{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:6FCKI3VPTTMAFSZSUUG4LIERX5","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":"65a39529bd2bc9e58e60998fd79e40c97cac70a2e1cde3bd1ee18fb8e12c172c","cross_cats_sorted":["math-ph","math.MP","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2018-05-04T06:20:44Z","title_canon_sha256":"479377d5f04371ac18a639f103adfd03934c54d34e01b59f3f82cb7166338af3"},"schema_version":"1.0","source":{"id":"1805.02510","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1805.02510","created_at":"2026-07-05T00:01:24Z"},{"alias_kind":"arxiv_version","alias_value":"1805.02510v2","created_at":"2026-07-05T00:01:24Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1805.02510","created_at":"2026-07-05T00:01:24Z"},{"alias_kind":"pith_short_12","alias_value":"6FCKI3VPTTMA","created_at":"2026-07-05T00:01:24Z"},{"alias_kind":"pith_short_16","alias_value":"6FCKI3VPTTMAFSZS","created_at":"2026-07-05T00:01:24Z"},{"alias_kind":"pith_short_8","alias_value":"6FCKI3VP","created_at":"2026-07-05T00:01:24Z"}],"graph_snapshots":[{"event_id":"sha256:205695528b75a7556258a71b59ee9a46640e01aa7a418206c24cfb90e488ea47","target":"graph","created_at":"2026-07-05T00:01:24Z","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/1805.02510/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We consider SU(N) QCD in a new quadratic gauge which highlights certain characteristic of the theory in the non-perturbative sector. By considering natural hermiticity property of the ghost fields we cast this model as non-Hermtian but symmetric under combined Parity (P) and Time reversal (T) transformations. We explicitly study the PT phase transition in this model. This is very first such study in the non-Hermitian gauge theory. The ghost fields condensate as a direct consequence of spontaneous breaking of PT symmetry. This leads to realize the transition from deconfined phase to confined ph","authors_text":"Bhabani Prasad Mandal, Haresh Raval","cross_cats":["math-ph","math.MP","quant-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2018-05-04T06:20:44Z","title":"Deconfinement to Confinement as PT phase transition"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1805.02510","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:e4f839eea1eb402a8645fed02e02dbedfa6f11af790e0e2a5280529bcaa8a60f","target":"record","created_at":"2026-07-05T00:01:24Z","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":"65a39529bd2bc9e58e60998fd79e40c97cac70a2e1cde3bd1ee18fb8e12c172c","cross_cats_sorted":["math-ph","math.MP","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2018-05-04T06:20:44Z","title_canon_sha256":"479377d5f04371ac18a639f103adfd03934c54d34e01b59f3f82cb7166338af3"},"schema_version":"1.0","source":{"id":"1805.02510","kind":"arxiv","version":2}},"canonical_sha256":"f144a46eaf9cd802cb32a50dc5a091bf5d1b9bdf97f2df311ac61729515d6913","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f144a46eaf9cd802cb32a50dc5a091bf5d1b9bdf97f2df311ac61729515d6913","first_computed_at":"2026-07-05T00:01:24.235876Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T00:01:24.235876Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"8ONqBYRF59VPgqI/Amjqo4vOEMLBaajPLAwR1RKE7XbZVcCmKSMSnWBjDSobt85/PZgcsrOggPFddY5c92kQBw==","signature_status":"signed_v1","signed_at":"2026-07-05T00:01:24.236335Z","signed_message":"canonical_sha256_bytes"},"source_id":"1805.02510","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:e4f839eea1eb402a8645fed02e02dbedfa6f11af790e0e2a5280529bcaa8a60f","sha256:205695528b75a7556258a71b59ee9a46640e01aa7a418206c24cfb90e488ea47"],"state_sha256":"35ac8c5eb96ef3241190536e48597ae69c7ae71f0f5d49af1855b41660af865a"}