{"as_of":"2026-08-07T01:04:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:0aa589b773f830f140c49f0fb2782d4f954d3d392d61a06c1272c402a1be57f3","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":9,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":9,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-06T06:34:29.942622+00:00","state":"measured"},{"denominator":9,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":9,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-06T10:24:37.775546Z","state":"measured"},{"denominator":1,"lane":"external_citation_measurements","note":"A source-named dated measurement, never combined with another source.","records_observed":0,"source":"pith","source_observed_at":"2026-07-10T15:47:23.111769Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"2208.14325","last_updated":"2022-08-30T15:05:34Z","snapshot_observed_at":"2026-08-02T08:22:22.343975Z","submitted_at":"2022-08-30T15:05:34Z","title":"The massless three-loop Wilson coefficients for the deep-inelastic structure functions $F_2, F_L, xF_3$ and $g_1$","version":1},"cited_work":{"arxiv_id":"2208.14325","doi":null,"metadata_source":"pith","pith_arxiv_id":"2208.14325","snapshot_observed_at":"2026-07-10T15:47:23.111769Z","title":"Bl¨ umlein, P","venue":"hep-ph","work_id":"3fefa6a8-4c39-416b-ac73-c694ed71c638","year":2022},"citing_paper":{"arxiv_id":"2507.07175","last_updated":"2026-04-19T20:16:30Z","snapshot_observed_at":"2026-07-06T21:54:43.509700Z","submitted_at":"2025-07-09T18:00:02Z","title":"Polarized Deep Inelastic Scattering as $x \\to 1$ using Soft Collinear Effective Theory","version":3},"reference_index":53,"source":"pdf_text","source_observed_at":"2026-05-19T05:33:43.406686Z"},"links":{"cited_paper":"/paper/2208.14325","citing_paper":"/paper/2507.07175"},"observation_digest":"sha256:caa6848192988bad5bd96e6d64203b6a66b2344afcbe9322a97439e5c45c8099","observation_id":"7bd10856-05f7-4dd9-b59a-269bbe2df8d9","resolution":{"observed_at":"2026-05-19T05:37:05.621523Z","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":"2208.14325","last_updated":"2022-08-30T15:05:34Z","snapshot_observed_at":"2026-08-02T08:22:22.343975Z","submitted_at":"2022-08-30T15:05:34Z","title":"The massless three-loop Wilson coefficients for the deep-inelastic structure functions $F_2, F_L, xF_3$ and $g_1$","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2208.14325","snapshot_observed_at":"2026-08-06T10:24:37.775546Z","title":"Bl¨ umlein, P","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2508.00195","last_updated":"2025-07-31T22:28:37Z","snapshot_observed_at":"2026-08-06T10:24:31.852349Z","submitted_at":"2025-07-31T22:28:37Z","title":"Analytic Solution for the Helicity Evolution Equations at Small $x$ and Large $N_c\\&N_f$","version":1},"reference_index":99,"source":"pdf_text","source_observed_at":"2026-08-06T10:24:37.775546Z"},"links":{"cited_paper":"/paper/2208.14325","citing_paper":"/paper/2508.00195"},"observation_digest":"sha256:a5261ca684dafae88179c147a500617c5c517277871563939b71ff233398f6cb","observation_id":"0b09e684-d5dd-452a-8483-95c4b3bbb153","resolution":{"observed_at":"2026-08-06T10:24:37.775546Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2208.14325","last_updated":"2022-08-30T15:05:34Z","snapshot_observed_at":"2026-08-02T08:22:22.343975Z","submitted_at":"2022-08-30T15:05:34Z","title":"The massless three-loop Wilson coefficients for the deep-inelastic structure functions $F_2, F_L, xF_3$ and $g_1$","version":1},"cited_work":{"arxiv_id":"2208.14325","doi":null,"metadata_source":"pith","pith_arxiv_id":"2208.14325","snapshot_observed_at":"2026-07-10T15:47:23.111769Z","title":"Bl¨ umlein, P","venue":"hep-ph","work_id":"3fefa6a8-4c39-416b-ac73-c694ed71c638","year":2022},"citing_paper":{"arxiv_id":"2509.03400","last_updated":"2026-05-05T09:50:41Z","snapshot_observed_at":"2026-07-06T22:23:00.681940Z","submitted_at":"2025-09-03T15:24:04Z","title":"Entanglement entropy, Monte Carlo event generators, and soft gluons DIScovery","version":2},"reference_index":45,"source":"pdf_text","source_observed_at":"2026-05-18T19:18:05.909669Z"},"links":{"cited_paper":"/paper/2208.14325","citing_paper":"/paper/2509.03400"},"observation_digest":"sha256:de24f8096577b0a28929a83423a9626a572baa273e4d493e037a575a7932b548","observation_id":"22da85d3-e729-426a-ab7c-cbf4cc851e41","resolution":{"observed_at":"2026-05-18T19:21:49.142199Z","resolver_source":"arxiv_id","status":"metadata_mismatch"},"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":"2208.14325","last_updated":"2022-08-30T15:05:34Z","snapshot_observed_at":"2026-08-02T08:22:22.343975Z","submitted_at":"2022-08-30T15:05:34Z","title":"The massless three-loop Wilson coefficients for the deep-inelastic structure functions $F_2, F_L, xF_3$ and $g_1$","version":1},"cited_work":{"arxiv_id":"2208.14325","doi":null,"metadata_source":"pith","pith_arxiv_id":"2208.14325","snapshot_observed_at":"2026-07-10T15:47:23.111769Z","title":"Bl¨ umlein, P","venue":"hep-ph","work_id":"3fefa6a8-4c39-416b-ac73-c694ed71c638","year":2022},"citing_paper":{"arxiv_id":"2509.17596","last_updated":"2026-06-18T09:31:35Z","snapshot_observed_at":"2026-08-04T15:52:34.995255Z","submitted_at":"2025-09-22T11:18:39Z","title":"Energy Correlators Resolving Proton Spin","version":5},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-05-21T22:52:40.921579Z"},"links":{"cited_paper":"/paper/2208.14325","citing_paper":"/paper/2509.17596"},"observation_digest":"sha256:8e16b8dd06bf4f5ab17d9b0e9dad62e010e0c38260f6c408695267b724ac6919","observation_id":"55c67949-4467-42fd-ad40-7add592f0fd0","resolution":{"observed_at":"2026-05-21T22:54:25.016956Z","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":"2208.14325","last_updated":"2022-08-30T15:05:34Z","snapshot_observed_at":"2026-08-02T08:22:22.343975Z","submitted_at":"2022-08-30T15:05:34Z","title":"The massless three-loop Wilson coefficients for the deep-inelastic structure functions $F_2, F_L, xF_3$ and $g_1$","version":1},"cited_work":{"arxiv_id":"2208.14325","doi":null,"metadata_source":"pith","pith_arxiv_id":"2208.14325","snapshot_observed_at":"2026-07-10T15:47:23.111769Z","title":"Bl¨ umlein, P","venue":"hep-ph","work_id":"3fefa6a8-4c39-416b-ac73-c694ed71c638","year":2022},"citing_paper":{"arxiv_id":"2605.10284","last_updated":"2026-05-29T14:48:36Z","snapshot_observed_at":"2026-08-06T21:58:38.920070Z","submitted_at":"2026-05-11T09:44:34Z","title":"Four-loop anomalous dimension of flavor non-singlet quark operator of twist two and Lorentz spin N for general gauge group: transcendental part","version":1},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-05-12T05:24:57.121356Z"},"links":{"cited_paper":"/paper/2208.14325","citing_paper":"/paper/2605.10284"},"observation_digest":"sha256:39f9d942ace7c315c433513b9305e339e99d411003cc01ee97a103e175136363","observation_id":"1b3580e0-e8b9-4831-a251-055a5ac7b778","resolution":{"observed_at":"2026-05-12T05:26:24.354036Z","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":"2208.14325","last_updated":"2022-08-30T15:05:34Z","snapshot_observed_at":"2026-08-02T08:22:22.343975Z","submitted_at":"2022-08-30T15:05:34Z","title":"The massless three-loop Wilson coefficients for the deep-inelastic structure functions $F_2, F_L, xF_3$ and $g_1$","version":1},"cited_work":{"arxiv_id":"2208.14325","doi":null,"metadata_source":"pith","pith_arxiv_id":"2208.14325","snapshot_observed_at":"2026-07-10T15:47:23.111769Z","title":"Bl¨ umlein, P","venue":"hep-ph","work_id":"3fefa6a8-4c39-416b-ac73-c694ed71c638","year":2022},"citing_paper":{"arxiv_id":"2605.10284","last_updated":"2026-05-29T14:48:36Z","snapshot_observed_at":"2026-08-06T21:58:38.920070Z","submitted_at":"2026-05-11T09:44:34Z","title":"Four-loop anomalous dimension of flavor non-singlet quark operator of twist two and Lorentz spin N for general gauge group: transcendental part","version":2},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-06-30T22:42:06.439017Z"},"links":{"cited_paper":"/paper/2208.14325","citing_paper":"/paper/2605.10284"},"observation_digest":"sha256:e36b7d99a6d9ff20402d028faf0326860642c16cb371799bb62a2eef1f0d39cf","observation_id":"331a75cd-244e-4903-a2b0-8b731343dab4","resolution":{"observed_at":"2026-06-30T22:45:07.455370Z","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":"2208.14325","last_updated":"2022-08-30T15:05:34Z","snapshot_observed_at":"2026-08-02T08:22:22.343975Z","submitted_at":"2022-08-30T15:05:34Z","title":"The massless three-loop Wilson coefficients for the deep-inelastic structure functions $F_2, F_L, xF_3$ and $g_1$","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2208.14325","snapshot_observed_at":"2026-07-11T07:37:18.331806Z","title":null,"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":40,"source":"pdf_text","source_observed_at":"2026-07-11T07:37:18.331806Z"},"links":{"cited_paper":"/paper/2208.14325","citing_paper":"/paper/2607.05235"},"observation_digest":"sha256:d49f63b49c6d59f3818bf13c55198eb5c1d3303515ca0e69ae162f0287976696","observation_id":"f849e580-ac4d-4a69-a4fd-14a7ff56ea09","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":"2208.14325","last_updated":"2022-08-30T15:05:34Z","snapshot_observed_at":"2026-08-02T08:22:22.343975Z","submitted_at":"2022-08-30T15:05:34Z","title":"The massless three-loop Wilson coefficients for the deep-inelastic structure functions $F_2, F_L, xF_3$ and $g_1$","version":1},"cited_work":{"arxiv_id":"2208.14325","doi":null,"metadata_source":"pith","pith_arxiv_id":"2208.14325","snapshot_observed_at":"2026-07-10T15:47:23.111769Z","title":"Bl¨ umlein, P","venue":"hep-ph","work_id":"3fefa6a8-4c39-416b-ac73-c694ed71c638","year":2022},"citing_paper":{"arxiv_id":"2607.07908","last_updated":"2026-07-08T20:44:56Z","snapshot_observed_at":"2026-08-04T23:26:17.225716Z","submitted_at":"2026-07-08T20:44:56Z","title":"QCD for electroweak precision measurements: Foundations","version":1},"reference_index":42,"source":"pdf_text","source_observed_at":"2026-07-11T11:50:26.030339Z"},"links":{"cited_paper":"/paper/2208.14325","citing_paper":"/paper/2607.07908"},"observation_digest":"sha256:ea08f715b4dfad131fe32abd0b1d31d664e1f0f4b0ec67947f02f246c271d047","observation_id":"db931118-cc31-46a4-b112-4207286ac754","resolution":{"observed_at":"2026-07-10T15:47:23.113183Z","resolver_source":"local_arxiv","status":"metadata_mismatch"},"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":"2208.14325","last_updated":"2022-08-30T15:05:34Z","snapshot_observed_at":"2026-08-02T08:22:22.343975Z","submitted_at":"2022-08-30T15:05:34Z","title":"The massless three-loop Wilson coefficients for the deep-inelastic structure functions $F_2, F_L, xF_3$ and $g_1$","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2208.14325","snapshot_observed_at":"2026-07-31T10:42:20.365072Z","title":"u mlein J , author Marquard P , 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":87,"source":"arxiv_source","source_observed_at":"2026-07-31T10:42:20.365072Z"},"links":{"cited_paper":"/paper/2208.14325","citing_paper":"/paper/2607.24613"},"observation_digest":"sha256:5260cb11cc65801768608e516247e71fcca6d7eef64cdf4ffd78e6da5ddcd9e2","observation_id":"aa654620-a211-475b-8eda-af3f13d05575","resolution":{"observed_at":"2026-07-31T10:42:20.365072Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"links":{"evidence":"/evidence","html":"/paper/2208.14325/citation-record","integrity":"/paper/2208.14325/integrity","json":"/paper/2208.14325/citation-record.json","paper":"/paper/2208.14325"},"outbound":[],"paper":{"arxiv_id":"2208.14325","last_updated":"2022-08-30T15:05:34Z","latest_version":1,"primary_category":"hep-ph","snapshot_observed_at":"2026-08-02T08:22:22.343975Z","submitted_at":"2022-08-30T15:05:34Z","title":"The massless three-loop Wilson coefficients for the deep-inelastic structure functions $F_2, F_L, xF_3$ and $g_1$"},"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 9 inbound Pith citation observations for arXiv:2208.14325."}