{"as_of":"2026-08-21T13:15:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:bf8601186b415c5e7cbaa079ba527a2aa9314493d750ff555a5c517db2573453","coverage":[{"denominator":38,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":38,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-08T23:10:26.763706Z","state":"measured"},{"denominator":38,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":38,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-21T06:32:19.484+00:00","state":"measured"},{"denominator":0,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":0,"source":"paper_references, paper_reference_links","source_observed_at":null,"state":"measured"},{"denominator":1,"lane":"external_citation_measurements","note":"A source-named dated measurement, never combined with another source.","records_observed":0,"source":"cited_works","source_observed_at":null,"state":"measured"}],"external_citation_measurements":[],"inbound":[],"links":{"evidence":"/evidence","html":"/paper/2502.04239/citation-record","integrity":"/paper/2502.04239/integrity","json":"/paper/2502.04239/citation-record.json","paper":"/paper/2502.04239"},"outbound":[{"citation":{"cited_paper":{"arxiv_id":"1803.01038","last_updated":"2018-05-17T12:05:25Z","snapshot_observed_at":"2026-08-15T05:28:32.240443Z","submitted_at":"2018-03-02T20:44:13Z","title":"Primordial gravitational waves, precisely: The role of thermodynamics in the Standard Model","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1803.01038","snapshot_observed_at":"2026-08-08T23:10:26.618414Z","title":"Saikawa and S","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2502.04239","last_updated":"2025-02-06T17:25:41Z","snapshot_observed_at":"2026-08-15T17:22:14.672598Z","submitted_at":"2025-02-06T17:25:41Z","title":"The Equation of State of QCD up to very high temperatures","version":1},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-08-08T23:10:26.618414Z"},"links":{"cited_paper":"/paper/1803.01038","citing_paper":"/paper/2502.04239"},"observation_digest":"sha256:b26e54e5deabab30467016d0728fabffe4dc484dca41e401dda84c426fdd5aa3","observation_id":"44ebf2fd-918c-4823-83fc-da9916bfc6aa","resolution":{"observed_at":"2026-08-08T23:10:26.618414Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2005.03544","last_updated":"2020-08-05T15:43:10Z","snapshot_observed_at":"2026-08-18T19:10:55.222742Z","submitted_at":"2020-05-07T15:13:00Z","title":"Precise WIMP Dark Matter Abundance and Standard Model Thermodynamics","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2005.03544","snapshot_observed_at":"2026-08-08T23:10:26.623029Z","title":"Saikawa and S","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2502.04239","last_updated":"2025-02-06T17:25:41Z","snapshot_observed_at":"2026-08-15T17:22:14.672598Z","submitted_at":"2025-02-06T17:25:41Z","title":"The Equation of State of QCD up to very high temperatures","version":1},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-08-08T23:10:26.623029Z"},"links":{"cited_paper":"/paper/2005.03544","citing_paper":"/paper/2502.04239"},"observation_digest":"sha256:88d7fd5bbd6ebb6a9d0b8c2babe33ae207188445c5913ec89f39b5929cc61ae1","observation_id":"35a9eef7-b96c-4fda-9b0f-5e05b82f2de5","resolution":{"observed_at":"2026-08-08T23:10:26.623029Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1309.5258","last_updated":"2014-02-17T16:41:25Z","snapshot_observed_at":"2026-08-15T00:02:27.326889Z","submitted_at":"2013-09-20T13:01:55Z","title":"Full result for the QCD equation of state with 2+1 flavors","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1309.5258","snapshot_observed_at":"2026-08-08T23:10:26.627255Z","title":"Borsanyi, Z","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2502.04239","last_updated":"2025-02-06T17:25:41Z","snapshot_observed_at":"2026-08-15T17:22:14.672598Z","submitted_at":"2025-02-06T17:25:41Z","title":"The Equation of State of QCD up to very high temperatures","version":1},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-08-08T23:10:26.627255Z"},"links":{"cited_paper":"/paper/1309.5258","citing_paper":"/paper/2502.04239"},"observation_digest":"sha256:33830e948c18dec378eb5ee2034d22504f35bce00f46862781f6a6c944474cf1","observation_id":"c74c6fa9-bd30-4202-9762-316f2c8c3ba4","resolution":{"observed_at":"2026-08-08T23:10:26.627255Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1407.6387","last_updated":"2014-11-24T21:18:03Z","snapshot_observed_at":"2026-08-14T23:25:37.241679Z","submitted_at":"2014-07-23T20:48:29Z","title":"The equation of state in (2+1)-flavor QCD","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1407.6387","snapshot_observed_at":"2026-08-08T23:10:26.631371Z","title":null,"venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2502.04239","last_updated":"2025-02-06T17:25:41Z","snapshot_observed_at":"2026-08-15T17:22:14.672598Z","submitted_at":"2025-02-06T17:25:41Z","title":"The Equation of State of QCD up to very high temperatures","version":1},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-08T23:10:26.631371Z"},"links":{"cited_paper":"/paper/1407.6387","citing_paper":"/paper/2502.04239"},"observation_digest":"sha256:5cc20d2cea4840683affa34ddcd56093d9b8cf4d3d455c7f7d340bf3573c0908","observation_id":"4d7ffc89-3065-4d16-b556-8c303c1ac6f5","resolution":{"observed_at":"2026-08-08T23:10:26.631371Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1710.05024","last_updated":"2018-03-23T16:11:12Z","snapshot_observed_at":"2026-08-14T20:23:58.981550Z","submitted_at":"2017-10-13T17:55:37Z","title":"Equation of State in 2+1 Flavor QCD at High Temperatures","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1710.05024","snapshot_observed_at":"2026-08-08T23:10:26.635510Z","title":"Bazavov, P","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2502.04239","last_updated":"2025-02-06T17:25:41Z","snapshot_observed_at":"2026-08-15T17:22:14.672598Z","submitted_at":"2025-02-06T17:25:41Z","title":"The Equation of State of QCD up to very high temperatures","version":1},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-08-08T23:10:26.635510Z"},"links":{"cited_paper":"/paper/1710.05024","citing_paper":"/paper/2502.04239"},"observation_digest":"sha256:1270668fbc764061f0e6812159771e0f883764a3c11a420c9e3dbbd1afcaad97","observation_id":"2f73b8f1-54e7-4508-a74e-97511165274d","resolution":{"observed_at":"2026-08-08T23:10:26.635510Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1606.07494","last_updated":"2016-06-27T15:04:19Z","snapshot_observed_at":"2026-08-14T21:51:22.714333Z","submitted_at":"2016-06-23T21:55:26Z","title":"Lattice QCD for Cosmology","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1606.07494","snapshot_observed_at":"2026-08-08T23:10:26.639486Z","title":"Borsanyi et al.,Calculation of the axion mass based on high-temperature lattice quantum chromodynamics, Nature 539 (2016) 69 [1606.07494]","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2502.04239","last_updated":"2025-02-06T17:25:41Z","snapshot_observed_at":"2026-08-15T17:22:14.672598Z","submitted_at":"2025-02-06T17:25:41Z","title":"The Equation of State of QCD up to very high temperatures","version":1},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-08T23:10:26.639486Z"},"links":{"cited_paper":"/paper/1606.07494","citing_paper":"/paper/2502.04239"},"observation_digest":"sha256:638431ba0f4f6569d5071a04bb1e253db177a9208c29e79d69194f41363e64d8","observation_id":"3013de69-6064-40e5-bcbc-55c2a82099f2","resolution":{"observed_at":"2026-08-08T23:10:26.639486Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T23:10:27.334522Z","title":"Appelquist and R.D","venue":null,"work_id":"600017d7-0132-44ac-8261-a0a23e7433fe","year":1981},"citing_paper":{"arxiv_id":"2502.04239","last_updated":"2025-02-06T17:25:41Z","snapshot_observed_at":"2026-08-15T17:22:14.672598Z","submitted_at":"2025-02-06T17:25:41Z","title":"The Equation of State of QCD up to very high temperatures","version":1},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-08T23:10:26.644221Z"},"links":{"citing_paper":"/paper/2502.04239"},"observation_digest":"sha256:82bba16012fa4e424f03a7e9e029c5441ea3a480c85c3e5f2bb4555089f9d4ff","observation_id":"29d14b22-8ba5-4bbd-b2f1-4bb35cb8bd49","resolution":{"observed_at":"2026-08-08T23:10:27.338179Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"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":"hep-ph/0211321","last_updated":"2003-03-18T17:10:56Z","snapshot_observed_at":"2026-07-07T03:58:15.324410Z","submitted_at":"2002-11-20T16:27:55Z","title":"The pressure of hot QCD up to g^6 ln(1/g)","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0211321","snapshot_observed_at":"2026-08-08T23:10:26.648034Z","title":"Kajantie, M","venue":null,"work_id":null,"year":2003},"citing_paper":{"arxiv_id":"2502.04239","last_updated":"2025-02-06T17:25:41Z","snapshot_observed_at":"2026-08-15T17:22:14.672598Z","submitted_at":"2025-02-06T17:25:41Z","title":"The Equation of State of QCD up to very high temperatures","version":1},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-08T23:10:26.648034Z"},"links":{"cited_paper":"/paper/hep-ph/0211321","citing_paper":"/paper/2502.04239"},"observation_digest":"sha256:d1ea09f8402e13563dd53c897221520c7918bb35162425ecf11550a141de6fdc","observation_id":"737dcb7f-375a-441f-9e02-c4ea4ba4f83f","resolution":{"observed_at":"2026-08-08T23:10:26.648034Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1005.1603","last_updated":"2010-09-15T11:47:12Z","snapshot_observed_at":"2026-08-15T05:19:28.740803Z","submitted_at":"2010-05-10T16:25:33Z","title":"Three-loop HTL gluon thermodynamics at intermediate coupling","version":4},"cited_work":{"arxiv_id":"1005.1603","doi":null,"metadata_source":"pith","pith_arxiv_id":"1005.1603","snapshot_observed_at":"2026-08-08T23:10:27.185857Z","title":"Three-loop HTL gluon thermodynamics at intermediate coupling","venue":"hep-ph","work_id":"45dec09c-948b-4b9e-947d-64a3731c2a03","year":2010},"citing_paper":{"arxiv_id":"2502.04239","last_updated":"2025-02-06T17:25:41Z","snapshot_observed_at":"2026-08-15T17:22:14.672598Z","submitted_at":"2025-02-06T17:25:41Z","title":"The Equation of State of QCD up to very high temperatures","version":1},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-08T23:10:26.651750Z"},"links":{"cited_paper":"/paper/1005.1603","citing_paper":"/paper/2502.04239"},"observation_digest":"sha256:5d16b5f3d4df632e161180b54e5e7dd6add1441af278cdb34d4e950a5435aeb0","observation_id":"6cbe71c9-b9bd-4d82-a289-f91822749d36","resolution":{"observed_at":"2026-08-08T23:10:27.189599Z","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":"1103.2528","last_updated":"2011-08-20T12:15:10Z","snapshot_observed_at":"2026-08-15T04:52:22.533799Z","submitted_at":"2011-03-13T17:06:24Z","title":"Three-loop HTL QCD thermodynamics","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1103.2528","snapshot_observed_at":"2026-08-08T23:10:26.655422Z","title":"Andersen, L.E","venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"2502.04239","last_updated":"2025-02-06T17:25:41Z","snapshot_observed_at":"2026-08-15T17:22:14.672598Z","submitted_at":"2025-02-06T17:25:41Z","title":"The Equation of State of QCD up to very high temperatures","version":1},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-08T23:10:26.655422Z"},"links":{"cited_paper":"/paper/1103.2528","citing_paper":"/paper/2502.04239"},"observation_digest":"sha256:b5619b28c20ec3a1d001f6be1cf9d5c693a8b832eb535cf0274fb13fd3028329","observation_id":"afba865f-fa0a-4b30-b1f4-0da5335479be","resolution":{"observed_at":"2026-08-08T23:10:26.655422Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1612.00265","last_updated":"2017-04-27T08:56:25Z","snapshot_observed_at":"2026-08-19T16:46:27.778130Z","submitted_at":"2016-12-01T14:30:18Z","title":"Equation of state of the SU($3$) Yang-Mills theory: a precise determination from a moving frame","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1612.00265","snapshot_observed_at":"2026-08-08T23:10:26.659654Z","title":"Giusti and M","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2502.04239","last_updated":"2025-02-06T17:25:41Z","snapshot_observed_at":"2026-08-15T17:22:14.672598Z","submitted_at":"2025-02-06T17:25:41Z","title":"The Equation of State of QCD up to very high temperatures","version":1},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-08-08T23:10:26.659654Z"},"links":{"cited_paper":"/paper/1612.00265","citing_paper":"/paper/2502.04239"},"observation_digest":"sha256:ba1806d19b8e8604c2594c7fb060f83c747eee96e5562b55a704dee759bdd83d","observation_id":"1df2333f-0d74-418e-a3ee-766a06a9e5a4","resolution":{"observed_at":"2026-08-08T23:10:26.659654Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2112.05427","last_updated":"2022-04-07T08:59:09Z","snapshot_observed_at":"2026-08-19T14:45:46.754338Z","submitted_at":"2021-12-10T10:12:02Z","title":"Non-perturbative thermal QCD at all temperatures: the case of mesonic screening masses","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2112.05427","snapshot_observed_at":"2026-08-08T23:10:26.663463Z","title":"Dalla Brida, L","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2502.04239","last_updated":"2025-02-06T17:25:41Z","snapshot_observed_at":"2026-08-15T17:22:14.672598Z","submitted_at":"2025-02-06T17:25:41Z","title":"The Equation of State of QCD up to very high temperatures","version":1},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-08-08T23:10:26.663463Z"},"links":{"cited_paper":"/paper/2112.05427","citing_paper":"/paper/2502.04239"},"observation_digest":"sha256:51d70d00a99349fffd0c26710a07124b840166f475cdcfffef81627414b29446","observation_id":"3a1a116c-abc3-4b5e-b1f5-327fcf4ef055","resolution":{"observed_at":"2026-08-08T23:10:26.663463Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2405.04182","last_updated":"2024-05-07T10:39:32Z","snapshot_observed_at":"2026-08-16T13:54:45.224103Z","submitted_at":"2024-05-07T10:39:32Z","title":"Baryonic screening masses in QCD at high temperature","version":1},"cited_work":{"arxiv_id":"2405.04182","doi":null,"metadata_source":"pith","pith_arxiv_id":"2405.04182","snapshot_observed_at":"2026-08-08T23:10:27.141253Z","title":"Baryonic screening masses in QCD at high temperature","venue":"hep-lat","work_id":"d41163f0-71bb-4565-8104-6fa1c54a234e","year":2024},"citing_paper":{"arxiv_id":"2502.04239","last_updated":"2025-02-06T17:25:41Z","snapshot_observed_at":"2026-08-15T17:22:14.672598Z","submitted_at":"2025-02-06T17:25:41Z","title":"The Equation of State of QCD up to very high temperatures","version":1},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-08T23:10:26.666981Z"},"links":{"cited_paper":"/paper/2405.04182","citing_paper":"/paper/2502.04239"},"observation_digest":"sha256:8c4270762bfe1277beb53b6e379d64e89721310b7fa7489290320a09eb6487b8","observation_id":"9f1f3634-6260-4ed3-a8cc-8c0b63f9840e","resolution":{"observed_at":"2026-08-08T23:10:27.145520Z","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":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T23:10:26.670654Z","title":"Bresciani, M.D","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2502.04239","last_updated":"2025-02-06T17:25:41Z","snapshot_observed_at":"2026-08-15T17:22:14.672598Z","submitted_at":"2025-02-06T17:25:41Z","title":"The Equation of State of QCD up to very high temperatures","version":1},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-08T23:10:26.670654Z"},"links":{"citing_paper":"/paper/2502.04239"},"observation_digest":"sha256:2145588f9041e3ecedbf58e60429fe40d899864aa49d3eae48c0566182733641","observation_id":"565b4342-3316-4e9a-8840-361b1862e0c5","resolution":{"observed_at":"2026-08-08T23:10:26.670654Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1211.6669","last_updated":"2012-11-28T17:29:18Z","snapshot_observed_at":"2026-08-19T20:55:05.663225Z","submitted_at":"2012-11-28T17:29:18Z","title":"Implications of Poincare symmetry for thermal field theories in finite-volume","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1211.6669","snapshot_observed_at":"2026-08-08T23:10:26.674490Z","title":"Giusti and H.B","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2502.04239","last_updated":"2025-02-06T17:25:41Z","snapshot_observed_at":"2026-08-15T17:22:14.672598Z","submitted_at":"2025-02-06T17:25:41Z","title":"The Equation of State of QCD up to very high temperatures","version":1},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-08-08T23:10:26.674490Z"},"links":{"cited_paper":"/paper/1211.6669","citing_paper":"/paper/2502.04239"},"observation_digest":"sha256:e782ea9aba53f22633ae0459749eb61315c4a71e21ccfa8b757b37bb6a99a573","observation_id":"5a07be70-641c-48dd-9ff6-9a3b064d2526","resolution":{"observed_at":"2026-08-08T23:10:26.674490Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2002.06897","last_updated":"2020-03-19T19:08:30Z","snapshot_observed_at":"2026-08-20T18:18:54.573652Z","submitted_at":"2020-02-17T11:42:50Z","title":"Non-perturbative definition of the QCD energy-momentum tensor on the lattice","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2002.06897","snapshot_observed_at":"2026-08-08T23:10:26.678320Z","title":"Dalla Brida, L","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2502.04239","last_updated":"2025-02-06T17:25:41Z","snapshot_observed_at":"2026-08-15T17:22:14.672598Z","submitted_at":"2025-02-06T17:25:41Z","title":"The Equation of State of QCD up to very high temperatures","version":1},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-08-08T23:10:26.678320Z"},"links":{"cited_paper":"/paper/2002.06897","citing_paper":"/paper/2502.04239"},"observation_digest":"sha256:e762babb95e5c474dcad62e46c0bbf886e370859dd19d9434f68da6de98652a8","observation_id":"d741c618-a724-4995-8393-d7bc886fe957","resolution":{"observed_at":"2026-08-08T23:10:26.678320Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1802.05243","last_updated":"2018-06-06T09:31:23Z","snapshot_observed_at":"2026-08-14T19:45:50.295970Z","submitted_at":"2018-02-14T18:05:15Z","title":"Non-perturbative quark mass renormalisation and running in $N_f=3$ QCD","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1802.05243","snapshot_observed_at":"2026-08-08T23:10:26.682158Z","title":null,"venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2502.04239","last_updated":"2025-02-06T17:25:41Z","snapshot_observed_at":"2026-08-15T17:22:14.672598Z","submitted_at":"2025-02-06T17:25:41Z","title":"The Equation of State of QCD up to very high temperatures","version":1},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-08-08T23:10:26.682158Z"},"links":{"cited_paper":"/paper/1802.05243","citing_paper":"/paper/2502.04239"},"observation_digest":"sha256:1807c26d372d04143ba4c530130a2b8046ae70bdf4b86dd444e4e84a77ffa189","observation_id":"8d102bf0-7335-4a0a-a7f7-04cbbf0c66bc","resolution":{"observed_at":"2026-08-08T23:10:26.682158Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1803.10230","last_updated":"2018-03-27T11:04:40Z","snapshot_observed_at":"2026-08-14T19:32:04.427755Z","submitted_at":"2018-03-27T11:04:40Z","title":"A non-perturbative exploration of the high energy regime in $N_\\text{f}=3$ QCD","version":1},"cited_work":{"arxiv_id":"1803.10230","doi":null,"metadata_source":"pith","pith_arxiv_id":"1803.10230","snapshot_observed_at":"2026-08-08T23:10:27.029916Z","title":"A non-perturbative exploration of the high energy regime in $N_\\text{f}=3$ QCD","venue":"hep-lat","work_id":"fc0af29d-82c9-44c6-95c5-95b6341ce16b","year":2018},"citing_paper":{"arxiv_id":"2502.04239","last_updated":"2025-02-06T17:25:41Z","snapshot_observed_at":"2026-08-15T17:22:14.672598Z","submitted_at":"2025-02-06T17:25:41Z","title":"The Equation of State of QCD up to very high temperatures","version":1},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-08-08T23:10:26.685861Z"},"links":{"cited_paper":"/paper/1803.10230","citing_paper":"/paper/2502.04239"},"observation_digest":"sha256:b510514987ed356954d2bdb9d69cb27cd4d19c4ee668371b18b517f1a84eb452","observation_id":"93026eb6-41ff-4a4a-9266-86c32831c849","resolution":{"observed_at":"2026-08-08T23:10:27.033862Z","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":"1706.03821","last_updated":"2017-07-12T15:56:18Z","snapshot_observed_at":"2026-08-19T14:56:16.928697Z","submitted_at":"2017-06-12T19:47:23Z","title":"The strong coupling from a nonperturbative determination of the $\\Lambda$ parameter in three-flavor QCD","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1706.03821","snapshot_observed_at":"2026-08-08T23:10:26.689675Z","title":null,"venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2502.04239","last_updated":"2025-02-06T17:25:41Z","snapshot_observed_at":"2026-08-15T17:22:14.672598Z","submitted_at":"2025-02-06T17:25:41Z","title":"The Equation of State of QCD up to very high temperatures","version":1},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-08-08T23:10:26.689675Z"},"links":{"cited_paper":"/paper/1706.03821","citing_paper":"/paper/2502.04239"},"observation_digest":"sha256:b345b9c7b2e835c509cc8268592c9d018b821011a90a4af8303e5a5691a591c0","observation_id":"67cbe030-112c-4b81-9203-68e01461fdbe","resolution":{"observed_at":"2026-08-08T23:10:26.689675Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1503.07042","last_updated":"2015-06-04T14:33:24Z","snapshot_observed_at":"2026-08-17T01:29:13.614251Z","submitted_at":"2015-03-24T13:56:39Z","title":"Energy-momentum tensor on the lattice: non-perturbative renormalization in Yang--Mills theory","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1503.07042","snapshot_observed_at":"2026-08-08T23:10:26.693553Z","title":"Giusti and M","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2502.04239","last_updated":"2025-02-06T17:25:41Z","snapshot_observed_at":"2026-08-15T17:22:14.672598Z","submitted_at":"2025-02-06T17:25:41Z","title":"The Equation of State of QCD up to very high temperatures","version":1},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-08-08T23:10:26.693553Z"},"links":{"cited_paper":"/paper/1503.07042","citing_paper":"/paper/2502.04239"},"observation_digest":"sha256:587991f5e8205efe87e3fba5f1c1f7400ebadcf90ac79936172fc175ef8e806c","observation_id":"0cfb8731-380d-4765-867b-ae075874fe4d","resolution":{"observed_at":"2026-08-08T23:10:26.693553Z","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":"2203.14754","doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T23:10:26.988908Z","title":"Bresciani, M","venue":null,"work_id":"0f55eb9f-e098-46ed-ab59-2b791fc2c9db","year":2022},"citing_paper":{"arxiv_id":"2502.04239","last_updated":"2025-02-06T17:25:41Z","snapshot_observed_at":"2026-08-15T17:22:14.672598Z","submitted_at":"2025-02-06T17:25:41Z","title":"The Equation of State of QCD up to very high temperatures","version":1},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-08-08T23:10:26.697680Z"},"links":{"citing_paper":"/paper/2502.04239"},"observation_digest":"sha256:fb9c3fa11fee3727b22ca143019f4a5bf487c09443b0a5c53404a5d65a9f544d","observation_id":"d344947c-1a93-41b7-9eab-31df1f8ef78c","resolution":{"observed_at":"2026-08-08T23:10:26.995288Z","resolver_source":"raw_fallback","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":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T23:10:27.322756Z","title":"Adler,Overrelaxation Algorithms for Lattice Field Theories, Phys","venue":null,"work_id":"715e7c7d-e835-4e16-b6ef-5d8f55de40a7","year":1988},"citing_paper":{"arxiv_id":"2502.04239","last_updated":"2025-02-06T17:25:41Z","snapshot_observed_at":"2026-08-15T17:22:14.672598Z","submitted_at":"2025-02-06T17:25:41Z","title":"The Equation of State of QCD up to very high temperatures","version":1},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-08-08T23:10:26.701400Z"},"links":{"citing_paper":"/paper/2502.04239"},"observation_digest":"sha256:01411b3f13068636f48c7f9e83bf57bc14f2de6793a9aecf1b3ae2dc7e964108","observation_id":"21f0b40a-2732-4bdd-9271-9cfd81d8a114","resolution":{"observed_at":"2026-08-08T23:10:27.327608Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"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":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T23:10:27.311741Z","title":"Cabibbo and E","venue":null,"work_id":"27dde706-5caa-4d3c-8b4d-691b0fbd8306","year":1982},"citing_paper":{"arxiv_id":"2502.04239","last_updated":"2025-02-06T17:25:41Z","snapshot_observed_at":"2026-08-15T17:22:14.672598Z","submitted_at":"2025-02-06T17:25:41Z","title":"The Equation of State of QCD up to very high temperatures","version":1},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-08-08T23:10:26.705144Z"},"links":{"citing_paper":"/paper/2502.04239"},"observation_digest":"sha256:fc895594551279971a348e71fd83a95d4538733feb4225e8aa64319413b7fb01","observation_id":"2e4a8deb-3ceb-41f7-9453-4f72fa1287cc","resolution":{"observed_at":"2026-08-08T23:10:27.315280Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"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":"2209.14188","last_updated":"2023-03-18T14:33:26Z","snapshot_observed_at":"2026-08-16T16:29:12.988474Z","submitted_at":"2022-09-28T16:01:01Z","title":"On fits to correlated and auto-correlated data","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2209.14188","snapshot_observed_at":"2026-08-08T23:10:26.708950Z","title":"Bruno and R","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2502.04239","last_updated":"2025-02-06T17:25:41Z","snapshot_observed_at":"2026-08-15T17:22:14.672598Z","submitted_at":"2025-02-06T17:25:41Z","title":"The Equation of State of QCD up to very high temperatures","version":1},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-08-08T23:10:26.708950Z"},"links":{"cited_paper":"/paper/2209.14188","citing_paper":"/paper/2502.04239"},"observation_digest":"sha256:36c6b653b6a51ef3699bfb0fb1a20d989272d06cc935373725adde1342abf61d","observation_id":"c02ca7e8-6188-4fb1-b624-887ee10729b5","resolution":{"observed_at":"2026-08-08T23:10:26.708950Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2209.14371","last_updated":"2023-04-07T11:38:41Z","snapshot_observed_at":"2026-08-19T07:42:38.808223Z","submitted_at":"2022-09-28T19:01:13Z","title":"pyerrors: a python framework for error analysis of Monte Carlo data","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2209.14371","snapshot_observed_at":"2026-08-08T23:10:26.713057Z","title":"Joswig, S","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2502.04239","last_updated":"2025-02-06T17:25:41Z","snapshot_observed_at":"2026-08-15T17:22:14.672598Z","submitted_at":"2025-02-06T17:25:41Z","title":"The Equation of State of QCD up to very high temperatures","version":1},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-08-08T23:10:26.713057Z"},"links":{"cited_paper":"/paper/2209.14371","citing_paper":"/paper/2502.04239"},"observation_digest":"sha256:50e4cd496a8f7f0acacaf84281d7390d26c9473e653a04754ca267900313e2ea","observation_id":"6bb66844-b237-4d15-927d-4835b79a31fa","resolution":{"observed_at":"2026-08-08T23:10:26.713057Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1809.01289","last_updated":"2019-02-06T18:09:31Z","snapshot_observed_at":"2026-08-14T18:32:57.584745Z","submitted_at":"2018-09-05T01:20:28Z","title":"Automatic differentiation for error analysis of Monte Carlo data","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1809.01289","snapshot_observed_at":"2026-08-08T23:10:26.716977Z","title":"Ramos,Automatic differentiation for error analysis of Monte Carlo data, Comput","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2502.04239","last_updated":"2025-02-06T17:25:41Z","snapshot_observed_at":"2026-08-15T17:22:14.672598Z","submitted_at":"2025-02-06T17:25:41Z","title":"The Equation of State of QCD up to very high temperatures","version":1},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-08-08T23:10:26.716977Z"},"links":{"cited_paper":"/paper/1809.01289","citing_paper":"/paper/2502.04239"},"observation_digest":"sha256:ae343a092c7d1e7562cb8592043a8e90cfd6534bd185972b49a593109936e870","observation_id":"59a347d8-04c4-41de-bb8b-565b689086ec","resolution":{"observed_at":"2026-08-08T23:10:26.716977Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1912.08498","last_updated":"2019-12-18T10:23:01Z","snapshot_observed_at":"2026-08-14T20:43:53.703063Z","submitted_at":"2019-12-18T10:23:01Z","title":"Asymptotic behavior of cutoff effects in Yang-Mills theory and in Wilson's lattice QCD","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1912.08498","snapshot_observed_at":"2026-08-08T23:10:26.721537Z","title":"Husung, P","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2502.04239","last_updated":"2025-02-06T17:25:41Z","snapshot_observed_at":"2026-08-15T17:22:14.672598Z","submitted_at":"2025-02-06T17:25:41Z","title":"The Equation of State of QCD up to very high temperatures","version":1},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-08-08T23:10:26.721537Z"},"links":{"cited_paper":"/paper/1912.08498","citing_paper":"/paper/2502.04239"},"observation_digest":"sha256:e8131b1c4555ea54852c19db4f6c5d32a5b32fd44d369ab5a0261950d6a0b84f","observation_id":"8e6f3bc5-5c5c-4ac7-ae01-30b6c9f1a917","resolution":{"observed_at":"2026-08-08T23:10:26.721537Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2111.02347","last_updated":"2024-10-17T04:55:01Z","snapshot_observed_at":"2026-08-16T17:44:15.947406Z","submitted_at":"2021-11-03T17:01:48Z","title":"The asymptotic approach to the continuum of lattice QCD spectral observables","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2111.02347","snapshot_observed_at":"2026-08-08T23:10:26.725600Z","title":"Husung, P","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2502.04239","last_updated":"2025-02-06T17:25:41Z","snapshot_observed_at":"2026-08-15T17:22:14.672598Z","submitted_at":"2025-02-06T17:25:41Z","title":"The Equation of State of QCD up to very high temperatures","version":1},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-08-08T23:10:26.725600Z"},"links":{"cited_paper":"/paper/2111.02347","citing_paper":"/paper/2502.04239"},"observation_digest":"sha256:93a64551f6f4154f2dddf9fc45d8a3d4a5132f4eb397367572b382ef7c89a07b","observation_id":"72bb74c0-d853-41b3-814e-b176144e8b29","resolution":{"observed_at":"2026-08-08T23:10:26.725600Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2206.03536","last_updated":"2022-09-30T12:15:32Z","snapshot_observed_at":"2026-08-18T09:00:54.090823Z","submitted_at":"2022-06-07T18:59:49Z","title":"Logarithmic corrections to O($a$) and O($a^2$) effects in lattice QCD with Wilson or Ginsparg-Wilson quarks","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2206.03536","snapshot_observed_at":"2026-08-08T23:10:26.729436Z","title":"Husung,Logarithmic corrections to O(a) and O(𝑎2) effects in lattice QCD with Wilson or Ginsparg–Wilson quarks, Eur","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2502.04239","last_updated":"2025-02-06T17:25:41Z","snapshot_observed_at":"2026-08-15T17:22:14.672598Z","submitted_at":"2025-02-06T17:25:41Z","title":"The Equation of State of QCD up to very high temperatures","version":1},"reference_index":29,"source":"pdf_text","source_observed_at":"2026-08-08T23:10:26.729436Z"},"links":{"cited_paper":"/paper/2206.03536","citing_paper":"/paper/2502.04239"},"observation_digest":"sha256:270d02f1bb170f5dcae5acf428cd5645185a6a91dd2b9251b99859a1ae966d8a","observation_id":"1ea611b0-f316-4b72-a173-1274c60a4746","resolution":{"observed_at":"2026-08-08T23:10:26.729436Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1606.08659","last_updated":"2016-08-03T10:34:19Z","snapshot_observed_at":"2026-08-16T13:06:50.992137Z","submitted_at":"2016-06-28T11:38:13Z","title":"Five-Loop Running of the QCD coupling constant","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1606.08659","snapshot_observed_at":"2026-08-08T23:10:26.733567Z","title":"Baikov, K.G","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2502.04239","last_updated":"2025-02-06T17:25:41Z","snapshot_observed_at":"2026-08-15T17:22:14.672598Z","submitted_at":"2025-02-06T17:25:41Z","title":"The Equation of State of QCD up to very high temperatures","version":1},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-08-08T23:10:26.733567Z"},"links":{"cited_paper":"/paper/1606.08659","citing_paper":"/paper/2502.04239"},"observation_digest":"sha256:dcc5658ad6f0b1eec59daed9b044fb5978d4c13c8b2cf9efc85f4c68f85825d4","observation_id":"0a953967-7022-4eb2-8d65-cc81ac16a70b","resolution":{"observed_at":"2026-08-08T23:10:26.733567Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0603048","last_updated":"2006-05-05T08:18:10Z","snapshot_observed_at":"2026-07-07T04:10:22.826502Z","submitted_at":"2006-03-06T16:28:06Z","title":"Quark mass thresholds in QCD thermodynamics","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0603048","snapshot_observed_at":"2026-08-08T23:10:26.737699Z","title":"Laine and Y","venue":null,"work_id":null,"year":2006},"citing_paper":{"arxiv_id":"2502.04239","last_updated":"2025-02-06T17:25:41Z","snapshot_observed_at":"2026-08-15T17:22:14.672598Z","submitted_at":"2025-02-06T17:25:41Z","title":"The Equation of State of QCD up to very high temperatures","version":1},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-08-08T23:10:26.737699Z"},"links":{"cited_paper":"/paper/hep-ph/0603048","citing_paper":"/paper/2502.04239"},"observation_digest":"sha256:cb07ade5c0c36a5c0091147817f808651ef9eb4a316103d68aed1c8d35a80764","observation_id":"35ce10fe-8027-414e-a6f6-35bae72358a8","resolution":{"observed_at":"2026-08-08T23:10:26.737699Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1011.2727","last_updated":"2011-03-20T19:13:30Z","snapshot_observed_at":"2026-08-15T05:03:13.513130Z","submitted_at":"2010-11-11T18:09:05Z","title":"Thermal momentum distribution from path integrals with shifted boundary conditions","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1011.2727","snapshot_observed_at":"2026-08-08T23:10:26.741531Z","title":"Giusti and H.B","venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"2502.04239","last_updated":"2025-02-06T17:25:41Z","snapshot_observed_at":"2026-08-15T17:22:14.672598Z","submitted_at":"2025-02-06T17:25:41Z","title":"The Equation of State of QCD up to very high temperatures","version":1},"reference_index":32,"source":"pdf_text","source_observed_at":"2026-08-08T23:10:26.741531Z"},"links":{"cited_paper":"/paper/1011.2727","citing_paper":"/paper/2502.04239"},"observation_digest":"sha256:d7ccaf178643dfd540b1ba352a7ae3a34f690a8dbdf3ca999487ebbe40b2b983","observation_id":"9696be67-bd72-4985-b4bf-a2896713d8db","resolution":{"observed_at":"2026-08-08T23:10:26.741531Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2312.11009","last_updated":"2023-12-18T08:12:10Z","snapshot_observed_at":"2026-08-16T14:33:52.672265Z","submitted_at":"2023-12-18T08:12:10Z","title":"Progresses on high-temperature QCD: Equation of State and energy-momentum tensor","version":1},"cited_work":{"arxiv_id":"2312.11009","doi":null,"metadata_source":"pith","pith_arxiv_id":"2312.11009","snapshot_observed_at":"2026-08-08T23:10:26.806263Z","title":"Progresses on high-temperature QCD: Equation of State and energy-momentum tensor","venue":"hep-lat","work_id":"0fce69bd-b831-4b0b-9c3f-7a2487fc8d5f","year":2023},"citing_paper":{"arxiv_id":"2502.04239","last_updated":"2025-02-06T17:25:41Z","snapshot_observed_at":"2026-08-15T17:22:14.672598Z","submitted_at":"2025-02-06T17:25:41Z","title":"The Equation of State of QCD up to very high temperatures","version":1},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-08-08T23:10:26.745372Z"},"links":{"cited_paper":"/paper/2312.11009","citing_paper":"/paper/2502.04239"},"observation_digest":"sha256:71a6464b13a77898793417b7aa8922ba155cb6d1013742e68db1cf8e02b81587","observation_id":"bbd71527-04ab-47c8-9bed-87e6e1d8d928","resolution":{"observed_at":"2026-08-08T23:10:26.812358Z","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":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T23:10:27.299809Z","title":"Caracciolo, G","venue":null,"work_id":"643e2407-49b2-4d4f-9c3d-277063966311","year":1990},"citing_paper":{"arxiv_id":"2502.04239","last_updated":"2025-02-06T17:25:41Z","snapshot_observed_at":"2026-08-15T17:22:14.672598Z","submitted_at":"2025-02-06T17:25:41Z","title":"The Equation of State of QCD up to very high temperatures","version":1},"reference_index":34,"source":"pdf_text","source_observed_at":"2026-08-08T23:10:26.749105Z"},"links":{"citing_paper":"/paper/2502.04239"},"observation_digest":"sha256:84b10b54688b748111eef273472b9099d82d24078f56477577078eced2cebdba","observation_id":"3891b811-04d3-4936-850b-d73e79dc02eb","resolution":{"observed_at":"2026-08-08T23:10:27.304302Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"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":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T23:10:27.288853Z","title":"Caracciolo, G","venue":null,"work_id":"0b7c0ab4-a8ea-4ef9-8807-f053022913a7","year":1989},"citing_paper":{"arxiv_id":"2502.04239","last_updated":"2025-02-06T17:25:41Z","snapshot_observed_at":"2026-08-15T17:22:14.672598Z","submitted_at":"2025-02-06T17:25:41Z","title":"The Equation of State of QCD up to very high temperatures","version":1},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-08-08T23:10:26.752668Z"},"links":{"citing_paper":"/paper/2502.04239"},"observation_digest":"sha256:52b1815ab6cfd66fd3f7647afa0061ded694d45ec8ec19cc044b35a8dc924a59","observation_id":"5f41abb7-467d-4b65-af8b-2232b8b3d07a","resolution":{"observed_at":"2026-08-08T23:10:27.292979Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"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":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T23:10:27.278425Z","title":"Caracciolo, P","venue":null,"work_id":"b4c9bb26-e01e-46ad-9939-50a0bd54a40a","year":1991},"citing_paper":{"arxiv_id":"2502.04239","last_updated":"2025-02-06T17:25:41Z","snapshot_observed_at":"2026-08-15T17:22:14.672598Z","submitted_at":"2025-02-06T17:25:41Z","title":"The Equation of State of QCD up to very high temperatures","version":1},"reference_index":36,"source":"pdf_text","source_observed_at":"2026-08-08T23:10:26.756324Z"},"links":{"citing_paper":"/paper/2502.04239"},"observation_digest":"sha256:5924a6688d00c2ddf559b83d294477731a5b019414520a2e36f761c467aa9d7d","observation_id":"711fb6eb-960b-4815-b897-050110113fea","resolution":{"observed_at":"2026-08-08T23:10:27.281965Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"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":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T23:10:27.266766Z","title":"Caracciolo, P","venue":null,"work_id":"ee75c2f0-0dfe-4e33-9769-724413c02ee0","year":1992},"citing_paper":{"arxiv_id":"2502.04239","last_updated":"2025-02-06T17:25:41Z","snapshot_observed_at":"2026-08-15T17:22:14.672598Z","submitted_at":"2025-02-06T17:25:41Z","title":"The Equation of State of QCD up to very high temperatures","version":1},"reference_index":37,"source":"pdf_text","source_observed_at":"2026-08-08T23:10:26.759908Z"},"links":{"citing_paper":"/paper/2502.04239"},"observation_digest":"sha256:54c684dde6bd627623685c2e32c6e47867739c896e6c3aba6272b3d7704b9fae","observation_id":"91838e0f-7ede-4620-bd65-f878c10df4ea","resolution":{"observed_at":"2026-08-08T23:10:27.271127Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"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":"1104.3708","last_updated":"2011-06-09T21:45:41Z","snapshot_observed_at":"2026-08-15T04:48:57.428506Z","submitted_at":"2011-04-19T10:58:06Z","title":"Transport Properties of the Quark-Gluon Plasma -- A Lattice QCD Perspective","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1104.3708","snapshot_observed_at":"2026-08-08T23:10:26.763706Z","title":"Meyer,Transport Properties of the Quark-Gluon Plasma: A Lattice QCD Perspective, Eur","venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"2502.04239","last_updated":"2025-02-06T17:25:41Z","snapshot_observed_at":"2026-08-15T17:22:14.672598Z","submitted_at":"2025-02-06T17:25:41Z","title":"The Equation of State of QCD up to very high temperatures","version":1},"reference_index":38,"source":"pdf_text","source_observed_at":"2026-08-08T23:10:26.763706Z"},"links":{"cited_paper":"/paper/1104.3708","citing_paper":"/paper/2502.04239"},"observation_digest":"sha256:ec4158ccda8d0c15eb624d4f7ec3d27540c18ce152ddd00b95fcf83150a2a82d","observation_id":"479d0dd3-b447-4402-951c-19e6d0f6728d","resolution":{"observed_at":"2026-08-08T23:10:26.763706Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"paper":{"arxiv_id":"2502.04239","last_updated":"2025-02-06T17:25:41Z","latest_version":1,"primary_category":"hep-lat","snapshot_observed_at":"2026-08-15T17:22:14.672598Z","submitted_at":"2025-02-06T17:25:41Z","title":"The Equation of State of QCD up to very high temperatures"},"reference_resolution":{"displayed":38,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":26,"verified_exact":5,"verified_fuzzy":7},"total_outbound_references":38},"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 21 August 2026, this Paper Citation Record lists 38 of 38 outbound references and 0 inbound Pith citation observations for arXiv:2502.04239."}