{"as_of":"2026-08-15T10:48:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:327e5b93a1bbb8f1d6a4b71475b1bccd946c67b54b00fbd87bc0b0b6f163cd44","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":2,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":2,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-15T06:32:42.880941+00:00","state":"measured"},{"denominator":2,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":2,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-14T13:35:27.518570Z","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":"2026-08-07T12:48:30.202098Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"1603.06692","last_updated":"2016-03-22T07:28:06Z","snapshot_observed_at":"2026-08-14T22:05:02.421306Z","submitted_at":"2016-03-22T07:28:06Z","title":"Configuration mixings and light-front relativistic quark model predictions for the electroexcitation of the Delta(1232)3/2+, N(1440)1/2+, and Delta(1600)3/2+","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1603.06692","snapshot_observed_at":"2026-08-14T13:35:27.518570Z","title":"Configuration mixings and light-front relativistic quark model predictions for the electroexcitation of the Delta(1232)3/2+, N(1440)1/2+, and Delta(1600)3/2+,","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"1908.05729","last_updated":"2019-08-14T03:25:12Z","snapshot_observed_at":"2026-08-15T09:11:25.696300Z","submitted_at":"2019-08-14T03:25:12Z","title":"Nucleon-to-Resonance Form Factors at Large Photon Virtualities","version":1},"reference_index":66,"source":"pdf_text","source_observed_at":"2026-08-14T13:35:27.518570Z"},"links":{"cited_paper":"/paper/1603.06692","citing_paper":"/paper/1908.05729"},"observation_digest":"sha256:25d048fbc923fd49bb72c28dd75f49ffe6f693e33172b2f18c3be15ef0cdf1ed","observation_id":"534ac89c-0e06-4b29-a80d-f98f0c120d6a","resolution":{"observed_at":"2026-08-14T13:35:27.518570Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1603.06692","last_updated":"2016-03-22T07:28:06Z","snapshot_observed_at":"2026-08-14T22:05:02.421306Z","submitted_at":"2016-03-22T07:28:06Z","title":"Configuration mixings and light-front relativistic quark model predictions for the electroexcitation of the Delta(1232)3/2+, N(1440)1/2+, and Delta(1600)3/2+","version":1},"cited_work":{"arxiv_id":"1603.06692","doi":null,"metadata_source":"pith","pith_arxiv_id":"1603.06692","snapshot_observed_at":"2026-08-07T12:48:30.202098Z","title":"Configuration mixings and light-front relativistic quark model predictions for the electroexcitation of the Delta(1232)3/2+, N(1440)1/2+, and Delta(1600)3/2+","venue":"hep-ph","work_id":"062213b1-72db-4a60-bbca-080cba7cafdf","year":2016},"citing_paper":{"arxiv_id":"2505.23550","last_updated":"2025-06-03T14:24:14Z","snapshot_observed_at":"2026-08-11T13:20:45.906974Z","submitted_at":"2025-05-29T15:27:56Z","title":"Electroexcitation of Nucleon Resonances and the Emergence of Hadron Mass","version":2},"reference_index":136,"source":"pdf_text","source_observed_at":"2026-08-07T12:48:18.373882Z"},"links":{"cited_paper":"/paper/1603.06692","citing_paper":"/paper/2505.23550"},"observation_digest":"sha256:96d6d793bf34021d2f506f3572eb11725bacc211e5bd950b0dbf08accbe0b352","observation_id":"ee1390e1-549c-41dc-bae7-b59469a49be7","resolution":{"observed_at":"2026-08-07T12:48:30.266523Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}}],"links":{"evidence":"/evidence","html":"/paper/1603.06692/citation-record","integrity":"/paper/1603.06692/integrity","json":"/paper/1603.06692/citation-record.json","paper":"/paper/1603.06692"},"outbound":[],"paper":{"arxiv_id":"1603.06692","last_updated":"2016-03-22T07:28:06Z","latest_version":1,"primary_category":"hep-ph","snapshot_observed_at":"2026-08-14T22:05:02.421306Z","submitted_at":"2016-03-22T07:28:06Z","title":"Configuration mixings and light-front relativistic quark model predictions for the electroexcitation of the Delta(1232)3/2+, N(1440)1/2+, and Delta(1600)3/2+"},"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":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"thesis":"As of 15 August 2026, this Paper Citation Record lists 0 of 0 outbound references and 2 inbound Pith citation observations for arXiv:1603.06692."}