{"as_of":"2026-08-11T21:11:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:8c317c7f286406e3afa23167475762d72372bd9f8e332cc4afb66f4ccea4e440","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":"2026-08-11T06:34:44.6726+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":"2026-08-11T00:36:14.368166Z","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":"2026-07-04T01:49:21.810948Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"2112.12131","last_updated":"2022-06-20T13:05:33Z","snapshot_observed_at":"2026-08-11T15:02:11.795020Z","submitted_at":"2021-12-22T18:46:23Z","title":"Gearing up for the next generation of LFV experiments, via on-shell methods","version":2},"cited_work":{"arxiv_id":"2112.12131","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2112.12131","snapshot_observed_at":"2026-07-04T01:49:21.810948Z","title":"Elias Miro, C","venue":null,"work_id":"bc07e3b2-b525-45ce-b9ef-81ff1dd689ab","year":2022},"citing_paper":{"arxiv_id":"2504.12855","last_updated":"2026-04-24T22:12:29Z","snapshot_observed_at":"2026-07-06T02:11:23.670680Z","submitted_at":"2025-04-17T11:22:34Z","title":"Amplitudes and partial wave unitarity bounds","version":2},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-05-22T19:18:01.919414Z"},"links":{"cited_paper":"/paper/2112.12131","citing_paper":"/paper/2504.12855"},"observation_digest":"sha256:f410b02e403733306ad04a960d70ae8aa6638c5ab0cf0a16371832ddeba3a2fc","observation_id":"dadd0a07-d0d6-4983-8b48-26effda2769c","resolution":{"observed_at":"2026-05-22T19:21:58.958918Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2112.12131","last_updated":"2022-06-20T13:05:33Z","snapshot_observed_at":"2026-08-11T15:02:11.795020Z","submitted_at":"2021-12-22T18:46:23Z","title":"Gearing up for the next generation of LFV experiments, via on-shell methods","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2112.12131","snapshot_observed_at":"2026-08-04T09:47:57.157348Z","title":"Elias Miro, C","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2510.13953","last_updated":"2026-07-18T09:58:36Z","snapshot_observed_at":"2026-08-05T03:57:41.891474Z","submitted_at":"2025-10-15T18:00:02Z","title":"Positivity and partial wave unitarity bounds on ALP theories via amplitude methods","version":2},"reference_index":66,"source":"pdf_text","source_observed_at":"2026-08-04T09:47:57.157348Z"},"links":{"cited_paper":"/paper/2112.12131","citing_paper":"/paper/2510.13953"},"observation_digest":"sha256:820bc907b0c6c8f1e1106184e7cd175af4742731ded1c9cf417a34743f1846a6","observation_id":"d888bc24-c794-48e1-a70e-07130524c35b","resolution":{"observed_at":"2026-08-04T09:47:57.157348Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2112.12131","last_updated":"2022-06-20T13:05:33Z","snapshot_observed_at":"2026-08-11T15:02:11.795020Z","submitted_at":"2021-12-22T18:46:23Z","title":"Gearing up for the next generation of LFV experiments, via on-shell methods","version":2},"cited_work":{"arxiv_id":"2112.12131","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2112.12131","snapshot_observed_at":"2026-07-04T01:49:21.810948Z","title":"Elias Miro, C","venue":null,"work_id":"bc07e3b2-b525-45ce-b9ef-81ff1dd689ab","year":2022},"citing_paper":{"arxiv_id":"2606.19202","last_updated":"2026-06-17T15:40:05Z","snapshot_observed_at":"2026-08-08T13:40:30.316163Z","submitted_at":"2026-06-17T15:40:05Z","title":"Renormalization of the SMEFT to Dimension Eight: Fermionic Interactions II","version":1},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-06-26T20:15:25.735943Z"},"links":{"cited_paper":"/paper/2112.12131","citing_paper":"/paper/2606.19202"},"observation_digest":"sha256:877b0981d33e5a2a2adb1fd7f28025b976d59b4345e850352fb252d650331a14","observation_id":"5af0766a-1e93-4b97-9e2f-cdd65c9be250","resolution":{"observed_at":"2026-07-04T01:49:21.812352Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2112.12131","last_updated":"2022-06-20T13:05:33Z","snapshot_observed_at":"2026-08-11T15:02:11.795020Z","submitted_at":"2021-12-22T18:46:23Z","title":"Gearing up for the next generation of LFV experiments, via on-shell methods","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2112.12131","snapshot_observed_at":"2026-08-11T00:36:14.368166Z","title":"Elias Miro, C","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2608.07657","last_updated":"2026-08-07T18:00:01Z","snapshot_observed_at":"2026-08-11T20:13:05.534516Z","submitted_at":"2026-08-07T18:00:01Z","title":"Neutrinoless Double-Beta Decays from Operator Mixing","version":1},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-08-11T00:36:14.368166Z"},"links":{"cited_paper":"/paper/2112.12131","citing_paper":"/paper/2608.07657"},"observation_digest":"sha256:1eee1a5cbbd7b5fc6af043ea5781c7a70ecb202a865582eca483ca8fd2b1f4f5","observation_id":"12f122df-8434-4741-abd6-09b17cbb8acd","resolution":{"observed_at":"2026-08-11T00:36:14.368166Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"links":{"evidence":"/evidence","html":"/paper/2112.12131/citation-record","integrity":"/paper/2112.12131/integrity","json":"/paper/2112.12131/citation-record.json","paper":"/paper/2112.12131"},"outbound":[],"paper":{"arxiv_id":"2112.12131","last_updated":"2022-06-20T13:05:33Z","latest_version":2,"primary_category":"hep-ph","snapshot_observed_at":"2026-08-11T15:02:11.795020Z","submitted_at":"2021-12-22T18:46:23Z","title":"Gearing up for the next generation of LFV experiments, via on-shell methods"},"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":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"thesis":"As of 11 August 2026, this Paper Citation Record lists 0 of 0 outbound references and 4 inbound Pith citation observations for arXiv:2112.12131."}