{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2020:P3QJUU2KJ4ROIDLKRLWDNQMVAI","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"bbf62800ecc9f4130f686ce623dd56d448ff4fdcf2509ac8a9728ceb6e3d56b5","cross_cats_sorted":["hep-lat","nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2020-02-03T19:00:02Z","title_canon_sha256":"b90c1c4177d455889280ba3aa9cab2cbb6dd2694bb5880de99ea1c935e92174b"},"schema_version":"1.0","source":{"id":"2002.00968","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2002.00968","created_at":"2026-07-05T01:20:52Z"},{"alias_kind":"arxiv_version","alias_value":"2002.00968v1","created_at":"2026-07-05T01:20:52Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2002.00968","created_at":"2026-07-05T01:20:52Z"},{"alias_kind":"pith_short_12","alias_value":"P3QJUU2KJ4RO","created_at":"2026-07-05T01:20:52Z"},{"alias_kind":"pith_short_16","alias_value":"P3QJUU2KJ4ROIDLK","created_at":"2026-07-05T01:20:52Z"},{"alias_kind":"pith_short_8","alias_value":"P3QJUU2K","created_at":"2026-07-05T01:20:52Z"}],"graph_snapshots":[{"event_id":"sha256:c8bacfd348fa1fcf73ae3cdc1351c0ec698754fdcd6e18056920a4b09ef50ace","target":"graph","created_at":"2026-07-05T01:20:52Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2002.00968/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"At a nonzero temperature T, a constant field $\\overline{A}_0 \\sim T/g$ generates nontrivial eigenvalues of the thermal Wilson line. We discuss contributions to the free energy of such a holonomous plasma when the coupling constant, $g$, is weak. We review the computation to $\\sim g^2$ by several alternate methods, and show that gauge invariant sources, which are nonlinear in the gauge potential $A_0$, generate novel contributions to the gluon self energy at $\\sim g^2$. These ensure the gluon self energy remains transverse to $\\sim g^2$, and are essential in computing contributions to the free ","authors_text":"Chris P. Korthals Altes, Hiromichi Nishimura, Robert D. Pisarski, Vladimir V. Skokov","cross_cats":["hep-lat","nucl-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2020-02-03T19:00:02Z","title":"Free energy of a Holonomous Plasma"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2002.00968","kind":"arxiv","version":1},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:a15b5296c60f3486722c94f0b017317abf2565ec88fd87a74f5e9de25bd34ca2","target":"record","created_at":"2026-07-05T01:20:52Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"bbf62800ecc9f4130f686ce623dd56d448ff4fdcf2509ac8a9728ceb6e3d56b5","cross_cats_sorted":["hep-lat","nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2020-02-03T19:00:02Z","title_canon_sha256":"b90c1c4177d455889280ba3aa9cab2cbb6dd2694bb5880de99ea1c935e92174b"},"schema_version":"1.0","source":{"id":"2002.00968","kind":"arxiv","version":1}},"canonical_sha256":"7ee09a534a4f22e40d6a8aec36c195020c24ddeaba474692797f72c0481154c0","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"7ee09a534a4f22e40d6a8aec36c195020c24ddeaba474692797f72c0481154c0","first_computed_at":"2026-07-05T01:20:52.797843Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T01:20:52.797843Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"UVDHJyu7QGTwD5U/Hyo3P68229O21CVp+gYlgLXbG+gyowruaZFpD+R60o3MoKIuPKaA7OGAnmr4deUq1IgcBw==","signature_status":"signed_v1","signed_at":"2026-07-05T01:20:52.798309Z","signed_message":"canonical_sha256_bytes"},"source_id":"2002.00968","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:a15b5296c60f3486722c94f0b017317abf2565ec88fd87a74f5e9de25bd34ca2","sha256:c8bacfd348fa1fcf73ae3cdc1351c0ec698754fdcd6e18056920a4b09ef50ace"],"state_sha256":"ac0ef49a6a2087670c362375bab13de89c348f5bde857b240310039e632f529b"}