{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:1998:GKHZ4QP74OV5MHCWYMODSTXZ34","short_pith_number":"pith:GKHZ4QP7","canonical_record":{"source":{"id":"hep-ph/9803285","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1998-03-09T15:14:51Z","cross_cats_sorted":["hep-lat"],"title_canon_sha256":"f010c8986195da20958a0b67d2f27abd2df48e9c2e123cfec6b6cbba0c6ce649","abstract_canon_sha256":"ed4f214f5e52696fb2a17c3feeb5036de376ee24882e3b830c4045d5d24611e9"},"schema_version":"1.0"},"canonical_sha256":"328f9e41ffe3abd61c56c31c394ef9df150aa6fc661a9653a117ab38fcbfb126","source":{"kind":"arxiv","id":"hep-ph/9803285","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/9803285","created_at":"2026-07-04T16:09:11Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9803285v2","created_at":"2026-07-04T16:09:11Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9803285","created_at":"2026-07-04T16:09:11Z"},{"alias_kind":"pith_short_12","alias_value":"GKHZ4QP74OV5","created_at":"2026-07-04T16:09:11Z"},{"alias_kind":"pith_short_16","alias_value":"GKHZ4QP74OV5MHCW","created_at":"2026-07-04T16:09:11Z"},{"alias_kind":"pith_short_8","alias_value":"GKHZ4QP7","created_at":"2026-07-04T16:09:11Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:1998:GKHZ4QP74OV5MHCWYMODSTXZ34","target":"record","payload":{"canonical_record":{"source":{"id":"hep-ph/9803285","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1998-03-09T15:14:51Z","cross_cats_sorted":["hep-lat"],"title_canon_sha256":"f010c8986195da20958a0b67d2f27abd2df48e9c2e123cfec6b6cbba0c6ce649","abstract_canon_sha256":"ed4f214f5e52696fb2a17c3feeb5036de376ee24882e3b830c4045d5d24611e9"},"schema_version":"1.0"},"canonical_sha256":"328f9e41ffe3abd61c56c31c394ef9df150aa6fc661a9653a117ab38fcbfb126","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:09:11.238186Z","signature_b64":"DKJKYZUHVJWyDNFR3WhUxr59qr6T5WJ8khqELXL+YvGcCII66AbsvnNOMWkvey/Rn/YPl+Rs8qfFeIGBK8zZDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"328f9e41ffe3abd61c56c31c394ef9df150aa6fc661a9653a117ab38fcbfb126","last_reissued_at":"2026-07-04T16:09:11.237845Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:09:11.237845Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-ph/9803285","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-04T16:09:11Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"20abbtPWvuxJOx/YFe/De4EEdnlCE+Dhw5tVTAjY4fZhU79RfTinQnsxxm4HB5ELsOaMEIXS9jaRTl4bfZL+BQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-17T21:42:18.093802Z"},"content_sha256":"6cdb7f2360385975d9eceb1f91aea5b1d9b7e74891fb265f0be0003221c3f94b","schema_version":"1.0","event_id":"sha256:6cdb7f2360385975d9eceb1f91aea5b1d9b7e74891fb265f0be0003221c3f94b"},{"event_type":"graph_snapshot","subject_pith_number":"pith:1998:GKHZ4QP74OV5MHCWYMODSTXZ34","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Evidence for quantum chaos in the plasma phase of QCD","license":"","headline":"","cross_cats":["hep-lat"],"primary_cat":"hep-ph","authors_text":"H. Markum, K. Rabitsch, R. Pullirsch, T. Wettig","submitted_at":"1998-03-09T15:14:51Z","abstract_excerpt":"We investigate the eigenvalue spectrum of the staggered Dirac matrix in SU(3) gauge theory and in full QCD on a $6^3\\times 4$ lattice. As a measure of the fluctuation properties of the eigenvalues, we study the nearest-neighbor spacing distribution $P(s)$ for various values of $\\beta$ both in the confinement and in the deconfinement phase. In both phases except far into the deconfinement region, the lattice data agree with the Wigner surmise of random-matrix theory which is indicative of quantum chaos. We do not find signs of a transition to Poisson regularity at the deconfinement phase transi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9803285","kind":"arxiv","version":2},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/hep-ph/9803285/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-04T16:09:11Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"dL4qdT0Jhqg5a8mvpNAwQKvkEtLvLGobf/C6zg2iERCgmUtdMawnWt058sue0xC7mKu8ZhSPqMdTKWmdq4LSCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-17T21:42:18.094337Z"},"content_sha256":"3a7242ca87ccaf5e69904927bb300022102da55cff6bb28e2a339e6d73b9700c","schema_version":"1.0","event_id":"sha256:3a7242ca87ccaf5e69904927bb300022102da55cff6bb28e2a339e6d73b9700c"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/GKHZ4QP74OV5MHCWYMODSTXZ34/bundle.json","state_url":"https://pith.science/pith/GKHZ4QP74OV5MHCWYMODSTXZ34/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/GKHZ4QP74OV5MHCWYMODSTXZ34/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-08-17T21:42:18Z","links":{"resolver":"https://pith.science/pith/GKHZ4QP74OV5MHCWYMODSTXZ34","bundle":"https://pith.science/pith/GKHZ4QP74OV5MHCWYMODSTXZ34/bundle.json","state":"https://pith.science/pith/GKHZ4QP74OV5MHCWYMODSTXZ34/state.json","well_known_bundle":"https://pith.science/.well-known/pith/GKHZ4QP74OV5MHCWYMODSTXZ34/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:1998:GKHZ4QP74OV5MHCWYMODSTXZ34","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":"ed4f214f5e52696fb2a17c3feeb5036de376ee24882e3b830c4045d5d24611e9","cross_cats_sorted":["hep-lat"],"license":"","primary_cat":"hep-ph","submitted_at":"1998-03-09T15:14:51Z","title_canon_sha256":"f010c8986195da20958a0b67d2f27abd2df48e9c2e123cfec6b6cbba0c6ce649"},"schema_version":"1.0","source":{"id":"hep-ph/9803285","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/9803285","created_at":"2026-07-04T16:09:11Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9803285v2","created_at":"2026-07-04T16:09:11Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9803285","created_at":"2026-07-04T16:09:11Z"},{"alias_kind":"pith_short_12","alias_value":"GKHZ4QP74OV5","created_at":"2026-07-04T16:09:11Z"},{"alias_kind":"pith_short_16","alias_value":"GKHZ4QP74OV5MHCW","created_at":"2026-07-04T16:09:11Z"},{"alias_kind":"pith_short_8","alias_value":"GKHZ4QP7","created_at":"2026-07-04T16:09:11Z"}],"graph_snapshots":[{"event_id":"sha256:3a7242ca87ccaf5e69904927bb300022102da55cff6bb28e2a339e6d73b9700c","target":"graph","created_at":"2026-07-04T16:09:11Z","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/hep-ph/9803285/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We investigate the eigenvalue spectrum of the staggered Dirac matrix in SU(3) gauge theory and in full QCD on a $6^3\\times 4$ lattice. As a measure of the fluctuation properties of the eigenvalues, we study the nearest-neighbor spacing distribution $P(s)$ for various values of $\\beta$ both in the confinement and in the deconfinement phase. In both phases except far into the deconfinement region, the lattice data agree with the Wigner surmise of random-matrix theory which is indicative of quantum chaos. We do not find signs of a transition to Poisson regularity at the deconfinement phase transi","authors_text":"H. Markum, K. Rabitsch, R. Pullirsch, T. Wettig","cross_cats":["hep-lat"],"headline":"","license":"","primary_cat":"hep-ph","submitted_at":"1998-03-09T15:14:51Z","title":"Evidence for quantum chaos in the plasma phase of QCD"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9803285","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":"sha256:6cdb7f2360385975d9eceb1f91aea5b1d9b7e74891fb265f0be0003221c3f94b","target":"record","created_at":"2026-07-04T16:09:11Z","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":"ed4f214f5e52696fb2a17c3feeb5036de376ee24882e3b830c4045d5d24611e9","cross_cats_sorted":["hep-lat"],"license":"","primary_cat":"hep-ph","submitted_at":"1998-03-09T15:14:51Z","title_canon_sha256":"f010c8986195da20958a0b67d2f27abd2df48e9c2e123cfec6b6cbba0c6ce649"},"schema_version":"1.0","source":{"id":"hep-ph/9803285","kind":"arxiv","version":2}},"canonical_sha256":"328f9e41ffe3abd61c56c31c394ef9df150aa6fc661a9653a117ab38fcbfb126","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"328f9e41ffe3abd61c56c31c394ef9df150aa6fc661a9653a117ab38fcbfb126","first_computed_at":"2026-07-04T16:09:11.237845Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T16:09:11.237845Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"DKJKYZUHVJWyDNFR3WhUxr59qr6T5WJ8khqELXL+YvGcCII66AbsvnNOMWkvey/Rn/YPl+Rs8qfFeIGBK8zZDQ==","signature_status":"signed_v1","signed_at":"2026-07-04T16:09:11.238186Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-ph/9803285","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:6cdb7f2360385975d9eceb1f91aea5b1d9b7e74891fb265f0be0003221c3f94b","sha256:3a7242ca87ccaf5e69904927bb300022102da55cff6bb28e2a339e6d73b9700c"],"state_sha256":"f6afebde4630e1e12d55b45e28504b7bb2c7984cfe0b8f17fb1deadbbec134a6"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"oija0PFkJgM5LrL9oJZOF0Al7qUqMU5kuzXx44BvDWinWBz0/G7afy80B/FQ2ZHTf8RxHi8a/fg615boOQufAA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-17T21:42:18.099386Z","bundle_sha256":"377d8c226852d043458cfa1123076007cc57bdea7a6d61a02991b341900d0bd9"}}