{"as_of":"2026-08-07T03:31:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:b842ba136a47c5442568dce7e723a6b1366703dd6d00456fc9b73bf89e508f13","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":4,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":4,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-06T06:34:29.942622+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":"2026-08-02T06:20:24.151859Z","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":"2026-07-04T07:19:38.537137Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"2211.05462","last_updated":"2022-11-10T10:16:22Z","snapshot_observed_at":"2026-08-01T14:50:13.911953Z","submitted_at":"2022-11-10T10:16:22Z","title":"The Unpolarized and Polarized Single-Mass Three-Loop Heavy Flavor Operator Matrix Elements $A_{gg,Q}$ and $\\Delta A_{gg,Q}$","version":1},"cited_work":{"arxiv_id":"2211.05462","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2211.05462","snapshot_observed_at":"2026-07-04T07:19:38.537137Z","title":"Ablinger, A","venue":null,"work_id":"c16941b4-d1d0-4125-9fb2-68f30b93d7ff","year":2022},"citing_paper":{"arxiv_id":"2606.21702","last_updated":"2026-06-19T19:21:28Z","snapshot_observed_at":"2026-08-04T01:53:42.788431Z","submitted_at":"2026-06-19T19:21:28Z","title":"Analytic results for heavy-quark contributions to charged-current DIS at NNLO","version":1},"reference_index":38,"source":"pdf_text","source_observed_at":"2026-06-26T13:32:17.923022Z"},"links":{"cited_paper":"/paper/2211.05462","citing_paper":"/paper/2606.21702"},"observation_digest":"sha256:beeea9ea906ef8f29274e988aa57457a0a7978b86de040cb0a7255b99668ad49","observation_id":"671e0a8b-787e-4b55-b326-ee5ba4904a66","resolution":{"observed_at":"2026-07-04T07:19:38.538431Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-06T06:34:29.942622+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-06T06:34:29.942622+00:00","source":"crossref"},{"observed_at":"2026-08-06T06:34:23.284952+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2211.05462","last_updated":"2022-11-10T10:16:22Z","snapshot_observed_at":"2026-08-01T14:50:13.911953Z","submitted_at":"2022-11-10T10:16:22Z","title":"The Unpolarized and Polarized Single-Mass Three-Loop Heavy Flavor Operator Matrix Elements $A_{gg,Q}$ and $\\Delta A_{gg,Q}$","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2211.05462","snapshot_observed_at":"2026-07-11T07:37:18.331806Z","title":"Ablinger, A","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2607.05235","last_updated":"2026-07-06T15:46:10Z","snapshot_observed_at":"2026-08-01T04:53:31.888131Z","submitted_at":"2026-07-06T15:46:10Z","title":"The variable flavor number scheme to three-loop order","version":1},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-07-11T07:37:18.331806Z"},"links":{"cited_paper":"/paper/2211.05462","citing_paper":"/paper/2607.05235"},"observation_digest":"sha256:414ca0e829737119fa14f86f80f722ee56bdde3bcf4dc2427bbab260bb632214","observation_id":"704731f3-a4fc-42f6-ba26-25581ea87dce","resolution":{"observed_at":"2026-07-11T07:37:18.331806Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2211.05462","last_updated":"2022-11-10T10:16:22Z","snapshot_observed_at":"2026-08-01T14:50:13.911953Z","submitted_at":"2022-11-10T10:16:22Z","title":"The Unpolarized and Polarized Single-Mass Three-Loop Heavy Flavor Operator Matrix Elements $A_{gg,Q}$ and $\\Delta A_{gg,Q}$","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2211.05462","snapshot_observed_at":"2026-08-02T06:20:24.151859Z","title":"Ablinger, A","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2607.14151","last_updated":"2026-07-19T22:32:22Z","snapshot_observed_at":"2026-08-06T23:35:36.992422Z","submitted_at":"2026-07-14T15:25:29Z","title":"Candia-v2: Logarithmic expansions for DGLAP evolution in $x$-space","version":2},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-08-02T06:20:24.151859Z"},"links":{"cited_paper":"/paper/2211.05462","citing_paper":"/paper/2607.14151"},"observation_digest":"sha256:b66082ede0af565138e1af050b9f01df631024fc2dcd1c25c6bb6c1e293aa08c","observation_id":"fa3a2dc3-849e-4be9-8a55-fc5e98a1aa19","resolution":{"observed_at":"2026-08-02T06:20:24.151859Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2211.05462","last_updated":"2022-11-10T10:16:22Z","snapshot_observed_at":"2026-08-01T14:50:13.911953Z","submitted_at":"2022-11-10T10:16:22Z","title":"The Unpolarized and Polarized Single-Mass Three-Loop Heavy Flavor Operator Matrix Elements $A_{gg,Q}$ and $\\Delta A_{gg,Q}$","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2211.05462","snapshot_observed_at":"2026-07-31T10:42:20.186534Z","title":"u mlein J , author De Freitas A , author Goedicke A , author von Manteuffel A , author Schneider C and author Sch \\","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2607.24613","last_updated":"2026-07-27T16:12:29Z","snapshot_observed_at":"2026-08-06T05:34:00.951187Z","submitted_at":"2026-07-27T16:12:29Z","title":"Global analyses of helicity-dependent parton distribution functions","version":1},"reference_index":10,"source":"arxiv_source","source_observed_at":"2026-07-31T10:42:20.186534Z"},"links":{"cited_paper":"/paper/2211.05462","citing_paper":"/paper/2607.24613"},"observation_digest":"sha256:fefa31690c13c4daadfdeb7a451a1690242b2caddaae188efa3a14cc42cdea79","observation_id":"6fe73c9f-5af8-40b9-81ec-f89b18fc5472","resolution":{"observed_at":"2026-07-31T10:42:20.186534Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"links":{"evidence":"/evidence","html":"/paper/2211.05462/citation-record","integrity":"/paper/2211.05462/integrity","json":"/paper/2211.05462/citation-record.json","paper":"/paper/2211.05462"},"outbound":[],"paper":{"arxiv_id":"2211.05462","last_updated":"2022-11-10T10:16:22Z","latest_version":1,"primary_category":"hep-ph","snapshot_observed_at":"2026-08-01T14:50:13.911953Z","submitted_at":"2022-11-10T10:16:22Z","title":"The Unpolarized and Polarized Single-Mass Three-Loop Heavy Flavor Operator Matrix Elements $A_{gg,Q}$ and $\\Delta A_{gg,Q}$"},"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":"2026-08-06T06:34:29.942622+00:00","source":"crossref"},{"observed_at":"2026-08-06T06:34:23.284952+00:00","source":"retraction_watch"}],"thesis":"As of 7 August 2026, this Paper Citation Record lists 0 of 0 outbound references and 4 inbound Pith citation observations for arXiv:2211.05462."}