{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:T2DZ3AKZE7Z5VOVFKHOZ3O2MN3","short_pith_number":"pith:T2DZ3AKZ","canonical_record":{"source":{"id":"1410.0978","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2014-10-03T21:06:23Z","cross_cats_sorted":[],"title_canon_sha256":"c27e82fa9c4636339aaff63fe8e30f14de8bc2d31c5e05a8f96c1afbbda551d7","abstract_canon_sha256":"d5fb4077046fd39ece79946b3ba2517f5c279f0cacba3a8736143b54974994f4"},"schema_version":"1.0"},"canonical_sha256":"9e879d815927f3dabaa551dd9dbb4c6ec1b24950b2fd0196eeb6cac174d0418d","source":{"kind":"arxiv","id":"1410.0978","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1410.0978","created_at":"2026-05-18T01:41:52Z"},{"alias_kind":"arxiv_version","alias_value":"1410.0978v1","created_at":"2026-05-18T01:41:52Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1410.0978","created_at":"2026-05-18T01:41:52Z"},{"alias_kind":"pith_short_12","alias_value":"T2DZ3AKZE7Z5","created_at":"2026-05-18T12:28:49Z"},{"alias_kind":"pith_short_16","alias_value":"T2DZ3AKZE7Z5VOVF","created_at":"2026-05-18T12:28:49Z"},{"alias_kind":"pith_short_8","alias_value":"T2DZ3AKZ","created_at":"2026-05-18T12:28:49Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:T2DZ3AKZE7Z5VOVFKHOZ3O2MN3","target":"record","payload":{"canonical_record":{"source":{"id":"1410.0978","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2014-10-03T21:06:23Z","cross_cats_sorted":[],"title_canon_sha256":"c27e82fa9c4636339aaff63fe8e30f14de8bc2d31c5e05a8f96c1afbbda551d7","abstract_canon_sha256":"d5fb4077046fd39ece79946b3ba2517f5c279f0cacba3a8736143b54974994f4"},"schema_version":"1.0"},"canonical_sha256":"9e879d815927f3dabaa551dd9dbb4c6ec1b24950b2fd0196eeb6cac174d0418d","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:41:52.646722Z","signature_b64":"hBFAw3JlOA10l7XrInixCyqSlWON5TB5uFrBq8L+5kmyQqvLjh3LGulI+MbAEquj1fdIklBCsSw40D7gCx7kAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9e879d815927f3dabaa551dd9dbb4c6ec1b24950b2fd0196eeb6cac174d0418d","last_reissued_at":"2026-05-18T01:41:52.646145Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:41:52.646145Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1410.0978","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":"2026-05-18T01:41:52Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"+f7eJGt2bbaRHcwKlKhaDriC+oM7L/ePVBhQS3G6tkPWU4DfGwlR5MJjYN+7oprPNdgo054JvaNNIEI0yknZBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T20:06:45.927114Z"},"content_sha256":"63e7eeff1a74a1d5b643027e6f5392cbd0c5c65ed5c4f14dc92297500d1b7c4c","schema_version":"1.0","event_id":"sha256:63e7eeff1a74a1d5b643027e6f5392cbd0c5c65ed5c4f14dc92297500d1b7c4c"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:T2DZ3AKZE7Z5VOVFKHOZ3O2MN3","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Effective temperature from fluctuation-dissipation theorem in systems with bipartite eigenmode entanglement","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.stat-mech","authors_text":"A. Iucci, T. S. Bortolin","submitted_at":"2014-10-03T21:06:23Z","abstract_excerpt":"In thermal equilibrium, the fluctuation-dissipation theorem relates the linear response and correlation functions in a model and observable independent fashion. Out of equilibrium, these relations still hold if the equilibrium temperature is replaced by an observable and frequency-dependent parameter (effective temperature). When the system achieves a long time thermal state all of these effective temperatures should be equal and constant. Following this approach we examine the long times regime after a quantum quench in a system with bipartite entanglement in which the asymptotic values of th"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1410.0978","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":"2026-05-18T01:41:52Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"MvzJ1gY8T6gPFh6EgFS4oZ6mARZSqMHBPmVnSc+tfzc0hsx0dJOXwdtTZyBBuS5z47zfTBTZvdNwudmpiXluCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T20:06:45.927777Z"},"content_sha256":"c733953ce3b6eb774fe10ba08a5006353096ea14a12284207684613a8527edff","schema_version":"1.0","event_id":"sha256:c733953ce3b6eb774fe10ba08a5006353096ea14a12284207684613a8527edff"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/T2DZ3AKZE7Z5VOVFKHOZ3O2MN3/bundle.json","state_url":"https://pith.science/pith/T2DZ3AKZE7Z5VOVFKHOZ3O2MN3/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/T2DZ3AKZE7Z5VOVFKHOZ3O2MN3/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":"2026-05-27T20:06:45Z","links":{"resolver":"https://pith.science/pith/T2DZ3AKZE7Z5VOVFKHOZ3O2MN3","bundle":"https://pith.science/pith/T2DZ3AKZE7Z5VOVFKHOZ3O2MN3/bundle.json","state":"https://pith.science/pith/T2DZ3AKZE7Z5VOVFKHOZ3O2MN3/state.json","well_known_bundle":"https://pith.science/.well-known/pith/T2DZ3AKZE7Z5VOVFKHOZ3O2MN3/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:T2DZ3AKZE7Z5VOVFKHOZ3O2MN3","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":"d5fb4077046fd39ece79946b3ba2517f5c279f0cacba3a8736143b54974994f4","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2014-10-03T21:06:23Z","title_canon_sha256":"c27e82fa9c4636339aaff63fe8e30f14de8bc2d31c5e05a8f96c1afbbda551d7"},"schema_version":"1.0","source":{"id":"1410.0978","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1410.0978","created_at":"2026-05-18T01:41:52Z"},{"alias_kind":"arxiv_version","alias_value":"1410.0978v1","created_at":"2026-05-18T01:41:52Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1410.0978","created_at":"2026-05-18T01:41:52Z"},{"alias_kind":"pith_short_12","alias_value":"T2DZ3AKZE7Z5","created_at":"2026-05-18T12:28:49Z"},{"alias_kind":"pith_short_16","alias_value":"T2DZ3AKZE7Z5VOVF","created_at":"2026-05-18T12:28:49Z"},{"alias_kind":"pith_short_8","alias_value":"T2DZ3AKZ","created_at":"2026-05-18T12:28:49Z"}],"graph_snapshots":[{"event_id":"sha256:c733953ce3b6eb774fe10ba08a5006353096ea14a12284207684613a8527edff","target":"graph","created_at":"2026-05-18T01:41:52Z","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":"In thermal equilibrium, the fluctuation-dissipation theorem relates the linear response and correlation functions in a model and observable independent fashion. Out of equilibrium, these relations still hold if the equilibrium temperature is replaced by an observable and frequency-dependent parameter (effective temperature). When the system achieves a long time thermal state all of these effective temperatures should be equal and constant. Following this approach we examine the long times regime after a quantum quench in a system with bipartite entanglement in which the asymptotic values of th","authors_text":"A. Iucci, T. S. Bortolin","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2014-10-03T21:06:23Z","title":"Effective temperature from fluctuation-dissipation theorem in systems with bipartite eigenmode entanglement"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1410.0978","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":"sha256:63e7eeff1a74a1d5b643027e6f5392cbd0c5c65ed5c4f14dc92297500d1b7c4c","target":"record","created_at":"2026-05-18T01:41:52Z","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":"d5fb4077046fd39ece79946b3ba2517f5c279f0cacba3a8736143b54974994f4","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2014-10-03T21:06:23Z","title_canon_sha256":"c27e82fa9c4636339aaff63fe8e30f14de8bc2d31c5e05a8f96c1afbbda551d7"},"schema_version":"1.0","source":{"id":"1410.0978","kind":"arxiv","version":1}},"canonical_sha256":"9e879d815927f3dabaa551dd9dbb4c6ec1b24950b2fd0196eeb6cac174d0418d","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"9e879d815927f3dabaa551dd9dbb4c6ec1b24950b2fd0196eeb6cac174d0418d","first_computed_at":"2026-05-18T01:41:52.646145Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:41:52.646145Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"hBFAw3JlOA10l7XrInixCyqSlWON5TB5uFrBq8L+5kmyQqvLjh3LGulI+MbAEquj1fdIklBCsSw40D7gCx7kAg==","signature_status":"signed_v1","signed_at":"2026-05-18T01:41:52.646722Z","signed_message":"canonical_sha256_bytes"},"source_id":"1410.0978","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:63e7eeff1a74a1d5b643027e6f5392cbd0c5c65ed5c4f14dc92297500d1b7c4c","sha256:c733953ce3b6eb774fe10ba08a5006353096ea14a12284207684613a8527edff"],"state_sha256":"a750449b6023b56653d7c1ede75d7f74a290182a9295612aa44757d833bbed27"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Ir3Ye2tHCbYcFPbbKzh/VvDVMVg61S4rSVbyWaTwdUjnnhmi7W5hTu8mnkgWC7of3HTeV3GSL6QcziGHPnc6Bw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-27T20:06:45.931337Z","bundle_sha256":"9c50c2abd63ada365b7eda0a14d4bca451fa0097db6c74baf892fbcbde4a97d6"}}