{"as_of":"2026-08-17T16:09:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:b1ba9483684f0b7704611250ac7f6f6f950844a1a525424bdb5b9d2191cc6aaa","coverage":[{"denominator":103,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":100,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-15T21:29:14.444513Z","state":"measured"},{"denominator":101,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":101,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-17T06:30:58.91139+00:00","state":"measured"},{"denominator":1,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":1,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-15T21:29:13.987844Z","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":[{"citation":{"cited_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2608.12883","snapshot_observed_at":"2026-08-15T21:29:13.987844Z","title":null,"venue":null,"work_id":null,"year":2026},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:13.987844Z"},"links":{"cited_paper":"/paper/2608.12883","citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:d93189529fd0524f20fa3718c9fe8d200a240e0d5896f2e76c85b8d67b0b5f70","observation_id":"5647eb42-63f6-4349-b900-7d6824f6408f","resolution":{"observed_at":"2026-08-15T21:29:13.987844Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"links":{"evidence":"/evidence","html":"/paper/2608.12883/citation-record","integrity":"/paper/2608.12883/integrity","json":"/paper/2608.12883/citation-record.json","paper":"/paper/2608.12883"},"outbound":[{"citation":{"cited_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2608.12883","snapshot_observed_at":"2026-08-15T21:29:13.987844Z","title":null,"venue":null,"work_id":null,"year":2026},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:13.987844Z"},"links":{"cited_paper":"/paper/2608.12883","citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:d93189529fd0524f20fa3718c9fe8d200a240e0d5896f2e76c85b8d67b0b5f70","observation_id":"5647eb42-63f6-4349-b900-7d6824f6408f","resolution":{"observed_at":"2026-08-15T21:29:13.987844Z","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":"2026-08-15T21:29:13.994608Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:13.994608Z"},"links":{"citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:d13dc43d76fa94fcd8a4fe97080d79797dbb5e8513183d137904239dddcd4ddc","observation_id":"8475fda4-4fa3-459a-a9da-cf3b865c8672","resolution":{"observed_at":"2026-08-15T21:29:13.994608Z","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":"2026-08-15T21:29:13.999722Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:13.999722Z"},"links":{"citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:221f8962a8f8de67a2370a2ebec6c20932f2a2410cfed8332838c50c8b8c8e87","observation_id":"74d632e8-2007-46fe-867b-60c2807b15d5","resolution":{"observed_at":"2026-08-15T21:29:13.999722Z","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":"2026-08-15T21:29:14.010577Z","title":"Non-perturbative aspects of fundamental inter- actions, in the Standard Model and beyond","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.010577Z"},"links":{"citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:815c314e34bba20fa621f8b905f59108d53b79d77a1b69c231c266179fb60474","observation_id":"b43568b9-7c0d-430b-9f55-a0616f757a0c","resolution":{"observed_at":"2026-08-15T21:29:14.010577Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0803.1593","last_updated":"2013-02-06T08:39:29Z","snapshot_observed_at":"2026-08-15T10:19:46.869952Z","submitted_at":"2008-03-11T14:12:31Z","title":"Theta dependence of SU(N) gauge theories in the presence of a topological term","version":5},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0803.1593","snapshot_observed_at":"2026-08-15T21:29:14.015747Z","title":"Vicari and H","venue":null,"work_id":null,"year":2009},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.015747Z"},"links":{"cited_paper":"/paper/0803.1593","citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:8808288e552ac8aa12be43fb8759050fc81e891b9702e2ecedabfdb21150b591","observation_id":"50001d47-8abb-4b43-a427-0fb93baadb77","resolution":{"observed_at":"2026-08-15T21:29:14.015747Z","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":"2026-08-15T21:29:14.021119Z","title":"Bonanno, C","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.021119Z"},"links":{"citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:0f367ee79ae29098db0af3cad6a871efc5c1cd111aa336e177c879e4d3bc69ff","observation_id":"ef9a44af-a023-4a1e-828f-04a2e4faec38","resolution":{"observed_at":"2026-08-15T21:29:14.021119Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2604.28035","last_updated":"2026-05-01T15:55:24Z","snapshot_observed_at":"2026-07-06T23:13:24.960159Z","submitted_at":"2026-04-30T15:47:45Z","title":"Topological Susceptibility and QCD at Finite Theta Angle","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2604.28035","snapshot_observed_at":"2026-08-15T21:29:14.025663Z","title":"Bonanno, C","venue":null,"work_id":null,"year":2026},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.025663Z"},"links":{"cited_paper":"/paper/2604.28035","citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:407efc4317c2802acae86b0b89c3b5b77dbe38ee636b14c649f3c2c917bca330","observation_id":"0bfb105e-7624-4aca-afce-54fb8f0d4290","resolution":{"observed_at":"2026-08-15T21:29:14.025663Z","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":"2026-08-15T21:29:14.030092Z","title":null,"venue":null,"work_id":null,"year":1981},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.030092Z"},"links":{"citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:1dbeb92dc96c66efa64294835b416beaa2aef7113b1a2bc89cfcb2f02ba8c1e2","observation_id":"29e9314a-eb9c-4499-8591-d86749164284","resolution":{"observed_at":"2026-08-15T21:29:14.030092Z","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":"2026-08-15T21:29:14.034674Z","title":null,"venue":null,"work_id":null,"year":1980},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.034674Z"},"links":{"citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:22b3c645e643af413c412e2196bbb9d941ced01927ef43102043663fb4026b44","observation_id":"b714fbe7-8c93-43ea-8d10-e9f8648ab5ac","resolution":{"observed_at":"2026-08-15T21:29:14.034674Z","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":"2026-08-15T21:29:14.039009Z","title":"Teper, Axial Anomaly Suppression (and Axial U(1) Symmetry Restoration) at High Temperatures: A Lat- tice Monte Carlo S tudy, Phys","venue":null,"work_id":null,"year":1986},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.039009Z"},"links":{"citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:ea4139aa82f13415a847db4a13c2bc51c977d1d9a2d685e184ea18e984174136","observation_id":"9bb928e8-f6b5-4cad-867c-8894b681bda8","resolution":{"observed_at":"2026-08-15T21:29:14.039009Z","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":"2026-08-15T21:29:14.043156Z","title":"Teper, The Topological Susceptibility in SU(2) Lat- tice Gauge Theory: An Exploratory Study, Phys","venue":null,"work_id":null,"year":1986},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.043156Z"},"links":{"citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:a2f1ab3d1e4b402940f03d85e258446505346175937fbb04b0563154ba2e82d9","observation_id":"a41a8eb0-b268-48c9-a323-7a9cb0a7ceb5","resolution":{"observed_at":"2026-08-15T21:29:14.043156Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-lat/9706016","last_updated":"1997-06-19T09:53:15Z","snapshot_observed_at":"2026-08-16T09:23:17.071276Z","submitted_at":"1997-06-19T09:53:15Z","title":"Topology at zero and finite T in SU(2) Yang-Mills theory","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-lat/9706016","snapshot_observed_at":"2026-08-15T21:29:14.047396Z","title":"All´ es, M","venue":null,"work_id":null,"year":1997},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.047396Z"},"links":{"cited_paper":"/paper/hep-lat/9706016","citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:9a906978c03a654f4309703f0d1e0333d4b0e7bb9ea40c68dbbf46ebca870af5","observation_id":"80dff7a5-7a67-4e09-aeca-80b212b1ad7f","resolution":{"observed_at":"2026-08-15T21:29:14.047396Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-lat/9605013","last_updated":"2004-03-04T16:58:43Z","snapshot_observed_at":"2026-07-07T03:45:17.091043Z","submitted_at":"1996-05-11T09:57:37Z","title":"Topological susceptibility at zero and finite $T$ in SU(3) Yang-Mills theory","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-lat/9605013","snapshot_observed_at":"2026-08-15T21:29:14.051623Z","title":"All´ es, M","venue":null,"work_id":null,"year":1997},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.051623Z"},"links":{"cited_paper":"/paper/hep-lat/9605013","citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:32505d1f06370af640be90929b8ac214efb2ee1a3df5b558611c1ef548ca195a","observation_id":"d5a7d468-3027-42b6-ab3b-335745c14fea","resolution":{"observed_at":"2026-08-15T21:29:14.051623Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/0407068","last_updated":"2004-09-17T10:49:21Z","snapshot_observed_at":"2026-08-13T09:36:35.049918Z","submitted_at":"2004-07-09T10:04:41Z","title":"Topological susceptibility of SU(N) gauge theories at finite temperature","version":2},"cited_work":{"arxiv_id":"hep-th/0407068","doi":null,"metadata_source":"pith","pith_arxiv_id":"hep-th/0407068","snapshot_observed_at":"2026-08-15T21:29:16.400070Z","title":"Topological susceptibility of SU(N) gauge theories at finite temperature","venue":"hep-th","work_id":"a47ed419-a95f-4a5e-984e-242f88d1231e","year":2004},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.056861Z"},"links":{"cited_paper":"/paper/hep-th/0407068","citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:686acf7bbc7f9d7f6324db0e41abb47eddfd8284458c25fca3045bb155841322","observation_id":"234dfc81-cf0e-4657-8eef-2cf5ba841c3c","resolution":{"observed_at":"2026-08-15T21:29:16.406302Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1505.07455","last_updated":"2015-05-27T20:00:27Z","snapshot_observed_at":"2026-08-16T09:22:10.232457Z","submitted_at":"2015-05-27T20:00:27Z","title":"Lattice QCD input for axion cosmology","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1505.07455","snapshot_observed_at":"2026-08-15T21:29:14.062583Z","title":"Berkowitz, M","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.062583Z"},"links":{"cited_paper":"/paper/1505.07455","citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:963bef5125cc91c461bae29daa5a4914cf207f9ef5c6f4a903e87b525e8e1d8f","observation_id":"10535bda-42b0-440a-a9e7-8a242da24768","resolution":{"observed_at":"2026-08-15T21:29:14.062583Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1508.06917","last_updated":"2015-08-27T16:10:27Z","snapshot_observed_at":"2026-08-16T09:14:14.501688Z","submitted_at":"2015-08-27T16:10:27Z","title":"Axion cosmology, lattice QCD and the dilute instanton gas","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1508.06917","snapshot_observed_at":"2026-08-15T21:29:14.066971Z","title":"Borsanyi, M","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.066971Z"},"links":{"cited_paper":"/paper/1508.06917","citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:6972d3c1f920a795b77e73d98eb9a9d553284d8c28054f3ed83977952913a724","observation_id":"5c29f2e1-eb82-4d88-95ac-f0c4314d6b88","resolution":{"observed_at":"2026-08-15T21:29:14.066971Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1606.07175","last_updated":"2016-08-30T05:05:12Z","snapshot_observed_at":"2026-08-16T09:20:41.422036Z","submitted_at":"2016-06-23T04:00:56Z","title":"Topological susceptibility at high temperature on the lattice","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1606.07175","snapshot_observed_at":"2026-08-15T21:29:14.071028Z","title":"Frison, R","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.071028Z"},"links":{"cited_paper":"/paper/1606.07175","citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:8b359368761ef33659e61c912d4b42213f641284851139888883c7ddac0ac4ba","observation_id":"ece84e1a-9192-4901-8914-4e31567cabf9","resolution":{"observed_at":"2026-08-15T21:29:14.071028Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1506.00370","last_updated":"2015-10-21T01:37:40Z","snapshot_observed_at":"2026-08-16T09:20:12.918636Z","submitted_at":"2015-06-01T07:41:27Z","title":"Topology in QCD and the axion abundance","version":2},"cited_work":{"arxiv_id":"1506.00370","doi":null,"metadata_source":"pith","pith_arxiv_id":"1506.00370","snapshot_observed_at":"2026-08-15T21:29:16.326477Z","title":"Topology in QCD and the axion abundance","venue":"hep-ph","work_id":"7baf0b99-510b-4e62-8b91-75b70944e4b4","year":2015},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.075191Z"},"links":{"cited_paper":"/paper/1506.00370","citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:86fa091d95d981b43f33e1bd31a48ec48362aa9e5a3791846f2bb4bb182fba01","observation_id":"1816b53e-facf-493f-8d5c-8f1435ec3b31","resolution":{"observed_at":"2026-08-15T21:29:16.331101Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2101.03383","last_updated":"2021-02-25T08:43:55Z","snapshot_observed_at":"2026-08-16T18:53:20.677070Z","submitted_at":"2021-01-09T15:47:22Z","title":"Topological susceptibility of pure gauge theory using Density of States","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2101.03383","snapshot_observed_at":"2026-08-15T21:29:14.080043Z","title":"Borsanyi and D","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.080043Z"},"links":{"cited_paper":"/paper/2101.03383","citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:73a9306c2d9cd7f6d89ffc9d5c762f61052064419af13e8f5afa0ce990ee276b","observation_id":"c4e1e3da-d246-4977-bc80-c3cbcca859e0","resolution":{"observed_at":"2026-08-15T21:29:14.080043Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2212.08684","last_updated":"2022-12-16T19:18:43Z","snapshot_observed_at":"2026-08-16T16:08:02.871033Z","submitted_at":"2022-12-16T19:18:43Z","title":"Topological features of the deconfinement transition","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2212.08684","snapshot_observed_at":"2026-08-15T21:29:14.084392Z","title":"Borsanyi, Z","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.084392Z"},"links":{"cited_paper":"/paper/2212.08684","citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:bc1726e611139bfaa419c9f3451792fa9a24ce41c3e002abc755f913a6700794","observation_id":"c40a179c-063a-4495-9e2c-2302c5b7afb5","resolution":{"observed_at":"2026-08-15T21:29:14.084392Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2312.12202","last_updated":"2024-02-08T14:17:15Z","snapshot_observed_at":"2026-08-16T14:33:21.541674Z","submitted_at":"2023-12-19T14:38:33Z","title":"The $\\theta$-dependence of the $\\mathrm{SU}(N)$ critical temperature at large $N$","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2312.12202","snapshot_observed_at":"2026-08-15T21:29:14.088534Z","title":"Bonanno, M","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.088534Z"},"links":{"cited_paper":"/paper/2312.12202","citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:ca98323cab705465291726c110c36a6b52ba56117c5f4ae6dc7e6699a15e2382","observation_id":"f7f1a3e4-3863-4a37-b250-fd892bfddd58","resolution":{"observed_at":"2026-08-15T21:29:14.088534Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1807.06558","last_updated":"2018-10-08T09:55:49Z","snapshot_observed_at":"2026-08-14T18:50:52.630964Z","submitted_at":"2018-07-17T17:07:12Z","title":"$\\theta$ dependence in trace deformed $SU(3)$ Yang-Mills theory: a lattice study","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1807.06558","snapshot_observed_at":"2026-08-15T21:29:14.092828Z","title":"Bonati, M","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.092828Z"},"links":{"cited_paper":"/paper/1807.06558","citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:32e7501b6069d3f6a6f725d978172a274c95ef587e9952266dad7b0353f06fe3","observation_id":"39d588c0-f02e-471f-893f-0fccfd8dac87","resolution":{"observed_at":"2026-08-15T21:29:14.092828Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1912.02662","last_updated":"2019-12-05T15:49:58Z","snapshot_observed_at":"2026-08-16T09:21:28.659534Z","submitted_at":"2019-12-05T15:49:58Z","title":"$\\theta$-dependence and center symmetry in Yang-Mills theories","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1912.02662","snapshot_observed_at":"2026-08-15T21:29:14.096996Z","title":"Bonati, M","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.096996Z"},"links":{"cited_paper":"/paper/1912.02662","citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:00b4cebe58483e591967b056a62f7f31dcd082807356ccda2b54f81d4fe7a6e1","observation_id":"9bf4d1ac-dfb9-42bf-b21b-3facc84cf915","resolution":{"observed_at":"2026-08-15T21:29:14.096996Z","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":"2026-08-15T21:29:14.101206Z","title":"Roberge and N","venue":null,"work_id":null,"year":1986},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.101206Z"},"links":{"citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:235dd72dc6b117f815982010cbfa9eaa0c9d704cf95ce67413bcca2d30520c17","observation_id":"c5b8bc58-9b53-421b-9d2f-48e72db6e2a5","resolution":{"observed_at":"2026-08-15T21:29:14.101206Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1602.01426","last_updated":"2016-04-12T08:29:54Z","snapshot_observed_at":"2026-08-17T04:34:56.278394Z","submitted_at":"2016-02-03T19:41:25Z","title":"Roberge-Weiss endpoint at the physical point of $N_f = 2+1$ QCD","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1602.01426","snapshot_observed_at":"2026-08-15T21:29:14.105710Z","title":"Bonati, M","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.105710Z"},"links":{"cited_paper":"/paper/1602.01426","citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:311095b19f7d3be8ce17640e8104caf519e6713e2081aa467abeeee05184d954","observation_id":"0fb9ba8d-9f43-4523-8382-00b482a0245f","resolution":{"observed_at":"2026-08-15T21:29:14.105710Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1807.02106","last_updated":"2018-07-05T17:54:42Z","snapshot_observed_at":"2026-08-16T09:20:34.511799Z","submitted_at":"2018-07-05T17:54:42Z","title":"Roberge-Weiss endpoint and chiral symmetry restoration in $N_f = 2+1$ QCD","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1807.02106","snapshot_observed_at":"2026-08-15T21:29:14.110681Z","title":"Bonati, E","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.110681Z"},"links":{"cited_paper":"/paper/1807.02106","citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:142dee7a85c34f080ec3c5fadd1a710b99b062366872ee83639a9883987717bc","observation_id":"e3c370be-8866-4120-90d4-1180136e4e60","resolution":{"observed_at":"2026-08-15T21:29:14.110681Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2205.12707","last_updated":"2022-05-25T12:04:54Z","snapshot_observed_at":"2026-08-16T16:57:45.923374Z","submitted_at":"2022-05-25T12:04:54Z","title":"Towards the chiral phase transition in the Roberge-Weiss plane","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2205.12707","snapshot_observed_at":"2026-08-15T21:29:14.115287Z","title":"Cuteri, J","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.115287Z"},"links":{"cited_paper":"/paper/2205.12707","citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:b470b596fee7eb19a62ad1c412decf7d4d09874d189497a8326f8ac02d9f343d","observation_id":"e59e6d8e-8c0e-45d5-b080-404de09962d1","resolution":{"observed_at":"2026-08-15T21:29:14.115287Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2110.10029","last_updated":"2021-10-19T14:53:20Z","snapshot_observed_at":"2026-08-16T17:48:08.525866Z","submitted_at":"2021-10-19T14:53:20Z","title":"Localization properties of Dirac modes at the Roberge-Weiss phase transition","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2110.10029","snapshot_observed_at":"2026-08-15T21:29:14.120028Z","title":"Cardinali, M","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":29,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.120028Z"},"links":{"cited_paper":"/paper/2110.10029","citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:54346cc8bdaa25ea4d3cb0ee9b7f10a376ad44d611361e6de3a28ad0cfef8934","observation_id":"a64e60d3-c299-42ca-b3ab-ab3a742607a8","resolution":{"observed_at":"2026-08-15T21:29:14.120028Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2604.07284","last_updated":"2026-04-08T16:45:19Z","snapshot_observed_at":"2026-08-16T10:38:36.193135Z","submitted_at":"2026-04-08T16:45:19Z","title":"The Roberge-Weiss transition as a probe for conformality in many-flavor QCD","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2604.07284","snapshot_observed_at":"2026-08-15T21:29:14.124552Z","title":"D’Elia, M","venue":null,"work_id":null,"year":2026},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.124552Z"},"links":{"cited_paper":"/paper/2604.07284","citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:1301a4fd8b19f5afc10c1f6d53528be75b1fd398655dd43237f56322700004d9","observation_id":"a9cb0394-a217-42ee-9729-35730a6c25f9","resolution":{"observed_at":"2026-08-15T21:29:14.124552Z","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":"2026-08-15T21:29:14.128665Z","title":"Weisz, Continuum Limit Improved Lattice Action for Pure Yang-Mills Theory","venue":null,"work_id":null,"year":1983},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.128665Z"},"links":{"citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:08852fa95b3910e3ac6a18d1a3478b043177ccf981f2c979b84a93c5768eda17","observation_id":"db7f78b5-8834-4303-9f37-ffb51d3b976a","resolution":{"observed_at":"2026-08-15T21:29:14.128665Z","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":"2026-08-15T21:29:14.132878Z","title":"Curci, P","venue":null,"work_id":null,"year":1983},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":32,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.132878Z"},"links":{"citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:9c1b986cb8a33b29b332231d8ba256df0fe0eeb78fafbb64b4d8483ee03e167d","observation_id":"1b6721bb-6430-4aac-a12f-16dda9690ddb","resolution":{"observed_at":"2026-08-15T21:29:14.132878Z","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":"2026-08-15T21:29:14.136629Z","title":null,"venue":null,"work_id":null,"year":1975},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.136629Z"},"links":{"citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:ab06c8543745bbc1e5d1d8853cffe02f3a97a656f63fe3b86c90293705cdb37a","observation_id":"88bf5c98-ac1e-40b3-afda-11512717ddac","resolution":{"observed_at":"2026-08-15T21:29:14.136629Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-lat/0311018","last_updated":"2003-11-11T17:47:49Z","snapshot_observed_at":"2026-07-07T03:42:05.598734Z","submitted_at":"2003-11-11T17:47:49Z","title":"Analytic Smearing of SU(3) Link Variables in Lattice QCD","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-lat/0311018","snapshot_observed_at":"2026-08-15T21:29:14.140556Z","title":"Morningstar and M","venue":null,"work_id":null,"year":2004},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":34,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.140556Z"},"links":{"cited_paper":"/paper/hep-lat/0311018","citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:212e704a056634dfe44f038b4bdd59a786d47c7248ae829f1c31a1f1cc844f26","observation_id":"b86060d5-8c8e-4ab6-938d-fb826668a2b4","resolution":{"observed_at":"2026-08-15T21:29:14.140556Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2002.12347","last_updated":"2021-04-22T22:09:34Z","snapshot_observed_at":"2026-08-16T23:10:53.954259Z","submitted_at":"2020-02-27T18:59:53Z","title":"Leading hadronic contribution to the muon magnetic moment from lattice QCD","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2002.12347","snapshot_observed_at":"2026-08-15T21:29:14.144934Z","title":"Borsanyiet al., Leading hadronic contribution to the muon magnetic moment from lattice QCD, Nature593, 51 (2021), arXiv:2002.12347 [hep-lat]","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.144934Z"},"links":{"cited_paper":"/paper/2002.12347","citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:05d89587c59501fd7d499a84ebcb8d79ce4fc0d755fe22e79117e547ab6531c3","observation_id":"bc426741-f5d3-415a-a77d-8f5f21f9db7a","resolution":{"observed_at":"2026-08-15T21:29:14.144934Z","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":"2026-08-15T21:29:14.149515Z","title":"Berg, Dislocations and topological background in the lattice O(3)σ-model, Physics Letters B104, 475 (1981)","venue":null,"work_id":null,"year":1981},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":36,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.149515Z"},"links":{"citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:856e04b6f48b6ad34c723a3ce7c9d0b2aa175adc363415b4992afcd1f579ec20","observation_id":"dca94d64-5d42-417e-b704-76628729910d","resolution":{"observed_at":"2026-08-15T21:29:14.149515Z","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":"2026-08-15T21:29:14.153630Z","title":"Iwasaki and T","venue":null,"work_id":null,"year":1983},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":37,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.153630Z"},"links":{"citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:4ed836ec31816e17ad656c81490fe318fd1f8a78bdd90efe6dad1d4ae9d1119f","observation_id":"0f9748e8-3098-4f9b-90b2-d39b6e41c1ed","resolution":{"observed_at":"2026-08-15T21:29:14.153630Z","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":"2026-08-15T21:29:14.157913Z","title":null,"venue":null,"work_id":null,"year":1984},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":38,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.157913Z"},"links":{"citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:46e9a4f39ca25bbec1ed2f6d6a0feb67581d5a848e9c04845810b5fb2bf05d7b","observation_id":"ef8ba1d7-19e1-4123-ad06-e3013dfa60ba","resolution":{"observed_at":"2026-08-15T21:29:14.157913Z","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":"2026-08-15T21:29:14.162171Z","title":"Teper, Instantons in the Quantized SU(2) Vacuum: A Lattice Monte Carlo Investigation, Phys","venue":null,"work_id":null,"year":1985},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":39,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.162171Z"},"links":{"citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:77abc1c7c52acf06a26a4f63f37aa34e4d251cfe3b8aed8fc21644e6c4d4a2bb","observation_id":"ba9a6ad0-d881-422f-8068-d9a8c8ffe0c5","resolution":{"observed_at":"2026-08-15T21:29:14.162171Z","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":"2026-08-15T21:29:14.166206Z","title":"Ilgenfritz, M","venue":null,"work_id":null,"year":1986},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":40,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.166206Z"},"links":{"citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:b06b90e1925108cc2478060614263325b2deff871a6c39619fee1fb0c4470bc7","observation_id":"f6ecd019-b72a-4ecc-a27b-63c535e389c9","resolution":{"observed_at":"2026-08-15T21:29:14.166206Z","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":"2026-08-15T21:29:14.170673Z","title":"Campostrini, A","venue":null,"work_id":null,"year":1990},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":41,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.170673Z"},"links":{"citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:3879e5b050191d3cfa369cabac1dcf8953cd06d28c63d474b6fa16ddefafca2a","observation_id":"2aea0fc6-eee5-4f43-ac41-1b6aad09ab43","resolution":{"observed_at":"2026-08-15T21:29:14.170673Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-lat/0001027","last_updated":"2000-01-24T10:05:21Z","snapshot_observed_at":"2026-07-07T03:40:06.478084Z","submitted_at":"2000-01-24T10:05:21Z","title":"Topology in 2D CP**(N-1) models on the lattice: a critical comparison of different cooling techniques","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-lat/0001027","snapshot_observed_at":"2026-08-15T21:29:14.175119Z","title":"Alles, L","venue":null,"work_id":null,"year":2000},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":42,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.175119Z"},"links":{"cited_paper":"/paper/hep-lat/0001027","citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:dcb6b31a73b96856a726d2a066db18239f750892552c6790b71f62e5ce22f13d","observation_id":"3479fbfd-7b18-4315-9d79-bb2c4835a358","resolution":{"observed_at":"2026-08-15T21:29:14.175119Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1401.2441","last_updated":"2014-05-13T07:51:54Z","snapshot_observed_at":"2026-08-15T19:04:06.314278Z","submitted_at":"2014-01-10T20:11:07Z","title":"Comparison of the gradient flow with cooling in $SU(3)$ pure gauge theory","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1401.2441","snapshot_observed_at":"2026-08-15T21:29:14.181226Z","title":"Bonati and M","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":43,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.181226Z"},"links":{"cited_paper":"/paper/1401.2441","citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:f3ba146e83eac158ad6c45315ddbe0f2cd5ad5fcc2cf0027ab20a0a301c9c712","observation_id":"54d3e53f-7b00-49a4-a392-7732d90cfb1a","resolution":{"observed_at":"2026-08-15T21:29:14.181226Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1708.00696","last_updated":"2020-04-28T15:31:53Z","snapshot_observed_at":"2026-08-16T10:37:50.908110Z","submitted_at":"2017-08-02T10:48:27Z","title":"Comparison of topological charge definitions in Lattice QCD","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1708.00696","snapshot_observed_at":"2026-08-15T21:29:14.186137Z","title":"Alexandrou, A","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":44,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.186137Z"},"links":{"cited_paper":"/paper/1708.00696","citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:9bbe6870d35a74dd74fb74080f1934eb12ee91d3f720df299895a18d01bbbe78","observation_id":"06e1b9ac-e7a9-452a-aec1-7bf7f8ca3cb4","resolution":{"observed_at":"2026-08-15T21:29:14.186137Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1509.04259","last_updated":"2015-09-14T19:53:20Z","snapshot_observed_at":"2026-08-16T09:21:34.864329Z","submitted_at":"2015-09-14T19:53:20Z","title":"Topological charge using cooling and the gradient flow","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1509.04259","snapshot_observed_at":"2026-08-15T21:29:14.190990Z","title":"Alexandrou, A","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":45,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.190990Z"},"links":{"cited_paper":"/paper/1509.04259","citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:07cd706a07c4eab28a07a9eb11d23bd1deb55d9681e3e4f1776242e7e1cf4c37","observation_id":"a0939aa4-52dc-4e46-a2bc-c50f348c299a","resolution":{"observed_at":"2026-08-15T21:29:14.190990Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/0204125","last_updated":"2002-08-12T16:45:10Z","snapshot_observed_at":"2026-08-11T19:59:36.904915Z","submitted_at":"2002-04-16T13:30:34Z","title":"Theta dependence of SU(N) gauge theories","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/0204125","snapshot_observed_at":"2026-08-15T21:29:14.195709Z","title":"Del Debbio, H","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":46,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.195709Z"},"links":{"cited_paper":"/paper/hep-th/0204125","citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:301ec72127efab3d7652e86898164e5bbb3ce1c268072a709501c00e5b737925","observation_id":"6bedb1b8-afe7-44b7-bedc-badbf032e8aa","resolution":{"observed_at":"2026-08-15T21:29:14.195709Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1512.01544","last_updated":"2016-01-27T18:32:04Z","snapshot_observed_at":"2026-08-16T09:21:37.529322Z","submitted_at":"2015-12-04T20:58:19Z","title":"$\\theta$ dependence in $SU(3)$ Yang-Mills theory from analytic continuation","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1512.01544","snapshot_observed_at":"2026-08-15T21:29:14.200539Z","title":"Bonati, M","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":47,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.200539Z"},"links":{"cited_paper":"/paper/1512.01544","citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:e0b0d7d174a4160c47d14cbca7f1548035768ba6629cd61972b085abc3a91834","observation_id":"fa0fbeb0-5bcf-4a34-8be6-efcd9ae166fe","resolution":{"observed_at":"2026-08-15T21:29:14.200539Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2402.03096","last_updated":"2024-05-10T13:00:34Z","snapshot_observed_at":"2026-08-16T14:21:23.507215Z","submitted_at":"2024-02-05T15:27:10Z","title":"The $\\theta$-dependence of the Yang-Mills spectrum from analytic continuation","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2402.03096","snapshot_observed_at":"2026-08-15T21:29:14.204999Z","title":"Bonanno, C","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":48,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.204999Z"},"links":{"cited_paper":"/paper/2402.03096","citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:118da46a422ea52231636fd053a93e4329c20e956ed837cb0d5f36feffd201c8","observation_id":"476c92f2-6b98-49d3-9e02-40f0e27e415b","resolution":{"observed_at":"2026-08-15T21:29:14.204999Z","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":"2026-08-15T21:29:14.209745Z","title":null,"venue":null,"work_id":null,"year":1999},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":49,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.209745Z"},"links":{"citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:927fe3ce013599e386f2cd4c176313417a8906dac66214fc76096d17913f9730","observation_id":"fe79588a-8985-49ee-8279-fc4f806f1760","resolution":{"observed_at":"2026-08-15T21:29:14.209745Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-lat/9908006","last_updated":"1999-08-05T17:36:18Z","snapshot_observed_at":"2026-08-16T09:22:19.213940Z","submitted_at":"1999-08-05T17:36:18Z","title":"Finite density (might well be easier) at finite temperature","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-lat/9908006","snapshot_observed_at":"2026-08-15T21:29:14.213808Z","title":"Lombardo, Finite density (might well be easier) at finite temperature, Nucl","venue":null,"work_id":null,"year":2000},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":50,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.213808Z"},"links":{"cited_paper":"/paper/hep-lat/9908006","citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:2e3c6065a5f9ae18841c2ee6e8b112d1603d5e9daffbb153bcb589ad35c88464","observation_id":"3ca6c269-c9d5-4979-a80e-be6bd16cdb27","resolution":{"observed_at":"2026-08-15T21:29:14.213808Z","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":"2026-08-15T21:29:14.218521Z","title":"de Forcrand and O","venue":null,"work_id":null,"year":2002},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":51,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.218521Z"},"links":{"citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:ccb5025b10c0c44b9e8839898f20d9ae44dc31ca729d994d88f0800af8823d16","observation_id":"1fc278c5-5b4c-4283-a035-f3a1d7ed665e","resolution":{"observed_at":"2026-08-15T21:29:14.218521Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-lat/0209146","last_updated":"2002-10-01T15:26:56Z","snapshot_observed_at":"2026-08-11T14:19:35.799558Z","submitted_at":"2002-09-21T17:42:13Z","title":"Finite density QCD via imaginary chemical potential","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-lat/0209146","snapshot_observed_at":"2026-08-15T21:29:14.222280Z","title":"D’Elia and M.-P","venue":null,"work_id":null,"year":2003},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":52,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.222280Z"},"links":{"cited_paper":"/paper/hep-lat/0209146","citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:22893e75bac16bc663ffe68f19eb7bdcb25a52135081794c8b11ac5114d6e7c2","observation_id":"4bea4f23-8310-43b8-b0d9-91506e7afcaf","resolution":{"observed_at":"2026-08-15T21:29:14.222280Z","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":"2026-08-15T21:29:14.226395Z","title":"de Forcrand and O","venue":null,"work_id":null,"year":2003},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":53,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.226395Z"},"links":{"citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:b39f979560eb4ca8c608143987eeb9a0a829ef5fd93b950e31e0e67ba28121f9","observation_id":"84a85358-a03c-4d01-967f-8e6e2440b005","resolution":{"observed_at":"2026-08-15T21:29:14.226395Z","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":"2026-08-15T21:29:14.230315Z","title":"D’Elia and M","venue":null,"work_id":null,"year":2004},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":54,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.230315Z"},"links":{"citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:09b3ad4903e153e756bfc7d12974a930330b2816acb82f6a42edc46061f8c7ca","observation_id":"072aa40a-522a-42d0-a3d5-d141a2960a2a","resolution":{"observed_at":"2026-08-15T21:29:14.230315Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-lat/0401024","last_updated":"2004-09-07T17:45:20Z","snapshot_observed_at":"2026-07-07T03:42:10.488918Z","submitted_at":"2004-01-16T13:57:19Z","title":"Real and imaginary chemical potential in 2-color QCD","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-lat/0401024","snapshot_observed_at":"2026-08-15T21:29:14.235313Z","title":"Giudice and A","venue":null,"work_id":null,"year":2004},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":55,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.235313Z"},"links":{"cited_paper":"/paper/hep-lat/0401024","citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:111f599e456a29846be1c65c9c9f50afc9b8d05f38fed08caf8f75e72b574918","observation_id":"050f8e8e-5644-4e03-b7e0-88839c173a0b","resolution":{"observed_at":"2026-08-15T21:29:14.235313Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-lat/0411023","last_updated":"2005-08-16T03:30:46Z","snapshot_observed_at":"2026-08-16T09:23:16.672794Z","submitted_at":"2004-11-17T16:25:29Z","title":"Phase diagram of QCD at finite temperature and chemical potential from lattice simulations with dynamical Wilson quarks","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-lat/0411023","snapshot_observed_at":"2026-08-15T21:29:14.240238Z","title":"Chen and X.-Q","venue":null,"work_id":null,"year":2005},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":56,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.240238Z"},"links":{"cited_paper":"/paper/hep-lat/0411023","citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:5e027751c2d70508c03b7254a288ce50c710a9d9ba1a6c8c0b76e12ac707da6f","observation_id":"9c0e1563-9ad1-4d59-93ac-468bbd361ee9","resolution":{"observed_at":"2026-08-15T21:29:14.240238Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-lat/0503010","last_updated":"2005-07-19T06:38:18Z","snapshot_observed_at":"2026-08-16T09:23:07.731543Z","submitted_at":"2005-03-10T20:09:18Z","title":"Phase diagram of QCD with four quark flavors at finite temperature and baryon density","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-lat/0503010","snapshot_observed_at":"2026-08-15T21:29:14.244458Z","title":"Azcoiti, G","venue":null,"work_id":null,"year":2005},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":57,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.244458Z"},"links":{"cited_paper":"/paper/hep-lat/0503010","citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:5635bc9aeb09018aad5c2ba62a93c352c69a1e48f4f5fa6e3441fc2f23edc9fe","observation_id":"21096a06-4cf3-4507-8722-fe1a7ac23f4c","resolution":{"observed_at":"2026-08-15T21:29:14.244458Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0705.3814","last_updated":"2007-06-07T17:23:33Z","snapshot_observed_at":"2026-08-15T10:40:03.491832Z","submitted_at":"2007-05-25T17:36:26Z","title":"The strongly interacting Quark Gluon Plasma, and the critical behaviour of QCD at imaginary chemical potential","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0705.3814","snapshot_observed_at":"2026-08-15T21:29:14.248417Z","title":"D’Elia, F","venue":null,"work_id":null,"year":2007},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":58,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.248417Z"},"links":{"cited_paper":"/paper/0705.3814","citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:98e05814fb884a300129448c67cf6eff723f20d7ac733dd02fb30df2dd66457d","observation_id":"33ee823b-4954-4a5d-83dd-a73c270c772a","resolution":{"observed_at":"2026-08-15T21:29:14.248417Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0909.0254","last_updated":"2010-01-28T10:40:06Z","snapshot_observed_at":"2026-08-15T05:40:06.611041Z","submitted_at":"2009-09-01T19:53:43Z","title":"The order of the Roberge-Weiss endpoint (finite size transition) in QCD","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0909.0254","snapshot_observed_at":"2026-08-15T21:29:14.252370Z","title":"D’Elia and F","venue":null,"work_id":null,"year":2009},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":59,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.252370Z"},"links":{"cited_paper":"/paper/0909.0254","citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:56c7f59e865347eaaec74a046c44a7189c4bdd1a4cfdf75d593b90dd782b501b","observation_id":"20911e66-3e33-4708-a358-c5c5ff8b9f5c","resolution":{"observed_at":"2026-08-15T21:29:14.252370Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0905.1292","last_updated":"2009-10-12T12:26:24Z","snapshot_observed_at":"2026-08-15T05:48:51.636679Z","submitted_at":"2009-05-08T17:08:12Z","title":"Analytic continuation of the critical line: suggestions for QCD","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0905.1292","snapshot_observed_at":"2026-08-15T21:29:14.257001Z","title":null,"venue":null,"work_id":null,"year":2009},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":60,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.257001Z"},"links":{"cited_paper":"/paper/0905.1292","citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:50efe99fa0c9001929f4a41791a6ff096176bf61d583c95f6894969e5d5b8acf","observation_id":"fcc99b7d-bf36-4939-93ff-8cf8295ea147","resolution":{"observed_at":"2026-08-15T21:29:14.257001Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1004.3144","last_updated":"2010-04-19T10:01:48Z","snapshot_observed_at":"2026-08-16T19:22:08.218495Z","submitted_at":"2010-04-19T10:01:48Z","title":"Constraining the QCD phase diagram by tricritical lines at imaginary chemical potential","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1004.3144","snapshot_observed_at":"2026-08-15T21:29:14.261232Z","title":"de Forcrand and O","venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":61,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.261232Z"},"links":{"cited_paper":"/paper/1004.3144","citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:e8fb518ba01b5d67102d616a80634222d872603133e5312897a57a1f3e8aa1e8","observation_id":"3f2e48ea-4abd-45e6-bf7a-7b757674c554","resolution":{"observed_at":"2026-08-15T21:29:14.261232Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1011.4515","last_updated":"2011-07-08T18:00:58Z","snapshot_observed_at":"2026-08-15T05:02:27.947785Z","submitted_at":"2010-11-19T20:58:04Z","title":"The Roberge-Weiss endpoint in N_f = 2 QCD","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1011.4515","snapshot_observed_at":"2026-08-15T21:29:14.265645Z","title":"Bonati, G","venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":62,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.265645Z"},"links":{"cited_paper":"/paper/1011.4515","citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:9714f394c3b74a08507a67dc2740d48f5a37dc556a24f672afe7b4b75d24eb12","observation_id":"a80b0a13-5073-4825-ac44-db99714c5dd7","resolution":{"observed_at":"2026-08-15T21:29:14.265645Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1202.5700","last_updated":"2012-02-25T21:57:26Z","snapshot_observed_at":"2026-08-17T14:03:08.167633Z","submitted_at":"2012-02-25T21:57:26Z","title":"The critical line of two-flavor QCD at finite isospin or baryon densities from imaginary chemical potentials","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1202.5700","snapshot_observed_at":"2026-08-15T21:29:14.270258Z","title":null,"venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":63,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.270258Z"},"links":{"cited_paper":"/paper/1202.5700","citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:b262c07fb2d0e097a039baa6466c23cf02795ec9405a1595628baad77d906dfc","observation_id":"76fb9143-ff8c-4ad7-a8cb-efef9310150c","resolution":{"observed_at":"2026-08-15T21:29:14.270258Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1303.0336","last_updated":"2013-05-27T03:00:08Z","snapshot_observed_at":"2026-08-15T00:26:52.099439Z","submitted_at":"2013-03-02T02:51:30Z","title":"Nature of the Roberge-Weiss transition end points in two-flavor lattice QCD with Wilson quarks","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1303.0336","snapshot_observed_at":"2026-08-15T21:29:14.274523Z","title":"Wu and X.-F","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":64,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.274523Z"},"links":{"cited_paper":"/paper/1303.0336","citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:110ffa0269c79387ba40fa691093786a9e292b8889978528de2cbb7a7a9e5bb6","observation_id":"47fb8914-e5f3-4b05-9b3f-1954337be065","resolution":{"observed_at":"2026-08-15T21:29:14.274523Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1402.0838","last_updated":"2014-02-04T19:23:55Z","snapshot_observed_at":"2026-08-14T23:45:50.755837Z","submitted_at":"2014-02-04T19:23:55Z","title":"The nature of the Roberge-Weiss transition in $N_f=2$ QCD with Wilson fermions","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1402.0838","snapshot_observed_at":"2026-08-15T21:29:14.278860Z","title":"Philipsen and C","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":65,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.278860Z"},"links":{"cited_paper":"/paper/1402.0838","citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:7f04dc9649f23092a0040d23b410c22d6686a3ed262a91b7d2eb8393291df438","observation_id":"af3cc908-1649-4a27-8386-22d079d58329","resolution":{"observed_at":"2026-08-15T21:29:14.278860Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1408.5086","last_updated":"2014-10-29T11:28:14Z","snapshot_observed_at":"2026-08-14T23:22:20.712924Z","submitted_at":"2014-08-21T17:56:36Z","title":"The chiral phase transition in two-flavor QCD from imaginary chemical potential","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1408.5086","snapshot_observed_at":"2026-08-15T21:29:14.284373Z","title":"Bonati, P","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":66,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.284373Z"},"links":{"cited_paper":"/paper/1408.5086","citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:837d94569b9e7f3da7a03c67021b82c2d2a3998817ca89fecc3e627437bdb37c","observation_id":"78b95b3c-2c7d-4351-8155-81c0db8b1686","resolution":{"observed_at":"2026-08-15T21:29:14.284373Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1405.2425","last_updated":"2014-10-26T02:20:37Z","snapshot_observed_at":"2026-08-14T23:34:33.660566Z","submitted_at":"2014-05-10T11:52:53Z","title":"Nature of Roberge-Weiss transition end points for heavy quarks in $N_f=2$ lattice QCD with Wilson fermions","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1405.2425","snapshot_observed_at":"2026-08-15T21:29:14.289193Z","title":"Wu and X.-F","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":67,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.289193Z"},"links":{"cited_paper":"/paper/1405.2425","citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:af87f33f9c3add7bfef252e441ee19b59e474e7a396e8bceca2ae9509344033c","observation_id":"36cf5211-8e24-4db3-b12d-07f3da05efce","resolution":{"observed_at":"2026-08-15T21:29:14.289193Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1512.07180","last_updated":"2016-04-26T09:30:18Z","snapshot_observed_at":"2026-08-16T09:21:16.251403Z","submitted_at":"2015-12-22T18:01:15Z","title":"Roberge-Weiss transition in $N_\\text{f}=2$ QCD with Wilson fermions and $N_\\tau=6$","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1512.07180","snapshot_observed_at":"2026-08-15T21:29:14.293981Z","title":"Czaban, F","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":68,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.293981Z"},"links":{"cited_paper":"/paper/1512.07180","citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:630d3ea5ede4af1118b0bad1faf018016bc638677de76442595b47ac631030ad","observation_id":"0cc4d4df-0eb9-4702-a6ef-0fb1ce91733b","resolution":{"observed_at":"2026-08-15T21:29:14.293981Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1909.12253","last_updated":"2020-01-22T16:34:07Z","snapshot_observed_at":"2026-08-16T09:22:12.023193Z","submitted_at":"2019-09-26T16:58:44Z","title":"Finite size and cut-off effects on the Roberge-Weiss transition in $N_\\text{f}=2$ QCD with Staggered fermions","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1909.12253","snapshot_observed_at":"2026-08-15T21:29:14.297957Z","title":"Philipsen and A","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":69,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.297957Z"},"links":{"cited_paper":"/paper/1909.12253","citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:744a577f479139831d3aa3a48674a09ef93c2b12f06f3508b74ddb0bc40a3992","observation_id":"a3273dca-22a5-425d-a01e-8f8a07739a86","resolution":{"observed_at":"2026-08-15T21:29:14.297957Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2207.10117","last_updated":"2022-07-20T18:01:48Z","snapshot_observed_at":"2026-08-16T16:44:28.550371Z","submitted_at":"2022-07-20T18:01:48Z","title":"The light Roberge-Weiss tricritical endpoint at imaginary isospin and baryon chemical potential","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2207.10117","snapshot_observed_at":"2026-08-15T21:29:14.302124Z","title":null,"venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":70,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.302124Z"},"links":{"cited_paper":"/paper/2207.10117","citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:0fb63579c173f643ccf7e07f5ac8ed8d87dd7eb7af3837f5c85aff51401408e3","observation_id":"a4be71fb-5f0f-4a3d-b723-72eca11e923c","resolution":{"observed_at":"2026-08-15T21:29:14.302124Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2207.10586","last_updated":"2022-07-21T16:28:31Z","snapshot_observed_at":"2026-08-16T16:44:15.666469Z","submitted_at":"2022-07-21T16:28:31Z","title":"The light Roberge-Weiss tricritical endpoint at imaginary isospin chemical potential","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2207.10586","snapshot_observed_at":"2026-08-15T21:29:14.311151Z","title":null,"venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":71,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.311151Z"},"links":{"cited_paper":"/paper/2207.10586","citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:0b430624a6ebad7e93e3b03ce8e21ce5dc2cd2170b5850e1cf0c3352e0dc0472","observation_id":"56a331ae-a821-4f82-9f90-79a9580f9697","resolution":{"observed_at":"2026-08-15T21:29:14.311151Z","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":"2603.22046","doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-15T21:29:15.428478Z","title":"Endrodi, G","venue":null,"work_id":"effbf2a4-db67-4816-af67-5fbb4834f3e5","year":2026},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":72,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.314972Z"},"links":{"citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:0306bbdc92a6bb7ba6871953230b56e2082e1a019f1748a6ff2c852a6d2fe244","observation_id":"e4be7613-254c-4e6b-9be8-0482e1e0dfa0","resolution":{"observed_at":"2026-08-15T21:29:15.436258Z","resolver_source":"raw_fallback","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2501.00792","last_updated":"2025-01-10T09:28:37Z","snapshot_observed_at":"2026-08-16T07:02:20.311535Z","submitted_at":"2025-01-01T10:03:53Z","title":"First-order phase transition in dynamical 3-flavor QCD at imaginary isospin","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2501.00792","snapshot_observed_at":"2026-08-15T21:29:14.318974Z","title":"Endr˝ odi, G","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":73,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.318974Z"},"links":{"cited_paper":"/paper/2501.00792","citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:641f182731650098ea8e8e3abc039650200798265cd76c29b715e2c430f41801","observation_id":"a850e157-c184-4bc3-aaba-6768829c4f61","resolution":{"observed_at":"2026-08-15T21:29:14.318974Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2502.19294","last_updated":"2025-02-26T16:52:25Z","snapshot_observed_at":"2026-08-16T12:54:56.751989Z","submitted_at":"2025-02-26T16:52:25Z","title":"The Roberge-Weiss transition for QCD in a magnetic background","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2502.19294","snapshot_observed_at":"2026-08-15T21:29:14.323347Z","title":"D’Elia, L","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":74,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.323347Z"},"links":{"cited_paper":"/paper/2502.19294","citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:ffa7d9ab7daca2d98f0d9a89efd5e54e6d9547048a3e6e4cc557f1323facde14","observation_id":"91fe5297-deef-4b0b-8bd3-107d683d0956","resolution":{"observed_at":"2026-08-15T21:29:14.323347Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2412.06326","last_updated":"2024-12-09T09:24:16Z","snapshot_observed_at":"2026-08-16T09:20:34.066877Z","submitted_at":"2024-12-09T09:24:16Z","title":"The Roberge-Weiss endpoint in $(2+1)$-flavor QCD with background magnetic fields","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2412.06326","snapshot_observed_at":"2026-08-15T21:29:14.327343Z","title":"Zambello, M","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":75,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.327343Z"},"links":{"cited_paper":"/paper/2412.06326","citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:c6f2cd2be8197d93d57502961dcff9a91327f5fac835de08b4a515e38cdb8af9","observation_id":"865d6b47-ad47-40d4-a730-b94c4cff9243","resolution":{"observed_at":"2026-08-15T21:29:14.327343Z","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":"2026-08-15T21:29:14.331349Z","title":null,"venue":null,"work_id":null,"year":1995},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":76,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.331349Z"},"links":{"citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:5bd8a9af54cff880a9e9ce53b523482ae3c85eddbf7ac964e847487907ec85c7","observation_id":"a2e020b1-b056-4640-8e96-d45b0aabbf38","resolution":{"observed_at":"2026-08-15T21:29:14.331349Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-lat/9809092","last_updated":"1998-09-14T18:11:49Z","snapshot_observed_at":"2026-08-14T03:29:29.906371Z","submitted_at":"1998-09-14T18:11:49Z","title":"A New Exact Method for Dynamical Fermion Computations with Non-Local Actions","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-lat/9809092","snapshot_observed_at":"2026-08-15T21:29:14.335657Z","title":null,"venue":null,"work_id":null,"year":1999},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":77,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.335657Z"},"links":{"cited_paper":"/paper/hep-lat/9809092","citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:37122e796011b0d9235e96a61644a2d86293a2c947bb3bf488c2a8007ddd832a","observation_id":"902e2be2-a85d-4af4-b25f-50e2926f8ce7","resolution":{"observed_at":"2026-08-15T21:29:14.335657Z","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":"2026-08-15T21:29:14.339924Z","title":null,"venue":null,"work_id":null,"year":2007},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":78,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.339924Z"},"links":{"citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:604b55ae653303cf9061bb5251a6e5b91d5a5e0c7c69156eb93cbf1aea6142b1","observation_id":"ffba6dbc-ac95-45b3-97f0-2d1e6be6e91c","resolution":{"observed_at":"2026-08-15T21:29:14.339924Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1701.00426","last_updated":"2017-01-02T15:42:40Z","snapshot_observed_at":"2026-08-16T09:22:14.076258Z","submitted_at":"2017-01-02T15:42:40Z","title":"Design and optimization of a portable LQCD Monte Carlo code using OpenACC","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1701.00426","snapshot_observed_at":"2026-08-15T21:29:14.344182Z","title":"Bonati, E","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":79,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.344182Z"},"links":{"cited_paper":"/paper/1701.00426","citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:f7971a46b642cfc566fb03fb832ccb6812f5e59f481b93c1188ca817624b82c3","observation_id":"4e5d033f-e399-49f9-b9e5-ad758e9adcd7","resolution":{"observed_at":"2026-08-15T21:29:14.344182Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1801.01473","last_updated":"2018-01-04T18:03:02Z","snapshot_observed_at":"2026-08-16T09:21:53.971180Z","submitted_at":"2018-01-04T18:03:02Z","title":"Portable multi-node LQCD Monte Carlo simulations using OpenACC","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1801.01473","snapshot_observed_at":"2026-08-15T21:29:14.348406Z","title":"Bonati, E","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":80,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.348406Z"},"links":{"cited_paper":"/paper/1801.01473","citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:b7be36e90f2bd10c7eca91ed871d51a2fd979a3937146cd21f172dc06ab31566","observation_id":"6e4bf5ba-47a9-406d-bfd5-4f709a2a97d2","resolution":{"observed_at":"2026-08-15T21:29:14.348406Z","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":"2026-08-15T21:29:14.352431Z","title":"DeGrand and R","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":81,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.352431Z"},"links":{"citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:0c164468cb325888cefeb86fb83f1cf80f7c30e9a3b0da8d8c58bb2e4b129fad","observation_id":"fb5a63c1-f8d7-40f1-96ca-2a007ec967af","resolution":{"observed_at":"2026-08-15T21:29:14.352431Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0711.4290","last_updated":"2007-11-27T15:58:33Z","snapshot_observed_at":"2026-08-15T10:26:54.406888Z","submitted_at":"2007-11-27T15:58:33Z","title":"More about QCD on compact spaces","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0711.4290","snapshot_observed_at":"2026-08-15T21:29:14.356370Z","title":"DeGrand, R","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":82,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.356370Z"},"links":{"cited_paper":"/paper/0711.4290","citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:7c48dea95e3165afc108bf1c7e63ac26bc0d128f3014322bfc3e88dc0987a6f2","observation_id":"e2160437-3c39-4156-a0cf-d697c260bf3c","resolution":{"observed_at":"2026-08-15T21:29:14.356370Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/0702167","last_updated":"2007-05-21T16:08:37Z","snapshot_observed_at":"2026-08-15T18:50:05.577054Z","submitted_at":"2007-02-20T20:30:11Z","title":"Baryon currents in QCD with compact dimensions","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/0702167","snapshot_observed_at":"2026-08-15T21:29:14.360615Z","title":"Lucini, A","venue":null,"work_id":null,"year":2007},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":83,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.360615Z"},"links":{"cited_paper":"/paper/hep-th/0702167","citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:ea4cd4c8ed05a235f74206ce9acbac562ecad92cf9b52006ecaa15ad295bf265","observation_id":"bd79adbb-376a-4e3e-8db4-be7ab4be3710","resolution":{"observed_at":"2026-08-15T21:29:14.360615Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0904.3479","last_updated":"2009-04-22T15:36:31Z","snapshot_observed_at":"2026-08-15T05:50:01.111895Z","submitted_at":"2009-04-22T15:36:31Z","title":"Discrete symmetry breaking and baryon currents in U(N) and SU(N) gauge theories","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0904.3479","snapshot_observed_at":"2026-08-15T21:29:14.365034Z","title":"Lucini and A","venue":null,"work_id":null,"year":2009},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":84,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.365034Z"},"links":{"cited_paper":"/paper/0904.3479","citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:4b61577fb06f3107e293cf40355c1c4a58f165fae460fd9698ece232e4d0daf2","observation_id":"009e2ce2-90d3-4de8-b2c4-a7fb46b131af","resolution":{"observed_at":"2026-08-15T21:29:14.365034Z","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":"2026-08-15T21:29:14.369804Z","title":"Dong and K.-F","venue":null,"work_id":null,"year":1994},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":85,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.369804Z"},"links":{"citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:d7e91d81e1af77eb7a6e2c1ba6c036752ffe378f11e4cf8a7bdf3991b16947f2","observation_id":"9e6d1980-bdc3-4557-930f-88f4eb26aa24","resolution":{"observed_at":"2026-08-15T21:29:14.369804Z","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":"2026-08-15T21:29:14.374445Z","title":"Vafa and E","venue":null,"work_id":null,"year":1984},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":86,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.374445Z"},"links":{"citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:fb315a4e12c7c3e5d290572c24f35b7061abcf1272a80211ad0a0d12f02a8c59","observation_id":"7a59a75a-7589-429e-9585-f9aeb20077f0","resolution":{"observed_at":"2026-08-15T21:29:14.374445Z","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":"2026-08-15T21:29:14.379319Z","title":"Di Vecchia and G","venue":null,"work_id":null,"year":1980},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":87,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.379319Z"},"links":{"citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:f684df1177ac680d5791673b28493d52d24ca3c2579261b6e6f812998d13d808","observation_id":"60dff094-0de0-45c5-a7e0-4d3465c38cb2","resolution":{"observed_at":"2026-08-15T21:29:14.379319Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1511.02867","last_updated":"2016-01-08T17:28:37Z","snapshot_observed_at":"2026-08-14T22:24:10.986419Z","submitted_at":"2015-11-09T21:00:03Z","title":"The QCD axion, precisely","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1511.02867","snapshot_observed_at":"2026-08-15T21:29:14.384327Z","title":"Grilli di Cortona, E","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":88,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.384327Z"},"links":{"cited_paper":"/paper/1511.02867","citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:5a5820b8cf36b6c85961b5fda43b890340f391d27b67dbf557740e5198dc5e2c","observation_id":"8dcb6fc3-e916-40a1-9453-9bf4dfc823be","resolution":{"observed_at":"2026-08-15T21:29:14.384327Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2001.03383","last_updated":"2020-03-11T23:47:17Z","snapshot_observed_at":"2026-08-16T09:21:19.785943Z","submitted_at":"2020-01-10T11:02:15Z","title":"The semi-classical approximation at high temperature revisited","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2001.03383","snapshot_observed_at":"2026-08-15T21:29:14.390253Z","title":"Boccaletti and D","venue":null,"work_id":null,"year":2001},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":89,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.390253Z"},"links":{"cited_paper":"/paper/2001.03383","citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:3f5cbd5e3617f6b48c1f633b37429d128635ed7181acd61f94036ef50f28a475","observation_id":"96ad9efb-ddda-4026-8f84-ed7d3a9a03aa","resolution":{"observed_at":"2026-08-15T21:29:14.390253Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1512.06746","last_updated":"2016-04-12T08:40:50Z","snapshot_observed_at":"2026-08-16T09:21:18.748946Z","submitted_at":"2015-12-21T18:29:47Z","title":"Axion phenomenology and $\\theta$-dependence from $N_f = 2+1$ lattice QCD","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1512.06746","snapshot_observed_at":"2026-08-15T21:29:14.395479Z","title":"Bonati, M","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":90,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.395479Z"},"links":{"cited_paper":"/paper/1512.06746","citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:b43af6d0bf2d64a44a90ea9a162bb8779dc1cf8a63768a44bc665bebb2d972a7","observation_id":"dc75ce8d-1733-42b6-aa10-e31fce8a9dea","resolution":{"observed_at":"2026-08-15T21:29:14.395479Z","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":"2026-08-15T21:29:14.399977Z","title":"Borsanyiet al., Calculation of the axion mass based on high-temperature lattice quantum chromodynamics, Nature539, 69 (2016), arXiv:1606.07494 [hep-lat]","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":91,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.399977Z"},"links":{"cited_paper":"/paper/1606.07494","citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:7e1f9044a3b51f161fc2729bd5155906699de110138ad229a8dd9ffd8ff6390f","observation_id":"2ed610af-dca5-478c-a9e8-e00414e7763a","resolution":{"observed_at":"2026-08-15T21:29:14.399977Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1709.06596","last_updated":"2017-09-19T18:25:37Z","snapshot_observed_at":"2026-08-16T09:22:12.196838Z","submitted_at":"2017-09-19T18:25:37Z","title":"Topological susceptibility from twisted mass fermions using spectral projectors and the gradient flow","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1709.06596","snapshot_observed_at":"2026-08-15T21:29:14.404559Z","title":"Alexandrou, A","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":92,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.404559Z"},"links":{"cited_paper":"/paper/1709.06596","citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:d2069eb3c26b76607f218c1fba8a66925f8a9179601956dc141ea2336b674f85","observation_id":"8bcb19dc-c6c9-4cb5-a04d-b14e9f90be1c","resolution":{"observed_at":"2026-08-15T21:29:14.404559Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2208.08921","last_updated":"2022-10-31T14:11:40Z","snapshot_observed_at":"2026-08-16T16:38:22.261443Z","submitted_at":"2022-08-18T15:44:34Z","title":"Topological susceptibility of $N_f=2+1$ QCD from staggered fermions spectral projectors at high temperatures","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2208.08921","snapshot_observed_at":"2026-08-15T21:29:14.409480Z","title":"Athenodorou, C","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":93,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.409480Z"},"links":{"cited_paper":"/paper/2208.08921","citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:7ca565e38de477013fe736fdddcc535c85514d43b83fe6e9c5f334a28d51ebb6","observation_id":"a19172ee-f915-451a-8890-584d06c29884","resolution":{"observed_at":"2026-08-15T21:29:14.409480Z","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":"lat/0004020","doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-15T21:29:14.882658Z","title":"Alles, M","venue":null,"work_id":"147d5b76-5f79-45e1-bb5d-531fe8ef76ab","year":2000},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":94,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.413711Z"},"links":{"citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:871913309d80d42f9cd04d1f91c14bf7a906ff56a23bc824e82707e344c62bae","observation_id":"d28bce57-a0aa-434c-b375-a507dbccb394","resolution":{"observed_at":"2026-08-15T21:29:14.890445Z","resolver_source":"raw_fallback","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1606.03145","last_updated":"2016-11-23T17:03:55Z","snapshot_observed_at":"2026-08-16T09:22:12.504059Z","submitted_at":"2016-06-09T23:50:14Z","title":"The topological susceptibility in finite temperature QCD and axion cosmology","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1606.03145","snapshot_observed_at":"2026-08-15T21:29:14.418112Z","title":"Petreczky, H.-P","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":95,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.418112Z"},"links":{"cited_paper":"/paper/1606.03145","citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:29c384e9bb0bac059d6f707390d5d7ce7581b18807a1be328d4eb4499a6d39e8","observation_id":"d539853b-a709-4c35-b931-04ce63e364c7","resolution":{"observed_at":"2026-08-15T21:29:14.418112Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1807.07954","last_updated":"2018-12-11T15:36:41Z","snapshot_observed_at":"2026-08-16T09:21:55.817846Z","submitted_at":"2018-07-20T17:56:10Z","title":"Topology in full QCD at high temperature: a multicanonical approach","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1807.07954","snapshot_observed_at":"2026-08-15T21:29:14.422580Z","title":"Bonati, M","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":96,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.422580Z"},"links":{"cited_paper":"/paper/1807.07954","citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:69936f5c7910e38b5c8511978cb2b98a38a53d20e624e57955ea9628db12aa87","observation_id":"d7dff398-0da4-4969-9fb7-52f0b0eb67f6","resolution":{"observed_at":"2026-08-15T21:29:14.422580Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1705.01847","last_updated":"2017-05-04T14:11:35Z","snapshot_observed_at":"2026-08-16T09:21:19.255466Z","submitted_at":"2017-05-04T14:11:35Z","title":"Topology (and axion's properties) from lattice QCD with a dynamical charm","version":1},"cited_work":{"arxiv_id":"1705.01847","doi":null,"metadata_source":"pith","pith_arxiv_id":"1705.01847","snapshot_observed_at":"2026-08-15T21:29:14.614790Z","title":"Topology (and axion's properties) from lattice QCD with a dynamical charm","venue":"hep-lat","work_id":"eafa135d-30c2-4909-a209-01d56365698e","year":2017},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":97,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.427080Z"},"links":{"cited_paper":"/paper/1705.01847","citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:c173182f801beacff44b9fe99a58afb186293aeed50bd27892776bbd95acc464","observation_id":"85540cdb-953b-4adb-837c-dc36649d058a","resolution":{"observed_at":"2026-08-15T21:29:14.621803Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2204.01556","last_updated":"2022-09-20T09:47:22Z","snapshot_observed_at":"2026-08-16T17:09:26.616616Z","submitted_at":"2022-04-04T15:04:40Z","title":"Topological susceptibility in finite temperature QCD with physical $(u/d, s, c)$ domain-wall quarks","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2204.01556","snapshot_observed_at":"2026-08-15T21:29:14.431450Z","title":"Chen, T.-W","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":98,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.431450Z"},"links":{"cited_paper":"/paper/2204.01556","citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:a22ea8e46d7a4d12f29c40f1316faa66bc371fb8335d81ad69172feac90a9a8c","observation_id":"fdd78d5c-fa74-446b-9caf-923f5a471789","resolution":{"observed_at":"2026-08-15T21:29:14.431450Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2502.15407","last_updated":"2025-07-21T14:35:16Z","snapshot_observed_at":"2026-08-16T12:56:22.080879Z","submitted_at":"2025-02-21T12:11:43Z","title":"Topological observables and $\\theta$ dependence in high temperature QCD from lattice simulations","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2502.15407","snapshot_observed_at":"2026-08-15T21:29:14.435687Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":99,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.435687Z"},"links":{"cited_paper":"/paper/2502.15407","citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:b84c175edff57d20878ff116d0a07edd697ffcff9f50ea5b58a012078d283fd1","observation_id":"015c1c79-0695-4061-a702-718b3dafeebc","resolution":{"observed_at":"2026-08-15T21:29:14.435687Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1301.7640","last_updated":"2013-06-20T06:58:48Z","snapshot_observed_at":"2026-08-15T00:30:24.242196Z","submitted_at":"2013-01-31T15:18:28Z","title":"Change of theta dependence in 4D SU(N) gauge theories across the deconfinement transition","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1301.7640","snapshot_observed_at":"2026-08-15T21:29:14.440227Z","title":"Bonati, M","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":100,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.440227Z"},"links":{"cited_paper":"/paper/1301.7640","citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:182d8dfffa90b6abb4afc376e00f303f6f46ed06605b2d8a6f3a548e9cad155c","observation_id":"c05423e2-12a1-45ba-8b6f-3ab7558d2ae5","resolution":{"observed_at":"2026-08-15T21:29:14.440227Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1607.06360","last_updated":"2016-10-24T08:30:00Z","snapshot_observed_at":"2026-08-14T21:47:23.638679Z","submitted_at":"2016-07-21T15:18:40Z","title":"$\\theta$ dependence of 4D $SU(N)$ gauge theories in the large-$N$ limit","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1607.06360","snapshot_observed_at":"2026-08-15T21:29:14.444513Z","title":"Bonati, M","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD","version":1},"reference_index":101,"source":"pdf_text","source_observed_at":"2026-08-15T21:29:14.444513Z"},"links":{"cited_paper":"/paper/1607.06360","citing_paper":"/paper/2608.12883"},"observation_digest":"sha256:13c9021441aab57e5316b4bcbdd7605c88342b79ed7237083f28a3a8190144ab","observation_id":"03c8f95f-7c4b-4dac-90e4-2e73ec452fb3","resolution":{"observed_at":"2026-08-15T21:29:14.444513Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"paper":{"arxiv_id":"2608.12883","last_updated":"2026-08-13T06:53:50Z","latest_version":1,"primary_category":"hep-lat","snapshot_observed_at":"2026-08-17T12:13:49.121609Z","submitted_at":"2026-08-13T06:53:50Z","title":"Topological properties around the Roberge-Weiss transition in $N_f = 2 + 1 + 1$ QCD"},"reference_resolution":{"displayed":100,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":95,"verified_exact":5,"verified_fuzzy":0},"total_outbound_references":103},"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":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"thesis":"As of 17 August 2026, this Paper Citation Record lists 100 of 103 outbound references and 1 inbound Pith citation observation for arXiv:2608.12883."}