{"as_of":"2026-08-20T19:44:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:550b2f045368f78006887d73e24df7c7e0aaa85c24f8bc38f9ec04837353d948","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":1,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":1,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-20T06:33:59.587034+00:00","state":"measured"},{"denominator":1,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":1,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-06T20:58:12.414216Z","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":[{"citation":{"cited_paper":{"arxiv_id":"2208.06455","last_updated":"2022-08-12T18:50:15Z","snapshot_observed_at":"2026-08-16T16:39:29.838417Z","submitted_at":"2022-08-12T18:50:15Z","title":"Skyrme-Hartree-Fock-Bogoliubov mass models on a 3D mesh: II. Time-reversal symmetry breaking","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2208.06455","snapshot_observed_at":"2026-08-06T20:58:12.414216Z","title":"Skyrme–Hartree–Fock–Bogoliubov Mass Models on a 3D Mesh: II. Time-reversal Symmetry Breaking","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2507.01454","last_updated":"2025-07-02T08:13:02Z","snapshot_observed_at":"2026-08-14T08:52:52.648692Z","submitted_at":"2025-07-02T08:13:02Z","title":"Nuclear Physics Confronts Relativistic Collisions Of Isobars","version":1},"reference_index":94,"source":"pdf_text","source_observed_at":"2026-08-06T20:58:12.414216Z"},"links":{"cited_paper":"/paper/2208.06455","citing_paper":"/paper/2507.01454"},"observation_digest":"sha256:a16efaf9a1ae74fe0a133a205aef533ca0d21d6da9491eaf0c2aee1e98486c3d","observation_id":"501e0331-2810-4a50-9719-d12303ab5a62","resolution":{"observed_at":"2026-08-06T20:58:12.414216Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"links":{"evidence":"/evidence","html":"/paper/2208.06455/citation-record","integrity":"/paper/2208.06455/integrity","json":"/paper/2208.06455/citation-record.json","paper":"/paper/2208.06455"},"outbound":[],"paper":{"arxiv_id":"2208.06455","last_updated":"2022-08-12T18:50:15Z","latest_version":1,"primary_category":"nucl-th","snapshot_observed_at":"2026-08-16T16:39:29.838417Z","submitted_at":"2022-08-12T18:50:15Z","title":"Skyrme-Hartree-Fock-Bogoliubov mass models on a 3D mesh: II. Time-reversal symmetry breaking"},"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":"2026-08-20T06:33:59.587034+00:00","source":"crossref"},{"observed_at":"2026-08-20T06:33:54.927442+00:00","source":"retraction_watch"}],"thesis":"As of 20 August 2026, this Paper Citation Record lists 0 of 0 outbound references and 1 inbound Pith citation observation for arXiv:2208.06455."}