{"as_of":"2026-08-05T08:10:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:6c1cc1e443d673765052f7906f20a56ae9785629371b06dd21c9e5af7301067b","coverage":[{"denominator":85,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":85,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-03T13:37:12.466619Z","state":"measured"},{"denominator":87,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":87,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-05T06:32:48.257954+00:00","state":"measured"},{"denominator":2,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":2,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-04T05:53:28.034722Z","state":"measured"},{"denominator":1,"lane":"external_citation_measurements","note":"A source-named dated measurement, never combined with another source.","records_observed":0,"source":"pith","source_observed_at":"2026-07-01T11:05:41.637757Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2512.24072","snapshot_observed_at":"2026-08-04T05:53:28.034722Z","title":null,"venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2603.12589","last_updated":"2026-08-03T02:46:22Z","snapshot_observed_at":"2026-08-05T07:33:17.062007Z","submitted_at":"2026-03-13T02:43:32Z","title":"Quarkonium spectra with magnetically induced anisotropic confinement","version":2},"reference_index":69,"source":"pdf_text","source_observed_at":"2026-08-04T05:53:28.034722Z"},"links":{"cited_paper":"/paper/2512.24072","citing_paper":"/paper/2603.12589"},"observation_digest":"sha256:f0e32db58598805e312abb16b0eb1f0becc00f7e36b08349de90f03c0d8de9db","observation_id":"fd6341e0-bdfe-400c-8703-9bd01bc147f4","resolution":{"observed_at":"2026-08-04T05:53:28.034722Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"cited_work":{"arxiv_id":"2512.24072","doi":null,"metadata_source":"pith","pith_arxiv_id":"2512.24072","snapshot_observed_at":"2026-07-01T11:05:41.637757Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","venue":"hep-ph","work_id":"26e7a347-0132-4d47-bd3e-6b7887e0833d","year":2025},"citing_paper":{"arxiv_id":"2606.31697","last_updated":"2026-06-30T14:08:20Z","snapshot_observed_at":"2026-07-07T00:05:22.503928Z","submitted_at":"2026-06-30T14:08:20Z","title":"Hadronic exceptional points","version":1},"reference_index":102,"source":"pdf_text","source_observed_at":"2026-07-01T04:48:30.563853Z"},"links":{"cited_paper":"/paper/2512.24072","citing_paper":"/paper/2606.31697"},"observation_digest":"sha256:d07571498def536ea8a529b311701b6fc76ecdbf3e1177ce2bde5e98171ce156","observation_id":"fcde7cea-6daf-47d6-be85-837d53a4452c","resolution":{"observed_at":"2026-07-01T11:05:41.639044Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-05T06:32:48.257954+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-05T06:32:48.257954+00:00","source":"crossref"},{"observed_at":"2026-08-05T06:32:44.755628+00:00","source":"retraction_watch"}],"state":"measured"}}],"links":{"evidence":"/evidence","html":"/paper/2512.24072/citation-record","integrity":"/paper/2512.24072/integrity","json":"/paper/2512.24072/citation-record.json","paper":"/paper/2512.24072"},"outbound":[{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-03T13:37:02.892358Z","title":"Figure 3 shows the time evolution for three representative sweep rates, starting from aψ= (1,0) T initial state","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:02.892358Z"},"links":{"citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:463df90a1e753a68ac32425a873a3d409bfbbe4ff6d705d41847e7887547de76","observation_id":"5c738996-3858-4173-94f1-c6d75839e812","resolution":{"observed_at":"2026-08-03T13:37:02.892358Z","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":"2026-08-03T13:37:02.981885Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:02.981885Z"},"links":{"citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:493b6f3ac6e472702b3f1a2e6e4b2075e13bb45bee379df99ca61d9d9fcbc353","observation_id":"19a47c8d-d744-4848-a513-ceece1c55741","resolution":{"observed_at":"2026-08-03T13:37:02.981885Z","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":"2026-08-03T13:37:03.095994Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:03.095994Z"},"links":{"citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:e06b79bd33945942abf7a0a7f3a54e52b0d345939743fa811a8fea83d7e74cf3","observation_id":"3b9b21ad-bccc-4ba0-806c-a11c43844ed6","resolution":{"observed_at":"2026-08-03T13:37:03.095994Z","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":"2026-08-03T13:37:03.181976Z","title":null,"venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:03.181976Z"},"links":{"citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:5ffb8e8ba6352cf21d68ab639c37e00bc6920b804d29968981e56c324c86c803","observation_id":"161a98cd-2c1c-4575-808f-45a334f5ae57","resolution":{"observed_at":"2026-08-03T13:37:03.181976Z","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":"2026-08-03T13:37:03.256050Z","title":"The instantaneous level spacing (at ∆ = 0) isν eff =|α 1 −α 2|νB","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:03.256050Z"},"links":{"citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:22898af7917c4934ac15fd3b520a69ce3e3cb72e5fd7a7949c51fb2f9fdb5486","observation_id":"539f4b44-3b45-4526-894a-e89e38b16033","resolution":{"observed_at":"2026-08-03T13:37:03.256050Z","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":"2026-08-03T13:37:03.338292Z","title":"Each passage coherently splits the wave function between the adiabatic branches (left panel of Fig","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:03.338292Z"},"links":{"citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:ed8bf76e29912a1398519374ea507a8335964ea7b354496b4962ff65078ecce0","observation_id":"427116e2-1bf7-4da5-bdcb-841ca8cc7050","resolution":{"observed_at":"2026-08-03T13:37:03.338292Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1111.4956","last_updated":"2012-02-28T10:08:46Z","snapshot_observed_at":"2026-07-06T02:37:57.246464Z","submitted_at":"2011-11-21T17:58:30Z","title":"The QCD phase diagram for external magnetic fields","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1111.4956","snapshot_observed_at":"2026-08-03T13:37:03.407863Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:03.407863Z"},"links":{"cited_paper":"/paper/1111.4956","citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:774186703b35766998927245b5d6ce1363daec47112aa1cbe41c53a0c384dd01","observation_id":"515241e3-b957-4468-8d0b-a741d95396b0","resolution":{"observed_at":"2026-08-03T13:37:03.407863Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1203.5699","last_updated":"2014-01-08T19:06:51Z","snapshot_observed_at":"2026-07-06T02:45:12.497813Z","submitted_at":"2012-03-26T15:20:06Z","title":"The $\\rho$ and $A$ mesons in strong abelian magnetic field in SU(2) lattice gauge theory","version":6},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1203.5699","snapshot_observed_at":"2026-08-03T13:37:03.480595Z","title":null,"venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:03.480595Z"},"links":{"cited_paper":"/paper/1203.5699","citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:21f6832a9353502c57a94a1960939fcb7d9d1d0aa4ff6a49c5cc9872fc3ab7f5","observation_id":"9cbf7fdd-50a9-4c9e-b7ff-b924824cd3ee","resolution":{"observed_at":"2026-08-03T13:37:03.480595Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1209.0007","last_updated":"2013-05-07T02:21:21Z","snapshot_observed_at":"2026-07-06T02:54:44.378468Z","submitted_at":"2012-08-31T20:00:01Z","title":"Charged vector mesons in a strong magnetic field","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1209.0007","snapshot_observed_at":"2026-08-03T13:37:03.564738Z","title":"Hidaka and A","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:03.564738Z"},"links":{"cited_paper":"/paper/1209.0007","citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:75ed7f6ec322fa333bb949994617c2bb7c290957958c890bef2ba0efc02708e0","observation_id":"308cd1d9-e751-44cc-b761-9bfcaa4d116e","resolution":{"observed_at":"2026-08-03T13:37:03.564738Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1411.4284","last_updated":"2015-02-27T12:25:24Z","snapshot_observed_at":"2026-07-31T09:13:10.802998Z","submitted_at":"2014-11-16T17:34:11Z","title":"Magnetic polarizabilities of light mesons in $SU(3)$ lattice gauge theory","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1411.4284","snapshot_observed_at":"2026-08-03T13:37:03.636963Z","title":null,"venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:03.636963Z"},"links":{"cited_paper":"/paper/1411.4284","citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:33a4cef47f7da8252e2e50c8573a297fcdc12b3d70802b80a6895e748f2b3838","observation_id":"bc10ae65-6763-40a8-9bc2-b34d074213cf","resolution":{"observed_at":"2026-08-03T13:37:03.636963Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1511.09316","last_updated":"2016-08-19T12:31:13Z","snapshot_observed_at":"2026-07-06T04:38:11.475052Z","submitted_at":"2015-11-30T14:14:12Z","title":"Magnetic polarizability of pion","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1511.09316","snapshot_observed_at":"2026-08-03T13:37:03.740138Z","title":null,"venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:03.740138Z"},"links":{"cited_paper":"/paper/1511.09316","citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:3d7b2e3c9a009a66322dd40ca85336af5478963502db060c2129e4ac37fc3bfb","observation_id":"a43f0f95-74de-41af-8c74-c87f74ae36ce","resolution":{"observed_at":"2026-08-03T13:37:03.740138Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1707.05600","last_updated":"2018-03-05T15:55:33Z","snapshot_observed_at":"2026-08-01T20:52:23.159223Z","submitted_at":"2017-07-18T13:25:24Z","title":"Meson masses in electromagnetic fields with Wilson fermions","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1707.05600","snapshot_observed_at":"2026-08-03T13:37:03.923122Z","title":null,"venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:03.923122Z"},"links":{"cited_paper":"/paper/1707.05600","citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:5ae844db88e107ba7d5e0f19240100deefadad6363b3a59e037600d24d1878d4","observation_id":"4a2916c7-3de4-4766-a52e-90981c576a85","resolution":{"observed_at":"2026-08-03T13:37:03.923122Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1805.10971","last_updated":"2018-08-14T14:08:35Z","snapshot_observed_at":"2026-07-06T06:41:36.871103Z","submitted_at":"2018-05-28T15:25:55Z","title":"Weak decay of magnetized pions","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1805.10971","snapshot_observed_at":"2026-08-03T13:37:03.991901Z","title":null,"venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:03.991901Z"},"links":{"cited_paper":"/paper/1805.10971","citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:5d2d156151fa4cc8326f6a7392544ab00ee9f5f7400b0d04e47a9efed879ab28","observation_id":"b6ee7dbc-6684-45c9-bfe9-b4be42605593","resolution":{"observed_at":"2026-08-03T13:37:03.991901Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1811.02344","last_updated":"2018-11-06T13:40:18Z","snapshot_observed_at":"2026-07-06T07:12:58.513914Z","submitted_at":"2018-11-06T13:40:18Z","title":"Tensor polarizability of the vector mesons from $SU(3)$ lattice gauge theory","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1811.02344","snapshot_observed_at":"2026-08-03T13:37:04.069917Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:04.069917Z"},"links":{"cited_paper":"/paper/1811.02344","citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:0a38622f21da68433ae1d17bb1615de1b2533925cc9a033211e8fd18a3fbc47b","observation_id":"0ff99715-cce4-4623-9a82-fcf501d50e30","resolution":{"observed_at":"2026-08-03T13:37:04.069917Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1901.10182","last_updated":"2019-04-05T02:50:44Z","snapshot_observed_at":"2026-07-06T07:29:41.179060Z","submitted_at":"2019-01-29T08:59:57Z","title":"Meson deformation by magnetic fields in lattice QCD","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1901.10182","snapshot_observed_at":"2026-08-03T13:37:04.192240Z","title":"Hattori and A","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:04.192240Z"},"links":{"cited_paper":"/paper/1901.10182","citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:583256ed5bbb40154b221e3513317d357e0a67cec7e8ae5de458ce2cd9a7a792","observation_id":"fb596d68-25e2-457b-a116-ede1aaeb839b","resolution":{"observed_at":"2026-08-03T13:37:04.192240Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1910.14244","last_updated":"2020-05-19T03:24:49Z","snapshot_observed_at":"2026-07-06T08:33:36.825270Z","submitted_at":"2019-10-31T03:59:21Z","title":"Pion in a uniform background magnetic field with clover fermions","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1910.14244","snapshot_observed_at":"2026-08-03T13:37:04.308102Z","title":"Bignell, W","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:04.308102Z"},"links":{"cited_paper":"/paper/1910.14244","citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:f47434991406d9571f72a1bc80401100a63f51423369588216c2349a5ac87837","observation_id":"31d2d907-fe99-4639-8ef8-484844e9e12c","resolution":{"observed_at":"2026-08-03T13:37:04.308102Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2005.10453","last_updated":"2020-11-06T03:41:12Z","snapshot_observed_at":"2026-07-06T09:22:11.370674Z","submitted_at":"2020-05-21T03:49:09Z","title":"Pion magnetic polarisability using the background field method","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2005.10453","snapshot_observed_at":"2026-08-03T13:37:04.437120Z","title":"Bignell, W","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:04.437120Z"},"links":{"cited_paper":"/paper/2005.10453","citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:f9fa9d7be6b47909bff1a3783eca1d5f44d21ac7c1d800d3d4e6a85b519ba1d7","observation_id":"4a81e795-fb7a-4d0a-92d6-503555a15a9f","resolution":{"observed_at":"2026-08-03T13:37:04.437120Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2008.00493","last_updated":"2021-07-06T08:33:43Z","snapshot_observed_at":"2026-07-06T09:43:50.033941Z","submitted_at":"2020-08-02T14:33:34Z","title":"Chiral properties of (2+1)-flavor QCD in strong magnetic fields at zero temperature","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2008.00493","snapshot_observed_at":"2026-08-03T13:37:04.564262Z","title":"Ding, S.-T","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:04.564262Z"},"links":{"cited_paper":"/paper/2008.00493","citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:785599064c5335bc3a5b93872985e481ee5cd07de672f41e581e896f22318e62","observation_id":"8a5faf5f-ae86-475c-9e99-5bd5ce1acbdb","resolution":{"observed_at":"2026-08-03T13:37:04.564262Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2201.02349","last_updated":"2022-02-10T03:01:37Z","snapshot_observed_at":"2026-07-06T12:25:23.259452Z","submitted_at":"2022-01-07T07:11:55Z","title":"Chiral condensates and screening masses of neutral pseudoscalar mesons in thermomagnetic QCD medium","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2201.02349","snapshot_observed_at":"2026-08-03T13:37:04.725360Z","title":"Ding, S.-T","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:04.725360Z"},"links":{"cited_paper":"/paper/2201.02349","citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:04535462efcf2cd6b1dd6ef6697b69d593307609eccfc385db82fa52d69e2917","observation_id":"70e15afa-0025-4a1c-8d8f-ff831aa2a881","resolution":{"observed_at":"2026-08-03T13:37:04.725360Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2501.11262","last_updated":"2025-04-28T03:33:28Z","snapshot_observed_at":"2026-07-06T20:23:13.049815Z","submitted_at":"2025-01-20T04:08:25Z","title":"Chiral condensates and screening masses of neutral pseudoscalar mesons from lattice QCD at physical quark masses","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2501.11262","snapshot_observed_at":"2026-08-03T13:37:04.904201Z","title":"Ding, J.-B","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:04.904201Z"},"links":{"cited_paper":"/paper/2501.11262","citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:fc610b7bfde839ab60a543bce1a8a19143efb58dc877f671b09a10a868c102f8","observation_id":"ff7b3fa1-dd5c-4485-b50d-01be4e0dd325","resolution":{"observed_at":"2026-08-03T13:37:04.904201Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2406.19780","last_updated":"2025-01-07T17:55:36Z","snapshot_observed_at":"2026-08-02T14:05:23.422269Z","submitted_at":"2024-06-28T09:35:46Z","title":"QCD with background electromagnetic fields on the lattice: a review","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2406.19780","snapshot_observed_at":"2026-08-03T13:37:05.109229Z","title":"Endr˝ odi, QCD with background electromagnetic fields on the lattice: A review, Prog","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:05.109229Z"},"links":{"cited_paper":"/paper/2406.19780","citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:4caf34195e68dadfbc1db806a931f375e61fad2d610c515c2fbebaecb817857b","observation_id":"f963d798-1753-44f5-a1ab-56259db6e94c","resolution":{"observed_at":"2026-08-03T13:37:05.109229Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1910.00257","last_updated":"2019-10-01T08:43:23Z","snapshot_observed_at":"2026-08-04T20:30:45.277295Z","submitted_at":"2019-10-01T08:43:23Z","title":"Review on novel methods for lattice gauge theories","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1910.00257","snapshot_observed_at":"2026-08-03T13:37:05.277789Z","title":null,"venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:05.277789Z"},"links":{"cited_paper":"/paper/1910.00257","citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:e0591a789e2ae23cec988d8b30627f21e16506bd701cc6acb944fcffc27772db","observation_id":"91499fa5-2cdb-4984-bacb-9018f840004b","resolution":{"observed_at":"2026-08-03T13:37:05.277789Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1103.1329","last_updated":"2011-10-26T21:41:50Z","snapshot_observed_at":"2026-07-06T02:24:30.281224Z","submitted_at":"2011-03-07T18:48:39Z","title":"Quarkonium dissociation in quark-gluon plasma via ionization in magnetic field","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1103.1329","snapshot_observed_at":"2026-08-03T13:37:05.423538Z","title":"Marasinghe and K","venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:05.423538Z"},"links":{"cited_paper":"/paper/1103.1329","citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:b7c421a9c3c9f718fc9a930bc0e1444609c1d0a1ca21dbbf7e1a61efedfc671c","observation_id":"09cf968c-9f82-42ec-8100-bdf4d8001a2f","resolution":{"observed_at":"2026-08-03T13:37:05.423538Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1105.5360","last_updated":"2011-10-26T21:44:10Z","snapshot_observed_at":"2026-07-31T00:28:33.046821Z","submitted_at":"2011-05-26T17:43:10Z","title":"J/Psi dissociation in parity-odd bubbles","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1105.5360","snapshot_observed_at":"2026-08-03T13:37:05.598512Z","title":"Tuchin, J/ψdissociation in parity-odd bubbles, Phys","venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:05.598512Z"},"links":{"cited_paper":"/paper/1105.5360","citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:7c929baeefd69d311d33fc483896cc82254d52c419853292e7454a31b89de2f2","observation_id":"70547e42-9a80-4715-9f85-e809f29dd496","resolution":{"observed_at":"2026-08-03T13:37:05.598512Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1108.2525","last_updated":"2011-12-13T06:02:02Z","snapshot_observed_at":"2026-07-06T02:32:19.472010Z","submitted_at":"2011-08-11T21:22:38Z","title":"$J/\\psi$ Production by Magnetic Excitation of $\\eta_c$","version":5},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1108.2525","snapshot_observed_at":"2026-08-03T13:37:05.694576Z","title":"Yang and B","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:05.694576Z"},"links":{"cited_paper":"/paper/1108.2525","citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:9303162e9a9978b31d2014a2e2a0fcba6e71ab5f1ce23c45ad868ca18ae1a39c","observation_id":"7ab5442c-3c80-40f4-869c-a766e5c4c590","resolution":{"observed_at":"2026-08-03T13:37:05.694576Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1301.0099","last_updated":"2013-01-17T21:30:47Z","snapshot_observed_at":"2026-07-06T03:03:05.619333Z","submitted_at":"2013-01-01T15:45:41Z","title":"Particle production in strong electromagnetic fields in relativistic heavy-ion collisions","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1301.0099","snapshot_observed_at":"2026-08-03T13:37:05.876145Z","title":"Tuchin, Particle production in strong electromagnetic fields in relativistic heavy-ion collisions, Adv","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:05.876145Z"},"links":{"cited_paper":"/paper/1301.0099","citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:9b44e1b42acb6c1c9b23cd61fb21444f5330dacdfdf08f906fb9da7113a5158a","observation_id":"8b249e13-6ecf-4e78-b1f4-fd7b0c2d569c","resolution":{"observed_at":"2026-08-03T13:37:05.876145Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1305.3308","last_updated":"2013-05-14T21:56:48Z","snapshot_observed_at":"2026-08-01T04:39:55.014203Z","submitted_at":"2013-05-14T21:56:48Z","title":"Heavy quarkonium production in a strong magnetic field","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1305.3308","snapshot_observed_at":"2026-08-03T13:37:06.064769Z","title":null,"venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:06.064769Z"},"links":{"cited_paper":"/paper/1305.3308","citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:c8887552347c4bf1d0fea56c4c7bb84eb359732cd799722a08c6a690365c2f3c","observation_id":"01408fcc-a44d-48ab-8572-083baaf1885b","resolution":{"observed_at":"2026-08-03T13:37:06.064769Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1309.3003","last_updated":"2013-09-11T23:36:16Z","snapshot_observed_at":"2026-07-06T03:22:48.140559Z","submitted_at":"2013-09-11T23:36:16Z","title":"Charmonia and Bottomonia in a Magnetic Field","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1309.3003","snapshot_observed_at":"2026-08-03T13:37:06.186967Z","title":"Alford and M","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:06.186967Z"},"links":{"cited_paper":"/paper/1309.3003","citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:b52d62b327e6d1183fc3e4d667a97b3f5b5e3eeec305abf5d79d937f567f2992","observation_id":"f5a31cf2-41ac-49d1-b5d2-2937ca000698","resolution":{"observed_at":"2026-08-03T13:37:06.186967Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1406.4586","last_updated":"2014-10-21T17:07:29Z","snapshot_observed_at":"2026-07-06T03:46:36.542478Z","submitted_at":"2014-06-18T03:42:34Z","title":"QCD sum rules for magnetically induced mixing between $\\eta_c$ and $J/\\psi$","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1406.4586","snapshot_observed_at":"2026-08-03T13:37:06.299572Z","title":null,"venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":29,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:06.299572Z"},"links":{"cited_paper":"/paper/1406.4586","citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:bf012915a8e9196b585e05f03b19920e57a9712f43a22205524e54397e96f2aa","observation_id":"071a3841-1a1b-4290-8ae3-4936b689c32c","resolution":{"observed_at":"2026-08-03T13:37:06.299572Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1410.3297","last_updated":"2015-04-20T08:04:58Z","snapshot_observed_at":"2026-08-03T08:32:10.074523Z","submitted_at":"2014-10-13T13:13:57Z","title":"The melting of charmonium in a magnetic field from an effective AdS/QCD model","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1410.3297","snapshot_observed_at":"2026-08-03T13:37:06.434482Z","title":"Dudal and T","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:06.434482Z"},"links":{"cited_paper":"/paper/1410.3297","citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:0af41d4e22b7cbd88a42bfb9219a150cf22a0fde54da38303a8f60bbeed64137","observation_id":"251acddc-96f1-4a16-a70a-c8246300ac34","resolution":{"observed_at":"2026-08-03T13:37:06.434482Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1411.7675","last_updated":"2015-02-22T22:13:39Z","snapshot_observed_at":"2026-07-06T04:01:55.849445Z","submitted_at":"2014-11-27T18:37:15Z","title":"Charmonium Spectroscopy in Strong Magnetic Fields by QCD Sum Rules: S-Wave Ground States","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1411.7675","snapshot_observed_at":"2026-08-03T13:37:06.563895Z","title":null,"venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:06.563895Z"},"links":{"cited_paper":"/paper/1411.7675","citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:2f385abb1315e3e7f172e25a5fea30399ebdd8f133916e1143e7b9b670d5a34f","observation_id":"86c5deb7-f5ba-4ed2-b74f-96e3eb8f5413","resolution":{"observed_at":"2026-08-03T13:37:06.563895Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1506.07890","last_updated":"2015-09-11T10:37:39Z","snapshot_observed_at":"2026-08-03T03:35:40.788393Z","submitted_at":"2015-06-25T20:07:45Z","title":"Heavy quarkonia in strong magnetic fields","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1506.07890","snapshot_observed_at":"2026-08-03T13:37:06.666075Z","title":"Bonati, M","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":32,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:06.666075Z"},"links":{"cited_paper":"/paper/1506.07890","citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:6a6d8503bfd266eaa0b61dc799d3896b0d31897747ad309e9b4d414621ca13cc","observation_id":"723bee58-9333-4d15-be08-921c3e7212be","resolution":{"observed_at":"2026-08-03T13:37:06.666075Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1510.06760","last_updated":"2016-01-13T18:37:55Z","snapshot_observed_at":"2026-07-06T04:34:00.009461Z","submitted_at":"2015-10-22T20:24:24Z","title":"The charmonium dissociation in an \"anomalous wind\"","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1510.06760","snapshot_observed_at":"2026-08-03T13:37:06.825160Z","title":"anomalous wind","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:06.825160Z"},"links":{"cited_paper":"/paper/1510.06760","citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:03c3068f9e3956cc5ce3cacd9a52be03fdcd692e38057480708755d26546a13c","observation_id":"a3fb4bc2-ea68-4508-8e3a-09f4ff7caec4","resolution":{"observed_at":"2026-08-03T13:37:06.825160Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1601.02178","last_updated":"2016-03-30T15:42:16Z","snapshot_observed_at":"2026-07-06T04:42:22.335935Z","submitted_at":"2016-01-10T05:17:21Z","title":"Cigar-shaped quarkonia under strong magnetic field","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1601.02178","snapshot_observed_at":"2026-08-03T13:37:06.893662Z","title":"Suzuki and T","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":34,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:06.893662Z"},"links":{"cited_paper":"/paper/1601.02178","citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:ffa5226e9b4159136acf0aadaf4619f57e6551de7258d4cda384c7b788056397","observation_id":"ab61d553-4c61-427e-b94e-e11858ba510f","resolution":{"observed_at":"2026-08-03T13:37:06.893662Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1607.04935","last_updated":"2016-11-04T03:37:28Z","snapshot_observed_at":"2026-07-06T05:03:54.726155Z","submitted_at":"2016-07-18T02:16:38Z","title":"Heavy meson spectroscopy under strong magnetic field","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1607.04935","snapshot_observed_at":"2026-08-03T13:37:07.005969Z","title":"Yoshida and K","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:07.005969Z"},"links":{"cited_paper":"/paper/1607.04935","citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:744423a835810505cad12d1bba91430c719e9f7ad3fcf6adf847d28b5125607d","observation_id":"c3eb6917-c8aa-4deb-8cea-7e76283c6eb3","resolution":{"observed_at":"2026-08-03T13:37:07.005969Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1703.10508","last_updated":"2017-09-22T07:52:29Z","snapshot_observed_at":"2026-07-06T05:35:51.699515Z","submitted_at":"2017-03-30T15:03:34Z","title":"Heavy Quark Potential in a static and strong homogeneous magnetic field","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1703.10508","snapshot_observed_at":"2026-08-03T13:37:07.164008Z","title":"Hasan, B","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":36,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:07.164008Z"},"links":{"cited_paper":"/paper/1703.10508","citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:531ea46c50a01dd8a18eddbedcb3e285388bdcc46a27b1bfb8e9f29282c7fb62","observation_id":"96965957-82df-44f4-be8b-b05a046f194b","resolution":{"observed_at":"2026-08-03T13:37:07.164008Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1711.03071","last_updated":"2018-06-06T12:59:24Z","snapshot_observed_at":"2026-07-06T06:08:26.962117Z","submitted_at":"2017-11-08T18:00:49Z","title":"Heavy quark complex potential in a strongly magnetized hot QGP medium","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1711.03071","snapshot_observed_at":"2026-08-03T13:37:07.272346Z","title":"Singh, L","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":37,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:07.272346Z"},"links":{"cited_paper":"/paper/1711.03071","citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:c30265f742776f388d92427e7f300040f4a44e959931b4bfaacb9adef7d89349","observation_id":"6a2e2ad3-1f17-43cd-b706-b8c4877cbe07","resolution":{"observed_at":"2026-08-03T13:37:07.272346Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1802.02084","last_updated":"2018-02-06T17:28:27Z","snapshot_observed_at":"2026-07-06T06:22:03.822627Z","submitted_at":"2018-02-06T17:28:27Z","title":"Heavy meson dissociation in a plasma with magnetic fields","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1802.02084","snapshot_observed_at":"2026-08-03T13:37:07.406314Z","title":null,"venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":38,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:07.406314Z"},"links":{"cited_paper":"/paper/1802.02084","citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:a4b1e07aff53e77749d4223a4500380363f0386a7510239b984ebdbd13562c14","observation_id":"2b879445-8d1e-4cbf-b1d5-3775009195cb","resolution":{"observed_at":"2026-08-03T13:37:07.406314Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1802.04971","last_updated":"2019-02-06T04:46:14Z","snapshot_observed_at":"2026-08-04T10:54:07.204900Z","submitted_at":"2018-02-14T07:04:07Z","title":"Hadronic Paschen-Back effect","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1802.04971","snapshot_observed_at":"2026-08-03T13:37:07.565634Z","title":"Iwasaki, M","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":39,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:07.565634Z"},"links":{"cited_paper":"/paper/1802.04971","citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:0598bbaa42be0de44519c752861302dfec5164f902a878b1d66ee9334ef1058a","observation_id":"f00ae1cc-1710-4913-ac5f-26e8440b6f3a","resolution":{"observed_at":"2026-08-03T13:37:07.565634Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1803.04322","last_updated":"2018-12-05T05:09:21Z","snapshot_observed_at":"2026-07-06T06:27:48.684931Z","submitted_at":"2018-03-12T15:48:28Z","title":"Charmonium states in strong magnetic fields","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1803.04322","snapshot_observed_at":"2026-08-03T13:37:07.693664Z","title":null,"venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":40,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:07.693664Z"},"links":{"cited_paper":"/paper/1803.04322","citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:6d43e143157d3c51df1c6cef074e12d8a4c2b5310b2023fd81f1d6e4b1b5f0f4","observation_id":"805abf4f-2d6e-42db-85d2-b5ac905940c2","resolution":{"observed_at":"2026-08-03T13:37:07.693664Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1805.09787","last_updated":"2018-09-27T15:56:23Z","snapshot_observed_at":"2026-07-06T06:41:03.009337Z","submitted_at":"2018-05-24T17:12:35Z","title":"Quarkonium radiative decays from the hadronic Paschen-Back effect","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1805.09787","snapshot_observed_at":"2026-08-03T13:37:07.879875Z","title":"Iwasaki and K","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":41,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:07.879875Z"},"links":{"cited_paper":"/paper/1805.09787","citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:1c4082f6aa8b72fa618aa72d2bafa7fe2789093d02a32a5fab270c71c659ab79","observation_id":"fc85160d-78f6-4d2d-b763-ac0ccce3ca50","resolution":{"observed_at":"2026-08-03T13:37:07.879875Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1802.06874","last_updated":"2018-02-16T13:23:22Z","snapshot_observed_at":"2026-07-06T06:24:15.593553Z","submitted_at":"2018-02-16T13:23:22Z","title":"Landau Damping in a strong magnetic field: Dissociation of Quarkonia","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1802.06874","snapshot_observed_at":"2026-08-03T13:37:07.974763Z","title":"Hasan, B","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":42,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:07.974763Z"},"links":{"cited_paper":"/paper/1802.06874","citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:7c14aff344a0ef77da2d935ae669147a9415aedfce837b62a0595a44d8206922","observation_id":"52f169cb-e550-422c-8488-0a5babbb9b85","resolution":{"observed_at":"2026-08-03T13:37:07.974763Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1905.11309","last_updated":"2019-05-27T15:50:10Z","snapshot_observed_at":"2026-08-04T02:56:08.286664Z","submitted_at":"2019-05-27T15:50:10Z","title":"Quasinormal modes for quarkonium in a plasma with magnetic fields","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1905.11309","snapshot_observed_at":"2026-08-03T13:37:08.165848Z","title":null,"venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":43,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:08.165848Z"},"links":{"cited_paper":"/paper/1905.11309","citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:b98e0ef9c3adb5eb1a96083aecdd6130c10ed861e0ac0b086436067b3a4021f5","observation_id":"5a2055d5-f91e-47dd-ab20-21a808a39856","resolution":{"observed_at":"2026-08-03T13:37:08.165848Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2004.12857","last_updated":"2020-08-14T15:22:37Z","snapshot_observed_at":"2026-08-04T01:59:44.388237Z","submitted_at":"2020-04-27T15:11:18Z","title":"Dissociation of heavy quarkonia in a weak magnetic field","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2004.12857","snapshot_observed_at":"2026-08-03T13:37:08.303149Z","title":"Hasan and B","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":44,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:08.303149Z"},"links":{"cited_paper":"/paper/2004.12857","citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:70555652a47020d6e822cd028c300354b305bb16e650afde04d5de1eb890e5a3","observation_id":"6f04da31-72e4-41d3-ae4e-2ea7792f1d8d","resolution":{"observed_at":"2026-08-03T13:37:08.303149Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2006.09062","last_updated":"2020-10-04T15:37:58Z","snapshot_observed_at":"2026-07-06T09:29:33.569862Z","submitted_at":"2020-06-16T10:45:47Z","title":"Thermodynamics of heavy quarkonium in magnetic field background","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2006.09062","snapshot_observed_at":"2026-08-03T13:37:08.420229Z","title":null,"venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":45,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:08.420229Z"},"links":{"cited_paper":"/paper/2006.09062","citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:09725e148a0a808060827996fa15722d8edf53cd45e88d63d81c18531c5869df","observation_id":"b3a88214-ac07-4686-bbfe-c2a49ed3b42f","resolution":{"observed_at":"2026-08-03T13:37:08.420229Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2008.10457","last_updated":"2020-08-24T13:59:12Z","snapshot_observed_at":"2026-07-06T09:49:41.599755Z","submitted_at":"2020-08-24T13:59:12Z","title":"Configuration entropy description of charmonium dissociation under the influence of magnetic fields","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2008.10457","snapshot_observed_at":"2026-08-03T13:37:08.537316Z","title":null,"venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":46,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:08.537316Z"},"links":{"cited_paper":"/paper/2008.10457","citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:9caf5f03358640ec14b29ab7e718398eed3493dde4ac7af77e4508c8d45b3276","observation_id":"37658180-43a6-4d7b-8fff-0d572beae22f","resolution":{"observed_at":"2026-08-03T13:37:08.537316Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2110.04560","last_updated":"2022-08-01T19:12:16Z","snapshot_observed_at":"2026-07-06T11:56:07.301485Z","submitted_at":"2021-10-09T12:57:45Z","title":"Configuration entropy and stability of bottomonium radial excitations in a plasma with magnetic fields","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2110.04560","snapshot_observed_at":"2026-08-03T13:37:08.651797Z","title":null,"venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":47,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:08.651797Z"},"links":{"cited_paper":"/paper/2110.04560","citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:96e57735474e82fe6458b508e49900607e5560dd4ed71c2f71584ac9b24ca528","observation_id":"93bca4c9-b60b-4f77-8b58-1aa11afe9901","resolution":{"observed_at":"2026-08-03T13:37:08.651797Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2202.01486","last_updated":"2022-04-14T04:13:51Z","snapshot_observed_at":"2026-07-06T12:34:03.763785Z","submitted_at":"2022-02-03T09:40:05Z","title":"Entropic force and real-time dynamics of holographic quarkonium in a magnetic field","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2202.01486","snapshot_observed_at":"2026-08-03T13:37:08.767440Z","title":null,"venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":48,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:08.767440Z"},"links":{"cited_paper":"/paper/2202.01486","citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:5ba07e79e4e2cecf52d4255ebaede48a30870735901befde2079d4b1c398bb8e","observation_id":"d999d4b0-a04d-4bce-952c-589ae670356f","resolution":{"observed_at":"2026-08-03T13:37:08.767440Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2202.07938","last_updated":"2022-02-16T09:06:08Z","snapshot_observed_at":"2026-07-06T12:38:19.702992Z","submitted_at":"2022-02-16T09:06:08Z","title":"Magnetic field induced hair structure in charmonium gluon-dissociation","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2202.07938","snapshot_observed_at":"2026-08-03T13:37:08.884316Z","title":null,"venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":49,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:08.884316Z"},"links":{"cited_paper":"/paper/2202.07938","citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:b2afa836eeea961078cc566fc8f7b8d58d845fd8916c3e38712271b9bd2eb989","observation_id":"d8163e61-2d89-44e8-b840-7ed7262236e7","resolution":{"observed_at":"2026-08-03T13:37:08.884316Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2204.02312","last_updated":"2022-11-10T05:18:58Z","snapshot_observed_at":"2026-07-06T12:57:05.374703Z","submitted_at":"2022-04-05T16:12:23Z","title":"Anisotropic tomography of heavy quark dissociation by using general propagator structure at finite magnetic field","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2204.02312","snapshot_observed_at":"2026-08-03T13:37:09.004469Z","title":"Ghosh, A","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":50,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:09.004469Z"},"links":{"cited_paper":"/paper/2204.02312","citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:540a7e44761fd521641977db3e23d8af10c9ebeed08e173997817965d0a5fd7b","observation_id":"c855d0f7-06f3-4d3e-b69b-4f25baa46fee","resolution":{"observed_at":"2026-08-03T13:37:09.004469Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2208.05856","last_updated":"2023-08-22T11:32:12Z","snapshot_observed_at":"2026-07-06T13:40:58.960056Z","submitted_at":"2022-08-11T14:55:42Z","title":"QCD sum rule analysis of Heavy Quarkonium states in magnetized matter -- effects of (inverse) magnetic catalysis","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2208.05856","snapshot_observed_at":"2026-08-03T13:37:09.119529Z","title":"Parui, S","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":51,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:09.119529Z"},"links":{"cited_paper":"/paper/2208.05856","citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:f890080126c0431eb916e553c96974584330e60dec4b30f76813f31cd3b825b1","observation_id":"504e0b05-fcd6-4740-9a05-05ad62857aed","resolution":{"observed_at":"2026-08-03T13:37:09.119529Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2308.04410","last_updated":"2023-11-02T10:14:14Z","snapshot_observed_at":"2026-08-04T02:53:49.232223Z","submitted_at":"2023-08-08T17:14:16Z","title":"Heavy quarkonia in QGP medium in an arbitrary magnetic field","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2308.04410","snapshot_observed_at":"2026-08-03T13:37:09.237330Z","title":"Sebastian, L","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":52,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:09.237330Z"},"links":{"cited_paper":"/paper/2308.04410","citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:c928088da9d4336fb4e9e2ef097a503e2ea54e3b4b73b93872b46921c6d51b4c","observation_id":"3abe2ec3-61be-4fb7-a11b-4ea23c224bc6","resolution":{"observed_at":"2026-08-03T13:37:09.237330Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2402.07848","last_updated":"2024-02-12T17:57:13Z","snapshot_observed_at":"2026-07-06T17:29:00.943463Z","submitted_at":"2024-02-12T17:57:13Z","title":"Quarkonia dissociation at finite magnetic field in the presence of momentum anisotropy","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2402.07848","snapshot_observed_at":"2026-08-03T13:37:09.354361Z","title":"Nilima, M","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":53,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:09.354361Z"},"links":{"cited_paper":"/paper/2402.07848","citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:3e689f186decc4cf63e6042fa7f11e86b4e1cd32875d6c27de7e3ee1564d5c84","observation_id":"8c09aef2-a57c-45c4-90da-2f1a3be3c989","resolution":{"observed_at":"2026-08-03T13:37:09.354361Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2408.14813","last_updated":"2024-12-17T09:20:05Z","snapshot_observed_at":"2026-07-06T19:06:23.640089Z","submitted_at":"2024-08-27T06:50:31Z","title":"A dynamical Einstein-Born-Infeld-dilaton model and holographic quarkonium melting in a magnetic field","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2408.14813","snapshot_observed_at":"2026-08-03T13:37:09.472501Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":54,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:09.472501Z"},"links":{"cited_paper":"/paper/2408.14813","citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:bc03c91748d9d799a77025a3b0ca441e8271623257aedcf63e6c7986f7522796","observation_id":"b3515c46-81cb-4f12-8c0f-40abea7245d7","resolution":{"observed_at":"2026-08-03T13:37:09.472501Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2411.17279","last_updated":"2025-05-20T11:00:15Z","snapshot_observed_at":"2026-07-06T19:57:10.411888Z","submitted_at":"2024-11-26T10:01:31Z","title":"Interplay of magnetic field and chemical potential induced anisotropy and frame dependent chaos of a $Q\\bar{Q}$ pair in holographic QCD","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2411.17279","snapshot_observed_at":"2026-08-03T13:37:09.590709Z","title":"Shukla, J","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":55,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:09.590709Z"},"links":{"cited_paper":"/paper/2411.17279","citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:1b726ad22be72057ddf9cd1f8bd9d66121166f56107edaa864cf4ddf547ad707","observation_id":"be10f01d-3c32-481d-9582-4edef0e41bba","resolution":{"observed_at":"2026-08-03T13:37:09.590709Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2504.03294","last_updated":"2025-06-19T00:53:11Z","snapshot_observed_at":"2026-08-04T21:38:34.306941Z","submitted_at":"2025-04-04T09:18:34Z","title":"Relativistic dynamics of charmonia in strong magnetic fields","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2504.03294","snapshot_observed_at":"2026-08-03T13:37:09.708577Z","title":null,"venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":56,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:09.708577Z"},"links":{"cited_paper":"/paper/2504.03294","citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:752f077a2634e81e22406ee6f5f8e91d5421ea544e9855d19813212699e919fa","observation_id":"43b999d7-7673-4b91-a79b-b5c9bad071df","resolution":{"observed_at":"2026-08-03T13:37:09.708577Z","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":"2026-08-03T13:37:09.825806Z","title":null,"venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":57,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:09.825806Z"},"links":{"citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:2d4acf4448a8caeadd9fae97435863c9979af7f501c0db02de807352803097a7","observation_id":"ba9737f4-f32c-4eef-8cb0-c442b0c4ce4d","resolution":{"observed_at":"2026-08-03T13:37:09.825806Z","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":"2026-08-03T13:37:09.971514Z","title":null,"venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":58,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:09.971514Z"},"links":{"citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:89c7ac4e6ab54ca524e9a24afb8b54806c7fed253ded01ffe986136d31795fee","observation_id":"1f3a7cb6-6c74-42c3-80af-b91ab70ec1f8","resolution":{"observed_at":"2026-08-03T13:37:09.971514Z","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":"2026-08-03T13:37:10.085808Z","title":null,"venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":59,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:10.085808Z"},"links":{"citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:095e708b451a7956a812a44066c9e36501603d237cc500e69355642e3343ea24","observation_id":"95c5d231-3b2e-48b2-ab93-90e68a9eec1e","resolution":{"observed_at":"2026-08-03T13:37:10.085808Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1609.00747","last_updated":"2017-01-13T03:32:16Z","snapshot_observed_at":"2026-07-06T05:09:08.360468Z","submitted_at":"2016-09-02T20:54:49Z","title":"Novel quantum phenomena induced by strong magnetic fields in heavy-ion collisions","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1609.00747","snapshot_observed_at":"2026-08-03T13:37:10.200905Z","title":"Hattori and X.-G","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":60,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:10.200905Z"},"links":{"cited_paper":"/paper/1609.00747","citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:9a2c33c18a07f6014e928eb0f0cf1a171b4c087df44e13668c40d9a38fa7e577","observation_id":"e567b54b-a1eb-4379-8bbd-eb3065391ded","resolution":{"observed_at":"2026-08-03T13:37:10.200905Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2005.08277","last_updated":"2020-05-17T15:17:04Z","snapshot_observed_at":"2026-07-06T09:21:01.123768Z","submitted_at":"2020-05-17T15:17:04Z","title":"Heavy flavors under extreme conditions in high energy nuclear collisions","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2005.08277","snapshot_observed_at":"2026-08-03T13:37:10.318112Z","title":null,"venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":61,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:10.318112Z"},"links":{"cited_paper":"/paper/2005.08277","citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:b8640d475af18316f7cf7fe99ccba8619bf3b4ccdf094aff5598d0fa22de156d","observation_id":"20177e7a-6eb5-40c6-ab07-b53862b5efac","resolution":{"observed_at":"2026-08-03T13:37:10.318112Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2104.13990","last_updated":"2021-07-22T10:31:15Z","snapshot_observed_at":"2026-07-31T04:11:41.258024Z","submitted_at":"2021-04-28T19:36:12Z","title":"A review of quarkonia under strong magnetic fields","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2104.13990","snapshot_observed_at":"2026-08-03T13:37:10.434783Z","title":"Iwasaki, M","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":62,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:10.434783Z"},"links":{"cited_paper":"/paper/2104.13990","citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:8a178aa0a224fc60b841d5abc964895fca7c094a9a039959f169509708e97f4c","observation_id":"f6b9241d-d17b-432e-ad33-06b978f97afe","resolution":{"observed_at":"2026-08-03T13:37:10.434783Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1502.04407","last_updated":"2015-02-16T02:33:21Z","snapshot_observed_at":"2026-07-06T04:09:17.739171Z","submitted_at":"2015-02-16T02:33:21Z","title":"Magnetic Field Effect on Charmonium Production in High Energy Nuclear Collisions","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1502.04407","snapshot_observed_at":"2026-08-03T13:37:10.550180Z","title":null,"venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":63,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:10.550180Z"},"links":{"cited_paper":"/paper/1502.04407","citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:23cdb0d1bf92475d43250a7a344c81a04277cd1b9cb47f42e40a24f32965d9ca","observation_id":"d787f4c3-9877-4feb-967b-75f1ffd4e130","resolution":{"observed_at":"2026-08-03T13:37:10.550180Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1610.09853","last_updated":"2017-09-09T17:37:20Z","snapshot_observed_at":"2026-07-06T05:16:45.051736Z","submitted_at":"2016-10-31T10:31:18Z","title":"Delayed versus accelerated quarkonium formation in a magnetic field","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1610.09853","snapshot_observed_at":"2026-08-03T13:37:10.667865Z","title":"Suzuki and S","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":64,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:10.667865Z"},"links":{"cited_paper":"/paper/1610.09853","citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:9ade83c0a1f579053560a0801159f1332b7087174cbc03ac840b1d53aa85ccf3","observation_id":"d5a50237-45df-4f09-86ae-77d026c2dd8b","resolution":{"observed_at":"2026-08-03T13:37:10.667865Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1704.04094","last_updated":"2017-04-15T07:06:25Z","snapshot_observed_at":"2026-07-06T05:37:42.496434Z","submitted_at":"2017-04-13T12:44:14Z","title":"Majorana flipping of quarkonium spin states in transient magnetic field","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1704.04094","snapshot_observed_at":"2026-08-03T13:37:10.813737Z","title":"Dutta and S","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":65,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:10.813737Z"},"links":{"cited_paper":"/paper/1704.04094","citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:57129b26b7be2eb058cda64215585bf8b08decd01034a1db61d99cfff46da4a0","observation_id":"4bb6ed20-6a41-41f1-a743-04fddeedc315","resolution":{"observed_at":"2026-08-03T13:37:10.813737Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1712.06871","last_updated":"2017-12-19T11:22:33Z","snapshot_observed_at":"2026-07-06T06:15:04.212559Z","submitted_at":"2017-12-19T11:22:33Z","title":"Electromagnetic field effects on $\\Upsilon$-meson dissociation in PbPb collisions at LHC energies","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1712.06871","snapshot_observed_at":"2026-08-03T13:37:10.899647Z","title":"Hoelck and G","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":66,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:10.899647Z"},"links":{"cited_paper":"/paper/1712.06871","citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:171c40dee1426dc2d492d0561ae72d1e1fdf434be6e7d7ddbd86e387ecc13455","observation_id":"2789117c-9722-45ca-9248-c0abb9c3f713","resolution":{"observed_at":"2026-08-03T13:37:10.899647Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1805.04082","last_updated":"2018-05-10T17:38:14Z","snapshot_observed_at":"2026-07-06T06:38:26.436174Z","submitted_at":"2018-05-10T17:38:14Z","title":"Dissociation of heavy quarkonium states in rapidly varying strong magnetic field","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1805.04082","snapshot_observed_at":"2026-08-03T13:37:11.016173Z","title":"Bagchi, N","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":67,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:11.016173Z"},"links":{"cited_paper":"/paper/1805.04082","citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:07419990c75784f4520a25c9fbd61441899f9f3f3e591fd9cda3882a5f463712","observation_id":"394dcd11-d12e-4d13-a536-427f1516af25","resolution":{"observed_at":"2026-08-03T13:37:11.016173Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2104.13989","last_updated":"2021-07-22T10:32:14Z","snapshot_observed_at":"2026-08-04T09:21:18.645278Z","submitted_at":"2021-04-28T19:36:08Z","title":"Survival probabilities of charmonia as a clue to measure transient magnetic fields","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2104.13989","snapshot_observed_at":"2026-08-03T13:37:11.101704Z","title":"Iwasaki, D","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":68,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:11.101704Z"},"links":{"cited_paper":"/paper/2104.13989","citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:1ab76163e476362f5aa954ba96a67685eaf8336e0f6c030b88d9274e35126f52","observation_id":"50aa41d8-54ed-4eee-9f6b-514f6c130f6d","resolution":{"observed_at":"2026-08-03T13:37:11.101704Z","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":"2026-08-03T13:37:11.185862Z","title":"Majorana, Atomi orientati in campo magnetico vari- abile, Nuovo Cim.9, 43 (1932)","venue":null,"work_id":null,"year":1932},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":69,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:11.185862Z"},"links":{"citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:e27648f3367a83094cfa26e646b289d4b8d8e76f440f1ff78a8a2d4970584bb5","observation_id":"5a7f6393-c763-4e7f-aff8-576edf5c0931","resolution":{"observed_at":"2026-08-03T13:37:11.185862Z","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":"2026-08-03T13:37:11.245864Z","title":null,"venue":null,"work_id":null,"year":1932},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":70,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:11.245864Z"},"links":{"citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:f0fe27cfea0458508667134f3593aacb7e378955cbc6ea2f64986104e9e2ed96","observation_id":"fe02166f-49f7-4e84-9edc-42da7bb8db04","resolution":{"observed_at":"2026-08-03T13:37:11.245864Z","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":"2026-08-03T13:37:11.296361Z","title":null,"venue":null,"work_id":null,"year":1932},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":71,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:11.296361Z"},"links":{"citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:7ea91b970eb8c2872ac5a978a5cdf0670d3986bff64091aece8c116aa05257f2","observation_id":"776818a8-5f58-4ada-9b46-a96b2a03e261","resolution":{"observed_at":"2026-08-03T13:37:11.296361Z","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":"2026-08-03T13:37:11.408835Z","title":"Zener, Non-adiabatic crossing of energy levels, Proc","venue":null,"work_id":null,"year":1932},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":72,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:11.408835Z"},"links":{"citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:249539264b1e70dc52c5c63f7699f2c3ba62f0231ccf3f6f55ed6056bc0828c7","observation_id":"43160b09-4895-4e18-993c-efb1f4fd24dc","resolution":{"observed_at":"2026-08-03T13:37:11.408835Z","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":"2026-08-03T13:37:11.584466Z","title":"St¨ uckelberg, Theorie der unelastischen st¨ osse zwischen atomen, Helv","venue":null,"work_id":null,"year":1932},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":73,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:11.584466Z"},"links":{"citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:78c315d04cadaa7a02d48929979404cc3874a925954e6ad209af3b8829ccc731","observation_id":"89647baf-f039-43fc-80ef-a374793cd2d9","resolution":{"observed_at":"2026-08-03T13:37:11.584466Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2203.16348","last_updated":"2022-11-15T10:13:48Z","snapshot_observed_at":"2026-07-06T12:54:47.156267Z","submitted_at":"2022-03-30T14:22:20Z","title":"Nonadiabatic Landau-Zener-St\\\"uckelberg-Majorana transitions, dynamics, and interference","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2203.16348","snapshot_observed_at":"2026-08-03T13:37:11.636470Z","title":null,"venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":74,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:11.636470Z"},"links":{"cited_paper":"/paper/2203.16348","citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:4eb9c1e3239c359d6b011a179582323de761f901c2d2a0ad7fa5ca50aa1b4503","observation_id":"b70ce677-443b-4863-9610-b9611e280d3a","resolution":{"observed_at":"2026-08-03T13:37:11.636470Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0911.1917","last_updated":"2010-07-11T15:03:54Z","snapshot_observed_at":"2026-07-06T02:02:47.945015Z","submitted_at":"2009-11-10T13:22:49Z","title":"Landau-Zener-Stuckelberg interferometry","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0911.1917","snapshot_observed_at":"2026-08-03T13:37:11.748199Z","title":null,"venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":75,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:11.748199Z"},"links":{"cited_paper":"/paper/0911.1917","citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:a94ffe4a8a69ea2b7197aeaa80057ae969b3e169592ca74f33fcc3b7c25e0c64","observation_id":"869c64a8-f566-45ec-b209-e671555247bb","resolution":{"observed_at":"2026-08-03T13:37:11.748199Z","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":"2026-08-03T13:37:11.811534Z","title":"Eichten, K","venue":null,"work_id":null,"year":1975},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":76,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:11.811534Z"},"links":{"citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:669d0cdd6e849a4e0b4ba36fde045dab10f07d4471ed0caa24f397255dbebcdd","observation_id":"5dd431b3-b80f-4c82-9f8a-20c63ed32194","resolution":{"observed_at":"2026-08-03T13:37:11.811534Z","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":"2026-08-03T13:37:11.888455Z","title":"Barnes, S","venue":null,"work_id":null,"year":2005},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":77,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:11.888455Z"},"links":{"citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:222df78df0f924627c6d8452fd87192e12f0cc524cedd71db5c64fd2ee2206db","observation_id":"6572d87b-1df8-44a5-a0d1-fca88e49a6c9","resolution":{"observed_at":"2026-08-03T13:37:11.888455Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1304.2533","last_updated":"2013-04-09T11:18:11Z","snapshot_observed_at":"2026-07-06T03:10:41.876327Z","submitted_at":"2013-04-09T11:18:11Z","title":"Meson Spectrum in Strong Magnetic Fields","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1304.2533","snapshot_observed_at":"2026-08-03T13:37:11.972447Z","title":null,"venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":78,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:11.972447Z"},"links":{"cited_paper":"/paper/1304.2533","citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:9d65090d85c67db9e2950049c8b2e56b2c95a412d6ba5aca59d3f65d83ed1090","observation_id":"fee23b98-1858-42fe-b578-b36fb10841f5","resolution":{"observed_at":"2026-08-03T13:37:11.972447Z","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":"2026-08-03T13:37:12.058052Z","title":"Kamimura, Nonadiabatic coupled-rearrangement- channel approach to muonic molecules, Phys","venue":null,"work_id":null,"year":1988},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":79,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:12.058052Z"},"links":{"citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:d33d51ebab65af119ba4e29c4318093efcc5d0bbd8867d12daa3f35807ac9dad","observation_id":"00c8479f-b334-49b2-b1ac-977e588cd87a","resolution":{"observed_at":"2026-08-03T13:37:12.058052Z","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":"2026-08-03T13:37:12.139931Z","title":"Hiyama, Y","venue":null,"work_id":null,"year":2003},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":80,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:12.139931Z"},"links":{"citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:c444691add615cc4427fc134d675774b10a9244cda91d8a0bcec4c31b1a547ff","observation_id":"f126cffb-b82e-4e9e-b38a-24b233b317ff","resolution":{"observed_at":"2026-08-03T13:37:12.139931Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1505.04440","last_updated":"2016-01-15T09:58:36Z","snapshot_observed_at":"2026-07-06T04:18:06.575803Z","submitted_at":"2015-05-17T19:29:49Z","title":"Real-time Dynamics in U(1) Lattice Gauge Theories with Tensor Networks","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1505.04440","snapshot_observed_at":"2026-08-03T13:37:12.198717Z","title":"Pichler, M","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":81,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:12.198717Z"},"links":{"cited_paper":"/paper/1505.04440","citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:cd945114418dae9113e79ae54d5e7d1fba22a4b073078402be7bfa38e15b34cb","observation_id":"0393250c-1042-4afa-89a8-9399d87a0f0d","resolution":{"observed_at":"2026-08-03T13:37:12.198717Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2105.03445","last_updated":"2023-09-21T13:34:30Z","snapshot_observed_at":"2026-07-06T11:07:21.848674Z","submitted_at":"2021-05-07T18:00:05Z","title":"Entanglement generation in $(1+1)D$ QED scattering processes","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2105.03445","snapshot_observed_at":"2026-08-03T13:37:12.312393Z","title":"Rigobello, S","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":82,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:12.312393Z"},"links":{"cited_paper":"/paper/2105.03445","citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:8c08fe44bb8c3a7a2143a49de9f8cd30e3de118c582fce0d0cbca57987a3cb1f","observation_id":"ef667d1d-d679-4aef-88a1-6917eb4b28c7","resolution":{"observed_at":"2026-08-03T13:37:12.312393Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2307.02522","last_updated":"2024-02-28T17:25:29Z","snapshot_observed_at":"2026-07-06T15:50:45.304340Z","submitted_at":"2023-07-05T18:00:00Z","title":"High-Energy Collision of Quarks and Mesons in the Schwinger Model: From Tensor Networks to Circuit QED","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2307.02522","snapshot_observed_at":"2026-08-03T13:37:12.398625Z","title":"Belyansky, S","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":83,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:12.398625Z"},"links":{"cited_paper":"/paper/2307.02522","citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:dc0c58fba0e7fe6ef23105c1504ff2a125350f0cd56febc7d0e0cd7325319ba2","observation_id":"b5147367-f5d0-4610-beec-d5da54672472","resolution":{"observed_at":"2026-08-03T13:37:12.398625Z","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":"2026-08-03T13:37:12.449087Z","title":"Nakamura, Electronic transitions in atomic and molec- ular dynamic processes, J","venue":null,"work_id":null,"year":1984},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":84,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:12.449087Z"},"links":{"citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:576c1dd634516dff62efe3dc94f8f1e47b2a87266b8f8378015baadcf538a787","observation_id":"67e97562-7d3c-4318-9a03-8b5f1f852b8d","resolution":{"observed_at":"2026-08-03T13:37:12.449087Z","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":"2026-08-03T13:37:12.466619Z","title":"Kayanuma, Phase coherence and nonadiabatic transi- tion at a level crossing in a periodically driven two-level system, Phys","venue":null,"work_id":null,"year":1993},"citing_paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia","version":2},"reference_index":85,"source":"pdf_text","source_observed_at":"2026-08-03T13:37:12.466619Z"},"links":{"citing_paper":"/paper/2512.24072"},"observation_digest":"sha256:43db10ab4e7ffd9b9b03a7e89ebf56fbdd1b7c7b56eb4cd7c2ca04258e6ce345","observation_id":"d47f09b4-49cd-49da-a94b-510d5a5afe0f","resolution":{"observed_at":"2026-08-03T13:37:12.466619Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"paper":{"arxiv_id":"2512.24072","last_updated":"2026-06-30T12:11:41Z","latest_version":2,"primary_category":"hep-ph","snapshot_observed_at":"2026-08-04T02:57:38.537421Z","submitted_at":"2025-12-30T08:29:58Z","title":"Landau-Zener-St\\\"uckelberg-Majorana dynamics of magnetized quarkonia"},"reference_resolution":{"displayed":85,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":85,"verified_exact":0,"verified_fuzzy":0},"total_outbound_references":85},"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":"2026-08-05T06:32:48.257954+00:00","source":"crossref"},{"observed_at":"2026-08-05T06:32:44.755628+00:00","source":"retraction_watch"}],"thesis":"As of 5 August 2026, this Paper Citation Record lists 85 of 85 outbound references and 2 inbound Pith citation observations for arXiv:2512.24072."}