{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2002:SPEIIA5FY5BSRRV7ZL7J3UNRBK","short_pith_number":"pith:SPEIIA5F","canonical_record":{"source":{"id":"cond-mat/0204195","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"cond-mat.stat-mech","submitted_at":"2002-04-09T17:17:54Z","cross_cats_sorted":[],"title_canon_sha256":"714b086987939e1a569ac7d76c382aa2c04feacea927b844ed90840d45287451","abstract_canon_sha256":"607b2848d11c9a1c8e4d7a1c6322c3817f56f591c81fcf7720c28cf23b77ac88"},"schema_version":"1.0"},"canonical_sha256":"93c88403a5c74328c6bfcafe9dd1b10a8220918c32fadb0be40a445d696ee9fc","source":{"kind":"arxiv","id":"cond-mat/0204195","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"cond-mat/0204195","created_at":"2026-05-18T01:40:03Z"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/0204195v1","created_at":"2026-05-18T01:40:03Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/0204195","created_at":"2026-05-18T01:40:03Z"},{"alias_kind":"pith_short_12","alias_value":"SPEIIA5FY5BS","created_at":"2026-05-18T12:25:51Z"},{"alias_kind":"pith_short_16","alias_value":"SPEIIA5FY5BSRRV7","created_at":"2026-05-18T12:25:51Z"},{"alias_kind":"pith_short_8","alias_value":"SPEIIA5F","created_at":"2026-05-18T12:25:51Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2002:SPEIIA5FY5BSRRV7ZL7J3UNRBK","target":"record","payload":{"canonical_record":{"source":{"id":"cond-mat/0204195","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"cond-mat.stat-mech","submitted_at":"2002-04-09T17:17:54Z","cross_cats_sorted":[],"title_canon_sha256":"714b086987939e1a569ac7d76c382aa2c04feacea927b844ed90840d45287451","abstract_canon_sha256":"607b2848d11c9a1c8e4d7a1c6322c3817f56f591c81fcf7720c28cf23b77ac88"},"schema_version":"1.0"},"canonical_sha256":"93c88403a5c74328c6bfcafe9dd1b10a8220918c32fadb0be40a445d696ee9fc","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:40:03.698617Z","signature_b64":"vMXwz+KKZKs4LdeI3IDe9lZzRukJesAIaaxMvWUXf2XCavmm3I2D6zNuG0UoabSrCxQATPVDW6pD+c7txapaDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"93c88403a5c74328c6bfcafe9dd1b10a8220918c32fadb0be40a445d696ee9fc","last_reissued_at":"2026-05-18T01:40:03.698110Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:40:03.698110Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"cond-mat/0204195","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:40:03Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"VVNu+HEAqIFJEk4tGvFojJYl1hRp/pyHY4F9eDfPgw7VDUKV/vmtioR0s3GaJ83O0HlAK7Ot9hsa/GlFA0lRBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T06:17:04.571541Z"},"content_sha256":"2d529d1c5c70c3faa3e59e29e89b90b6e12334912a58e80d138aaf9c61c3d8a5","schema_version":"1.0","event_id":"sha256:2d529d1c5c70c3faa3e59e29e89b90b6e12334912a58e80d138aaf9c61c3d8a5"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2002:SPEIIA5FY5BSRRV7ZL7J3UNRBK","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Non-equilibrium behavior at a liquid-gas critical point","license":"","headline":"","cross_cats":[],"primary_cat":"cond-mat.stat-mech","authors_text":"Blacksburg, Jaime E. Santos (Hahn-Meitner-Institut Berlin), Uwe C. Tauber (Virginia Tech, VA)","submitted_at":"2002-04-09T17:17:54Z","abstract_excerpt":"Second-order phase transitions in a non-equilibrium liquid-gas model with reversible mode couplings, i.e., model H for binary-fluid critical dynamics, are studied using dynamic field theory and the renormalization group. The system is driven out of equilibrium either by considering different values for the noise strengths in the Langevin equations describing the evolution of the dynamic variables (effectively placing these at different temperatures), or more generally by allowing for anisotropic noise strengths, i.e., by constraining the dynamics to be at different temperatures in d_par- and d"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/0204195","kind":"arxiv","version":1},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"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":"2026-05-18T01:40:03Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"xxBnCcAI6jAc7k9pGYFCSUh3YT3/rJNNQQlK5ogwNedt1jQP78bbhdydhZnIUvx3M9Q38AgIZoLomQgM/LTUCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T06:17:04.572226Z"},"content_sha256":"f5a587a7069b7328c0cb3090b21d12d5351a64d685098ac3992a0b31279f1207","schema_version":"1.0","event_id":"sha256:f5a587a7069b7328c0cb3090b21d12d5351a64d685098ac3992a0b31279f1207"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/SPEIIA5FY5BSRRV7ZL7J3UNRBK/bundle.json","state_url":"https://pith.science/pith/SPEIIA5FY5BSRRV7ZL7J3UNRBK/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/SPEIIA5FY5BSRRV7ZL7J3UNRBK/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":"2026-05-27T06:17:04Z","links":{"resolver":"https://pith.science/pith/SPEIIA5FY5BSRRV7ZL7J3UNRBK","bundle":"https://pith.science/pith/SPEIIA5FY5BSRRV7ZL7J3UNRBK/bundle.json","state":"https://pith.science/pith/SPEIIA5FY5BSRRV7ZL7J3UNRBK/state.json","well_known_bundle":"https://pith.science/.well-known/pith/SPEIIA5FY5BSRRV7ZL7J3UNRBK/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2002:SPEIIA5FY5BSRRV7ZL7J3UNRBK","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":"607b2848d11c9a1c8e4d7a1c6322c3817f56f591c81fcf7720c28cf23b77ac88","cross_cats_sorted":[],"license":"","primary_cat":"cond-mat.stat-mech","submitted_at":"2002-04-09T17:17:54Z","title_canon_sha256":"714b086987939e1a569ac7d76c382aa2c04feacea927b844ed90840d45287451"},"schema_version":"1.0","source":{"id":"cond-mat/0204195","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"cond-mat/0204195","created_at":"2026-05-18T01:40:03Z"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/0204195v1","created_at":"2026-05-18T01:40:03Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/0204195","created_at":"2026-05-18T01:40:03Z"},{"alias_kind":"pith_short_12","alias_value":"SPEIIA5FY5BS","created_at":"2026-05-18T12:25:51Z"},{"alias_kind":"pith_short_16","alias_value":"SPEIIA5FY5BSRRV7","created_at":"2026-05-18T12:25:51Z"},{"alias_kind":"pith_short_8","alias_value":"SPEIIA5F","created_at":"2026-05-18T12:25:51Z"}],"graph_snapshots":[{"event_id":"sha256:f5a587a7069b7328c0cb3090b21d12d5351a64d685098ac3992a0b31279f1207","target":"graph","created_at":"2026-05-18T01:40:03Z","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"},"paper":{"abstract_excerpt":"Second-order phase transitions in a non-equilibrium liquid-gas model with reversible mode couplings, i.e., model H for binary-fluid critical dynamics, are studied using dynamic field theory and the renormalization group. The system is driven out of equilibrium either by considering different values for the noise strengths in the Langevin equations describing the evolution of the dynamic variables (effectively placing these at different temperatures), or more generally by allowing for anisotropic noise strengths, i.e., by constraining the dynamics to be at different temperatures in d_par- and d","authors_text":"Blacksburg, Jaime E. Santos (Hahn-Meitner-Institut Berlin), Uwe C. Tauber (Virginia Tech, VA)","cross_cats":[],"headline":"","license":"","primary_cat":"cond-mat.stat-mech","submitted_at":"2002-04-09T17:17:54Z","title":"Non-equilibrium behavior at a liquid-gas critical point"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/0204195","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":"sha256:2d529d1c5c70c3faa3e59e29e89b90b6e12334912a58e80d138aaf9c61c3d8a5","target":"record","created_at":"2026-05-18T01:40:03Z","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":"607b2848d11c9a1c8e4d7a1c6322c3817f56f591c81fcf7720c28cf23b77ac88","cross_cats_sorted":[],"license":"","primary_cat":"cond-mat.stat-mech","submitted_at":"2002-04-09T17:17:54Z","title_canon_sha256":"714b086987939e1a569ac7d76c382aa2c04feacea927b844ed90840d45287451"},"schema_version":"1.0","source":{"id":"cond-mat/0204195","kind":"arxiv","version":1}},"canonical_sha256":"93c88403a5c74328c6bfcafe9dd1b10a8220918c32fadb0be40a445d696ee9fc","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"93c88403a5c74328c6bfcafe9dd1b10a8220918c32fadb0be40a445d696ee9fc","first_computed_at":"2026-05-18T01:40:03.698110Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:40:03.698110Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"vMXwz+KKZKs4LdeI3IDe9lZzRukJesAIaaxMvWUXf2XCavmm3I2D6zNuG0UoabSrCxQATPVDW6pD+c7txapaDQ==","signature_status":"signed_v1","signed_at":"2026-05-18T01:40:03.698617Z","signed_message":"canonical_sha256_bytes"},"source_id":"cond-mat/0204195","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:2d529d1c5c70c3faa3e59e29e89b90b6e12334912a58e80d138aaf9c61c3d8a5","sha256:f5a587a7069b7328c0cb3090b21d12d5351a64d685098ac3992a0b31279f1207"],"state_sha256":"04a691811c657a1cae4e290a6c5e08d418b46ed73774f422bc14023597d7b44a"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ePKCcB3u8btln/RgqcCntE8tZ+IYA5M23IR8bWKgnPod0dSn7esVrO+9enWHUgA+W0IBSws25lj/L17+w2zHBQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-27T06:17:04.575778Z","bundle_sha256":"cee8873b7fdf575f6c0cb0ab719bb76c64946c7a6394b063884c5bbed3c76f8b"}}