{"as_of":"2026-08-18T22:04:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:3e98eddd5f3eb2174caf36f13e779ea5d1ab5b38dc8f2ed29f2271afddd37274","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":7,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":7,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-18T06:34:40.430872+00:00","state":"measured"},{"denominator":7,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":7,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-12T11:28:57.264975Z","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":"2026-07-01T21:26:13.943903Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"2108.02730","last_updated":"2021-10-27T16:21:28Z","snapshot_observed_at":"2026-08-16T18:04:59.890953Z","submitted_at":"2021-08-05T16:50:23Z","title":"$D^0 D^0 \\pi^+$ mass distribution in the production of the $T_{cc}$ exotic state","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2108.02730","snapshot_observed_at":"2026-08-12T11:28:57.264975Z","title":"Feijoo, W.H","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2411.18257","last_updated":"2024-11-27T11:55:11Z","snapshot_observed_at":"2026-08-12T16:13:37.661002Z","submitted_at":"2024-11-27T11:55:11Z","title":"Production of exotic hadrons in $pp$ and nuclear collisions","version":1},"reference_index":115,"source":"pdf_text","source_observed_at":"2026-08-12T11:28:57.264975Z"},"links":{"cited_paper":"/paper/2108.02730","citing_paper":"/paper/2411.18257"},"observation_digest":"sha256:20699e3efd5e1da0cbabc774bc7b74aa4cadf97f5fc8456dfae565e65f0f9564","observation_id":"b8f96689-ae5d-4405-b50c-b1a7f072e4f1","resolution":{"observed_at":"2026-08-12T11:28:57.264975Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2108.02730","last_updated":"2021-10-27T16:21:28Z","snapshot_observed_at":"2026-08-16T18:04:59.890953Z","submitted_at":"2021-08-05T16:50:23Z","title":"$D^0 D^0 \\pi^+$ mass distribution in the production of the $T_{cc}$ exotic state","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2108.02730","snapshot_observed_at":"2026-08-11T00:18:36.608942Z","title":"D0D0 π+ mass distribution in the production of the Tcc exotic state,","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2412.19597","last_updated":"2025-05-06T09:40:40Z","snapshot_observed_at":"2026-08-17T14:27:12.972889Z","submitted_at":"2024-12-27T11:42:44Z","title":"Composite nature of the $T_{cc}$ state","version":2},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-08-11T00:18:36.608942Z"},"links":{"cited_paper":"/paper/2108.02730","citing_paper":"/paper/2412.19597"},"observation_digest":"sha256:fe4104c4d2e2f870c9026a923f82b4543cc6095727b381c87a60ca85bfdd9824","observation_id":"db3b1622-c47f-4364-94c4-11dddd60fc02","resolution":{"observed_at":"2026-08-11T00:18:36.608942Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2108.02730","last_updated":"2021-10-27T16:21:28Z","snapshot_observed_at":"2026-08-16T18:04:59.890953Z","submitted_at":"2021-08-05T16:50:23Z","title":"$D^0 D^0 \\pi^+$ mass distribution in the production of the $T_{cc}$ exotic state","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2108.02730","snapshot_observed_at":"2026-08-06T18:12:27.272616Z","title":"Feijoo, W","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2507.09191","last_updated":"2025-07-15T05:10:13Z","snapshot_observed_at":"2026-08-14T13:19:15.711951Z","submitted_at":"2025-07-12T08:18:06Z","title":"Production mechanism of doubly charmed exotic mesons $T_{cc}$","version":2},"reference_index":40,"source":"pdf_text","source_observed_at":"2026-08-06T18:12:27.272616Z"},"links":{"cited_paper":"/paper/2108.02730","citing_paper":"/paper/2507.09191"},"observation_digest":"sha256:db0ad7a783ab50c805b693d62c03a8a92fbd82d35785c3ef0f5104db329644ca","observation_id":"884973b2-df24-4fea-bc40-374e416cc639","resolution":{"observed_at":"2026-08-06T18:12:27.272616Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2108.02730","last_updated":"2021-10-27T16:21:28Z","snapshot_observed_at":"2026-08-16T18:04:59.890953Z","submitted_at":"2021-08-05T16:50:23Z","title":"$D^0 D^0 \\pi^+$ mass distribution in the production of the $T_{cc}$ exotic state","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2108.02730","snapshot_observed_at":"2026-08-05T16:10:10.168563Z","title":"Feijoo, W","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2508.19007","last_updated":"2025-08-26T13:05:08Z","snapshot_observed_at":"2026-08-16T08:31:55.818909Z","submitted_at":"2025-08-26T13:05:08Z","title":"$T_{bc\\bar s}$ states in the process $\\Upsilon \\to D^{-} \\bar B^{0} D_s^{+}$","version":1},"reference_index":61,"source":"pdf_text","source_observed_at":"2026-08-05T16:10:10.168563Z"},"links":{"cited_paper":"/paper/2108.02730","citing_paper":"/paper/2508.19007"},"observation_digest":"sha256:c0604383c86b66dabe786c8501e73684d82a03c14b4b37f9098bfd100a8a79f1","observation_id":"7f2a6285-6b01-4908-be4b-36e4a5e02605","resolution":{"observed_at":"2026-08-05T16:10:10.168563Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2108.02730","last_updated":"2021-10-27T16:21:28Z","snapshot_observed_at":"2026-08-16T18:04:59.890953Z","submitted_at":"2021-08-05T16:50:23Z","title":"$D^0 D^0 \\pi^+$ mass distribution in the production of the $T_{cc}$ exotic state","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2108.02730","snapshot_observed_at":"2026-08-05T14:23:56.331893Z","title":"Feijoo, W","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2508.21474","last_updated":"2025-09-08T10:50:00Z","snapshot_observed_at":"2026-08-17T14:31:19.479507Z","submitted_at":"2025-08-29T09:58:21Z","title":"Prediction of $QQqq\\bar{s}$ molecular pentaquarks within the extended local hidden gauge approach","version":2},"reference_index":77,"source":"pdf_text","source_observed_at":"2026-08-05T14:23:56.331893Z"},"links":{"cited_paper":"/paper/2108.02730","citing_paper":"/paper/2508.21474"},"observation_digest":"sha256:0252639a6f080c1a53831e92257f6e84bbdcabc20176fc40c7b47a607eb50c7c","observation_id":"236337b5-88ae-440d-a400-6adbd4ae5e74","resolution":{"observed_at":"2026-08-05T14:23:56.331893Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2108.02730","last_updated":"2021-10-27T16:21:28Z","snapshot_observed_at":"2026-08-16T18:04:59.890953Z","submitted_at":"2021-08-05T16:50:23Z","title":"$D^0 D^0 \\pi^+$ mass distribution in the production of the $T_{cc}$ exotic state","version":3},"cited_work":{"arxiv_id":"2108.02730","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2108.02730","snapshot_observed_at":"2026-07-01T21:26:13.943903Z","title":"Feijoo, W","venue":null,"work_id":"48fb0701-1d25-4da1-ba5b-c69dad724408","year":2021},"citing_paper":{"arxiv_id":"2605.21205","last_updated":"2026-05-20T14:03:28Z","snapshot_observed_at":"2026-08-16T21:40:27.763180Z","submitted_at":"2026-05-20T14:03:28Z","title":"Comprehensive study of hidden charm pentaquarks with an improved unitarization method","version":1},"reference_index":32,"source":"pdf_text","source_observed_at":"2026-05-21T04:10:31.648385Z"},"links":{"cited_paper":"/paper/2108.02730","citing_paper":"/paper/2605.21205"},"observation_digest":"sha256:45249b66d816670729626eee1f47e4400c0f9cd9922840322d9edb002cdd9615","observation_id":"4aa0b305-5763-477f-b0e8-e59b4963be09","resolution":{"observed_at":"2026-05-21T04:13:56.829385Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-18T06:34:40.430872+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-18T06:34:40.430872+00:00","source":"crossref"},{"observed_at":"2026-08-18T06:34:34.496301+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2108.02730","last_updated":"2021-10-27T16:21:28Z","snapshot_observed_at":"2026-08-16T18:04:59.890953Z","submitted_at":"2021-08-05T16:50:23Z","title":"$D^0 D^0 \\pi^+$ mass distribution in the production of the $T_{cc}$ exotic state","version":3},"cited_work":{"arxiv_id":"2108.02730","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2108.02730","snapshot_observed_at":"2026-07-01T21:26:13.943903Z","title":"Feijoo, W","venue":null,"work_id":"48fb0701-1d25-4da1-ba5b-c69dad724408","year":2021},"citing_paper":{"arxiv_id":"2606.01177","last_updated":"2026-05-31T11:33:48Z","snapshot_observed_at":"2026-08-02T07:03:48.516503Z","submitted_at":"2026-05-31T11:33:48Z","title":"Systematic Study of Coupled-Channel Dynamics in Doubly Heavy Hadronic Molecules","version":1},"reference_index":57,"source":"pdf_text","source_observed_at":"2026-06-28T17:12:34.273366Z"},"links":{"cited_paper":"/paper/2108.02730","citing_paper":"/paper/2606.01177"},"observation_digest":"sha256:13630b78c19b279318593d26d78c76ae36228af21a0355b4785b99824954b5fc","observation_id":"81781a9c-492d-410c-baf1-5977030279da","resolution":{"observed_at":"2026-07-01T21:26:13.945605Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-18T06:34:40.430872+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-18T06:34:40.430872+00:00","source":"crossref"},{"observed_at":"2026-08-18T06:34:34.496301+00:00","source":"retraction_watch"}],"state":"measured"}}],"links":{"evidence":"/evidence","html":"/paper/2108.02730/citation-record","integrity":"/paper/2108.02730/integrity","json":"/paper/2108.02730/citation-record.json","paper":"/paper/2108.02730"},"outbound":[],"paper":{"arxiv_id":"2108.02730","last_updated":"2021-10-27T16:21:28Z","latest_version":3,"primary_category":"hep-ph","snapshot_observed_at":"2026-08-16T18:04:59.890953Z","submitted_at":"2021-08-05T16:50:23Z","title":"$D^0 D^0 \\pi^+$ mass distribution in the production of the $T_{cc}$ exotic state"},"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":"2026-08-18T06:34:40.430872+00:00","source":"crossref"},{"observed_at":"2026-08-18T06:34:34.496301+00:00","source":"retraction_watch"}],"thesis":"As of 18 August 2026, this Paper Citation Record lists 0 of 0 outbound references and 7 inbound Pith citation observations for arXiv:2108.02730."}