{"as_of":"2026-08-23T14:59:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:0194e702b3ff3c70e85eabc71032e6641bb84e57649eb6717504f7a5975596be","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":"2026-08-23T06:30:58.430688+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":"2026-08-15T21:18:04.498160Z","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":"2026-08-06T21:10:30.657431Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"2010.05915","last_updated":"2021-02-13T10:14:54Z","snapshot_observed_at":"2026-08-20T04:06:13.813736Z","submitted_at":"2020-10-12T18:00:01Z","title":"The Present and Future of Four Top Operators","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2010.05915","snapshot_observed_at":"2026-08-15T21:18:04.498160Z","title":"Banelli, E","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2505.10381","last_updated":"2025-05-15T15:03:06Z","snapshot_observed_at":"2026-08-17T19:27:36.407454Z","submitted_at":"2025-05-15T15:03:06Z","title":"Invariant-mass threshold resummation for the production of four top quarks at the LHC","version":1},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-08-15T21:18:04.498160Z"},"links":{"cited_paper":"/paper/2010.05915","citing_paper":"/paper/2505.10381"},"observation_digest":"sha256:a896eb6bfdb361dc638e9770a0c13f027d5d1886531da18bd6a4d93dc56f6632","observation_id":"e18336f0-f988-45c6-bf46-8b1d168edbfa","resolution":{"observed_at":"2026-08-15T21:18:04.498160Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2010.05915","last_updated":"2021-02-13T10:14:54Z","snapshot_observed_at":"2026-08-20T04:06:13.813736Z","submitted_at":"2020-10-12T18:00:01Z","title":"The Present and Future of Four Top Operators","version":2},"cited_work":{"arxiv_id":"2010.05915","doi":null,"metadata_source":"pith","pith_arxiv_id":"2010.05915","snapshot_observed_at":"2026-08-06T21:10:30.657431Z","title":"The Present and Future of Four Top Operators","venue":"hep-ph","work_id":"9dbf294d-9af5-4058-bda3-6ba814cc5744","year":2020},"citing_paper":{"arxiv_id":"2507.01137","last_updated":"2026-07-04T15:31:04Z","snapshot_observed_at":"2026-08-20T17:06:35.430256Z","submitted_at":"2025-07-01T18:55:30Z","title":"Constraining four-heavy-quark operators with top-quark, Higgs, and electroweak precision data","version":2},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-06T21:10:20.624102Z"},"links":{"cited_paper":"/paper/2010.05915","citing_paper":"/paper/2507.01137"},"observation_digest":"sha256:ca8cad42f7474c8f6012984cbde008f956f2a1d14876e9892cd9770cf142ac14","observation_id":"88428bf8-fa64-4c82-9981-f2cc06d63979","resolution":{"observed_at":"2026-08-06T21:10:30.662943Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-23T06:30:58.430688+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-23T06:30:58.430688+00:00","source":"crossref"},{"observed_at":"2026-08-23T06:30:53.778098+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2010.05915","last_updated":"2021-02-13T10:14:54Z","snapshot_observed_at":"2026-08-20T04:06:13.813736Z","submitted_at":"2020-10-12T18:00:01Z","title":"The Present and Future of Four Top Operators","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2010.05915","snapshot_observed_at":"2026-08-01T09:38:03.113363Z","title":"Banelli, E","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2607.27323","last_updated":"2026-07-29T18:00:01Z","snapshot_observed_at":"2026-08-19T00:16:39.794895Z","submitted_at":"2026-07-29T18:00:01Z","title":"The inseparable three and four tops","version":1},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-01T09:38:03.113363Z"},"links":{"cited_paper":"/paper/2010.05915","citing_paper":"/paper/2607.27323"},"observation_digest":"sha256:455f4a9fcbeafd5477468605b756dacf28fcb7955fb32c247e4decc877ecc755","observation_id":"2d649532-235d-44aa-b7fc-0400a313ade3","resolution":{"observed_at":"2026-08-01T09:38:03.113363Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2010.05915","last_updated":"2021-02-13T10:14:54Z","snapshot_observed_at":"2026-08-20T04:06:13.813736Z","submitted_at":"2020-10-12T18:00:01Z","title":"The Present and Future of Four Top Operators","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2010.05915","snapshot_observed_at":"2026-08-14T04:24:09.954749Z","title":"Banelli, E","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2608.10064","last_updated":"2026-08-10T18:00:00Z","snapshot_observed_at":"2026-08-15T14:40:33.456912Z","submitted_at":"2026-08-10T18:00:00Z","title":"Electroweak precision observables at NLL order in the SMEFT","version":1},"reference_index":108,"source":"pdf_text","source_observed_at":"2026-08-14T04:24:09.954749Z"},"links":{"cited_paper":"/paper/2010.05915","citing_paper":"/paper/2608.10064"},"observation_digest":"sha256:2de83bcf0bd15ce1d66675007a8f566ae95483efc632703a3536e97f373f33cd","observation_id":"becd7904-0d02-4096-96ae-70425b967698","resolution":{"observed_at":"2026-08-14T04:24:09.954749Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"links":{"evidence":"/evidence","html":"/paper/2010.05915/citation-record","integrity":"/paper/2010.05915/integrity","json":"/paper/2010.05915/citation-record.json","paper":"/paper/2010.05915"},"outbound":[],"paper":{"arxiv_id":"2010.05915","last_updated":"2021-02-13T10:14:54Z","latest_version":2,"primary_category":"hep-ph","snapshot_observed_at":"2026-08-20T04:06:13.813736Z","submitted_at":"2020-10-12T18:00:01Z","title":"The Present and Future of Four Top Operators"},"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":"2026-08-23T06:30:58.430688+00:00","source":"crossref"},{"observed_at":"2026-08-23T06:30:53.778098+00:00","source":"retraction_watch"}],"thesis":"As of 23 August 2026, this Paper Citation Record lists 0 of 0 outbound references and 4 inbound Pith citation observations for arXiv:2010.05915."}