{"as_of":"2026-08-15T01:48:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:0f079529fc1bee525841e9da14e3268fe347ac70f45696c174843776b4ed68e6","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":"2026-08-14T06:32:32.682623+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":"2026-08-07T13:27:03.814666Z","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":"2026-05-17T02:18:52.719587Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"2403.18214","last_updated":"2024-03-27T02:52:16Z","snapshot_observed_at":"2026-08-13T00:44:12.948337Z","submitted_at":"2024-03-27T02:52:16Z","title":"Parity doublet model for baryon octets: ground states saturated by good diquarks and the role of bad diquarks for excited states","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2403.18214","snapshot_observed_at":"2026-08-07T13:27:03.814666Z","title":null,"venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2505.21970","last_updated":"2025-07-02T07:03:18Z","snapshot_observed_at":"2026-08-12T16:37:10.549348Z","submitted_at":"2025-05-28T04:48:19Z","title":"Constraints on the strength of first-order phase transition and its relation to nucleon mass","version":2},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-08-07T13:27:03.814666Z"},"links":{"cited_paper":"/paper/2403.18214","citing_paper":"/paper/2505.21970"},"observation_digest":"sha256:edc4cb8f9a07aae0bb715bc2c98d83ccff201896baa1a20c7dee42e43d12f695","observation_id":"c6e67ff6-d38e-43da-bcbf-9083c825deaf","resolution":{"observed_at":"2026-08-07T13:27:03.814666Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2403.18214","last_updated":"2024-03-27T02:52:16Z","snapshot_observed_at":"2026-08-13T00:44:12.948337Z","submitted_at":"2024-03-27T02:52:16Z","title":"Parity doublet model for baryon octets: ground states saturated by good diquarks and the role of bad diquarks for excited states","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2403.18214","snapshot_observed_at":"2026-08-05T11:21:41.776237Z","title":null,"venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2509.03008","last_updated":"2025-09-03T04:35:54Z","snapshot_observed_at":"2026-08-09T19:09:00.742011Z","submitted_at":"2025-09-03T04:35:54Z","title":"Origin of nucleon mass in the light of PSR J0614-3329 with quark-hadron crossover","version":1},"reference_index":38,"source":"pdf_text","source_observed_at":"2026-08-05T11:21:41.776237Z"},"links":{"cited_paper":"/paper/2403.18214","citing_paper":"/paper/2509.03008"},"observation_digest":"sha256:843bf54d88c1e2053af84e968560a5d8591f33e70e89f8513aa7e2d053f54624","observation_id":"9a07a137-67c9-4b65-8793-aa0c3b8202bf","resolution":{"observed_at":"2026-08-05T11:21:41.776237Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2403.18214","last_updated":"2024-03-27T02:52:16Z","snapshot_observed_at":"2026-08-13T00:44:12.948337Z","submitted_at":"2024-03-27T02:52:16Z","title":"Parity doublet model for baryon octets: ground states saturated by good diquarks and the role of bad diquarks for excited states","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2403.18214","snapshot_observed_at":"2026-08-05T11:21:17.477323Z","title":null,"venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2509.03138","last_updated":"2025-09-03T08:45:02Z","snapshot_observed_at":"2026-08-09T09:49:16.664450Z","submitted_at":"2025-09-03T08:45:02Z","title":"Suppression of dynamical momentum-space shell by chiral symmetry","version":1},"reference_index":58,"source":"pdf_text","source_observed_at":"2026-08-05T11:21:17.477323Z"},"links":{"cited_paper":"/paper/2403.18214","citing_paper":"/paper/2509.03138"},"observation_digest":"sha256:2727d6710c29867d08ddae1e8ec528b55177cc2cdc5272580d8134cadc0b1ea3","observation_id":"81f57cb7-554d-4846-8669-4ad02aeb203e","resolution":{"observed_at":"2026-08-05T11:21:17.477323Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2403.18214","last_updated":"2024-03-27T02:52:16Z","snapshot_observed_at":"2026-08-13T00:44:12.948337Z","submitted_at":"2024-03-27T02:52:16Z","title":"Parity doublet model for baryon octets: ground states saturated by good diquarks and the role of bad diquarks for excited states","version":1},"cited_work":{"arxiv_id":"2403.18214","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2403.18214","snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":null,"venue":null,"work_id":"f3b3b6e6-9998-4bec-98dd-0c392c2db153","year":2024},"citing_paper":{"arxiv_id":"2512.03894","last_updated":"2025-12-03T15:43:22Z","snapshot_observed_at":"2026-08-15T00:39:14.770860Z","submitted_at":"2025-12-03T15:43:22Z","title":"Kinetic Mixing and Axial Charges in the Parity-Doublet Model","version":1},"reference_index":68,"source":"pdf_text","source_observed_at":"2026-05-17T02:15:36.201839Z"},"links":{"cited_paper":"/paper/2403.18214","citing_paper":"/paper/2512.03894"},"observation_digest":"sha256:17973b9aa321880221787f169ea1241e0c2b3fcf82b8795ab2ee38694e3afa8a","observation_id":"86ab67b2-9dfa-467a-aa4c-8c9ee52b34a6","resolution":{"observed_at":"2026-05-17T02:18:52.721194Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}}],"links":{"evidence":"/evidence","html":"/paper/2403.18214/citation-record","integrity":"/paper/2403.18214/integrity","json":"/paper/2403.18214/citation-record.json","paper":"/paper/2403.18214"},"outbound":[],"paper":{"arxiv_id":"2403.18214","last_updated":"2024-03-27T02:52:16Z","latest_version":1,"primary_category":"hep-ph","snapshot_observed_at":"2026-08-13T00:44:12.948337Z","submitted_at":"2024-03-27T02:52:16Z","title":"Parity doublet model for baryon octets: ground states saturated by good diquarks and the role of bad diquarks for excited states"},"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":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"thesis":"As of 15 August 2026, this Paper Citation Record lists 0 of 0 outbound references and 4 inbound Pith citation observations for arXiv:2403.18214."}