{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2004:3Q7XRSBLRUJCFHEM76XTKGVJPL","short_pith_number":"pith:3Q7XRSBL","canonical_record":{"source":{"id":"cond-mat/0405598","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"cond-mat.other","submitted_at":"2004-05-26T08:51:16Z","cross_cats_sorted":[],"title_canon_sha256":"360454e27fd4cebed71ff735be65f69848a8ed1942a562cb9a13dde4b1a6072d","abstract_canon_sha256":"8c41110bd85808b83a923861d36eb4d98898b6c1d480765159278102146f51ca"},"schema_version":"1.0"},"canonical_sha256":"dc3f78c82b8d12229c8cffaf351aa97ad36d8c8ae9556750a1f24f8136280fb1","source":{"kind":"arxiv","id":"cond-mat/0405598","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"cond-mat/0405598","created_at":"2026-05-18T01:39:58Z"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/0405598v2","created_at":"2026-05-18T01:39:58Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/0405598","created_at":"2026-05-18T01:39:58Z"},{"alias_kind":"pith_short_12","alias_value":"3Q7XRSBLRUJC","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_16","alias_value":"3Q7XRSBLRUJCFHEM","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_8","alias_value":"3Q7XRSBL","created_at":"2026-05-18T12:25:52Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2004:3Q7XRSBLRUJCFHEM76XTKGVJPL","target":"record","payload":{"canonical_record":{"source":{"id":"cond-mat/0405598","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"cond-mat.other","submitted_at":"2004-05-26T08:51:16Z","cross_cats_sorted":[],"title_canon_sha256":"360454e27fd4cebed71ff735be65f69848a8ed1942a562cb9a13dde4b1a6072d","abstract_canon_sha256":"8c41110bd85808b83a923861d36eb4d98898b6c1d480765159278102146f51ca"},"schema_version":"1.0"},"canonical_sha256":"dc3f78c82b8d12229c8cffaf351aa97ad36d8c8ae9556750a1f24f8136280fb1","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:39:58.139102Z","signature_b64":"xa5Ln99R7sCalpoV3ndes3YQmrUGkpzuYvj0gaeT6uYCWYgBzO4BLW2sNZHDte75Zm5I5M99ovouQVikYtaNDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"dc3f78c82b8d12229c8cffaf351aa97ad36d8c8ae9556750a1f24f8136280fb1","last_reissued_at":"2026-05-18T01:39:58.138688Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:39:58.138688Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"cond-mat/0405598","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":"2026-05-18T01:39:58Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"jY+gMx4WbmheT03Hw3l98QZK7OD4KuPX/vUON8x/4tdrm7atbe3uiXMPfO3T4RourOAuoNMJ+TjNTUveeWEiBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-17T04:04:07.121671Z"},"content_sha256":"9169d4fa7dd1d357d13fd41ba8cf346ef2ef04376e87b6e79dd402c084d8da4f","schema_version":"1.0","event_id":"sha256:9169d4fa7dd1d357d13fd41ba8cf346ef2ef04376e87b6e79dd402c084d8da4f"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2004:3Q7XRSBLRUJCFHEM76XTKGVJPL","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Off equilibrium dynamics in the 3d-XY system","license":"","headline":"","cross_cats":[],"primary_cat":"cond-mat.other","authors_text":"Dragi Karevski, Stephane Abriet","submitted_at":"2004-05-26T08:51:16Z","abstract_excerpt":"We investigate through Monte Carlo simulations the non-equilibrium behaviour of the three-dimensional XY-model quenched from a high temperature state to its ferromagnetic and critical phases. The two-times autocorrelation and response functions are determined in the asymptotic (scaling) regime, from which the nonequilibrium exponents $\\lambda$ and critical $\\lambda^c$ are extracted. The form of the scaling function is in agreement with the prediction of local scale-invariance. The so-called limit fluctuation-dissipation ratio $X_\\infty$ is shown to vanish in the ordered phase and to reach a co"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/0405598","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":""},"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":"2026-05-18T01:39:58Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"5Njv6Gkd2SJoIGSQD1XywP800Bt2ldDRSAXIo6w/dmh+IzYY2W3Cw1fnIWBKRF8uP9scmIAJ6xSnqJrE8rF9Dg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-17T04:04:07.122132Z"},"content_sha256":"edd082e2cf6d21e2844ca1a9e4dd194a73570179c0bda72326cd21a0cab8003a","schema_version":"1.0","event_id":"sha256:edd082e2cf6d21e2844ca1a9e4dd194a73570179c0bda72326cd21a0cab8003a"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/3Q7XRSBLRUJCFHEM76XTKGVJPL/bundle.json","state_url":"https://pith.science/pith/3Q7XRSBLRUJCFHEM76XTKGVJPL/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/3Q7XRSBLRUJCFHEM76XTKGVJPL/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":"2026-08-17T04:04:07Z","links":{"resolver":"https://pith.science/pith/3Q7XRSBLRUJCFHEM76XTKGVJPL","bundle":"https://pith.science/pith/3Q7XRSBLRUJCFHEM76XTKGVJPL/bundle.json","state":"https://pith.science/pith/3Q7XRSBLRUJCFHEM76XTKGVJPL/state.json","well_known_bundle":"https://pith.science/.well-known/pith/3Q7XRSBLRUJCFHEM76XTKGVJPL/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2004:3Q7XRSBLRUJCFHEM76XTKGVJPL","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":"8c41110bd85808b83a923861d36eb4d98898b6c1d480765159278102146f51ca","cross_cats_sorted":[],"license":"","primary_cat":"cond-mat.other","submitted_at":"2004-05-26T08:51:16Z","title_canon_sha256":"360454e27fd4cebed71ff735be65f69848a8ed1942a562cb9a13dde4b1a6072d"},"schema_version":"1.0","source":{"id":"cond-mat/0405598","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"cond-mat/0405598","created_at":"2026-05-18T01:39:58Z"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/0405598v2","created_at":"2026-05-18T01:39:58Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/0405598","created_at":"2026-05-18T01:39:58Z"},{"alias_kind":"pith_short_12","alias_value":"3Q7XRSBLRUJC","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_16","alias_value":"3Q7XRSBLRUJCFHEM","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_8","alias_value":"3Q7XRSBL","created_at":"2026-05-18T12:25:52Z"}],"graph_snapshots":[{"event_id":"sha256:edd082e2cf6d21e2844ca1a9e4dd194a73570179c0bda72326cd21a0cab8003a","target":"graph","created_at":"2026-05-18T01:39:58Z","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":"We investigate through Monte Carlo simulations the non-equilibrium behaviour of the three-dimensional XY-model quenched from a high temperature state to its ferromagnetic and critical phases. The two-times autocorrelation and response functions are determined in the asymptotic (scaling) regime, from which the nonequilibrium exponents $\\lambda$ and critical $\\lambda^c$ are extracted. The form of the scaling function is in agreement with the prediction of local scale-invariance. The so-called limit fluctuation-dissipation ratio $X_\\infty$ is shown to vanish in the ordered phase and to reach a co","authors_text":"Dragi Karevski, Stephane Abriet","cross_cats":[],"headline":"","license":"","primary_cat":"cond-mat.other","submitted_at":"2004-05-26T08:51:16Z","title":"Off equilibrium dynamics in the 3d-XY system"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/0405598","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":"sha256:9169d4fa7dd1d357d13fd41ba8cf346ef2ef04376e87b6e79dd402c084d8da4f","target":"record","created_at":"2026-05-18T01:39:58Z","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":"8c41110bd85808b83a923861d36eb4d98898b6c1d480765159278102146f51ca","cross_cats_sorted":[],"license":"","primary_cat":"cond-mat.other","submitted_at":"2004-05-26T08:51:16Z","title_canon_sha256":"360454e27fd4cebed71ff735be65f69848a8ed1942a562cb9a13dde4b1a6072d"},"schema_version":"1.0","source":{"id":"cond-mat/0405598","kind":"arxiv","version":2}},"canonical_sha256":"dc3f78c82b8d12229c8cffaf351aa97ad36d8c8ae9556750a1f24f8136280fb1","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"dc3f78c82b8d12229c8cffaf351aa97ad36d8c8ae9556750a1f24f8136280fb1","first_computed_at":"2026-05-18T01:39:58.138688Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:39:58.138688Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"xa5Ln99R7sCalpoV3ndes3YQmrUGkpzuYvj0gaeT6uYCWYgBzO4BLW2sNZHDte75Zm5I5M99ovouQVikYtaNDg==","signature_status":"signed_v1","signed_at":"2026-05-18T01:39:58.139102Z","signed_message":"canonical_sha256_bytes"},"source_id":"cond-mat/0405598","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:9169d4fa7dd1d357d13fd41ba8cf346ef2ef04376e87b6e79dd402c084d8da4f","sha256:edd082e2cf6d21e2844ca1a9e4dd194a73570179c0bda72326cd21a0cab8003a"],"state_sha256":"d4582ab6f1d810eb0d87bf2495315632dc9b4fda28f1625ed4dc2643005a2d9b"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"C+8BcyWovFg1nEWr5pbNVLnzRkrlEJ1G4gpiayg5rKQwXGQjYYLP5xqbX2cfqDdGNzgn4kjM8H7cELi4PFk3DQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-17T04:04:07.133263Z","bundle_sha256":"fdd1ce5a305de7603cb200b40d9edbc7f103922dc6f4626240ecd7383ead3331"}}