{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2023:MTAZ2KZ3KENDGY275GRPTQECXF","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":"543fabc54eb71abf7529d68a045bd7943678f502b52981ee09b52109cb5208b7","cross_cats_sorted":["hep-ph","hep-th"],"license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","primary_cat":"hep-lat","submitted_at":"2023-11-07T12:40:40Z","title_canon_sha256":"384edf46210d54c0e076b464c574be404924a2f49615ebdad80550070ccbfb38"},"schema_version":"1.0","source":{"id":"2311.03947","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2311.03947","created_at":"2026-07-05T07:28:12Z"},{"alias_kind":"arxiv_version","alias_value":"2311.03947v1","created_at":"2026-07-05T07:28:12Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2311.03947","created_at":"2026-07-05T07:28:12Z"},{"alias_kind":"pith_short_12","alias_value":"MTAZ2KZ3KEND","created_at":"2026-07-05T07:28:12Z"},{"alias_kind":"pith_short_16","alias_value":"MTAZ2KZ3KENDGY27","created_at":"2026-07-05T07:28:12Z"},{"alias_kind":"pith_short_8","alias_value":"MTAZ2KZ3","created_at":"2026-07-05T07:28:12Z"}],"graph_snapshots":[{"event_id":"sha256:07fe15841977cce32849bf27c9a6a00b343cc72277cce60bea51ec75a2c37a53","target":"graph","created_at":"2026-07-05T07:28:12Z","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/2311.03947/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Using lattice simulations, we analyze the influence of uniform rotation on the equation of state of gluodynamics. For a sufficiently slow rotation, the free energy of the system can be expanded into a series of powers of angular velocity. We calculate the moment of inertia given by the quadratic coefficient of this expansion using both analytic continuation and derivative methods, which demonstrate a good agreement between the results. We find that the moment of inertia unexpectedly takes a negative value below the ``supervortical temperature'' $T_s = 1.50(10) T_c$, vanishes at $T = T_s$, and ","authors_text":"Artem A. Roenko, Dmitrii A. Sychev, Ilya E. Kudrov, Maxim N. Chernodub, Victor V. Braguta","cross_cats":["hep-ph","hep-th"],"headline":"","license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","primary_cat":"hep-lat","submitted_at":"2023-11-07T12:40:40Z","title":"Moment of inertia and supervortical temperature of gluon plasma"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2311.03947","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:ac6f1f6e6366a7fd700915c4bd1370c4822bc281301cf1afebdf2eadb9fb2ff2","target":"record","created_at":"2026-07-05T07:28:12Z","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":"543fabc54eb71abf7529d68a045bd7943678f502b52981ee09b52109cb5208b7","cross_cats_sorted":["hep-ph","hep-th"],"license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","primary_cat":"hep-lat","submitted_at":"2023-11-07T12:40:40Z","title_canon_sha256":"384edf46210d54c0e076b464c574be404924a2f49615ebdad80550070ccbfb38"},"schema_version":"1.0","source":{"id":"2311.03947","kind":"arxiv","version":1}},"canonical_sha256":"64c19d2b3b511a33635fe9a2f9c082b9547ccd658bbfb22e28d66c3f82208d1c","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"64c19d2b3b511a33635fe9a2f9c082b9547ccd658bbfb22e28d66c3f82208d1c","first_computed_at":"2026-07-05T07:28:12.028174Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T07:28:12.028174Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"1i07IPoCokjUldTyJBlxyYkW+g+U6t68OC5zGIcGSwAu0keL3j1vT0d8UxEQMK5pSDEbgrwP4qmhKVGe64i5BQ==","signature_status":"signed_v1","signed_at":"2026-07-05T07:28:12.028601Z","signed_message":"canonical_sha256_bytes"},"source_id":"2311.03947","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:ac6f1f6e6366a7fd700915c4bd1370c4822bc281301cf1afebdf2eadb9fb2ff2","sha256:07fe15841977cce32849bf27c9a6a00b343cc72277cce60bea51ec75a2c37a53"],"state_sha256":"236514bd3b3bed46f94cb2d9f9c2d5e6c072eda159bba740bddcf469866ce953"}