{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2025:BRTHCUA4JWAUZ5LN6CZMBWXF2R","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":"a6ddaaa49bc7f94f48a654f9f4c7260602b5458fecc8a73a33fe8624af027cca","cross_cats_sorted":["hep-lat","nucl-th"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2025-04-28T18:00:01Z","title_canon_sha256":"e56f4770047d4d028b97c8c2390a91df7eccc7626a58f74656525dd6f313e25a"},"schema_version":"1.0","source":{"id":"2504.20138","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2504.20138","created_at":"2026-07-05T11:49:09Z"},{"alias_kind":"arxiv_version","alias_value":"2504.20138v2","created_at":"2026-07-05T11:49:09Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2504.20138","created_at":"2026-07-05T11:49:09Z"},{"alias_kind":"pith_short_12","alias_value":"BRTHCUA4JWAU","created_at":"2026-07-05T11:49:09Z"},{"alias_kind":"pith_short_16","alias_value":"BRTHCUA4JWAUZ5LN","created_at":"2026-07-05T11:49:09Z"},{"alias_kind":"pith_short_8","alias_value":"BRTHCUA4","created_at":"2026-07-05T11:49:09Z"}],"graph_snapshots":[{"event_id":"sha256:e62e611c1c94d1f08e2f7fe933da118ae1a4d62d0de97313c803d60103ce69c6","target":"graph","created_at":"2026-07-05T11:49:09Z","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/2504.20138/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"At nonzero temperatures, the deconfining phase transition can be analyzed using an effective matrix model to characterize the change in holonomy. The model includes gluons and two-dimensional ghost fields in the adjoint representation, or ``teens''. As ghosts, the teen fields are responsible for the decrease of the pressure as $T \\rightarrow T_d$, with $T_d$ the transition temperature for deconfinement. Using the solution of this matrix model for a large number of colors, the parameters of the teen fields are adjusted so that the expectation value of the Polyakov loop is close to the values fr","authors_text":"Manas Debnath, Najmul Haque, Ritesh Ghosh, Robert D. Pisarski, Yoshimasa Hidaka","cross_cats":["hep-lat","nucl-th"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2025-04-28T18:00:01Z","title":"Shear and bulk viscosity for a pure glue theory using an effective matrix model"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2504.20138","kind":"arxiv","version":2},"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:ad1a87ea3e5afd0412bed5cf86d121e1abc6d9f834795610c1421653c632297a","target":"record","created_at":"2026-07-05T11:49:09Z","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":"a6ddaaa49bc7f94f48a654f9f4c7260602b5458fecc8a73a33fe8624af027cca","cross_cats_sorted":["hep-lat","nucl-th"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2025-04-28T18:00:01Z","title_canon_sha256":"e56f4770047d4d028b97c8c2390a91df7eccc7626a58f74656525dd6f313e25a"},"schema_version":"1.0","source":{"id":"2504.20138","kind":"arxiv","version":2}},"canonical_sha256":"0c6671501c4d814cf56df0b2c0dae5d4745fe2329a64a7cfaad43ebdaaa8e452","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"0c6671501c4d814cf56df0b2c0dae5d4745fe2329a64a7cfaad43ebdaaa8e452","first_computed_at":"2026-07-05T11:49:09.571337Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T11:49:09.571337Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"t1fy3DXxTUPrhYElKOwjjqi3f7J9+8GiIcRrloFnA6PGa7gKLXe9og6IaxrOBJJ80Uy7kmJgZn2Ai+/GGzmuBg==","signature_status":"signed_v1","signed_at":"2026-07-05T11:49:09.571777Z","signed_message":"canonical_sha256_bytes"},"source_id":"2504.20138","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:ad1a87ea3e5afd0412bed5cf86d121e1abc6d9f834795610c1421653c632297a","sha256:e62e611c1c94d1f08e2f7fe933da118ae1a4d62d0de97313c803d60103ce69c6"],"state_sha256":"421408cd76a0629c5087ef1fd60fb9c3e4951ad86ff3925f2ffbf9f3c58af56b"}