{"as_of":"2026-08-14T11:28:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:d8867a808bb42d32c176a25a0a5f6b7704861cb63fc610531da948d26fe01191","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":"2026-08-14T11:09:21.777052Z","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":"2026-05-16T22:32:54.277065Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"1606.06054","last_updated":"2016-09-20T05:43:21Z","snapshot_observed_at":"2026-07-06T05:00:33.838934Z","submitted_at":"2016-06-20T10:21:19Z","title":"$B^0-\\bar{B}^0$ Mixing at Next-to-Leading Order","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1606.06054","snapshot_observed_at":"2026-08-14T11:09:21.777052Z","title":null,"venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"1908.09713","last_updated":"2019-09-05T15:13:15Z","snapshot_observed_at":"2026-08-14T11:01:38.579431Z","submitted_at":"2019-08-26T14:48:00Z","title":"Constraints on New Physics from $B$ mesons","version":2},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-14T11:09:21.777052Z"},"links":{"cited_paper":"/paper/1606.06054","citing_paper":"/paper/1908.09713"},"observation_digest":"sha256:4cef04ee9b6f07127c850cfa7f360034f2e70a8d81092b65c75353d0feb95ff2","observation_id":"62214690-3171-4265-b0ec-0af2c6dba754","resolution":{"observed_at":"2026-08-14T11:09:21.777052Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1606.06054","last_updated":"2016-09-20T05:43:21Z","snapshot_observed_at":"2026-07-06T05:00:33.838934Z","submitted_at":"2016-06-20T10:21:19Z","title":"$B^0-\\bar{B}^0$ Mixing at Next-to-Leading Order","version":2},"cited_work":{"arxiv_id":"1606.06054","doi":null,"metadata_source":"pith","pith_arxiv_id":"1606.06054","snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"$B^0-\\bar{B}^0$ Mixing at Next-to-Leading Order","venue":"hep-ph","work_id":"f55f6061-2053-44f9-80ae-e7d4337415d8","year":2016},"citing_paper":{"arxiv_id":"2411.18639","last_updated":"2026-01-29T02:46:40Z","snapshot_observed_at":"2026-08-13T09:46:11.725160Z","submitted_at":"2024-11-25T03:52:24Z","title":"Averages of $b$-hadron, $c$-hadron, and $\\tau$-lepton properties as of 2023","version":2},"reference_index":173,"source":"pdf_text","source_observed_at":"2026-05-16T22:32:53.560690Z"},"links":{"cited_paper":"/paper/1606.06054","citing_paper":"/paper/2411.18639"},"observation_digest":"sha256:68cb2514305d37fff84aaa40c993d2636bc69b70943009d30aac6d8d39ea993a","observation_id":"8e82d454-4af4-457a-aaf4-461e45e70de5","resolution":{"observed_at":"2026-05-16T22:32:54.278447Z","resolver_source":"local_arxiv","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"}},{"citation":{"cited_paper":{"arxiv_id":"1606.06054","last_updated":"2016-09-20T05:43:21Z","snapshot_observed_at":"2026-07-06T05:00:33.838934Z","submitted_at":"2016-06-20T10:21:19Z","title":"$B^0-\\bar{B}^0$ Mixing at Next-to-Leading Order","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1606.06054","snapshot_observed_at":"2026-08-11T13:24:31.610893Z","title":null,"venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2412.13270","last_updated":"2025-04-15T15:56:51Z","snapshot_observed_at":"2026-08-13T17:18:32.941416Z","submitted_at":"2024-12-17T19:05:05Z","title":"HQET sum rules for matrix elements of dimension-six four-quark operators for meson lifetimes within and beyond the Standard Model","version":3},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-08-11T13:24:31.610893Z"},"links":{"cited_paper":"/paper/1606.06054","citing_paper":"/paper/2412.13270"},"observation_digest":"sha256:6c5e9251f9223c8f460a43bb4673ae0a260937da075f9f8d4604e9c2ab7c76a7","observation_id":"85cd9728-0ccb-47e9-9652-4bb9a37aa60e","resolution":{"observed_at":"2026-08-11T13:24:31.610893Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1606.06054","last_updated":"2016-09-20T05:43:21Z","snapshot_observed_at":"2026-07-06T05:00:33.838934Z","submitted_at":"2016-06-20T10:21:19Z","title":"$B^0-\\bar{B}^0$ Mixing at Next-to-Leading Order","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1606.06054","snapshot_observed_at":"2026-08-11T11:50:10.825127Z","title":null,"venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2412.14947","last_updated":"2024-12-19T15:27:12Z","snapshot_observed_at":"2026-08-14T09:06:04.023803Z","submitted_at":"2024-12-19T15:27:12Z","title":"Constraining $B$-Mesogenesis models with inclusive and exclusive decays","version":1},"reference_index":37,"source":"pdf_text","source_observed_at":"2026-08-11T11:50:10.825127Z"},"links":{"cited_paper":"/paper/1606.06054","citing_paper":"/paper/2412.14947"},"observation_digest":"sha256:ce0a70365baa7bd34fce5fa12e72b6c1677f853fdfc2eb3442456bfeaae37e61","observation_id":"87757509-ee53-46b4-931c-76f4ad7d5889","resolution":{"observed_at":"2026-08-11T11:50:10.825127Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"links":{"evidence":"/evidence","html":"/paper/1606.06054/citation-record","integrity":"/paper/1606.06054/integrity","json":"/paper/1606.06054/citation-record.json","paper":"/paper/1606.06054"},"outbound":[],"paper":{"arxiv_id":"1606.06054","last_updated":"2016-09-20T05:43:21Z","latest_version":2,"primary_category":"hep-ph","snapshot_observed_at":"2026-07-06T05:00:33.838934Z","submitted_at":"2016-06-20T10:21:19Z","title":"$B^0-\\bar{B}^0$ Mixing at Next-to-Leading Order"},"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 14 August 2026, this Paper Citation Record lists 0 of 0 outbound references and 4 inbound Pith citation observations for arXiv:1606.06054."}