{"as_of":"2026-08-10T17:06:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:e5ddcc0a86ccfd6755bcab5588204423e18497f57442dd753cedba4c247d8b85","coverage":[{"denominator":17,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":17,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-09T12:59:45.386258Z","state":"measured"},{"denominator":17,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":17,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-10T06:31:04.303077+00:00","state":"measured"},{"denominator":0,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":0,"source":"paper_references, paper_reference_links","source_observed_at":null,"state":"measured"},{"denominator":1,"lane":"external_citation_measurements","note":"A source-named dated measurement, never combined with another source.","records_observed":0,"source":"cited_works","source_observed_at":null,"state":"measured"}],"external_citation_measurements":[],"inbound":[],"links":{"evidence":"/evidence","html":"/paper/2502.02228/citation-record","integrity":"/paper/2502.02228/integrity","json":"/paper/2502.02228/citation-record.json","paper":"/paper/2502.02228"},"outbound":[{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-09T12:59:45.299405Z","title":null,"venue":null,"work_id":null,"year":1975},"citing_paper":{"arxiv_id":"2502.02228","last_updated":"2025-02-04T11:10:26Z","snapshot_observed_at":"2026-08-10T10:08:28.580231Z","submitted_at":"2025-02-04T11:10:26Z","title":"The real corrections to the Higgs impact factor at next-to-leading order with finite top mass","version":1},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-08-09T12:59:45.299405Z"},"links":{"citing_paper":"/paper/2502.02228"},"observation_digest":"sha256:2a33311893368a3748b89f6c53455919aafcc2c45405286d71dbbb3fd57e2ee1","observation_id":"5f2e6a0c-0415-4b25-9a73-a6f39fbbcc0c","resolution":{"observed_at":"2026-08-09T12:59:45.299405Z","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":"2026-08-09T12:59:45.895607Z","title":null,"venue":null,"work_id":"b8ca3394-e755-4474-a736-92a7e18a7e94","year":1976},"citing_paper":{"arxiv_id":"2502.02228","last_updated":"2025-02-04T11:10:26Z","snapshot_observed_at":"2026-08-10T10:08:28.580231Z","submitted_at":"2025-02-04T11:10:26Z","title":"The real corrections to the Higgs impact factor at next-to-leading order with finite top mass","version":1},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-08-09T12:59:45.304772Z"},"links":{"citing_paper":"/paper/2502.02228"},"observation_digest":"sha256:f440a32af63581f3e6db1579c35c4abbd0a5f155041935d98917ce89ed2b3232","observation_id":"9f53981b-9e3e-4339-a432-23d7b430219d","resolution":{"observed_at":"2026-08-09T12:59:45.900479Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+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":"2026-08-09T12:59:45.879428Z","title":null,"venue":null,"work_id":"c943f73b-615a-4fe9-bfcf-0711308902ee","year":1977},"citing_paper":{"arxiv_id":"2502.02228","last_updated":"2025-02-04T11:10:26Z","snapshot_observed_at":"2026-08-10T10:08:28.580231Z","submitted_at":"2025-02-04T11:10:26Z","title":"The real corrections to the Higgs impact factor at next-to-leading order with finite top mass","version":1},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-08-09T12:59:45.309685Z"},"links":{"citing_paper":"/paper/2502.02228"},"observation_digest":"sha256:be2fe36725d303611b08aba64ab25d4fcd639a079621882fa513b0cda19df758","observation_id":"a5de9c1f-204e-4f4a-b98f-e5c0eaf30404","resolution":{"observed_at":"2026-08-09T12:59:45.884362Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+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":"2026-08-09T12:59:45.864067Z","title":null,"venue":null,"work_id":"0bc4aa1e-5d8b-43ec-8b70-905058deb479","year":1978},"citing_paper":{"arxiv_id":"2502.02228","last_updated":"2025-02-04T11:10:26Z","snapshot_observed_at":"2026-08-10T10:08:28.580231Z","submitted_at":"2025-02-04T11:10:26Z","title":"The real corrections to the Higgs impact factor at next-to-leading order with finite top mass","version":1},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-09T12:59:45.315471Z"},"links":{"citing_paper":"/paper/2502.02228"},"observation_digest":"sha256:1aeff8ba64fdce932ed2efee7aa664255121c1e856e3bcf0d8a762793971ff7b","observation_id":"8a180552-f166-48ea-b5e6-8fd4c1c815bb","resolution":{"observed_at":"2026-08-09T12:59:45.869021Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9802290","last_updated":"1998-03-31T12:41:06Z","snapshot_observed_at":"2026-07-07T04:28:20.832511Z","submitted_at":"1998-02-10T15:59:27Z","title":"BFKL pomeron in the next-to-leading approximation","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9802290","snapshot_observed_at":"2026-08-09T12:59:45.322512Z","title":null,"venue":null,"work_id":null,"year":1998},"citing_paper":{"arxiv_id":"2502.02228","last_updated":"2025-02-04T11:10:26Z","snapshot_observed_at":"2026-08-10T10:08:28.580231Z","submitted_at":"2025-02-04T11:10:26Z","title":"The real corrections to the Higgs impact factor at next-to-leading order with finite top mass","version":1},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-08-09T12:59:45.322512Z"},"links":{"cited_paper":"/paper/hep-ph/9802290","citing_paper":"/paper/2502.02228"},"observation_digest":"sha256:7df696183777ea4493ad34f16e91e6c0e21ddc25ef38db3e57b7fb9088ed27f5","observation_id":"cdd2247e-fb06-4d24-982d-f0d79232156b","resolution":{"observed_at":"2026-08-09T12:59:45.322512Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9803389","last_updated":"1998-03-19T15:25:30Z","snapshot_observed_at":"2026-07-07T04:28:51.299507Z","submitted_at":"1998-03-19T15:25:30Z","title":"Energy Scale(s) and Next-to-leading BFKL Equation","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9803389","snapshot_observed_at":"2026-08-09T12:59:45.328185Z","title":"Ciafaloni and G","venue":null,"work_id":null,"year":1998},"citing_paper":{"arxiv_id":"2502.02228","last_updated":"2025-02-04T11:10:26Z","snapshot_observed_at":"2026-08-10T10:08:28.580231Z","submitted_at":"2025-02-04T11:10:26Z","title":"The real corrections to the Higgs impact factor at next-to-leading order with finite top mass","version":1},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-09T12:59:45.328185Z"},"links":{"cited_paper":"/paper/hep-ph/9803389","citing_paper":"/paper/2502.02228"},"observation_digest":"sha256:222a75e624e29bf9d30909f4831ccb062312378787e9eebb756c16a014cd6541","observation_id":"32de9346-d2fc-491b-b91d-73528fc79502","resolution":{"observed_at":"2026-08-09T12:59:45.328185Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2202.12227","last_updated":"2022-10-19T15:12:27Z","snapshot_observed_at":"2026-07-06T12:41:22.635071Z","submitted_at":"2022-02-24T17:44:32Z","title":"Diffractive semi-hard production of a $J/\\psi$ or a $\\Upsilon$ from single-parton fragmentation plus a jet in hybrid factorization","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2202.12227","snapshot_observed_at":"2026-08-09T12:59:45.334406Z","title":null,"venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2502.02228","last_updated":"2025-02-04T11:10:26Z","snapshot_observed_at":"2026-08-10T10:08:28.580231Z","submitted_at":"2025-02-04T11:10:26Z","title":"The real corrections to the Higgs impact factor at next-to-leading order with finite top mass","version":1},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-09T12:59:45.334406Z"},"links":{"cited_paper":"/paper/2202.12227","citing_paper":"/paper/2502.02228"},"observation_digest":"sha256:4f1f3637eadc3199072a962e12305e9ee2baf0110f8a98de83ba23ed88175d2d","observation_id":"35557665-6315-4f5c-89e6-b5f1640c0125","resolution":{"observed_at":"2026-08-09T12:59:45.334406Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2204.06497","last_updated":"2022-06-08T16:35:52Z","snapshot_observed_at":"2026-08-10T05:45:33.109793Z","submitted_at":"2022-04-13T16:27:10Z","title":"High-energy emissions of light mesons plus heavy flavor at the LHC and the Forward Physics Facility","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2204.06497","snapshot_observed_at":"2026-08-09T12:59:45.340386Z","title":null,"venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2502.02228","last_updated":"2025-02-04T11:10:26Z","snapshot_observed_at":"2026-08-10T10:08:28.580231Z","submitted_at":"2025-02-04T11:10:26Z","title":"The real corrections to the Higgs impact factor at next-to-leading order with finite top mass","version":1},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-09T12:59:45.340386Z"},"links":{"cited_paper":"/paper/2204.06497","citing_paper":"/paper/2502.02228"},"observation_digest":"sha256:4bfa846c14a6467bea24452d1a23e71d7f5c512da6db8cc5d4a3ebc9eb64da77","observation_id":"f65fa511-8ac9-423b-bfee-6e19e1a2e8b0","resolution":{"observed_at":"2026-08-09T12:59:45.340386Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2405.14773","last_updated":"2024-12-13T20:52:40Z","snapshot_observed_at":"2026-07-06T18:18:47.640933Z","submitted_at":"2024-05-23T16:42:34Z","title":"Fully charmed tetraquarks from LHC to FCC: Natural stability from fragmentation","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2405.14773","snapshot_observed_at":"2026-08-09T12:59:45.345244Z","title":null,"venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2502.02228","last_updated":"2025-02-04T11:10:26Z","snapshot_observed_at":"2026-08-10T10:08:28.580231Z","submitted_at":"2025-02-04T11:10:26Z","title":"The real corrections to the Higgs impact factor at next-to-leading order with finite top mass","version":1},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-09T12:59:45.345244Z"},"links":{"cited_paper":"/paper/2405.14773","citing_paper":"/paper/2502.02228"},"observation_digest":"sha256:1b29d547b1680542c48a5f65ae7710fd37f3a1743a38db9e8debea3751404ce7","observation_id":"8325705b-c655-4348-b36e-1754be7e46cd","resolution":{"observed_at":"2026-08-09T12:59:45.345244Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2409.20354","last_updated":"2024-09-30T14:50:53Z","snapshot_observed_at":"2026-08-01T14:46:26.796343Z","submitted_at":"2024-09-30T14:50:53Z","title":"The next-to-leading order Higgs impact factor at physical top mass: The real corrections","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2409.20354","snapshot_observed_at":"2026-08-09T12:59:45.350936Z","title":null,"venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2502.02228","last_updated":"2025-02-04T11:10:26Z","snapshot_observed_at":"2026-08-10T10:08:28.580231Z","submitted_at":"2025-02-04T11:10:26Z","title":"The real corrections to the Higgs impact factor at next-to-leading order with finite top mass","version":1},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-09T12:59:45.350936Z"},"links":{"cited_paper":"/paper/2409.20354","citing_paper":"/paper/2502.02228"},"observation_digest":"sha256:41dfb5588b4e58e2052217c789639d9f0cdcfc06fa0dcf42afd9b43b76488f7e","observation_id":"c8ef6e29-9fb2-444b-bf88-9cb833d6a052","resolution":{"observed_at":"2026-08-09T12:59:45.350936Z","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":"arxiv_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-09T12:59:45.747711Z","title":null,"venue":null,"work_id":"c8e6dc10-af12-4ec0-b770-a6c6ec3e8f0a","year":2019},"citing_paper":{"arxiv_id":"2502.02228","last_updated":"2025-02-04T11:10:26Z","snapshot_observed_at":"2026-08-10T10:08:28.580231Z","submitted_at":"2025-02-04T11:10:26Z","title":"The real corrections to the Higgs impact factor at next-to-leading order with finite top mass","version":1},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-08-09T12:59:45.355951Z"},"links":{"citing_paper":"/paper/2502.02228"},"observation_digest":"sha256:55fd8a43cc5775cf7a5072182c47a95df2a1287164c77616bf35f5be2062b5a5","observation_id":"2f519894-c00d-46fc-8c3d-2e87b5876d82","resolution":{"observed_at":"2026-08-09T12:59:45.753499Z","resolver_source":"arxiv_id_nonexistent","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2011.03193","last_updated":"2021-02-10T19:15:35Z","snapshot_observed_at":"2026-08-08T19:43:44.123154Z","submitted_at":"2020-11-06T05:08:49Z","title":"Forward Higgs production within high energy factorization in the heavy quark limit at next-to-leading order accuracy","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2011.03193","snapshot_observed_at":"2026-08-09T12:59:45.360944Z","title":"Hentschinski, K","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2502.02228","last_updated":"2025-02-04T11:10:26Z","snapshot_observed_at":"2026-08-10T10:08:28.580231Z","submitted_at":"2025-02-04T11:10:26Z","title":"The real corrections to the Higgs impact factor at next-to-leading order with finite top mass","version":1},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-08-09T12:59:45.360944Z"},"links":{"cited_paper":"/paper/2011.03193","citing_paper":"/paper/2502.02228"},"observation_digest":"sha256:9494693253bbc511c8529f371f395c885ae10c9af967ea1139073b7c3221b197","observation_id":"4a2ec2b5-d67f-4d8d-971f-be23e5ecd9eb","resolution":{"observed_at":"2026-08-09T12:59:45.360944Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2205.02681","last_updated":"2022-10-19T22:44:24Z","snapshot_observed_at":"2026-08-09T13:20:53.831526Z","submitted_at":"2022-05-05T14:40:03Z","title":"The next-to-leading order Higgs impact factor in the infinite top-mass limit","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2205.02681","snapshot_observed_at":"2026-08-09T12:59:45.366223Z","title":null,"venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2502.02228","last_updated":"2025-02-04T11:10:26Z","snapshot_observed_at":"2026-08-10T10:08:28.580231Z","submitted_at":"2025-02-04T11:10:26Z","title":"The real corrections to the Higgs impact factor at next-to-leading order with finite top mass","version":1},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-09T12:59:45.366223Z"},"links":{"cited_paper":"/paper/2205.02681","citing_paper":"/paper/2502.02228"},"observation_digest":"sha256:cbd522c94bccae2f102a24947fcd88b6e596375170fd1e971c1eaf1d7dbda77c","observation_id":"db3ee75b-6492-4ded-8715-53cc8fdbdf5d","resolution":{"observed_at":"2026-08-09T12:59:45.366223Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1802.07758","last_updated":"2018-05-24T09:13:17Z","snapshot_observed_at":"2026-07-06T06:24:39.727396Z","submitted_at":"2018-02-21T19:21:41Z","title":"Double resummation for Higgs production","version":2},"cited_work":{"arxiv_id":"1802.07758","doi":null,"metadata_source":"pith","pith_arxiv_id":"1802.07758","snapshot_observed_at":"2026-08-09T12:59:45.502121Z","title":"Double resummation for Higgs production","venue":"hep-ph","work_id":"c02c6c46-bd4e-4990-956c-156342317fd2","year":2018},"citing_paper":{"arxiv_id":"2502.02228","last_updated":"2025-02-04T11:10:26Z","snapshot_observed_at":"2026-08-10T10:08:28.580231Z","submitted_at":"2025-02-04T11:10:26Z","title":"The real corrections to the Higgs impact factor at next-to-leading order with finite top mass","version":1},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-09T12:59:45.371145Z"},"links":{"cited_paper":"/paper/1802.07758","citing_paper":"/paper/2502.02228"},"observation_digest":"sha256:5be54e08e7362ee814d11b125a7a4cf8f98e4dbb5cbe9a712dbc3bf45ccb63fd","observation_id":"611d3db8-0b7c-40c5-bcf2-d59d6fcbdfd3","resolution":{"observed_at":"2026-08-09T12:59:45.507562Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2008.00501","last_updated":"2021-04-08T14:01:13Z","snapshot_observed_at":"2026-08-08T04:54:55.744613Z","submitted_at":"2020-08-02T15:13:55Z","title":"High-energy resummed distributions for the inclusive Higgs-plus-jet production at the LHC","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2008.00501","snapshot_observed_at":"2026-08-09T12:59:45.376954Z","title":null,"venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2502.02228","last_updated":"2025-02-04T11:10:26Z","snapshot_observed_at":"2026-08-10T10:08:28.580231Z","submitted_at":"2025-02-04T11:10:26Z","title":"The real corrections to the Higgs impact factor at next-to-leading order with finite top mass","version":1},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-08-09T12:59:45.376954Z"},"links":{"cited_paper":"/paper/2008.00501","citing_paper":"/paper/2502.02228"},"observation_digest":"sha256:b2ead6b2281959b4ec0c0fa5d05de0a5ac64bfd57f3257218872e30fb9e7fe76","observation_id":"35b2a5b6-c37a-4aea-b334-4836176c5a5d","resolution":{"observed_at":"2026-08-09T12:59:45.376954Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1812.08072","last_updated":"2019-04-24T20:14:13Z","snapshot_observed_at":"2026-08-07T08:42:06.581453Z","submitted_at":"2018-12-19T16:48:15Z","title":"Finite Quark-Mass Effects in Higgs Boson Production With Dijets at Large Energies","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1812.08072","snapshot_observed_at":"2026-08-09T12:59:45.381567Z","title":null,"venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2502.02228","last_updated":"2025-02-04T11:10:26Z","snapshot_observed_at":"2026-08-10T10:08:28.580231Z","submitted_at":"2025-02-04T11:10:26Z","title":"The real corrections to the Higgs impact factor at next-to-leading order with finite top mass","version":1},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-08-09T12:59:45.381567Z"},"links":{"cited_paper":"/paper/1812.08072","citing_paper":"/paper/2502.02228"},"observation_digest":"sha256:40b6b9bae67fd5f9e1480158d9fd1080c8316a506e13b157ede5f35e94283925","observation_id":"4bb265ee-f42f-4d58-ae24-d71e83915fc7","resolution":{"observed_at":"2026-08-09T12:59:45.381567Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2401.17843","last_updated":"2024-04-16T18:03:33Z","snapshot_observed_at":"2026-08-10T00:34:21.244810Z","submitted_at":"2024-01-31T14:03:15Z","title":"On the breakdown of eikonal approximation and survival of Reggeization in presence of dimension-5 Higgs-gluon coupling","version":3},"cited_work":{"arxiv_id":"2401.17843","doi":null,"metadata_source":"pith","pith_arxiv_id":"2401.17843","snapshot_observed_at":"2026-08-09T12:59:45.440091Z","title":"On the breakdown of eikonal approximation and survival of Reggeization in presence of dimension-5 Higgs-gluon coupling","venue":"hep-ph","work_id":"0bcd2dc7-3191-49a6-9761-2288be32236c","year":2024},"citing_paper":{"arxiv_id":"2502.02228","last_updated":"2025-02-04T11:10:26Z","snapshot_observed_at":"2026-08-10T10:08:28.580231Z","submitted_at":"2025-02-04T11:10:26Z","title":"The real corrections to the Higgs impact factor at next-to-leading order with finite top mass","version":1},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-08-09T12:59:45.386258Z"},"links":{"cited_paper":"/paper/2401.17843","citing_paper":"/paper/2502.02228"},"observation_digest":"sha256:2dc9cf365976b46f0dade71489f5d7e6634ca57d2c12c087e86c8987d2505c77","observation_id":"444288b7-92ae-42fa-96fd-c4a88871a359","resolution":{"observed_at":"2026-08-09T12:59:45.448503Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}}],"paper":{"arxiv_id":"2502.02228","last_updated":"2025-02-04T11:10:26Z","latest_version":1,"primary_category":"hep-ph","snapshot_observed_at":"2026-08-10T10:08:28.580231Z","submitted_at":"2025-02-04T11:10:26Z","title":"The real corrections to the Higgs impact factor at next-to-leading order with finite top mass"},"reference_resolution":{"displayed":17,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":14,"verified_exact":3,"verified_fuzzy":0},"total_outbound_references":17},"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":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"thesis":"As of 10 August 2026, this Paper Citation Record lists 17 of 17 outbound references and 0 inbound Pith citation observations for arXiv:2502.02228."}