{"as_of":"2026-08-13T19:28:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:f72bce29f926a3260e9c6c2c4e317441d8585e47ec07c0450984bc6b6e55d435","coverage":[{"denominator":53,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":53,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-11T19:48:20.617471Z","state":"measured"},{"denominator":56,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":56,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-13T06:32:02.005865+00:00","state":"measured"},{"denominator":3,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":3,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-04T10:26:06.095078Z","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":"2026-05-10T06:26:27.174514Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"2412.06400","last_updated":"2025-03-04T04:39:39Z","snapshot_observed_at":"2026-08-11T19:39:54.876021Z","submitted_at":"2024-12-09T11:30:25Z","title":"Discovery potential of charmonium $2P$ states through the $e^+e^- \\to \\gamma D\\bar{D}$ processes","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2412.06400","snapshot_observed_at":"2026-08-04T10:26:06.095078Z","title":"Gao, R.-Q","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2510.10200","last_updated":"2025-10-11T12:44:18Z","snapshot_observed_at":"2026-08-08T21:15:22.436574Z","submitted_at":"2025-10-11T12:44:18Z","title":"Medium modifications of $1P$-wave charmonia $\\chi_{cJ}(1P)$ in cold nuclear matter","version":1},"reference_index":120,"source":"pdf_text","source_observed_at":"2026-08-04T10:26:06.095078Z"},"links":{"cited_paper":"/paper/2412.06400","citing_paper":"/paper/2510.10200"},"observation_digest":"sha256:808341abbb86aae7a61fe35a7ebbb0b73e04b521da124e7ff60d25aae1566476","observation_id":"15983438-400d-4bac-a9be-7af27e100278","resolution":{"observed_at":"2026-08-04T10:26:06.095078Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2412.06400","last_updated":"2025-03-04T04:39:39Z","snapshot_observed_at":"2026-08-11T19:39:54.876021Z","submitted_at":"2024-12-09T11:30:25Z","title":"Discovery potential of charmonium $2P$ states through the $e^+e^- \\to \\gamma D\\bar{D}$ processes","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2412.06400","snapshot_observed_at":"2026-08-02T21:37:24.347686Z","title":"Gao, R.-Q","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2602.19887","last_updated":"2026-08-05T09:25:10Z","snapshot_observed_at":"2026-08-08T23:09:17.996800Z","submitted_at":"2026-02-23T14:31:47Z","title":"Unquenched Charmonium and Beyond","version":2},"reference_index":237,"source":"pdf_text","source_observed_at":"2026-08-02T21:37:24.347686Z"},"links":{"cited_paper":"/paper/2412.06400","citing_paper":"/paper/2602.19887"},"observation_digest":"sha256:321c2df4a43b10e60a508e3a9fd81581241a26b53e75a9a25e525928f5262189","observation_id":"4f2b687e-247a-4c9e-9a1a-7f874161d37e","resolution":{"observed_at":"2026-08-02T21:37:24.347686Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2412.06400","last_updated":"2025-03-04T04:39:39Z","snapshot_observed_at":"2026-08-11T19:39:54.876021Z","submitted_at":"2024-12-09T11:30:25Z","title":"Discovery potential of charmonium $2P$ states through the $e^+e^- \\to \\gamma D\\bar{D}$ processes","version":2},"cited_work":{"arxiv_id":"2412.06400","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2412.06400","snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Gao, R.-Q","venue":null,"work_id":"849d5d9b-8f76-4db6-ad54-8e9f227f06b5","year":2025},"citing_paper":{"arxiv_id":"2604.17193","last_updated":"2026-07-13T14:16:46Z","snapshot_observed_at":"2026-08-12T04:13:09.009215Z","submitted_at":"2026-04-19T01:50:00Z","title":"Proposed mixing between $2P$ and $1F$ wave charmonia","version":1},"reference_index":78,"source":"pdf_text","source_observed_at":"2026-05-10T06:26:07.997732Z"},"links":{"cited_paper":"/paper/2412.06400","citing_paper":"/paper/2604.17193"},"observation_digest":"sha256:6d503ba4d7286b9d674e16d7d9ed779a6d85e39556bbea9542f8cd604001c204","observation_id":"4fd5f1b0-593a-4d29-9ab1-5c0a352685a4","resolution":{"observed_at":"2026-05-10T06:26:27.175790Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}}],"links":{"evidence":"/evidence","html":"/paper/2412.06400/citation-record","integrity":"/paper/2412.06400/integrity","json":"/paper/2412.06400/citation-record.json","paper":"/paper/2412.06400"},"outbound":[{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-11T19:48:23.060053Z","title":"(2𝑃) ③ 𝜓→𝛾𝜒!#(2𝑃) 𝛾∗ 𝛾 𝜒","venue":null,"work_id":"b2c102cc-212e-4a5b-8e67-0b3e5048b009","year":2010},"citing_paper":{"arxiv_id":"2412.06400","last_updated":"2025-03-04T04:39:39Z","snapshot_observed_at":"2026-08-11T19:39:54.876021Z","submitted_at":"2024-12-09T11:30:25Z","title":"Discovery potential of charmonium $2P$ states through the $e^+e^- \\to \\gamma D\\bar{D}$ processes","version":2},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-08-11T19:48:20.128533Z"},"links":{"citing_paper":"/paper/2412.06400"},"observation_digest":"sha256:68aeeedc3d1c1f0732b4f709b00f7acfb0b06cd427d3052b801c8a33435bddbf","observation_id":"1d8044b5-757f-4289-a695-fed368d8e637","resolution":{"observed_at":"2026-08-11T19:48:23.066313Z","resolver_source":"raw_fallback","status":"malformed_identifier"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ex/0309032","last_updated":"2003-10-31T02:41:22Z","snapshot_observed_at":"2026-08-05T20:18:03.265466Z","submitted_at":"2003-09-08T20:04:28Z","title":"Observation of a narrow charmonium-like state in exclusive B+ -> K+ pi+pi- J/psi decays","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ex/0309032","snapshot_observed_at":"2026-08-11T19:48:20.141767Z","title":null,"venue":null,"work_id":null,"year":2003},"citing_paper":{"arxiv_id":"2412.06400","last_updated":"2025-03-04T04:39:39Z","snapshot_observed_at":"2026-08-11T19:39:54.876021Z","submitted_at":"2024-12-09T11:30:25Z","title":"Discovery potential of charmonium $2P$ states through the $e^+e^- \\to \\gamma D\\bar{D}$ processes","version":2},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-08-11T19:48:20.141767Z"},"links":{"cited_paper":"/paper/hep-ex/0309032","citing_paper":"/paper/2412.06400"},"observation_digest":"sha256:efbeda92501d7c0211a42a6b630e8f1a644d7efcda2621a8726ba7d0daee30ae","observation_id":"bfb1c5db-fd75-4be6-850c-145c96978dcb","resolution":{"observed_at":"2026-08-11T19:48:20.141767Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0505002","last_updated":"2005-09-27T18:06:28Z","snapshot_observed_at":"2026-07-07T04:07:16.252774Z","submitted_at":"2005-04-29T21:23:40Z","title":"Higher Charmonia","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0505002","snapshot_observed_at":"2026-08-11T19:48:20.156415Z","title":"Barnes, S","venue":null,"work_id":null,"year":2005},"citing_paper":{"arxiv_id":"2412.06400","last_updated":"2025-03-04T04:39:39Z","snapshot_observed_at":"2026-08-11T19:39:54.876021Z","submitted_at":"2024-12-09T11:30:25Z","title":"Discovery potential of charmonium $2P$ states through the $e^+e^- \\to \\gamma D\\bar{D}$ processes","version":2},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-08-11T19:48:20.156415Z"},"links":{"cited_paper":"/paper/hep-ph/0505002","citing_paper":"/paper/2412.06400"},"observation_digest":"sha256:e5c6f478c8c04e59ea3069cff4e9d01880a1404974cee488386032b6f253bfa7","observation_id":"1dd9d83e-e3b6-4a97-808f-65ef14250b8f","resolution":{"observed_at":"2026-08-11T19:48:20.156415Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-11T19:48:20.163409Z","title":"Maiani, F","venue":null,"work_id":null,"year":2005},"citing_paper":{"arxiv_id":"2412.06400","last_updated":"2025-03-04T04:39:39Z","snapshot_observed_at":"2026-08-11T19:39:54.876021Z","submitted_at":"2024-12-09T11:30:25Z","title":"Discovery potential of charmonium $2P$ states through the $e^+e^- \\to \\gamma D\\bar{D}$ processes","version":2},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-11T19:48:20.163409Z"},"links":{"citing_paper":"/paper/2412.06400"},"observation_digest":"sha256:1814f87c7ce1c301158dc123b0e4cbab336808c3ee06cad68098d5c29ad8d1f3","observation_id":"10828b9f-a086-4a96-ae86-22234441baeb","resolution":{"observed_at":"2026-08-11T19:48:20.163409Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0511039","last_updated":"2006-03-01T12:31:09Z","snapshot_observed_at":"2026-07-07T04:09:11.749528Z","submitted_at":"2005-11-04T08:46:22Z","title":"A chromomagnetic mechanism for the X(3872) resonance","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0511039","snapshot_observed_at":"2026-08-11T19:48:20.170429Z","title":"Hogaasen, J","venue":null,"work_id":null,"year":2006},"citing_paper":{"arxiv_id":"2412.06400","last_updated":"2025-03-04T04:39:39Z","snapshot_observed_at":"2026-08-11T19:39:54.876021Z","submitted_at":"2024-12-09T11:30:25Z","title":"Discovery potential of charmonium $2P$ states through the $e^+e^- \\to \\gamma D\\bar{D}$ processes","version":2},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-08-11T19:48:20.170429Z"},"links":{"cited_paper":"/paper/hep-ph/0511039","citing_paper":"/paper/2412.06400"},"observation_digest":"sha256:52af98f6cb9b07ba905fd91686da956ae25b5d3b3acea616b40bbc15ff59dffd","observation_id":"51ffff8b-185d-4070-b1f0-4a6bf06923d0","resolution":{"observed_at":"2026-08-11T19:48:20.170429Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0607226","last_updated":"2006-07-20T12:31:07Z","snapshot_observed_at":"2026-08-10T01:27:53.153677Z","submitted_at":"2006-07-20T12:31:07Z","title":"The Possible Heavy Tetraquarks $qQ\\bar q \\bar Q$, $qq\\bar Q \\bar Q$ and $qQ\\bar Q \\bar Q$","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0607226","snapshot_observed_at":"2026-08-11T19:48:20.178983Z","title":"Cui, X.-L","venue":null,"work_id":null,"year":2007},"citing_paper":{"arxiv_id":"2412.06400","last_updated":"2025-03-04T04:39:39Z","snapshot_observed_at":"2026-08-11T19:39:54.876021Z","submitted_at":"2024-12-09T11:30:25Z","title":"Discovery potential of charmonium $2P$ states through the $e^+e^- \\to \\gamma D\\bar{D}$ processes","version":2},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-11T19:48:20.178983Z"},"links":{"cited_paper":"/paper/hep-ph/0607226","citing_paper":"/paper/2412.06400"},"observation_digest":"sha256:26a903dd73566726b09e979ca140e196be78025811396402abbbe053280573ed","observation_id":"f92b302b-7614-420e-b8ea-058c0af31eda","resolution":{"observed_at":"2026-08-11T19:48:20.178983Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0311088","last_updated":"2004-04-28T21:02:34Z","snapshot_observed_at":"2026-07-07T04:01:51.362822Z","submitted_at":"2003-11-07T15:59:05Z","title":"Molecular States of Heavy Quark Mesons","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0311088","snapshot_observed_at":"2026-08-11T19:48:20.188386Z","title":"Wong, Molecular states of heavy quark mesons, Phys","venue":null,"work_id":null,"year":2004},"citing_paper":{"arxiv_id":"2412.06400","last_updated":"2025-03-04T04:39:39Z","snapshot_observed_at":"2026-08-11T19:39:54.876021Z","submitted_at":"2024-12-09T11:30:25Z","title":"Discovery potential of charmonium $2P$ states through the $e^+e^- \\to \\gamma D\\bar{D}$ processes","version":2},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-11T19:48:20.188386Z"},"links":{"cited_paper":"/paper/hep-ph/0311088","citing_paper":"/paper/2412.06400"},"observation_digest":"sha256:6b878920c387dcd35f41a24befb619956563b06891b97069534a39b8d0bdf581","observation_id":"aee01b59-e7b9-45d6-8f44-36ab56e351d6","resolution":{"observed_at":"2026-08-11T19:48:20.188386Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0506141","last_updated":"2005-06-24T19:48:30Z","snapshot_observed_at":"2026-07-07T04:07:41.470689Z","submitted_at":"2005-06-14T19:58:11Z","title":"X(3872): Hadronic Molecules in Effective Field Theory","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0506141","snapshot_observed_at":"2026-08-11T19:48:20.199459Z","title":null,"venue":null,"work_id":null,"year":2006},"citing_paper":{"arxiv_id":"2412.06400","last_updated":"2025-03-04T04:39:39Z","snapshot_observed_at":"2026-08-11T19:39:54.876021Z","submitted_at":"2024-12-09T11:30:25Z","title":"Discovery potential of charmonium $2P$ states through the $e^+e^- \\to \\gamma D\\bar{D}$ processes","version":2},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-11T19:48:20.199459Z"},"links":{"cited_paper":"/paper/hep-ph/0506141","citing_paper":"/paper/2412.06400"},"observation_digest":"sha256:d43553626b85ac1862619a3163e9e2f1068cefbf86258e1786fcc23d9ac957ca","observation_id":"c19a6aa4-d206-4a56-a70d-19161756a210","resolution":{"observed_at":"2026-08-11T19:48:20.199459Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1903.07115","last_updated":"2019-05-21T07:13:28Z","snapshot_observed_at":"2026-08-13T07:08:15.367550Z","submitted_at":"2019-03-17T15:54:07Z","title":"Constructing $J/\\psi$ family with updated data of charmoniumlike $Y$ states","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1903.07115","snapshot_observed_at":"2026-08-11T19:48:20.206774Z","title":"Wang, D.-Y","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2412.06400","last_updated":"2025-03-04T04:39:39Z","snapshot_observed_at":"2026-08-11T19:39:54.876021Z","submitted_at":"2024-12-09T11:30:25Z","title":"Discovery potential of charmonium $2P$ states through the $e^+e^- \\to \\gamma D\\bar{D}$ processes","version":2},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-11T19:48:20.206774Z"},"links":{"cited_paper":"/paper/1903.07115","citing_paper":"/paper/2412.06400"},"observation_digest":"sha256:35d7393dd27503bfaa81f86d87337f1a2dcadd4f0ce9ca9311a8121ebec2de4e","observation_id":"88ee8beb-1a94-41c5-a4b6-3457dcdf1e28","resolution":{"observed_at":"2026-08-11T19:48:20.206774Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ex/0512035","last_updated":"2006-07-07T01:34:02Z","snapshot_observed_at":"2026-08-12T15:31:35.930171Z","submitted_at":"2005-12-15T06:36:03Z","title":"Observation of a chi'_(c2) candidate in gamma gamma --> D Dbar production at Belle","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ex/0512035","snapshot_observed_at":"2026-08-11T19:48:20.213444Z","title":"Uehara et al","venue":null,"work_id":null,"year":2006},"citing_paper":{"arxiv_id":"2412.06400","last_updated":"2025-03-04T04:39:39Z","snapshot_observed_at":"2026-08-11T19:39:54.876021Z","submitted_at":"2024-12-09T11:30:25Z","title":"Discovery potential of charmonium $2P$ states through the $e^+e^- \\to \\gamma D\\bar{D}$ processes","version":2},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-11T19:48:20.213444Z"},"links":{"cited_paper":"/paper/hep-ex/0512035","citing_paper":"/paper/2412.06400"},"observation_digest":"sha256:c53a0cc5fd0e9236777302d70cbddcbc72a87a4b64617d940e94799f1c12eed1","observation_id":"6d2624a6-5702-4d51-aee9-22a940227264","resolution":{"observed_at":"2026-08-11T19:48:20.213444Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0911.3694","last_updated":"2010-03-06T08:27:02Z","snapshot_observed_at":"2026-07-06T02:03:45.474968Z","submitted_at":"2009-11-19T13:52:52Z","title":"X(3915) and X(4350) as new members in P-wave charmonium family","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0911.3694","snapshot_observed_at":"2026-08-11T19:48:20.219070Z","title":"Liu, Z.-G","venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"2412.06400","last_updated":"2025-03-04T04:39:39Z","snapshot_observed_at":"2026-08-11T19:39:54.876021Z","submitted_at":"2024-12-09T11:30:25Z","title":"Discovery potential of charmonium $2P$ states through the $e^+e^- \\to \\gamma D\\bar{D}$ processes","version":2},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-08-11T19:48:20.219070Z"},"links":{"cited_paper":"/paper/0911.3694","citing_paper":"/paper/2412.06400"},"observation_digest":"sha256:6887162966201b8c32e16c2d22c3646d6afcfb094d818f6d5535d989c9c9af36","observation_id":"a3f81444-5ed6-45a8-b9b6-2ba29b41884b","resolution":{"observed_at":"2026-08-11T19:48:20.219070Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-11T19:48:22.912284Z","title":"Beringer et al","venue":null,"work_id":"21159307-f37c-447f-993b-42fb72a5b472","year":2012},"citing_paper":{"arxiv_id":"2412.06400","last_updated":"2025-03-04T04:39:39Z","snapshot_observed_at":"2026-08-11T19:39:54.876021Z","submitted_at":"2024-12-09T11:30:25Z","title":"Discovery potential of charmonium $2P$ states through the $e^+e^- \\to \\gamma D\\bar{D}$ processes","version":2},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-08-11T19:48:20.233921Z"},"links":{"citing_paper":"/paper/2412.06400"},"observation_digest":"sha256:08c9571043d96687cc6235da3aa83b25d9b9dd5f79e643091cff9c4a166a6fff","observation_id":"eba7fb07-f6b6-47fe-82f7-ea89c0418904","resolution":{"observed_at":"2026-08-11T19:48:22.974731Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1208.1134","last_updated":"2012-08-06T11:19:17Z","snapshot_observed_at":"2026-08-07T14:28:37.848737Z","submitted_at":"2012-08-06T11:19:17Z","title":"Where is the \\chi_{c0}(2P)?","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1208.1134","snapshot_observed_at":"2026-08-11T19:48:20.242926Z","title":"Guo and U.-G","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2412.06400","last_updated":"2025-03-04T04:39:39Z","snapshot_observed_at":"2026-08-11T19:39:54.876021Z","submitted_at":"2024-12-09T11:30:25Z","title":"Discovery potential of charmonium $2P$ states through the $e^+e^- \\to \\gamma D\\bar{D}$ processes","version":2},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-11T19:48:20.242926Z"},"links":{"cited_paper":"/paper/1208.1134","citing_paper":"/paper/2412.06400"},"observation_digest":"sha256:82ccd9aa8b0ad657475276c562580406f5afab2d7444081bd61dab45a9921354","observation_id":"6a63b5e6-08c3-4c0f-b3d9-b969c57aaca9","resolution":{"observed_at":"2026-08-11T19:48:20.242926Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1410.6534","last_updated":"2014-10-24T01:20:13Z","snapshot_observed_at":"2026-07-06T03:58:20.257214Z","submitted_at":"2014-10-24T01:20:13Z","title":"Is the X(3915) the chi_{c0}(2P)?","version":1},"cited_work":{"arxiv_id":"1410.6534","doi":null,"metadata_source":"pith","pith_arxiv_id":"1410.6534","snapshot_observed_at":"2026-08-11T19:48:22.467207Z","title":"Is the X(3915) the chi_{c0}(2P)?","venue":"hep-ex","work_id":"45c0ef65-87ca-4bd6-bceb-1311045443cc","year":2014},"citing_paper":{"arxiv_id":"2412.06400","last_updated":"2025-03-04T04:39:39Z","snapshot_observed_at":"2026-08-11T19:39:54.876021Z","submitted_at":"2024-12-09T11:30:25Z","title":"Discovery potential of charmonium $2P$ states through the $e^+e^- \\to \\gamma D\\bar{D}$ processes","version":2},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-11T19:48:20.255159Z"},"links":{"cited_paper":"/paper/1410.6534","citing_paper":"/paper/2412.06400"},"observation_digest":"sha256:6337b630d4c3d48776db3d9eeeec7ee2d3c63c73f9b3fd7f6ff497c53bec7fc2","observation_id":"5bd7a358-4fd3-4a0d-9af0-8f138aa8ac72","resolution":{"observed_at":"2026-08-11T19:48:22.479179Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1207.3561","last_updated":"2012-10-31T15:43:51Z","snapshot_observed_at":"2026-08-01T16:37:45.346094Z","submitted_at":"2012-07-16T01:33:25Z","title":"Does the enhancement observed in $\\gamma\\gamma\\to D\\bar{D}$ contain two $P$-wave higher charmonia?","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1207.3561","snapshot_observed_at":"2026-08-11T19:48:20.261240Z","title":null,"venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2412.06400","last_updated":"2025-03-04T04:39:39Z","snapshot_observed_at":"2026-08-11T19:39:54.876021Z","submitted_at":"2024-12-09T11:30:25Z","title":"Discovery potential of charmonium $2P$ states through the $e^+e^- \\to \\gamma D\\bar{D}$ processes","version":2},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-08-11T19:48:20.261240Z"},"links":{"cited_paper":"/paper/1207.3561","citing_paper":"/paper/2412.06400"},"observation_digest":"sha256:b65e969684c85c23513126352108896886f8345a17f4235879a93008ab3302df","observation_id":"d52ec07f-9c11-48ea-b808-c11b117411d2","resolution":{"observed_at":"2026-08-11T19:48:20.261240Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2002.03311","last_updated":"2020-03-17T00:22:16Z","snapshot_observed_at":"2026-08-13T13:07:44.310626Z","submitted_at":"2020-02-09T08:04:22Z","title":"Possibility of charmoniumlike state $X(3915)$ as $\\chi_{c0}(2P)$ state","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2002.03311","snapshot_observed_at":"2026-08-11T19:48:20.267256Z","title":"Duan, S.-Q","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2412.06400","last_updated":"2025-03-04T04:39:39Z","snapshot_observed_at":"2026-08-11T19:39:54.876021Z","submitted_at":"2024-12-09T11:30:25Z","title":"Discovery potential of charmonium $2P$ states through the $e^+e^- \\to \\gamma D\\bar{D}$ processes","version":2},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-08-11T19:48:20.267256Z"},"links":{"cited_paper":"/paper/2002.03311","citing_paper":"/paper/2412.06400"},"observation_digest":"sha256:fb928894f5c1bf2a983a7c85eb23e3fff33daa8312bb0d163bb5c437855ee73b","observation_id":"febab9fb-f523-4fa7-896d-ebcea036a2b1","resolution":{"observed_at":"2026-08-11T19:48:20.267256Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-11T19:48:20.275017Z","title":"Aaij et al","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2412.06400","last_updated":"2025-03-04T04:39:39Z","snapshot_observed_at":"2026-08-11T19:39:54.876021Z","submitted_at":"2024-12-09T11:30:25Z","title":"Discovery potential of charmonium $2P$ states through the $e^+e^- \\to \\gamma D\\bar{D}$ processes","version":2},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-08-11T19:48:20.275017Z"},"links":{"citing_paper":"/paper/2412.06400"},"observation_digest":"sha256:14462b77b66a7a538fac83d6f9b7612284b7c2592487c278fd7078c6a897da01","observation_id":"9fa989de-ea81-4a44-a5e4-2db137b6d231","resolution":{"observed_at":"2026-08-11T19:48:20.275017Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-11T19:48:20.281214Z","title":"Aaij et al","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2412.06400","last_updated":"2025-03-04T04:39:39Z","snapshot_observed_at":"2026-08-11T19:39:54.876021Z","submitted_at":"2024-12-09T11:30:25Z","title":"Discovery potential of charmonium $2P$ states through the $e^+e^- \\to \\gamma D\\bar{D}$ processes","version":2},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-08-11T19:48:20.281214Z"},"links":{"citing_paper":"/paper/2412.06400"},"observation_digest":"sha256:fe9154423432c2406c0336b22e529b00f58df9b7bda0a82006ec64d4967bb082","observation_id":"a8ed87c6-159e-4df9-9b04-4f983a3a8531","resolution":{"observed_at":"2026-08-11T19:48:20.281214Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0912.4451","last_updated":"2010-03-10T04:48:45Z","snapshot_observed_at":"2026-07-06T02:05:50.100718Z","submitted_at":"2009-12-22T17:10:10Z","title":"Observation of a charmonium-like enhancement in the gamma gamma --> omega J/psi process","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0912.4451","snapshot_observed_at":"2026-08-11T19:48:20.287689Z","title":"Uehara et al","venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"2412.06400","last_updated":"2025-03-04T04:39:39Z","snapshot_observed_at":"2026-08-11T19:39:54.876021Z","submitted_at":"2024-12-09T11:30:25Z","title":"Discovery potential of charmonium $2P$ states through the $e^+e^- \\to \\gamma D\\bar{D}$ processes","version":2},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-08-11T19:48:20.287689Z"},"links":{"cited_paper":"/paper/0912.4451","citing_paper":"/paper/2412.06400"},"observation_digest":"sha256:679a031556a1a200bec622dea195d9d647ccef262355331a36f18877a21d4108","observation_id":"75a326c5-b914-400c-8e30-175409659a95","resolution":{"observed_at":"2026-08-11T19:48:20.287689Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1311.6274","last_updated":"2015-04-09T02:19:35Z","snapshot_observed_at":"2026-07-06T03:29:07.875798Z","submitted_at":"2013-11-25T12:18:09Z","title":"Hidden-charm decays of $X(3915)$ and $Z(3930)$ as the P-wave charmonia","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1311.6274","snapshot_observed_at":"2026-08-11T19:48:20.298414Z","title":null,"venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2412.06400","last_updated":"2025-03-04T04:39:39Z","snapshot_observed_at":"2026-08-11T19:39:54.876021Z","submitted_at":"2024-12-09T11:30:25Z","title":"Discovery potential of charmonium $2P$ states through the $e^+e^- \\to \\gamma D\\bar{D}$ processes","version":2},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-08-11T19:48:20.298414Z"},"links":{"cited_paper":"/paper/1311.6274","citing_paper":"/paper/2412.06400"},"observation_digest":"sha256:6da005d69c9a3d258de3e91cec82240e013503437f9d4552431e2b536605d98d","observation_id":"e345fb7b-6d9c-41cc-9e92-1f750a290ebf","resolution":{"observed_at":"2026-08-11T19:48:20.298414Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2104.09132","last_updated":"2021-08-14T10:41:11Z","snapshot_observed_at":"2026-08-13T12:04:17.628478Z","submitted_at":"2021-04-19T08:28:28Z","title":"Role of the newly measured $B\\to KD\\bar{D}$ process to establish $\\chi_{c0}(2P)$ state","version":4},"cited_work":{"arxiv_id":"2104.09132","doi":null,"metadata_source":"pith","pith_arxiv_id":"2104.09132","snapshot_observed_at":"2026-08-11T19:48:21.936514Z","title":"Role of the newly measured $B\\to KD\\bar{D}$ process to establish $\\chi_{c0}(2P)$ state","venue":"hep-ph","work_id":"73a64948-77f7-44be-8a7b-fc5628b5f04f","year":2021},"citing_paper":{"arxiv_id":"2412.06400","last_updated":"2025-03-04T04:39:39Z","snapshot_observed_at":"2026-08-11T19:39:54.876021Z","submitted_at":"2024-12-09T11:30:25Z","title":"Discovery potential of charmonium $2P$ states through the $e^+e^- \\to \\gamma D\\bar{D}$ processes","version":2},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-08-11T19:48:20.307274Z"},"links":{"cited_paper":"/paper/2104.09132","citing_paper":"/paper/2412.06400"},"observation_digest":"sha256:29844bad1a9b55b13e0845e4a48e89768ca11cfaf1807327a7daf485df30b6f8","observation_id":"71d6c0a7-0126-49c6-9151-13269222ce43","resolution":{"observed_at":"2026-08-11T19:48:21.946061Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2212.00631","last_updated":"2023-03-13T10:32:03Z","snapshot_observed_at":"2026-08-13T13:29:57.041704Z","submitted_at":"2022-12-01T16:29:53Z","title":"Understanding the $0^{++}$ and $2^{++}$ charmonium(-like) states near 3.9 GeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2212.00631","snapshot_observed_at":"2026-08-11T19:48:20.314407Z","title":"Ji, X.-K","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2412.06400","last_updated":"2025-03-04T04:39:39Z","snapshot_observed_at":"2026-08-11T19:39:54.876021Z","submitted_at":"2024-12-09T11:30:25Z","title":"Discovery potential of charmonium $2P$ states through the $e^+e^- \\to \\gamma D\\bar{D}$ processes","version":2},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-08-11T19:48:20.314407Z"},"links":{"cited_paper":"/paper/2212.00631","citing_paper":"/paper/2412.06400"},"observation_digest":"sha256:2f29f452e2217c3e03776fbce720abfd834a9f30740dd1b46966d3a7d3b434ab","observation_id":"800f9770-dbc9-4f13-8126-b02e32e772b8","resolution":{"observed_at":"2026-08-11T19:48:20.314407Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1310.4101","last_updated":"2014-01-15T00:47:50Z","snapshot_observed_at":"2026-08-05T15:56:40.044179Z","submitted_at":"2013-10-15T16:13:45Z","title":"Observation of $e^{+} e^{-} \\to \\gamma X(3872)$ at BESIII","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1310.4101","snapshot_observed_at":"2026-08-11T19:48:20.327530Z","title":"Ablikim et al","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2412.06400","last_updated":"2025-03-04T04:39:39Z","snapshot_observed_at":"2026-08-11T19:39:54.876021Z","submitted_at":"2024-12-09T11:30:25Z","title":"Discovery potential of charmonium $2P$ states through the $e^+e^- \\to \\gamma D\\bar{D}$ processes","version":2},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-08-11T19:48:20.327530Z"},"links":{"cited_paper":"/paper/1310.4101","citing_paper":"/paper/2412.06400"},"observation_digest":"sha256:2fdca8487ec2b4224115995ca58a0a94c0f1cb6aace7906699dfc2a7077a2741","observation_id":"140fdcab-3aea-4560-beea-01db41b495f5","resolution":{"observed_at":"2026-08-11T19:48:20.327530Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1903.04695","last_updated":"2019-06-15T13:01:33Z","snapshot_observed_at":"2026-07-06T07:38:36.561289Z","submitted_at":"2019-03-12T01:50:24Z","title":"Study of $e^+e^- \\to \\gamma \\omega J/\\psi$ and Observation of $X(3872) \\to \\omega J/\\psi$","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1903.04695","snapshot_observed_at":"2026-08-11T19:48:20.337768Z","title":"Ablikim et al","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2412.06400","last_updated":"2025-03-04T04:39:39Z","snapshot_observed_at":"2026-08-11T19:39:54.876021Z","submitted_at":"2024-12-09T11:30:25Z","title":"Discovery potential of charmonium $2P$ states through the $e^+e^- \\to \\gamma D\\bar{D}$ processes","version":2},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-08-11T19:48:20.337768Z"},"links":{"cited_paper":"/paper/1903.04695","citing_paper":"/paper/2412.06400"},"observation_digest":"sha256:b6ce6ee1a7a694029b4f445243d57e2b5183f5910e630a86d067f669f27223b2","observation_id":"430a00dc-6a6f-44d3-a5e3-56f28e01eeaf","resolution":{"observed_at":"2026-08-11T19:48:20.337768Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1405.3831","last_updated":"2014-12-10T02:28:27Z","snapshot_observed_at":"2026-07-06T03:43:47.114292Z","submitted_at":"2014-05-15T13:02:18Z","title":"Prediction of a missing higher charmonium around 4.26 GeV in $J/\\psi$ family","version":3},"cited_work":{"arxiv_id":"1405.3831","doi":null,"metadata_source":"pith","pith_arxiv_id":"1405.3831","snapshot_observed_at":"2026-08-11T19:48:21.711114Z","title":"Prediction of a missing higher charmonium around 4.26 GeV in $J/\\psi$ family","venue":"hep-ph","work_id":"4200f3d2-7f12-4374-a6b2-f5fdddd5ab29","year":2014},"citing_paper":{"arxiv_id":"2412.06400","last_updated":"2025-03-04T04:39:39Z","snapshot_observed_at":"2026-08-11T19:39:54.876021Z","submitted_at":"2024-12-09T11:30:25Z","title":"Discovery potential of charmonium $2P$ states through the $e^+e^- \\to \\gamma D\\bar{D}$ processes","version":2},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-08-11T19:48:20.343338Z"},"links":{"cited_paper":"/paper/1405.3831","citing_paper":"/paper/2412.06400"},"observation_digest":"sha256:8b9b88f6b829235c25a2ae0230828ee5c93906d2a8188ca118597a8ce8636300","observation_id":"4cbcb141-3893-49e7-9f44-6c8f88759e8c","resolution":{"observed_at":"2026-08-11T19:48:21.765002Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"0903.5506","last_updated":"2009-05-07T15:15:49Z","snapshot_observed_at":"2026-08-13T17:14:47.844752Z","submitted_at":"2009-03-31T15:49:02Z","title":"Higher Charmonia and X,Y,Z states with Screened Potential","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0903.5506","snapshot_observed_at":"2026-08-11T19:48:20.354527Z","title":"Li and K.-T","venue":null,"work_id":null,"year":2009},"citing_paper":{"arxiv_id":"2412.06400","last_updated":"2025-03-04T04:39:39Z","snapshot_observed_at":"2026-08-11T19:39:54.876021Z","submitted_at":"2024-12-09T11:30:25Z","title":"Discovery potential of charmonium $2P$ states through the $e^+e^- \\to \\gamma D\\bar{D}$ processes","version":2},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-08-11T19:48:20.354527Z"},"links":{"cited_paper":"/paper/0903.5506","citing_paper":"/paper/2412.06400"},"observation_digest":"sha256:6ec2500b3b384669ea87defc2c06890e86ab21bf5b498b6e1605476221de86b1","observation_id":"d29b6122-fa4f-47a9-89fa-09da414ad2ea","resolution":{"observed_at":"2026-08-11T19:48:20.354527Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1708.01954","last_updated":"2018-03-23T16:20:09Z","snapshot_observed_at":"2026-07-06T05:54:16.759407Z","submitted_at":"2017-08-07T00:56:47Z","title":"Interference effect as resonance killer of newly observed charmoniumlike states $Y(4320)$ and $Y(4390)$","version":3},"cited_work":{"arxiv_id":"1708.01954","doi":null,"metadata_source":"pith","pith_arxiv_id":"1708.01954","snapshot_observed_at":"2026-08-11T19:48:21.640355Z","title":"Interference effect as resonance killer of newly observed charmoniumlike states $Y(4320)$ and $Y(4390)$","venue":"hep-ph","work_id":"d907455a-d7d5-43b0-9113-478cbb7a4063","year":2017},"citing_paper":{"arxiv_id":"2412.06400","last_updated":"2025-03-04T04:39:39Z","snapshot_observed_at":"2026-08-11T19:39:54.876021Z","submitted_at":"2024-12-09T11:30:25Z","title":"Discovery potential of charmonium $2P$ states through the $e^+e^- \\to \\gamma D\\bar{D}$ processes","version":2},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-08-11T19:48:20.361467Z"},"links":{"cited_paper":"/paper/1708.01954","citing_paper":"/paper/2412.06400"},"observation_digest":"sha256:1677ba978b869612337f1bc422b74b1170c091f0b82e4e236019237ae365adc2","observation_id":"bcc61cb6-f92d-4719-bb90-ddcf31d9433c","resolution":{"observed_at":"2026-08-11T19:48:21.648531Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1306.3096","last_updated":"2013-06-25T21:29:37Z","snapshot_observed_at":"2026-07-06T03:15:45.494656Z","submitted_at":"2013-06-13T12:29:36Z","title":"Production of the X(3872) in charmonia radiative decays","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1306.3096","snapshot_observed_at":"2026-08-11T19:48:20.366889Z","title":null,"venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2412.06400","last_updated":"2025-03-04T04:39:39Z","snapshot_observed_at":"2026-08-11T19:39:54.876021Z","submitted_at":"2024-12-09T11:30:25Z","title":"Discovery potential of charmonium $2P$ states through the $e^+e^- \\to \\gamma D\\bar{D}$ processes","version":2},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-08-11T19:48:20.366889Z"},"links":{"cited_paper":"/paper/1306.3096","citing_paper":"/paper/2412.06400"},"observation_digest":"sha256:0b2d8b761debeffc404e7a83b00af4dac72c3a304f0ec33898c9f1ee0b35c076","observation_id":"05269e85-abfd-4314-a227-80cc4ae44ed7","resolution":{"observed_at":"2026-08-11T19:48:20.366889Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0809.4818","last_updated":"2008-11-28T15:02:50Z","snapshot_observed_at":"2026-07-06T01:45:38.795094Z","submitted_at":"2008-09-28T04:24:19Z","title":"Are Y(4260) and {\\rm Z$_2^{+}$(4250)} ${\\rm D_1D}$ or ${\\rm D_0D^{*}}$ Hadronic Molecules?","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0809.4818","snapshot_observed_at":"2026-08-11T19:48:20.398391Z","title":"Ding, Are Y(4260) and Z+ 2 (4250) are D1D or D0D∗ Hadronic Molecules?, Phys","venue":null,"work_id":null,"year":2009},"citing_paper":{"arxiv_id":"2412.06400","last_updated":"2025-03-04T04:39:39Z","snapshot_observed_at":"2026-08-11T19:39:54.876021Z","submitted_at":"2024-12-09T11:30:25Z","title":"Discovery potential of charmonium $2P$ states through the $e^+e^- \\to \\gamma D\\bar{D}$ processes","version":2},"reference_index":29,"source":"pdf_text","source_observed_at":"2026-08-11T19:48:20.398391Z"},"links":{"cited_paper":"/paper/0809.4818","citing_paper":"/paper/2412.06400"},"observation_digest":"sha256:4aadc876863c1fcc7abebc342ef54b7ae4200b5644e97eac35797b2189153730","observation_id":"7a71f137-6693-400a-a87a-6959990e84cd","resolution":{"observed_at":"2026-08-11T19:48:20.398391Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1303.4140","last_updated":"2013-03-19T02:44:50Z","snapshot_observed_at":"2026-07-06T03:08:56.888332Z","submitted_at":"2013-03-18T02:30:21Z","title":"A Study of P-wave Heavy Meson Interactions in A Chiral Quark Model","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1303.4140","snapshot_observed_at":"2026-08-11T19:48:20.405043Z","title":"Li, W.-L","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2412.06400","last_updated":"2025-03-04T04:39:39Z","snapshot_observed_at":"2026-08-11T19:39:54.876021Z","submitted_at":"2024-12-09T11:30:25Z","title":"Discovery potential of charmonium $2P$ states through the $e^+e^- \\to \\gamma D\\bar{D}$ processes","version":2},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-08-11T19:48:20.405043Z"},"links":{"cited_paper":"/paper/1303.4140","citing_paper":"/paper/2412.06400"},"observation_digest":"sha256:aeeae04850b755ca39aa3f8e3ede815b6510017a673b9eaeffb2fed7a6077eb8","observation_id":"f75cc78a-31a0-4210-9d34-1d9c9c8d724d","resolution":{"observed_at":"2026-08-11T19:48:20.405043Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1303.6355","last_updated":"2013-09-12T20:38:17Z","snapshot_observed_at":"2026-08-12T16:14:31.702342Z","submitted_at":"2013-03-26T00:31:36Z","title":"Decoding the riddle of Y(4260) and $Z_c(3900)$","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1303.6355","snapshot_observed_at":"2026-08-11T19:48:20.412255Z","title":null,"venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2412.06400","last_updated":"2025-03-04T04:39:39Z","snapshot_observed_at":"2026-08-11T19:39:54.876021Z","submitted_at":"2024-12-09T11:30:25Z","title":"Discovery potential of charmonium $2P$ states through the $e^+e^- \\to \\gamma D\\bar{D}$ processes","version":2},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-08-11T19:48:20.412255Z"},"links":{"cited_paper":"/paper/1303.6355","citing_paper":"/paper/2412.06400"},"observation_digest":"sha256:cafcf6fbd019f94cf83b32cdc7a60924ea1410c4fd01c43ce1c92d09be41eb09","observation_id":"8671e508-c25d-4500-98da-06dba061b0f5","resolution":{"observed_at":"2026-08-11T19:48:20.412255Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1611.01317","last_updated":"2017-01-20T17:01:03Z","snapshot_observed_at":"2026-08-06T14:08:00.473463Z","submitted_at":"2016-11-04T10:41:23Z","title":"Precise measurement of the $e^+e^-\\to \\pi^+\\pi^-J/\\psi$ cross section at center-of-mass energies from 3.77 to 4.60 GeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1611.01317","snapshot_observed_at":"2026-08-11T19:48:20.422865Z","title":"Ablikim et al","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2412.06400","last_updated":"2025-03-04T04:39:39Z","snapshot_observed_at":"2026-08-11T19:39:54.876021Z","submitted_at":"2024-12-09T11:30:25Z","title":"Discovery potential of charmonium $2P$ states through the $e^+e^- \\to \\gamma D\\bar{D}$ processes","version":2},"reference_index":32,"source":"pdf_text","source_observed_at":"2026-08-11T19:48:20.422865Z"},"links":{"cited_paper":"/paper/1611.01317","citing_paper":"/paper/2412.06400"},"observation_digest":"sha256:df3a1ea246548ad9794bca313b3f1464f3b0bf1d60479c6aa2d5a2e8e0284a06","observation_id":"0f7cc5c1-70e1-4e19-a491-20d27973a961","resolution":{"observed_at":"2026-08-11T19:48:20.422865Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2001.00175","last_updated":"2020-01-22T02:25:44Z","snapshot_observed_at":"2026-07-06T08:47:59.030634Z","submitted_at":"2020-01-01T09:33:20Z","title":"Are the $Y$ states around 4.6 GeV from $e^+e^-$ annihilation higher charmonia?","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2001.00175","snapshot_observed_at":"2026-08-11T19:48:20.433680Z","title":"Wang, R.-Q","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2412.06400","last_updated":"2025-03-04T04:39:39Z","snapshot_observed_at":"2026-08-11T19:39:54.876021Z","submitted_at":"2024-12-09T11:30:25Z","title":"Discovery potential of charmonium $2P$ states through the $e^+e^- \\to \\gamma D\\bar{D}$ processes","version":2},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-08-11T19:48:20.433680Z"},"links":{"cited_paper":"/paper/2001.00175","citing_paper":"/paper/2412.06400"},"observation_digest":"sha256:2a927aa9d7e09ebbaa8af156d304fb47b7ff4a6159dc86971c894a227b3f6805","observation_id":"1af5f95d-7dcd-457c-8a18-1d1e6f54821a","resolution":{"observed_at":"2026-08-11T19:48:20.433680Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1705.00449","last_updated":"2017-12-22T15:54:43Z","snapshot_observed_at":"2026-08-04T15:40:38.973827Z","submitted_at":"2017-05-01T09:01:24Z","title":"$X(4260)$ Revisited: A Coupled Channel Perspective","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1705.00449","snapshot_observed_at":"2026-08-11T19:48:20.446573Z","title":null,"venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2412.06400","last_updated":"2025-03-04T04:39:39Z","snapshot_observed_at":"2026-08-11T19:39:54.876021Z","submitted_at":"2024-12-09T11:30:25Z","title":"Discovery potential of charmonium $2P$ states through the $e^+e^- \\to \\gamma D\\bar{D}$ processes","version":2},"reference_index":34,"source":"pdf_text","source_observed_at":"2026-08-11T19:48:20.446573Z"},"links":{"cited_paper":"/paper/1705.00449","citing_paper":"/paper/2412.06400"},"observation_digest":"sha256:dbb8207d081f9c84775c539d7b4999e5a478d409ca6c02d7ad805a7b2f67ca9b","observation_id":"fa660ee5-965c-43a2-8732-1e83bf9b1dec","resolution":{"observed_at":"2026-08-11T19:48:20.446573Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2502.08072","last_updated":"2025-06-04T08:45:07Z","snapshot_observed_at":"2026-08-13T15:57:28.628846Z","submitted_at":"2025-02-12T02:26:45Z","title":"Coupled-channel study of $4S$-$3D$ mixing dynamics in $\\psi(4220)$ and $\\psi(4380)$","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2502.08072","snapshot_observed_at":"2026-08-11T19:48:20.455352Z","title":"Man, S.-Q","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2412.06400","last_updated":"2025-03-04T04:39:39Z","snapshot_observed_at":"2026-08-11T19:39:54.876021Z","submitted_at":"2024-12-09T11:30:25Z","title":"Discovery potential of charmonium $2P$ states through the $e^+e^- \\to \\gamma D\\bar{D}$ processes","version":2},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-08-11T19:48:20.455352Z"},"links":{"cited_paper":"/paper/2502.08072","citing_paper":"/paper/2412.06400"},"observation_digest":"sha256:0d6be6bf3e43c6d378bd5f14b7d1f9d5ca7997a34f4462d95c74d73488072a95","observation_id":"63f329c1-4b46-43aa-a580-b3244dc88fd5","resolution":{"observed_at":"2026-08-11T19:48:20.455352Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ex/0502031","last_updated":"2005-03-29T10:04:03Z","snapshot_observed_at":"2026-07-07T03:36:56.508184Z","submitted_at":"2005-02-16T10:06:49Z","title":"Precise measurement of spin-averaged chi_{cJ}(1P) mass using photon conversions in psi(2S) -> gamma chi_{cJ}","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ex/0502031","snapshot_observed_at":"2026-08-11T19:48:20.465408Z","title":"Ablikim et al","venue":null,"work_id":null,"year":2005},"citing_paper":{"arxiv_id":"2412.06400","last_updated":"2025-03-04T04:39:39Z","snapshot_observed_at":"2026-08-11T19:39:54.876021Z","submitted_at":"2024-12-09T11:30:25Z","title":"Discovery potential of charmonium $2P$ states through the $e^+e^- \\to \\gamma D\\bar{D}$ processes","version":2},"reference_index":36,"source":"pdf_text","source_observed_at":"2026-08-11T19:48:20.465408Z"},"links":{"cited_paper":"/paper/hep-ex/0502031","citing_paper":"/paper/2412.06400"},"observation_digest":"sha256:0dafa5926f14653a76fc6a7c618dc670e2c0005dbea6bee8c3e8a0c55c13cac2","observation_id":"bdd2e000-219b-4a63-9a81-45f7691bdbcf","resolution":{"observed_at":"2026-08-11T19:48:20.465408Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":"ex/0411068","doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-11T19:48:21.365838Z","title":"Artuso et al","venue":null,"work_id":"d153c3d9-68c2-4459-b93c-2943fc2be306","year":2005},"citing_paper":{"arxiv_id":"2412.06400","last_updated":"2025-03-04T04:39:39Z","snapshot_observed_at":"2026-08-11T19:39:54.876021Z","submitted_at":"2024-12-09T11:30:25Z","title":"Discovery potential of charmonium $2P$ states through the $e^+e^- \\to \\gamma D\\bar{D}$ processes","version":2},"reference_index":37,"source":"pdf_text","source_observed_at":"2026-08-11T19:48:20.471370Z"},"links":{"citing_paper":"/paper/2412.06400"},"observation_digest":"sha256:f5ec76719d21eefe4128ae0a4cac62c17c2856b06ab4bfa5b11982b6a6af13e3","observation_id":"5f4ea04f-68d3-4b81-b21a-365ad37e5d8f","resolution":{"observed_at":"2026-08-11T19:48:21.376001Z","resolver_source":"raw_fallback","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0606191","last_updated":"2006-09-22T00:31:19Z","snapshot_observed_at":"2026-08-07T12:51:37.533217Z","submitted_at":"2006-06-19T01:40:38Z","title":"Study on contributions of hadronic loops to decays of $J/\\psi\\to$ vector $+$ pseudoscalar mesons","version":2},"cited_work":{"arxiv_id":"hep-ph/0606191","doi":null,"metadata_source":"pith","pith_arxiv_id":"hep-ph/0606191","snapshot_observed_at":"2026-08-11T19:48:21.252797Z","title":"Study on contributions of hadronic loops to decays of $J/\\psi\\to$ vector $+$ pseudoscalar mesons","venue":"hep-ph","work_id":"9555d3f2-1ce0-4073-a34d-b738ec914a44","year":2006},"citing_paper":{"arxiv_id":"2412.06400","last_updated":"2025-03-04T04:39:39Z","snapshot_observed_at":"2026-08-11T19:39:54.876021Z","submitted_at":"2024-12-09T11:30:25Z","title":"Discovery potential of charmonium $2P$ states through the $e^+e^- \\to \\gamma D\\bar{D}$ processes","version":2},"reference_index":38,"source":"pdf_text","source_observed_at":"2026-08-11T19:48:20.477778Z"},"links":{"cited_paper":"/paper/hep-ph/0606191","citing_paper":"/paper/2412.06400"},"observation_digest":"sha256:9e13c4b4def85aeb44bc70d52f095124c7d88edc182a95a33f6fb080b0dcf4a0","observation_id":"c32953f0-907a-4264-896a-b9a5d536d272","resolution":{"observed_at":"2026-08-11T19:48:21.261727Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"0902.0480","last_updated":"2009-04-16T13:37:02Z","snapshot_observed_at":"2026-07-06T01:50:54.859348Z","submitted_at":"2009-02-03T16:06:55Z","title":"The puzzle of excessive non-$D\\bar D$ component of the inclusive $\\psi(3770)$ decay and the long-distant contribution","version":5},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0902.0480","snapshot_observed_at":"2026-08-11T19:48:20.486360Z","title":null,"venue":null,"work_id":null,"year":2009},"citing_paper":{"arxiv_id":"2412.06400","last_updated":"2025-03-04T04:39:39Z","snapshot_observed_at":"2026-08-11T19:39:54.876021Z","submitted_at":"2024-12-09T11:30:25Z","title":"Discovery potential of charmonium $2P$ states through the $e^+e^- \\to \\gamma D\\bar{D}$ processes","version":2},"reference_index":39,"source":"pdf_text","source_observed_at":"2026-08-11T19:48:20.486360Z"},"links":{"cited_paper":"/paper/0902.0480","citing_paper":"/paper/2412.06400"},"observation_digest":"sha256:a7d2ffabf60af8ecb815041a8585c8013927aa35861efbcb15a3491606c4a7d2","observation_id":"14e3c7b0-045b-467d-8f13-cfda8f3ee454","resolution":{"observed_at":"2026-08-11T19:48:20.486360Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0902.1300","last_updated":"2009-04-20T04:46:48Z","snapshot_observed_at":"2026-08-07T19:50:37.815852Z","submitted_at":"2009-02-08T09:16:15Z","title":"Towards a dynamical understanding of the non-$D \\bar D$ decay of $\\psi(3770)$","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0902.1300","snapshot_observed_at":"2026-08-11T19:48:20.494048Z","title":"Zhang, G","venue":null,"work_id":null,"year":2009},"citing_paper":{"arxiv_id":"2412.06400","last_updated":"2025-03-04T04:39:39Z","snapshot_observed_at":"2026-08-11T19:39:54.876021Z","submitted_at":"2024-12-09T11:30:25Z","title":"Discovery potential of charmonium $2P$ states through the $e^+e^- \\to \\gamma D\\bar{D}$ processes","version":2},"reference_index":40,"source":"pdf_text","source_observed_at":"2026-08-11T19:48:20.494048Z"},"links":{"cited_paper":"/paper/0902.1300","citing_paper":"/paper/2412.06400"},"observation_digest":"sha256:a4e97d7a6585cfbb979901f73d8ff1dfe857690cf0162969f1396b33afa7475d","observation_id":"782252b2-ac4a-4101-80f2-2b6de8fbe772","resolution":{"observed_at":"2026-08-11T19:48:20.494048Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1304.0372","last_updated":"2013-05-03T13:01:13Z","snapshot_observed_at":"2026-07-06T03:10:05.317149Z","submitted_at":"2013-04-01T15:04:43Z","title":"Anomalous radiative transitions between $h_b(nP)$ and $\\eta_b(mS)$ and hadronic loop effect","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1304.0372","snapshot_observed_at":"2026-08-11T19:48:20.502045Z","title":null,"venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2412.06400","last_updated":"2025-03-04T04:39:39Z","snapshot_observed_at":"2026-08-11T19:39:54.876021Z","submitted_at":"2024-12-09T11:30:25Z","title":"Discovery potential of charmonium $2P$ states through the $e^+e^- \\to \\gamma D\\bar{D}$ processes","version":2},"reference_index":41,"source":"pdf_text","source_observed_at":"2026-08-11T19:48:20.502045Z"},"links":{"cited_paper":"/paper/1304.0372","citing_paper":"/paper/2412.06400"},"observation_digest":"sha256:c44f71ad3810e6ec1e3ad09e7dce285d7c21b25a88ffa3a61127a9b75edeb5a4","observation_id":"c8fd0b36-5258-421e-8f1e-7159118d2bcc","resolution":{"observed_at":"2026-08-11T19:48:20.502045Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0409317","last_updated":"2004-12-09T09:22:19Z","snapshot_observed_at":"2026-08-10T09:46:33.502769Z","submitted_at":"2004-09-28T02:39:42Z","title":"Final State Interactions in Hadronic B Decays","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0409317","snapshot_observed_at":"2026-08-11T19:48:20.520895Z","title":"Cheng, C.-K","venue":null,"work_id":null,"year":2005},"citing_paper":{"arxiv_id":"2412.06400","last_updated":"2025-03-04T04:39:39Z","snapshot_observed_at":"2026-08-11T19:39:54.876021Z","submitted_at":"2024-12-09T11:30:25Z","title":"Discovery potential of charmonium $2P$ states through the $e^+e^- \\to \\gamma D\\bar{D}$ processes","version":2},"reference_index":42,"source":"pdf_text","source_observed_at":"2026-08-11T19:48:20.520895Z"},"links":{"cited_paper":"/paper/hep-ph/0409317","citing_paper":"/paper/2412.06400"},"observation_digest":"sha256:655d791fd6c4f1e0d8d30a4203e47fcb6aa2a5d29d573b9279127d8e712a1870","observation_id":"b1a8ab33-426e-4ef2-a9cd-2a9c2c0e972c","resolution":{"observed_at":"2026-08-11T19:48:20.520895Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2403.06440","last_updated":"2024-03-11T05:16:56Z","snapshot_observed_at":"2026-08-13T00:57:56.192075Z","submitted_at":"2024-03-11T05:16:56Z","title":"The role of the short-distance interaction in $e^+e^-\\to \\gamma X(3872)$","version":1},"cited_work":{"arxiv_id":"2403.06440","doi":null,"metadata_source":"pith","pith_arxiv_id":"2403.06440","snapshot_observed_at":"2026-08-11T19:48:21.098043Z","title":"The role of the short-distance interaction in $e^+e^-\\to \\gamma X(3872)$","venue":"hep-ph","work_id":"c573027a-0166-40bf-bcaa-feb1406654f0","year":2024},"citing_paper":{"arxiv_id":"2412.06400","last_updated":"2025-03-04T04:39:39Z","snapshot_observed_at":"2026-08-11T19:39:54.876021Z","submitted_at":"2024-12-09T11:30:25Z","title":"Discovery potential of charmonium $2P$ states through the $e^+e^- \\to \\gamma D\\bar{D}$ processes","version":2},"reference_index":43,"source":"pdf_text","source_observed_at":"2026-08-11T19:48:20.529383Z"},"links":{"cited_paper":"/paper/2403.06440","citing_paper":"/paper/2412.06400"},"observation_digest":"sha256:dcf2d26634fb4d2016900e82888bdc888a2ff5f3c491df569336507f69a395d9","observation_id":"0f29c11d-961b-4d9b-9155-f5c25efed47f","resolution":{"observed_at":"2026-08-11T19:48:21.104842Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-11T19:48:20.541114Z","title":"Casalbuoni, A","venue":null,"work_id":null,"year":1997},"citing_paper":{"arxiv_id":"2412.06400","last_updated":"2025-03-04T04:39:39Z","snapshot_observed_at":"2026-08-11T19:39:54.876021Z","submitted_at":"2024-12-09T11:30:25Z","title":"Discovery potential of charmonium $2P$ states through the $e^+e^- \\to \\gamma D\\bar{D}$ processes","version":2},"reference_index":44,"source":"pdf_text","source_observed_at":"2026-08-11T19:48:20.541114Z"},"links":{"citing_paper":"/paper/2412.06400"},"observation_digest":"sha256:de85f2dc8fb39d2fdb2b75e9604ba7bf896ab1f2969e76437b7b029a7ceac8c9","observation_id":"0a810a3d-2e0b-4a3a-91c2-8b20f6bde7ab","resolution":{"observed_at":"2026-08-11T19:48:20.541114Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0310084","last_updated":"2003-10-07T14:39:46Z","snapshot_observed_at":"2026-07-07T04:01:31.058013Z","submitted_at":"2003-10-07T14:39:46Z","title":"Nonfactorizable contributions in B decays to charmonium: the case of $B^- \\to K^- h_c$","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0310084","snapshot_observed_at":"2026-08-11T19:48:20.549968Z","title":"Colangelo, F","venue":null,"work_id":null,"year":2004},"citing_paper":{"arxiv_id":"2412.06400","last_updated":"2025-03-04T04:39:39Z","snapshot_observed_at":"2026-08-11T19:39:54.876021Z","submitted_at":"2024-12-09T11:30:25Z","title":"Discovery potential of charmonium $2P$ states through the $e^+e^- \\to \\gamma D\\bar{D}$ processes","version":2},"reference_index":45,"source":"pdf_text","source_observed_at":"2026-08-11T19:48:20.549968Z"},"links":{"cited_paper":"/paper/hep-ph/0310084","citing_paper":"/paper/2412.06400"},"observation_digest":"sha256:c195d456cab07e1c412169d499d1ebfe3bdccdfacdad6e3fb6c61f059eadd654","observation_id":"030c0db9-8cfd-4c0e-afd7-384f76b8cdf3","resolution":{"observed_at":"2026-08-11T19:48:20.549968Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1605.04776","last_updated":"2016-07-20T14:17:05Z","snapshot_observed_at":"2026-07-06T04:56:26.545306Z","submitted_at":"2016-05-16T14:06:35Z","title":"Understanding $B^-\\rightarrow X(3823)K^-$ via rescattering mechanism and predicting $B^-\\to \\eta_{c2} (^1D_2)/\\psi_3(^3D_3)K^-$","version":2},"cited_work":{"arxiv_id":"1605.04776","doi":null,"metadata_source":"pith","pith_arxiv_id":"1605.04776","snapshot_observed_at":"2026-08-11T19:48:20.851024Z","title":"Understanding $B^-\\rightarrow X(3823)K^-$ via rescattering mechanism and predicting $B^-\\to \\eta_{c2} (^1D_2)/\\psi_3(^3D_3)K^-$","venue":"hep-ph","work_id":"156020be-75fc-4084-8f0f-ba2da1729066","year":2016},"citing_paper":{"arxiv_id":"2412.06400","last_updated":"2025-03-04T04:39:39Z","snapshot_observed_at":"2026-08-11T19:39:54.876021Z","submitted_at":"2024-12-09T11:30:25Z","title":"Discovery potential of charmonium $2P$ states through the $e^+e^- \\to \\gamma D\\bar{D}$ processes","version":2},"reference_index":46,"source":"pdf_text","source_observed_at":"2026-08-11T19:48:20.555613Z"},"links":{"cited_paper":"/paper/1605.04776","citing_paper":"/paper/2412.06400"},"observation_digest":"sha256:5f897091527b705c0f34ee834dc10bd6ba6c62e239cf8cbb507c0907467c6a6f","observation_id":"ae99083a-7b70-4f17-8917-e0a3f9b5549b","resolution":{"observed_at":"2026-08-11T19:48:20.860050Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2306.14695","last_updated":"2024-01-11T08:37:49Z","snapshot_observed_at":"2026-08-13T11:09:17.704657Z","submitted_at":"2023-06-26T13:40:58Z","title":"Identifying a characterized energy level structure of higher charmonium well matched to the peak structures in $e^+e^-\\to \\pi^+ D^0 D^{*-}$","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2306.14695","snapshot_observed_at":"2026-08-11T19:48:20.565799Z","title":"Wang and X","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2412.06400","last_updated":"2025-03-04T04:39:39Z","snapshot_observed_at":"2026-08-11T19:39:54.876021Z","submitted_at":"2024-12-09T11:30:25Z","title":"Discovery potential of charmonium $2P$ states through the $e^+e^- \\to \\gamma D\\bar{D}$ processes","version":2},"reference_index":47,"source":"pdf_text","source_observed_at":"2026-08-11T19:48:20.565799Z"},"links":{"cited_paper":"/paper/2306.14695","citing_paper":"/paper/2412.06400"},"observation_digest":"sha256:55318eb5cd27d0d525d2236282d0f2db1b728e73ef7c89250b4215b4e03a781c","observation_id":"701c583d-871b-438a-b430-3aab5f434777","resolution":{"observed_at":"2026-08-11T19:48:20.565799Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1808.02847","last_updated":"2019-04-02T14:44:02Z","snapshot_observed_at":"2026-08-04T07:44:19.254747Z","submitted_at":"2018-08-08T16:19:58Z","title":"Evidence of a resonant structure in the $e^+e^-\\to \\pi^+D^0D^{*-}$ cross section between 4.05 and 4.60 GeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1808.02847","snapshot_observed_at":"2026-08-11T19:48:20.572790Z","title":"Ablikim et al","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2412.06400","last_updated":"2025-03-04T04:39:39Z","snapshot_observed_at":"2026-08-11T19:39:54.876021Z","submitted_at":"2024-12-09T11:30:25Z","title":"Discovery potential of charmonium $2P$ states through the $e^+e^- \\to \\gamma D\\bar{D}$ processes","version":2},"reference_index":48,"source":"pdf_text","source_observed_at":"2026-08-11T19:48:20.572790Z"},"links":{"cited_paper":"/paper/1808.02847","citing_paper":"/paper/2412.06400"},"observation_digest":"sha256:a3a50f31bdbe9b15629bf38569d58c00197262e0cb3650c5e922e6f3bdaef5f3","observation_id":"e6d00a61-116b-490b-bf0f-58e105a1eaed","resolution":{"observed_at":"2026-08-11T19:48:20.572790Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2404.07681","last_updated":"2024-09-15T07:17:38Z","snapshot_observed_at":"2026-08-13T00:32:45.331143Z","submitted_at":"2024-04-11T12:18:59Z","title":"Productions of $X(3872)$/$Z_c(3900)$ and $X_2(4013)$/$Z_c(4020)$ in $Y(4220)$ and $Y(4360)$ decays","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2404.07681","snapshot_observed_at":"2026-08-11T19:48:20.579142Z","title":"Liu, X.-Z","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2412.06400","last_updated":"2025-03-04T04:39:39Z","snapshot_observed_at":"2026-08-11T19:39:54.876021Z","submitted_at":"2024-12-09T11:30:25Z","title":"Discovery potential of charmonium $2P$ states through the $e^+e^- \\to \\gamma D\\bar{D}$ processes","version":2},"reference_index":49,"source":"pdf_text","source_observed_at":"2026-08-11T19:48:20.579142Z"},"links":{"cited_paper":"/paper/2404.07681","citing_paper":"/paper/2412.06400"},"observation_digest":"sha256:0c31566b1a23cc73c443fd58136904e2b4355ae8ec54c97cbed1bd9ba7da63fb","observation_id":"6d8ecea5-4c1c-411c-a9a9-c393127ff5e4","resolution":{"observed_at":"2026-08-11T19:48:20.579142Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-11T19:48:20.593331Z","title":null,"venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2412.06400","last_updated":"2025-03-04T04:39:39Z","snapshot_observed_at":"2026-08-11T19:39:54.876021Z","submitted_at":"2024-12-09T11:30:25Z","title":"Discovery potential of charmonium $2P$ states through the $e^+e^- \\to \\gamma D\\bar{D}$ processes","version":2},"reference_index":50,"source":"pdf_text","source_observed_at":"2026-08-11T19:48:20.593331Z"},"links":{"citing_paper":"/paper/2412.06400"},"observation_digest":"sha256:ef4da936d96ee8d187041d79939adf37a0b80cd9f64decaf28caa0d4e815c3b3","observation_id":"19c5b11f-4ad1-4256-897a-4d4615f0a740","resolution":{"observed_at":"2026-08-11T19:48:20.593331Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1005.0066","last_updated":"2010-09-08T04:59:04Z","snapshot_observed_at":"2026-07-06T02:06:43.854684Z","submitted_at":"2010-05-01T12:57:39Z","title":"Long-distant contribution and $\\chi_{c1}$ radiative decays to light vector meson","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1005.0066","snapshot_observed_at":"2026-08-11T19:48:20.598219Z","title":"Chen, Y .-B","venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"2412.06400","last_updated":"2025-03-04T04:39:39Z","snapshot_observed_at":"2026-08-11T19:39:54.876021Z","submitted_at":"2024-12-09T11:30:25Z","title":"Discovery potential of charmonium $2P$ states through the $e^+e^- \\to \\gamma D\\bar{D}$ processes","version":2},"reference_index":51,"source":"pdf_text","source_observed_at":"2026-08-11T19:48:20.598219Z"},"links":{"cited_paper":"/paper/1005.0066","citing_paper":"/paper/2412.06400"},"observation_digest":"sha256:a65cca43b5e5cae46aca2cbda066414f9800b905425ecc0d1d3e71f1adb03b4b","observation_id":"2349eeb2-ea8d-4cd6-8dcf-a4d78fbd1efd","resolution":{"observed_at":"2026-08-11T19:48:20.598219Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1510.08305","last_updated":"2016-01-15T18:46:52Z","snapshot_observed_at":"2026-08-08T11:18:14.115128Z","submitted_at":"2015-10-28T13:42:07Z","title":"Properties of Excited Charm and Charm-Strange Mesons","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1510.08305","snapshot_observed_at":"2026-08-11T19:48:20.610211Z","title":"Godfrey and K","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2412.06400","last_updated":"2025-03-04T04:39:39Z","snapshot_observed_at":"2026-08-11T19:39:54.876021Z","submitted_at":"2024-12-09T11:30:25Z","title":"Discovery potential of charmonium $2P$ states through the $e^+e^- \\to \\gamma D\\bar{D}$ processes","version":2},"reference_index":52,"source":"pdf_text","source_observed_at":"2026-08-11T19:48:20.610211Z"},"links":{"cited_paper":"/paper/1510.08305","citing_paper":"/paper/2412.06400"},"observation_digest":"sha256:9602266cb5eefe2a71f9a448d1cad45075e2a08528a3a9fdaf5b0055dc44e2d6","observation_id":"8adae910-bc3c-4556-8ff1-0ffccd30a4fa","resolution":{"observed_at":"2026-08-11T19:48:20.610211Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2106.14123","last_updated":"2021-08-12T00:57:53Z","snapshot_observed_at":"2026-07-06T11:23:26.988614Z","submitted_at":"2021-06-27T01:49:57Z","title":"Hidden-bottom hadronic decays of $\\Upsilon(10753)$ with a $\\eta^{(\\prime)}$ or $\\omega$ emission","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2106.14123","snapshot_observed_at":"2026-08-11T19:48:20.617471Z","title":"Li, Z.-Y","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2412.06400","last_updated":"2025-03-04T04:39:39Z","snapshot_observed_at":"2026-08-11T19:39:54.876021Z","submitted_at":"2024-12-09T11:30:25Z","title":"Discovery potential of charmonium $2P$ states through the $e^+e^- \\to \\gamma D\\bar{D}$ processes","version":2},"reference_index":53,"source":"pdf_text","source_observed_at":"2026-08-11T19:48:20.617471Z"},"links":{"cited_paper":"/paper/2106.14123","citing_paper":"/paper/2412.06400"},"observation_digest":"sha256:76bb525bca506ebf211af4e49dc5a3bbb18a38aeff097ffa594453830bb1a4f1","observation_id":"6ed8440b-1dd3-4ce8-b6a6-71d22d18d3d0","resolution":{"observed_at":"2026-08-11T19:48:20.617471Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"paper":{"arxiv_id":"2412.06400","last_updated":"2025-03-04T04:39:39Z","latest_version":2,"primary_category":"hep-ph","snapshot_observed_at":"2026-08-11T19:39:54.876021Z","submitted_at":"2024-12-09T11:30:25Z","title":"Discovery potential of charmonium $2P$ states through the $e^+e^- \\to \\gamma D\\bar{D}$ processes"},"reference_resolution":{"displayed":53,"state_counts":{"malformed_identifier":1,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":43,"verified_exact":8,"verified_fuzzy":1},"total_outbound_references":53},"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":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"thesis":"As of 13 August 2026, this Paper Citation Record lists 53 of 53 outbound references and 3 inbound Pith citation observations for arXiv:2412.06400."}