06T18:22:27.080402Z","title":null,"venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"reference_index":48,"source":"pdf_text","source_observed_at":"2026-08-06T18:22:27.080402Z"},"links":{"cited_paper":"/paper/1004.2489","citing_paper":"/paper/2507.08558"},"observation_digest":"sha256:55a49fc253c17b64157a82513511e0a6c3fed07717a552ab788bb0d09f3e52c0","observation_id":"da4f800c-4afb-45b0-83c1-41216603acf0","resolution":{"observed_at":"2026-08-06T18:22:27.080402Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0910.0467","last_updated":"2010-05-26T15:04:46Z","snapshot_observed_at":"2026-07-06T01:58:40.635046Z","submitted_at":"2009-10-05T19:06:38Z","title":"Factorization at the LHC: From PDFs to Initial State Jets","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0910.0467","snapshot_observed_at":"2026-08-06T18:22:27.110279Z","title":null,"venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"reference_index":49,"source":"pdf_text","source_observed_at":"2026-08-06T18:22:27.110279Z"},"links":{"cited_paper":"/paper/0910.0467","citing_paper":"/paper/2507.08558"},"observation_digest":"sha256:97fb86f9b0deff85dc6b1fb158d2acd0e0200be3459b81ba8ae7e79f800100de","observation_id":"77aa1f25-3391-48f6-89ee-4dfb5d466c9e","resolution":{"observed_at":"2026-08-06T18:22:27.110279Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1111.5206","last_updated":"2012-03-05T19:38:09Z","snapshot_observed_at":"2026-08-07T07:33:15.620638Z","submitted_at":"2011-11-22T14:54:37Z","title":"Scattering Amplitudes with Open Loops","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1111.5206","snapshot_observed_at":"2026-08-06T18:22:27.149254Z","title":"Cascioli, P","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"reference_index":50,"source":"pdf_text","source_observed_at":"2026-08-06T18:22:27.149254Z"},"links":{"cited_paper":"/paper/1111.5206","citing_paper":"/paper/2507.08558"},"observation_digest":"sha256:e1431a7174738f751f46662550a178776c1e4a75fc261c4b0af8c46ce4a552ee","observation_id":"bedfd5e3-32c9-43d6-8880-3f5bd47244b5","resolution":{"observed_at":"2026-08-06T18:22:27.149254Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1710.11452","last_updated":"2018-01-19T14:47:33Z","snapshot_observed_at":"2026-08-07T21:16:18.864993Z","submitted_at":"2017-10-31T13:23:48Z","title":"On-the-fly reduction of open loops","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1710.11452","snapshot_observed_at":"2026-08-06T18:22:27.194288Z","title":"Buccioni, S","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"reference_index":51,"source":"pdf_text","source_observed_at":"2026-08-06T18:22:27.194288Z"},"links":{"cited_paper":"/paper/1710.11452","citing_paper":"/paper/2507.08558"},"observation_digest":"sha256:2372bbef648eae2099df7f802d04e4dfeb6fc17b192df0ec698186d2554f0c60","observation_id":"8e900aab-3da0-49a5-b477-0dffabf5f1bc","resolution":{"observed_at":"2026-08-06T18:22:27.194288Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1907.13071","last_updated":"2019-11-29T23:23:10Z","snapshot_observed_at":"2026-08-06T08:09:02.265370Z","submitted_at":"2019-07-30T16:57:21Z","title":"OpenLoops 2","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1907.13071","snapshot_observed_at":"2026-08-06T18:22:27.238114Z","title":"Buccioni, J.-N","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"reference_index":52,"source":"pdf_text","source_observed_at":"2026-08-06T18:22:27.238114Z"},"links":{"cited_paper":"/paper/1907.13071","citing_paper":"/paper/2507.08558"},"observation_digest":"sha256:1e505c566cdeeb1f0e6ac6bc6f9cff2b325482b6365c138b5432f2a4590f6180","observation_id":"9d3767af-7edf-42b6-86e3-9d3c586c649e","resolution":{"observed_at":"2026-08-06T18:22:27.238114Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0903.1126","last_updated":"2013-10-22T12:55:34Z","snapshot_observed_at":"2026-07-06T01:50:53.141205Z","submitted_at":"2009-03-05T22:50:50Z","title":"On the Structure of Infrared Singularities of Gauge-Theory Amplitudes","version":5},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0903.1126","snapshot_observed_at":"2026-08-06T18:22:27.270422Z","title":"Becher and M","venue":null,"work_id":null,"year":2009},"citing_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"reference_index":53,"source":"pdf_text","source_observed_at":"2026-08-06T18:22:27.270422Z"},"links":{"cited_paper":"/paper/0903.1126","citing_paper":"/paper/2507.08558"},"observation_digest":"sha256:a6b23ee6e4ff6f63619df6e17a702b6fecbb32ee3e569b66b1c48635796a2222","observation_id":"1eeb8600-e2a3-4e91-a2aa-57b6b5a0ae48","resolution":{"observed_at":"2026-08-06T18:22:27.270422Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1209.0673","last_updated":"2013-02-26T15:13:17Z","snapshot_observed_at":"2026-07-06T02:54:57.524436Z","submitted_at":"2012-09-04T15:29:31Z","title":"A next-to-next-to-leading order calculation of soft-virtual cross sections","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1209.0673","snapshot_observed_at":"2026-08-06T18:22:27.312002Z","title":"de Florian and J","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"reference_index":54,"source":"pdf_text","source_observed_at":"2026-08-06T18:22:27.312002Z"},"links":{"cited_paper":"/paper/1209.0673","citing_paper":"/paper/2507.08558"},"observation_digest":"sha256:ee52a01855a2d4b08f2b5a5254fc770f061bd94d8ce9f5aa54606aff3dc8a62d","observation_id":"8704415b-bb82-4694-9b48-36cbb67220d6","resolution":{"observed_at":"2026-08-06T18:22:27.312002Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9512328","last_updated":"1995-12-16T13:40:45Z","snapshot_observed_at":"2026-07-07T04:21:34.426325Z","submitted_at":"1995-12-16T13:40:45Z","title":"Three-jet cross sections to next-to-leading order","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9512328","snapshot_observed_at":"2026-08-06T18:22:27.362157Z","title":"Frixione, Z","venue":null,"work_id":null,"year":1996},"citing_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"reference_index":55,"source":"pdf_text","source_observed_at":"2026-08-06T18:22:27.362157Z"},"links":{"cited_paper":"/paper/hep-ph/9512328","citing_paper":"/paper/2507.08558"},"observation_digest":"sha256:392d3c2e944464caa04391acb3d72d4dbcff0e0f751084dc622e9116826f5eb9","observation_id":"7175debc-2049-4ca6-9d02-9d89573a1d8f","resolution":{"observed_at":"2026-08-06T18:22:27.362157Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1507.06937","last_updated":"2015-12-06T21:36:02Z","snapshot_observed_at":"2026-07-06T04:24:49.397781Z","submitted_at":"2015-07-24T18:12:20Z","title":"Vector boson production at hadron colliders: transverse-momentum resummation and leptonic decay","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1507.06937","snapshot_observed_at":"2026-08-06T18:22:27.410306Z","title":"Catani, D","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"reference_index":56,"source":"pdf_text","source_observed_at":"2026-08-06T18:22:27.410306Z"},"links":{"cited_paper":"/paper/1507.06937","citing_paper":"/paper/2507.08558"},"observation_digest":"sha256:3a1b6eea54b7141e31f733bf4c3eb11c9ae4bef48fb42ca53b19989acfb7d2bb","observation_id":"2d8f161a-f509-4adb-972b-69b595f1707e","resolution":{"observed_at":"2026-08-06T18:22:27.410306Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1510.03865","last_updated":"2015-11-12T15:51:25Z","snapshot_observed_at":"2026-08-02T23:55:05.199370Z","submitted_at":"2015-10-13T20:14:09Z","title":"PDF4LHC recommendations for LHC Run II","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1510.03865","snapshot_observed_at":"2026-08-06T18:22:27.527857Z","title":"Butterworth et al., PDF4LHC recommendations for LHC Run II , J","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"reference_index":57,"source":"pdf_text","source_observed_at":"2026-08-06T18:22:27.527857Z"},"links":{"cited_paper":"/paper/1510.03865","citing_paper":"/paper/2507.08558"},"observation_digest":"sha256:0a6de25f879392fa0c9b37e11743505207d0a48247e1b337e684b89970a554c0","observation_id":"7fa0777d-17b3-4924-99a4-bee01a17bc98","resolution":{"observed_at":"2026-08-06T18:22:27.527857Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2306.16458","last_updated":"2023-06-28T18:00:02Z","snapshot_observed_at":"2026-07-06T15:47:57.565746Z","submitted_at":"2023-06-28T18:00:02Z","title":"The $q_T$ spectrum for Higgs production via heavy quark annihilation at N$^3$LL$'$+aN$^3$LO","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2306.16458","snapshot_observed_at":"2026-08-06T18:22:27.618995Z","title":null,"venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"reference_index":58,"source":"pdf_text","source_observed_at":"2026-08-06T18:22:27.618995Z"},"links":{"cited_paper":"/paper/2306.16458","citing_paper":"/paper/2507.08558"},"observation_digest":"sha256:d88a1731708840b5300e4489076146ba60cab274462303baa31536278d558937","observation_id":"b5e0cacf-d24d-43b6-94ef-1457f81319f3","resolution":{"observed_at":"2026-08-06T18:22:27.618995Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1901.03331","last_updated":"2020-10-06T19:56:56Z","snapshot_observed_at":"2026-08-09T00:44:24.826937Z","submitted_at":"2019-01-10T19:00:00Z","title":"Joint Two-Dimensional Resummation in $q_T$ and $0$-Jettiness at NNLL","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1901.03331","snapshot_observed_at":"2026-08-06T18:22:27.730497Z","title":"Lustermans, J","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"reference_index":59,"source":"pdf_text","source_observed_at":"2026-08-06T18:22:27.730497Z"},"links":{"cited_paper":"/paper/1901.03331","citing_paper":"/paper/2507.08558"},"observation_digest":"sha256:d7fa0de8242d35f85f27955d11b57380f3fb996d2730113034fa715a7acf98b2","observation_id":"5a52b348-99d0-4757-9b35-241bec85ecfb","resolution":{"observed_at":"2026-08-06T18:22:27.730497Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2203.05506","last_updated":"2022-03-23T16:57:09Z","snapshot_observed_at":"2026-08-06T19:05:54.168387Z","submitted_at":"2022-03-10T17:49:52Z","title":"The PDF4LHC21 combination of global PDF fits for the LHC Run III","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2203.05506","snapshot_observed_at":"2026-08-06T18:22:27.812977Z","title":null,"venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"reference_index":60,"source":"pdf_text","source_observed_at":"2026-08-06T18:22:27.812977Z"},"links":{"cited_paper":"/paper/2203.05506","citing_paper":"/paper/2507.08558"},"observation_digest":"sha256:3bf2f85256bd257cad7a9a898959e099da4cbeba2f250fec722511d138784284","observation_id":"8ac5f08b-ab03-4587-960c-6f9914dd39b2","resolution":{"observed_at":"2026-08-06T18:22:27.812977Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1412.7420","last_updated":"2015-03-05T14:26:58Z","snapshot_observed_at":"2026-07-06T04:04:34.630458Z","submitted_at":"2014-12-23T15:57:21Z","title":"LHAPDF6: parton density access in the LHC precision era","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1412.7420","snapshot_observed_at":"2026-08-06T18:22:27.913620Z","title":"Buckley, J","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"reference_index":61,"source":"pdf_text","source_observed_at":"2026-08-06T18:22:27.913620Z"},"links":{"cited_paper":"/paper/1412.7420","citing_paper":"/paper/2507.08558"},"observation_digest":"sha256:a5ea0a0ed0377679a54e4461c4b693ad80d69bd507e085a5454b9c5d2b40e584","observation_id":"12c9e0e1-0d58-4fef-9cbb-e3a8734cfdeb","resolution":{"observed_at":"2026-08-06T18:22:27.913620Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1909.00811","last_updated":"2021-02-17T09:47:16Z","snapshot_observed_at":"2026-07-06T08:18:27.636489Z","submitted_at":"2019-09-02T18:00:00Z","title":"A Toolbox for $q_T$ and $0$-Jettiness Subtractions at N$^3$LO","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1909.00811","snapshot_observed_at":"2026-08-06T18:22:28.022559Z","title":"Billis, M","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"reference_index":62,"source":"pdf_text","source_observed_at":"2026-08-06T18:22:28.022559Z"},"links":{"cited_paper":"/paper/1909.00811","citing_paper":"/paper/2507.08558"},"observation_digest":"sha256:e6fcd062af05dc41e3f761f90b4529d9ff2f3b8c9224a19c8d00168345727db7","observation_id":"981ae6a1-c781-45f1-ad86-b5a46bad226c","resolution":{"observed_at":"2026-08-06T18:22:28.022559Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-06T18:22:30.856583Z","title":null,"venue":null,"work_id":"3087723e-0e4b-4010-9b24-56c753665fc9","year":null},"citing_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"reference_index":63,"source":"pdf_text","source_observed_at":"2026-08-06T18:22:28.042174Z"},"links":{"citing_paper":"/paper/2507.08558"},"observation_digest":"sha256:e51498da3bb84efc4674d02fbabc266159f2856c52c4511b697ec43ba7fdd198","observation_id":"3f3af9de-1d6b-4b0c-9fb9-98d1d5f58eaa","resolution":{"observed_at":"2026-08-06T18:22:30.962680Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1506.05057","last_updated":"2015-09-19T04:37:49Z","snapshot_observed_at":"2026-07-06T04:21:05.411585Z","submitted_at":"2015-06-16T18:21:17Z","title":"The midpoint between dipole and parton showers","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1506.05057","snapshot_observed_at":"2026-08-06T18:22:28.113150Z","title":"H¨ oche and S","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"reference_index":64,"source":"pdf_text","source_observed_at":"2026-08-06T18:22:28.113150Z"},"links":{"cited_paper":"/paper/1506.05057","citing_paper":"/paper/2507.08558"},"observation_digest":"sha256:c5fcffc7a9ea6e6b3e77615de5a4d86e3c1d8a4c1ab84f924dfc71d4a0fb7f5e","observation_id":"063860c9-b0d3-447b-836a-af0e789cad2d","resolution":{"observed_at":"2026-08-06T18:22:28.113150Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1905.09127","last_updated":"2019-09-03T17:41:38Z","snapshot_observed_at":"2026-07-06T07:54:40.999741Z","submitted_at":"2019-05-22T13:30:53Z","title":"Event Generation with Sherpa 2.2","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1905.09127","snapshot_observed_at":"2026-08-06T18:22:28.273593Z","title":"7 (2019) 034 [1905.09127]","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"reference_index":65,"source":"pdf_text","source_observed_at":"2026-08-06T18:22:28.273593Z"},"links":{"cited_paper":"/paper/1905.09127","citing_paper":"/paper/2507.08558"},"observation_digest":"sha256:7b9cf85b9e85c563588d789661dd748049392cde324f0bcf73bd0ee4f1f31021","observation_id":"e0b90e36-50e3-4e55-a9f6-c486ab6a85fe","resolution":{"observed_at":"2026-08-06T18:22:28.273593Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1410.3012","last_updated":"2014-10-11T17:01:19Z","snapshot_observed_at":"2026-07-06T02:11:23.670680Z","submitted_at":"2014-10-11T17:01:19Z","title":"An Introduction to PYTHIA 8.2","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1410.3012","snapshot_observed_at":"2026-08-06T18:22:28.410529Z","title":"Sj¨ ostrand, S","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"reference_index":66,"source":"pdf_text","source_observed_at":"2026-08-06T18:22:28.410529Z"},"links":{"cited_paper":"/paper/1410.3012","citing_paper":"/paper/2507.08558"},"observation_digest":"sha256:e32c328e78a23e874348761146a93670c860dd172ecab31c533a66dfd340771b","observation_id":"10eed4c5-a6b5-480d-9aac-11c3faee30f4","resolution":{"observed_at":"2026-08-06T18:22:28.410529Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1508.01475","last_updated":"2015-08-06T18:02:46Z","snapshot_observed_at":"2026-07-06T04:26:00.816487Z","submitted_at":"2015-08-06T18:02:46Z","title":"Drell-Yan Production at NNLL'+NNLO Matched to Parton Showers","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1508.01475","snapshot_observed_at":"2026-08-06T18:22:28.547347Z","title":"Alioli, C","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"reference_index":67,"source":"pdf_text","source_observed_at":"2026-08-06T18:22:28.547347Z"},"links":{"cited_paper":"/paper/1508.01475","citing_paper":"/paper/2507.08558"},"observation_digest":"sha256:671911b08dcfcdb3dbc5bb63c5a328b74e2326c63bb0434a6fc916e5757edb29","observation_id":"b1bbeed6-6864-4bda-b080-0d554dd2cf3f","resolution":{"observed_at":"2026-08-06T18:22:28.547347Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1605.07192","last_updated":"2017-03-14T17:12:21Z","snapshot_observed_at":"2026-07-06T04:57:17.761891Z","submitted_at":"2016-05-23T20:00:17Z","title":"Underlying event sensitive observables in Drell-Yan production using GENEVA","version":3},"cited_work":{"arxiv_id":"1605.07192","doi":null,"metadata_source":"pith","pith_arxiv_id":"1605.07192","snapshot_observed_at":"2026-08-06T18:22:28.871384Z","title":"Underlying event sensitive observables in Drell-Yan production using GENEVA","venue":"hep-ph","work_id":"fdea42a7-773c-48fc-85ed-713cebaed9e6","year":2016},"citing_paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA","version":1},"reference_index":68,"source":"pdf_text","source_observed_at":"2026-08-06T18:22:28.672073Z"},"links":{"cited_paper":"/paper/1605.07192","citing_paper":"/paper/2507.08558"},"observation_digest":"sha256:0c5f858dcc406cfa76600243f9d30179db0f89c150d9dfa67575e6fa2162718f","observation_id":"78b4bc50-85a5-41e4-8934-4775b04a7613","resolution":{"observed_at":"2026-08-06T18:22:29.049268Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}}],"paper":{"arxiv_id":"2507.08558","last_updated":"2025-07-11T12:59:11Z","latest_version":1,"primary_category":"hep-ph","snapshot_observed_at":"2026-08-08T14:45:14.003938Z","submitted_at":"2025-07-11T12:59:11Z","title":"NNLO+PS Double Higgs boson production with top-quark mass corrections in GENEVA"},"reference_resolution":{"displayed":68,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":60,"verified_exact":8,"verified_fuzzy":0},"total_outbound_references":68},"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":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"thesis":"As of 9 August 2026, this Paper Citation Record lists 68 of 68 outbound references and 4 inbound Pith citation observations for arXiv:2507.08558."}