{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:1998:LFEYPO4E42S3PUKXMHDKET2C65","short_pith_number":"pith:LFEYPO4E","canonical_record":{"source":{"id":"cond-mat/9809375","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"cond-mat.dis-nn","submitted_at":"1998-09-28T16:49:31Z","cross_cats_sorted":["cond-mat.stat-mech","math-ph","math.MP","math.PR"],"title_canon_sha256":"9cdde62b0472d45ff5ba1735368736c01253a8d30694342178d4304354ab60c4","abstract_canon_sha256":"5e0fb995cf7dd0f6488daa83af305401e5a043dd04dc53ddd641c6f33680759b"},"schema_version":"1.0"},"canonical_sha256":"594987bb84e6a5b7d15761c6a24f42f74627bec5ba9e76b91d918b7feed435dc","source":{"kind":"arxiv","id":"cond-mat/9809375","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"cond-mat/9809375","created_at":"2026-05-18T01:39:29Z"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/9809375v1","created_at":"2026-05-18T01:39:29Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/9809375","created_at":"2026-05-18T01:39:29Z"},{"alias_kind":"pith_short_12","alias_value":"LFEYPO4E42S3","created_at":"2026-05-18T12:25:49Z"},{"alias_kind":"pith_short_16","alias_value":"LFEYPO4E42S3PUKX","created_at":"2026-05-18T12:25:49Z"},{"alias_kind":"pith_short_8","alias_value":"LFEYPO4E","created_at":"2026-05-18T12:25:49Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:1998:LFEYPO4E42S3PUKXMHDKET2C65","target":"record","payload":{"canonical_record":{"source":{"id":"cond-mat/9809375","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"cond-mat.dis-nn","submitted_at":"1998-09-28T16:49:31Z","cross_cats_sorted":["cond-mat.stat-mech","math-ph","math.MP","math.PR"],"title_canon_sha256":"9cdde62b0472d45ff5ba1735368736c01253a8d30694342178d4304354ab60c4","abstract_canon_sha256":"5e0fb995cf7dd0f6488daa83af305401e5a043dd04dc53ddd641c6f33680759b"},"schema_version":"1.0"},"canonical_sha256":"594987bb84e6a5b7d15761c6a24f42f74627bec5ba9e76b91d918b7feed435dc","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:39:29.909273Z","signature_b64":"SB3DmHtlgvMh+CRfSGNs1nUNdETaWylGAN4ftvg+Rc9/yGEIeL7uDusbxqmMC15smN+7p/bOYLI7hmGAZboIAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"594987bb84e6a5b7d15761c6a24f42f74627bec5ba9e76b91d918b7feed435dc","last_reissued_at":"2026-05-18T01:39:29.908662Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:39:29.908662Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"cond-mat/9809375","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":"2026-05-18T01:39:29Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"OXATH/13Xj8yGPcl++5T/gw7rRyLXwomLhI22noOjDKIlmJyLfth8PCoccRfVrI/wg6hid5LyJPJ9p9DU0EDAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-05T15:17:59.131729Z"},"content_sha256":"049653fa67db4b30e1dd62aebdba920e613fa5a53dc65820942190d9200af583","schema_version":"1.0","event_id":"sha256:049653fa67db4b30e1dd62aebdba920e613fa5a53dc65820942190d9200af583"},{"event_type":"graph_snapshot","subject_pith_number":"pith:1998:LFEYPO4E42S3PUKXMHDKET2C65","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Equilibrium Pure States and Nonequilibrium Chaos","license":"","headline":"","cross_cats":["cond-mat.stat-mech","math-ph","math.MP","math.PR"],"primary_cat":"cond-mat.dis-nn","authors_text":"C.M. Newman (Courant Institute of Mathematical Sciences, D.L. Stein (Departments of Physics, Mathematics, New York University), University of Arizona)","submitted_at":"1998-09-28T16:49:31Z","abstract_excerpt":"We consider nonequilibrium systems such as the Edwards-Anderson Ising spin glass at a temperature where, in equilibrium, there are presumed to be (two or many) broken symmetry pure states. Following a deep quench, we argue that as time goes to infinity, although the system is usually in some pure state locally, either it never settles permanently on a fixed lengthscale into a single pure state, or it does but then the pure state depends on both the initial spin configuration and the realization of the stochastic dynamics. But this latter case can occur only if there exists an uncountable numbe"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/9809375","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":"2026-05-18T01:39:29Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"doYKyPb1euZtRhj+LMusD/Jqa3xTktUPKFCqFSOOVjZetO42TXQyRI9LcZ496WvAjwjJzSfxlbtkOkf09+XKDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-05T15:17:59.132082Z"},"content_sha256":"1599ec82026c865f9604bb9f4a4ce6441c77c9d5b5347db9bae80636eac74abb","schema_version":"1.0","event_id":"sha256:1599ec82026c865f9604bb9f4a4ce6441c77c9d5b5347db9bae80636eac74abb"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/LFEYPO4E42S3PUKXMHDKET2C65/bundle.json","state_url":"https://pith.science/pith/LFEYPO4E42S3PUKXMHDKET2C65/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/LFEYPO4E42S3PUKXMHDKET2C65/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":"2026-06-05T15:17:59Z","links":{"resolver":"https://pith.science/pith/LFEYPO4E42S3PUKXMHDKET2C65","bundle":"https://pith.science/pith/LFEYPO4E42S3PUKXMHDKET2C65/bundle.json","state":"https://pith.science/pith/LFEYPO4E42S3PUKXMHDKET2C65/state.json","well_known_bundle":"https://pith.science/.well-known/pith/LFEYPO4E42S3PUKXMHDKET2C65/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:1998:LFEYPO4E42S3PUKXMHDKET2C65","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":"5e0fb995cf7dd0f6488daa83af305401e5a043dd04dc53ddd641c6f33680759b","cross_cats_sorted":["cond-mat.stat-mech","math-ph","math.MP","math.PR"],"license":"","primary_cat":"cond-mat.dis-nn","submitted_at":"1998-09-28T16:49:31Z","title_canon_sha256":"9cdde62b0472d45ff5ba1735368736c01253a8d30694342178d4304354ab60c4"},"schema_version":"1.0","source":{"id":"cond-mat/9809375","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"cond-mat/9809375","created_at":"2026-05-18T01:39:29Z"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/9809375v1","created_at":"2026-05-18T01:39:29Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/9809375","created_at":"2026-05-18T01:39:29Z"},{"alias_kind":"pith_short_12","alias_value":"LFEYPO4E42S3","created_at":"2026-05-18T12:25:49Z"},{"alias_kind":"pith_short_16","alias_value":"LFEYPO4E42S3PUKX","created_at":"2026-05-18T12:25:49Z"},{"alias_kind":"pith_short_8","alias_value":"LFEYPO4E","created_at":"2026-05-18T12:25:49Z"}],"graph_snapshots":[{"event_id":"sha256:1599ec82026c865f9604bb9f4a4ce6441c77c9d5b5347db9bae80636eac74abb","target":"graph","created_at":"2026-05-18T01:39:29Z","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 consider nonequilibrium systems such as the Edwards-Anderson Ising spin glass at a temperature where, in equilibrium, there are presumed to be (two or many) broken symmetry pure states. Following a deep quench, we argue that as time goes to infinity, although the system is usually in some pure state locally, either it never settles permanently on a fixed lengthscale into a single pure state, or it does but then the pure state depends on both the initial spin configuration and the realization of the stochastic dynamics. But this latter case can occur only if there exists an uncountable numbe","authors_text":"C.M. Newman (Courant Institute of Mathematical Sciences, D.L. Stein (Departments of Physics, Mathematics, New York University), University of Arizona)","cross_cats":["cond-mat.stat-mech","math-ph","math.MP","math.PR"],"headline":"","license":"","primary_cat":"cond-mat.dis-nn","submitted_at":"1998-09-28T16:49:31Z","title":"Equilibrium Pure States and Nonequilibrium Chaos"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/9809375","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":"sha256:049653fa67db4b30e1dd62aebdba920e613fa5a53dc65820942190d9200af583","target":"record","created_at":"2026-05-18T01:39:29Z","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":"5e0fb995cf7dd0f6488daa83af305401e5a043dd04dc53ddd641c6f33680759b","cross_cats_sorted":["cond-mat.stat-mech","math-ph","math.MP","math.PR"],"license":"","primary_cat":"cond-mat.dis-nn","submitted_at":"1998-09-28T16:49:31Z","title_canon_sha256":"9cdde62b0472d45ff5ba1735368736c01253a8d30694342178d4304354ab60c4"},"schema_version":"1.0","source":{"id":"cond-mat/9809375","kind":"arxiv","version":1}},"canonical_sha256":"594987bb84e6a5b7d15761c6a24f42f74627bec5ba9e76b91d918b7feed435dc","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"594987bb84e6a5b7d15761c6a24f42f74627bec5ba9e76b91d918b7feed435dc","first_computed_at":"2026-05-18T01:39:29.908662Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:39:29.908662Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"SB3DmHtlgvMh+CRfSGNs1nUNdETaWylGAN4ftvg+Rc9/yGEIeL7uDusbxqmMC15smN+7p/bOYLI7hmGAZboIAg==","signature_status":"signed_v1","signed_at":"2026-05-18T01:39:29.909273Z","signed_message":"canonical_sha256_bytes"},"source_id":"cond-mat/9809375","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:049653fa67db4b30e1dd62aebdba920e613fa5a53dc65820942190d9200af583","sha256:1599ec82026c865f9604bb9f4a4ce6441c77c9d5b5347db9bae80636eac74abb"],"state_sha256":"f1aba067860b3975b6178884c6de912f0cbf24d3f3aad683b86f42bbd83ecb0a"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"xnMPk7hksPGsRsBn+ICF9iRDxzdyHYRYS8oS8bDYLNgDZMPPK76gQ3b48aLPTOBgy6ByRtCqlBQtu+1bKKhuCw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-05T15:17:59.134142Z","bundle_sha256":"faf70fbe6d822b2dc161e3be7df308b198f3d6cd60eaed8de5f45c3518ae3d2d"}}