{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2023:HJQ2CCOKIEK47R22CQP5SWCUP3","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":"997c9b301bb5e6524ce695d115de86aef590d46a9384a192e4272c1ae2260811","cross_cats_sorted":["cond-mat.stat-mech"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"math.PR","submitted_at":"2023-11-18T03:29:28Z","title_canon_sha256":"e88750dde2b432e3c9d557d42cc60efb00f2533a6b7eea03f8fa975abc3b2be9"},"schema_version":"1.0","source":{"id":"2311.10957","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2311.10957","created_at":"2026-07-05T08:30:48Z"},{"alias_kind":"arxiv_version","alias_value":"2311.10957v2","created_at":"2026-07-05T08:30:48Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2311.10957","created_at":"2026-07-05T08:30:48Z"},{"alias_kind":"pith_short_12","alias_value":"HJQ2CCOKIEK4","created_at":"2026-07-05T08:30:48Z"},{"alias_kind":"pith_short_16","alias_value":"HJQ2CCOKIEK47R22","created_at":"2026-07-05T08:30:48Z"},{"alias_kind":"pith_short_8","alias_value":"HJQ2CCOK","created_at":"2026-07-05T08:30:48Z"}],"graph_snapshots":[{"event_id":"sha256:cc9f3a3a14dca551fd8602f1cbf6c0fa78a5a4503034564a6fe7674a42879eb7","target":"graph","created_at":"2026-07-05T08:30:48Z","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/2311.10957/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"The global steady state of a system in thermal equilibrium exponentially favors configurations with lesser energy. This principle is a powerful explanation of self-organization because energy is a local property of a configuration. For nonequilibrium systems, there is no such property for which an analogous principle holds, hence no common explanation of the diverse forms of self-organization they exhibit. However, a flurry of recent work demonstrates that a local property of configurations called \"rattling\" predicts the global steady states of a broad class of nonequilibrium systems. We inter","authors_text":"Dana Randall, Jacob Calvert","cross_cats":["cond-mat.stat-mech"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"math.PR","submitted_at":"2023-11-18T03:29:28Z","title":"A local-global principle for nonequilibrium steady states"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2311.10957","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":"sha256:41bcf9e9969239af59083133a66b7271b91f2bc2fdeb48a282457c0b4f0a3269","target":"record","created_at":"2026-07-05T08:30:48Z","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":"997c9b301bb5e6524ce695d115de86aef590d46a9384a192e4272c1ae2260811","cross_cats_sorted":["cond-mat.stat-mech"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"math.PR","submitted_at":"2023-11-18T03:29:28Z","title_canon_sha256":"e88750dde2b432e3c9d557d42cc60efb00f2533a6b7eea03f8fa975abc3b2be9"},"schema_version":"1.0","source":{"id":"2311.10957","kind":"arxiv","version":2}},"canonical_sha256":"3a61a109ca4115cfc75a141fd958547eec74cafbb253f195a0d6de1a210debc1","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"3a61a109ca4115cfc75a141fd958547eec74cafbb253f195a0d6de1a210debc1","first_computed_at":"2026-07-05T08:30:48.899003Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T08:30:48.899003Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"3EF+zy8SAcrWRpAVzyBWqDHH+kbd2gEwnfi0uGZGvjIbCRPFONekRYWIuei4Su9bvkzD148BjjplHe/tniW6Bg==","signature_status":"signed_v1","signed_at":"2026-07-05T08:30:48.899512Z","signed_message":"canonical_sha256_bytes"},"source_id":"2311.10957","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:41bcf9e9969239af59083133a66b7271b91f2bc2fdeb48a282457c0b4f0a3269","sha256:cc9f3a3a14dca551fd8602f1cbf6c0fa78a5a4503034564a6fe7674a42879eb7"],"state_sha256":"eeb754c7d5ec795572c69fb8892622c673a72ccbe4792e3d1e78769a7e8987d7"}