{"as_of":"2026-08-10T22:13:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:f23073a5dbb2748f0333ffc87259614bef3c0965298fe331176fa38c36bbcb57","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":"2026-08-10T06:31:04.303077+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":"2026-08-10T18:31:50.613742Z","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":"2026-07-02T04:26:35.237270Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"2306.01848","last_updated":"2025-06-20T07:51:45Z","snapshot_observed_at":"2026-07-06T15:37:23.958419Z","submitted_at":"2023-06-02T18:09:34Z","title":"Quark mass dependence of the $D_{s0}^*(2317)$ and $D_{s1}(2460)$ resonances","version":6},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2306.01848","snapshot_observed_at":"2026-08-10T18:31:50.613742Z","title":"Gil-Dom ´ınguez and R","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2501.11358","last_updated":"2025-07-03T02:48:14Z","snapshot_observed_at":"2026-08-10T20:38:51.122984Z","submitted_at":"2025-01-20T09:40:15Z","title":"Implication of the existence of $J^{PC}=0^{--}$ $\\bar{D}_sDK$ bound state on nature of $D_{s0}^*(2317)$ and new configuration of exotic state","version":2},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-10T18:31:50.613742Z"},"links":{"cited_paper":"/paper/2306.01848","citing_paper":"/paper/2501.11358"},"observation_digest":"sha256:47eef7fc42f0f1df7ba0951d091d4f6d49f2fda683bde9f462efd6425a86673b","observation_id":"bf7fd007-cbda-4001-8e21-23797e4050d9","resolution":{"observed_at":"2026-08-10T18:31:50.613742Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2306.01848","last_updated":"2025-06-20T07:51:45Z","snapshot_observed_at":"2026-07-06T15:37:23.958419Z","submitted_at":"2023-06-02T18:09:34Z","title":"Quark mass dependence of the $D_{s0}^*(2317)$ and $D_{s1}(2460)$ resonances","version":6},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2306.01848","snapshot_observed_at":"2026-08-09T19:08:57.249624Z","title":"Gil-Dom ´ınguez and R","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2502.00438","last_updated":"2025-02-01T14:14:44Z","snapshot_observed_at":"2026-08-09T20:50:17.545358Z","submitted_at":"2025-02-01T14:14:44Z","title":"Effect of a repulsive three-body interaction on the $DD^{(*)}K$ molecule","version":1},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-08-09T19:08:57.249624Z"},"links":{"cited_paper":"/paper/2306.01848","citing_paper":"/paper/2502.00438"},"observation_digest":"sha256:5b2c10db8a32ca8133739b9ae84c8312326b1805487abb87eb9148afc7227f8f","observation_id":"100fca5c-5694-4607-b4d5-6f0402cad21e","resolution":{"observed_at":"2026-08-09T19:08:57.249624Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2306.01848","last_updated":"2025-06-20T07:51:45Z","snapshot_observed_at":"2026-07-06T15:37:23.958419Z","submitted_at":"2023-06-02T18:09:34Z","title":"Quark mass dependence of the $D_{s0}^*(2317)$ and $D_{s1}(2460)$ resonances","version":6},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2306.01848","snapshot_observed_at":"2026-08-06T21:47:57.414951Z","title":"Gil-Dom ´ınguez and R","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2506.23476","last_updated":"2026-05-26T16:15:23Z","snapshot_observed_at":"2026-08-06T21:38:57.228294Z","submitted_at":"2025-06-30T02:42:57Z","title":"Probing the structure of the $D_{s 0}^*(2317)$ and $X(3872)$ states through correlation functions","version":2},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-08-06T21:47:57.414951Z"},"links":{"cited_paper":"/paper/2306.01848","citing_paper":"/paper/2506.23476"},"observation_digest":"sha256:0d442dd8229a0166411596e5100507f380f75c1dcfbc3c202844ad113fb5bb80","observation_id":"b15628ce-d030-42e4-be0a-9543e18b8a20","resolution":{"observed_at":"2026-08-06T21:47:57.414951Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2306.01848","last_updated":"2025-06-20T07:51:45Z","snapshot_observed_at":"2026-07-06T15:37:23.958419Z","submitted_at":"2023-06-02T18:09:34Z","title":"Quark mass dependence of the $D_{s0}^*(2317)$ and $D_{s1}(2460)$ resonances","version":6},"cited_work":{"arxiv_id":"2306.01848","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2306.01848","snapshot_observed_at":"2026-07-02T04:26:35.237270Z","title":"Gil-Dom ´ınguez and R","venue":null,"work_id":"1c00cf7e-77fc-474a-8bb0-cf7f705bdd82","year":2024},"citing_paper":{"arxiv_id":"2606.03826","last_updated":"2026-06-02T16:08:38Z","snapshot_observed_at":"2026-08-04T14:58:33.300924Z","submitted_at":"2026-06-02T16:08:38Z","title":"Revealing the $D_0^*(2300)$ two-pole structure from lattice data and the SU(3) limit","version":1},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-06-28T09:14:21.956153Z"},"links":{"cited_paper":"/paper/2306.01848","citing_paper":"/paper/2606.03826"},"observation_digest":"sha256:3b9853c558f78aa1dfe2ede0467dc7745710c1a1b719f0adde7b558e2798a2df","observation_id":"b6b4bc16-20ee-4461-869b-285506032574","resolution":{"observed_at":"2026-07-02T04:26:35.238992Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}}],"links":{"evidence":"/evidence","html":"/paper/2306.01848/citation-record","integrity":"/paper/2306.01848/integrity","json":"/paper/2306.01848/citation-record.json","paper":"/paper/2306.01848"},"outbound":[],"paper":{"arxiv_id":"2306.01848","last_updated":"2025-06-20T07:51:45Z","latest_version":6,"primary_category":"hep-ph","snapshot_observed_at":"2026-07-06T15:37:23.958419Z","submitted_at":"2023-06-02T18:09:34Z","title":"Quark mass dependence of the $D_{s0}^*(2317)$ and $D_{s1}(2460)$ resonances"},"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":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"thesis":"As of 10 August 2026, this Paper Citation Record lists 0 of 0 outbound references and 4 inbound Pith citation observations for arXiv:2306.01848."}