{"as_of":"2026-08-22T04:47:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:ff40d3d05162603a5180a87a713a86f545024ccebea65a4648452d77472de29a","coverage":[{"denominator":0,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":0,"source":"paper_references, paper_reference_links","source_observed_at":null,"state":"measured"},{"denominator":8,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":8,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-21T06:32:19.484+00:00","state":"measured"},{"denominator":8,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":8,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-15T21:00:52.797656Z","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":"2026-07-08T14:14:59.031045Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"1509.07366","last_updated":"2015-11-10T19:13:59Z","snapshot_observed_at":"2026-08-15T01:59:02.553977Z","submitted_at":"2015-09-24T13:34:52Z","title":"Quarkonium at finite temperature: Towards realistic phenomenology from first principles","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1509.07366","snapshot_observed_at":"2026-08-14T12:57:08.134138Z","title":"Burnier, O","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"1908.06293","last_updated":"2019-10-03T05:28:03Z","snapshot_observed_at":"2026-08-16T18:16:08.768014Z","submitted_at":"2019-08-17T10:53:17Z","title":"Quantum Brownian motion of a heavy quark pair in the quark-gluon plasma","version":2},"reference_index":69,"source":"pdf_text","source_observed_at":"2026-08-14T12:57:08.134138Z"},"links":{"cited_paper":"/paper/1509.07366","citing_paper":"/paper/1908.06293"},"observation_digest":"sha256:98272de68dbc7618de6125d84223c127c308039e08422f0ba053fd98601171d5","observation_id":"544c8a0d-9ceb-43bc-b906-4dad0f00e9e7","resolution":{"observed_at":"2026-08-14T12:57:08.134138Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1509.07366","last_updated":"2015-11-10T19:13:59Z","snapshot_observed_at":"2026-08-15T01:59:02.553977Z","submitted_at":"2015-09-24T13:34:52Z","title":"Quarkonium at finite temperature: Towards realistic phenomenology from first principles","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1509.07366","snapshot_observed_at":"2026-08-12T10:16:43.565531Z","title":"Burnier, O","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2411.19446","last_updated":"2025-02-24T06:26:53Z","snapshot_observed_at":"2026-08-16T08:57:21.161360Z","submitted_at":"2024-11-29T03:08:24Z","title":"Centre vortex evidence for a second finite-temperature QCD transition","version":2},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-12T10:16:43.565531Z"},"links":{"cited_paper":"/paper/1509.07366","citing_paper":"/paper/2411.19446"},"observation_digest":"sha256:fb98b5e3b8a4f59c9691eadc27c6cb8a3109cabc1d3165c7c6c5cf5272bd2be7","observation_id":"113c2527-e36f-433a-9ba1-33c347fb0e86","resolution":{"observed_at":"2026-08-12T10:16:43.565531Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1509.07366","last_updated":"2015-11-10T19:13:59Z","snapshot_observed_at":"2026-08-15T01:59:02.553977Z","submitted_at":"2015-09-24T13:34:52Z","title":"Quarkonium at finite temperature: Towards realistic phenomenology from first principles","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1509.07366","snapshot_observed_at":"2026-08-10T18:33:00.065784Z","title":"Burnier, O","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2501.11257","last_updated":"2025-05-17T10:43:00Z","snapshot_observed_at":"2026-08-10T20:54:47.024817Z","submitted_at":"2025-01-20T03:52:13Z","title":"In-medium bottomonium properties from lattice NRQCD calculations with extended meson operators","version":2},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-08-10T18:33:00.065784Z"},"links":{"cited_paper":"/paper/1509.07366","citing_paper":"/paper/2501.11257"},"observation_digest":"sha256:64a84a2e8220bc2381790dc1f36cc0110ebcd6139ed667a1b4211ae41e7656ac","observation_id":"be0d333c-0667-4ad6-9eb3-0dfc0a13d4ac","resolution":{"observed_at":"2026-08-10T18:33:00.065784Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1509.07366","last_updated":"2015-11-10T19:13:59Z","snapshot_observed_at":"2026-08-15T01:59:02.553977Z","submitted_at":"2015-09-24T13:34:52Z","title":"Quarkonium at finite temperature: Towards realistic phenomenology from first principles","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1509.07366","snapshot_observed_at":"2026-08-15T21:00:52.797656Z","title":"Burnier, O","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2505.11313","last_updated":"2025-05-16T14:39:38Z","snapshot_observed_at":"2026-08-18T13:49:49.557822Z","submitted_at":"2025-05-16T14:39:38Z","title":"Thermal Static Potential and Pseudo-Scalar Quarkonium Spectral Functions from 2+1 Flavor Lattice QCD","version":1},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-08-15T21:00:52.797656Z"},"links":{"cited_paper":"/paper/1509.07366","citing_paper":"/paper/2505.11313"},"observation_digest":"sha256:20cb835fcb54388b47b6fa0262b72b0f34d755e155b3422377c0d4b33d52b4a8","observation_id":"6cbd2acd-3655-4805-bfbe-dc56b33d9dd2","resolution":{"observed_at":"2026-08-15T21:00:52.797656Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1509.07366","last_updated":"2015-11-10T19:13:59Z","snapshot_observed_at":"2026-08-15T01:59:02.553977Z","submitted_at":"2015-09-24T13:34:52Z","title":"Quarkonium at finite temperature: Towards realistic phenomenology from first principles","version":2},"cited_work":{"arxiv_id":"1509.07366","doi":null,"metadata_source":"pith","pith_arxiv_id":"1509.07366","snapshot_observed_at":"2026-07-08T14:14:59.031045Z","title":"Quarkonium at finite temperature: Towards realistic phenomenology from first principles","venue":"hep-ph","work_id":"aacf76e0-a3e6-4e67-9dd1-194afb46497b","year":2015},"citing_paper":{"arxiv_id":"2604.00618","last_updated":"2026-04-01T08:24:00Z","snapshot_observed_at":"2026-07-06T22:51:26.754746Z","submitted_at":"2026-04-01T08:24:00Z","title":"Absorption of 1$P$-wave heavy charmonium $\\chi_{c1}(1P)$ in nuclei","version":1},"reference_index":53,"source":"pdf_text","source_observed_at":"2026-05-21T10:46:35.534418Z"},"links":{"cited_paper":"/paper/1509.07366","citing_paper":"/paper/2604.00618"},"observation_digest":"sha256:e5b22632c879cacfd642d88d7c7d8ec37bbd854ea0e1c5d3a7c67b6a57dfbc02","observation_id":"19eec2bb-b7bc-464f-8b2f-6c10efcd5cae","resolution":{"observed_at":"2026-05-21T10:50:01.339254Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1509.07366","last_updated":"2015-11-10T19:13:59Z","snapshot_observed_at":"2026-08-15T01:59:02.553977Z","submitted_at":"2015-09-24T13:34:52Z","title":"Quarkonium at finite temperature: Towards realistic phenomenology from first principles","version":2},"cited_work":{"arxiv_id":"1509.07366","doi":null,"metadata_source":"pith","pith_arxiv_id":"1509.07366","snapshot_observed_at":"2026-07-08T14:14:59.031045Z","title":"Quarkonium at finite temperature: Towards realistic phenomenology from first principles","venue":"hep-ph","work_id":"aacf76e0-a3e6-4e67-9dd1-194afb46497b","year":2015},"citing_paper":{"arxiv_id":"2605.20034","last_updated":"2026-05-19T15:54:40Z","snapshot_observed_at":"2026-08-15T10:33:43.562071Z","submitted_at":"2026-05-19T15:54:40Z","title":"Charmonium properties at high temperatures from lattice QCD","version":1},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-05-20T03:24:24.352814Z"},"links":{"cited_paper":"/paper/1509.07366","citing_paper":"/paper/2605.20034"},"observation_digest":"sha256:49f9c99ffa26131d1619ded70e13d46e7c61bb88921da94c805d9be31a322618","observation_id":"ee18eafa-9920-4ce4-b189-1e4f1e7430c4","resolution":{"observed_at":"2026-05-20T03:28:01.378855Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1509.07366","last_updated":"2015-11-10T19:13:59Z","snapshot_observed_at":"2026-08-15T01:59:02.553977Z","submitted_at":"2015-09-24T13:34:52Z","title":"Quarkonium at finite temperature: Towards realistic phenomenology from first principles","version":2},"cited_work":{"arxiv_id":"1509.07366","doi":null,"metadata_source":"pith","pith_arxiv_id":"1509.07366","snapshot_observed_at":"2026-07-08T14:14:59.031045Z","title":"Quarkonium at finite temperature: Towards realistic phenomenology from first principles","venue":"hep-ph","work_id":"aacf76e0-a3e6-4e67-9dd1-194afb46497b","year":2015},"citing_paper":{"arxiv_id":"2607.06191","last_updated":"2026-07-07T12:15:10Z","snapshot_observed_at":"2026-08-15T16:39:20.838814Z","submitted_at":"2026-07-07T12:15:10Z","title":"Bottomonium production in an open quantum system approach with interactions from lattice quantum chromodynamic","version":1},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-07-11T11:50:26.030339Z"},"links":{"cited_paper":"/paper/1509.07366","citing_paper":"/paper/2607.06191"},"observation_digest":"sha256:559c67fc632f77bb10c82f0a96a19db9a35aa7ecad9fb421ed85faca9b23aece","observation_id":"fbab4217-d8ee-4933-83bd-f2aa907acfc9","resolution":{"observed_at":"2026-07-08T14:14:59.032546Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1509.07366","last_updated":"2015-11-10T19:13:59Z","snapshot_observed_at":"2026-08-15T01:59:02.553977Z","submitted_at":"2015-09-24T13:34:52Z","title":"Quarkonium at finite temperature: Towards realistic phenomenology from first principles","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1509.07366","snapshot_observed_at":"2026-08-01T06:56:55.630443Z","title":"Burnier, O","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2607.21729","last_updated":"2026-07-23T18:26:57Z","snapshot_observed_at":"2026-08-17T13:06:02.784771Z","submitted_at":"2026-07-23T18:26:57Z","title":"Lattice study of spin interactions between heavy quarks in the quark-gluon plasma","version":1},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-08-01T06:56:55.630443Z"},"links":{"cited_paper":"/paper/1509.07366","citing_paper":"/paper/2607.21729"},"observation_digest":"sha256:93f74cb13fdfec8c1fb3c03ea5f7bf8a26c38974eb8c2e2a9019ca8bc13ab350","observation_id":"6535da70-b813-4b16-a18a-1b44f8de432b","resolution":{"observed_at":"2026-08-01T06:56:55.630443Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"links":{"evidence":"/evidence","html":"/paper/1509.07366/citation-record","integrity":"/paper/1509.07366/integrity","json":"/paper/1509.07366/citation-record.json","paper":"/paper/1509.07366"},"outbound":[],"paper":{"arxiv_id":"1509.07366","last_updated":"2015-11-10T19:13:59Z","latest_version":2,"primary_category":"hep-ph","snapshot_observed_at":"2026-08-15T01:59:02.553977Z","submitted_at":"2015-09-24T13:34:52Z","title":"Quarkonium at finite temperature: Towards realistic phenomenology from first principles"},"reference_resolution":{"displayed":0,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":0,"verified_exact":0,"verified_fuzzy":0},"total_outbound_references":0},"refusal":"A citation records a reference. It does not transfer a finding from one paper to another.","schema":"pith.paper-citation-record.v1","standing_sources":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"thesis":"As of 22 August 2026, this Paper Citation Record lists 0 of 0 outbound references and 8 inbound Pith citation observations for arXiv:1509.07366."}