{"as_of":"2026-08-09T04:32:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:bf12c5099ab119f81146162262ce96ef81c9abfcaf89480402b321b81c5d45ea","coverage":[{"denominator":0,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":0,"source":"paper_references, paper_reference_links","source_observed_at":null,"state":"measured"},{"denominator":10,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":10,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-08T06:32:00.761636+00:00","state":"measured"},{"denominator":10,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":10,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-08T13:57:12.919137Z","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":"2026-07-04T20:30:07.423870Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"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":"2026-08-07T10:50:51.039521Z","title":"Bagnaschi, G","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2506.04323","last_updated":"2025-09-05T18:02:48Z","snapshot_observed_at":"2026-08-07T10:42:29.528660Z","submitted_at":"2025-06-04T18:00:02Z","title":"{\\tt ggxy}: a flexible library to compute gluon-induced cross sections","version":2},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-08-07T10:50:51.039521Z"},"links":{"cited_paper":"/paper/2309.10525","citing_paper":"/paper/2506.04323"},"observation_digest":"sha256:358d6f0346cce6f813df605b6f36d5ef7d3f0a1b1af735e84c00ca2545a98e49","observation_id":"4fdf037d-2336-45d3-809e-c39e2b227b6b","resolution":{"observed_at":"2026-08-07T10:50:51.039521Z","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":"2309.10525","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2309.10525","snapshot_observed_at":"2026-07-04T20:30:07.423870Z","title":"Bagnaschi, G","venue":null,"work_id":"f70d4d3a-544e-4a76-9e9d-3e3fb72a8942","year":2023},"citing_paper":{"arxiv_id":"2507.03495","last_updated":"2026-04-22T15:50:58Z","snapshot_observed_at":"2026-07-06T21:52:18.525939Z","submitted_at":"2025-07-04T11:42:19Z","title":"Study of Higgs boson pair production in the $HH \\rightarrow b \\overline{b} \\gamma \\gamma$ final state with 308 fb$^{-1}$ of data collected at $\\sqrt{s} =$ 13 TeV and 13.6 TeV by the ATLAS experiment","version":2},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-05-19T06:22:26.045210Z"},"links":{"cited_paper":"/paper/2309.10525","citing_paper":"/paper/2507.03495"},"observation_digest":"sha256:ea7d5e0fcc9fb42886f3772d5ea41068b370f48c171c6184867c63b664bfbafd","observation_id":"024ab00f-0bd7-4ef0-b097-ceb8b9ca3441","resolution":{"observed_at":"2026-05-19T06:22:59.439523Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+00:00","source":"retraction_watch"}],"state":"measured"}},{"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":"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":"2026-08-04T13:34:57.690883Z","title":"Bagnaschi, G","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2510.00686","last_updated":"2026-05-26T10:36:09Z","snapshot_observed_at":"2026-08-09T01:43:01.321129Z","submitted_at":"2025-10-01T09:08:33Z","title":"Phenomenology of a Kinetic Higgs Portal","version":2},"reference_index":92,"source":"pdf_text","source_observed_at":"2026-08-04T13:34:57.690883Z"},"links":{"cited_paper":"/paper/2309.10525","citing_paper":"/paper/2510.00686"},"observation_digest":"sha256:b04d026eb634fc840857025489ae0a88dba1b263b67e538dbe77f408240a2677","observation_id":"dea7bec6-77e5-4809-99d8-e647330185f5","resolution":{"observed_at":"2026-08-04T13:34:57.690883Z","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":"2309.10525","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2309.10525","snapshot_observed_at":"2026-07-04T20:30:07.423870Z","title":"Bagnaschi, G","venue":null,"work_id":"f70d4d3a-544e-4a76-9e9d-3e3fb72a8942","year":2023},"citing_paper":{"arxiv_id":"2511.23411","last_updated":"2026-05-08T15:44:36Z","snapshot_observed_at":"2026-07-06T02:11:23.670680Z","submitted_at":"2025-11-28T18:04:45Z","title":"Higgs pair production in gluon fusion to higher orders in Higgs Effective Field Theory","version":2},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-05-17T04:14:55.243806Z"},"links":{"cited_paper":"/paper/2309.10525","citing_paper":"/paper/2511.23411"},"observation_digest":"sha256:ff12108b08b05907659161c04d2d0accb2050bedfa61c51f9dbbf55644a1497f","observation_id":"15f72252-1c72-4831-b474-43ebd490abe0","resolution":{"observed_at":"2026-05-17T04:19:01.275055Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+00:00","source":"retraction_watch"}],"state":"measured"}},{"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":"2026-08-03T07:40:49.809780Z","title":"Bagnaschi, G","venue":null,"work_id":null,"year":2023},"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":47,"source":"pdf_text","source_observed_at":"2026-08-03T07:40:49.809780Z"},"links":{"cited_paper":"/paper/2309.10525","citing_paper":"/paper/2601.19990"},"observation_digest":"sha256:d3c2ef5fb5cd97e4f282f8ba0fadc47606d2d19e7622b90d4367690b1589f2eb","observation_id":"4d4e9d5d-a44b-49ab-950e-e0e850b50e52","resolution":{"observed_at":"2026-08-03T07:40:49.809780Z","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":"2309.10525","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2309.10525","snapshot_observed_at":"2026-07-04T20:30:07.423870Z","title":"Bagnaschi, G","venue":null,"work_id":"f70d4d3a-544e-4a76-9e9d-3e3fb72a8942","year":2023},"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":9,"source":"pdf_text","source_observed_at":"2026-06-25T20:07:31.995758Z"},"links":{"cited_paper":"/paper/2309.10525","citing_paper":"/paper/2606.25928"},"observation_digest":"sha256:045b83e7e6d20f0e554ba90d89699662e6b91c353803594e5dbd752869b8a47d","observation_id":"4cc83c1b-7455-4c40-8f3a-b415c0cb5297","resolution":{"observed_at":"2026-07-04T20:30:07.425289Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+00:00","source":"retraction_watch"}],"state":"measured"}},{"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":"2026-07-11T08:06:43.415495Z","title":"Higgs boson pair production at NLO in the POWHEG approach and the top quark mass uncertainties","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2607.05145","last_updated":"2026-07-06T14:27:16Z","snapshot_observed_at":"2026-08-08T22:47:34.777487Z","submitted_at":"2026-07-06T14:27:16Z","title":"Search for nonresonant triple Higgs boson production in the final state with six bottom quarks in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-07-11T08:06:43.415495Z"},"links":{"cited_paper":"/paper/2309.10525","citing_paper":"/paper/2607.05145"},"observation_digest":"sha256:ce05577d342dbc83e099295eb2ff88f7195e46df5a6d0c690db35dece1eea4ea","observation_id":"4fb73677-46fd-441d-a59a-cc4018d1778d","resolution":{"observed_at":"2026-07-11T08:06:43.415495Z","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":"2026-07-30T18:22:13.590540Z","title":"Bagnaschi, G","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2607.26879","last_updated":"2026-07-29T13:09:08Z","snapshot_observed_at":"2026-08-01T23:37:39.587230Z","submitted_at":"2026-07-29T13:09:08Z","title":"Improved analysis of non-resonant Higgs boson pair production in the $b\\bar{b}\\tau^+\\tau^-$ final state with $196$ fb$^{-1}$ of data collected at $\\sqrt{s}$ = 13 TeV and 13.6 TeV with the ATLAS detector","version":1},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-07-30T18:22:13.590540Z"},"links":{"cited_paper":"/paper/2309.10525","citing_paper":"/paper/2607.26879"},"observation_digest":"sha256:00d42e646f3d7b83e5d325990e5d45655035e3d5dbdd960a95a4ee1cbf6a0096","observation_id":"c423dbb5-ee9a-4e40-a241-b7f222223479","resolution":{"observed_at":"2026-07-30T18:22:13.590540Z","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":"2026-08-08T13:57:12.919137Z","title":"Bagnaschi, G","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2608.05401","last_updated":"2026-08-05T20:37:00Z","snapshot_observed_at":"2026-08-09T04:10:56.986292Z","submitted_at":"2026-08-05T20:37:00Z","title":"HiggsTools for LHC Run 3 and Beyond","version":1},"reference_index":42,"source":"pdf_text","source_observed_at":"2026-08-08T13:57:12.919137Z"},"links":{"cited_paper":"/paper/2309.10525","citing_paper":"/paper/2608.05401"},"observation_digest":"sha256:14206af1b42c1250d709053e1d308dcdff297e05ac9fb9f5c396c494170393fc","observation_id":"3b77622f-9e69-410d-84be-6c62928dc43c","resolution":{"observed_at":"2026-08-08T13:57:12.919137Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"links":{"evidence":"/evidence","html":"/paper/2309.10525/citation-record","integrity":"/paper/2309.10525/integrity","json":"/paper/2309.10525/citation-record.json","paper":"/paper/2309.10525"},"outbound":[],"paper":{"arxiv_id":"2309.10525","last_updated":"2023-09-19T11:10:53Z","latest_version":1,"primary_category":"hep-ph","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"},"reference_resolution":{"displayed":0,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":0,"verified_exact":0,"verified_fuzzy":0},"total_outbound_references":0},"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":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+00:00","source":"retraction_watch"}],"thesis":"As of 9 August 2026, this Paper Citation Record lists 0 of 0 outbound references and 10 inbound Pith citation observations for arXiv:2309.10525."}