{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2019:W5ABFXY55DWBKPY3536L7SSH67","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":"6be56d1355154154c36216f9ae3c94d585da88df52d37de30eb82c180404c830","cross_cats_sorted":["physics.soc-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nlin.AO","submitted_at":"2019-04-27T16:36:57Z","title_canon_sha256":"02cfe2d200f0154195d1388a61a2b4d63336d703fe244fa5e5dad04ca2f8f012"},"schema_version":"1.0","source":{"id":"1904.12174","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1904.12174","created_at":"2026-07-05T00:23:04Z"},{"alias_kind":"arxiv_version","alias_value":"1904.12174v2","created_at":"2026-07-05T00:23:04Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1904.12174","created_at":"2026-07-05T00:23:04Z"},{"alias_kind":"pith_short_12","alias_value":"W5ABFXY55DWB","created_at":"2026-07-05T00:23:04Z"},{"alias_kind":"pith_short_16","alias_value":"W5ABFXY55DWBKPY3","created_at":"2026-07-05T00:23:04Z"},{"alias_kind":"pith_short_8","alias_value":"W5ABFXY5","created_at":"2026-07-05T00:23:04Z"}],"graph_snapshots":[{"event_id":"sha256:503bf280dbb9dfb2a6a36f6559a92240bc9343bcb4647d491540d73452977999","target":"graph","created_at":"2026-07-05T00:23:04Z","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/1904.12174/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Many networks must maintain synchrony despite the fact that they operate in noisy environments. Important examples are stochastic inertial oscillators, which are known to exhibit fluctuations with broad tails in many applications, including electric power networks with renewable energy sources. Such non-Gaussian fluctuations can result in rare network desynchronization. Here we build a general theory for inertial oscillator network desynchronization by non-Gaussian noise. We compute the rate of desynchronization and show that higher-moments of noise enter at specific powers of coupling: either","authors_text":"Ira B. Schwartz, Jason Hindes, Philippe Jacquod","cross_cats":["physics.soc-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nlin.AO","submitted_at":"2019-04-27T16:36:57Z","title":"Network desynchronization by non-Gaussian fluctuations"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1904.12174","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:bf62ffc2bff9f2b886c8a24eeb1aaaff9dac69eddfbc4828a48e417dd93a5781","target":"record","created_at":"2026-07-05T00:23:04Z","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":"6be56d1355154154c36216f9ae3c94d585da88df52d37de30eb82c180404c830","cross_cats_sorted":["physics.soc-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nlin.AO","submitted_at":"2019-04-27T16:36:57Z","title_canon_sha256":"02cfe2d200f0154195d1388a61a2b4d63336d703fe244fa5e5dad04ca2f8f012"},"schema_version":"1.0","source":{"id":"1904.12174","kind":"arxiv","version":2}},"canonical_sha256":"b74012df1de8ec153f1beefcbfca47f7f0e3a0fa9648c00a4fc7e5d4647f5027","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"b74012df1de8ec153f1beefcbfca47f7f0e3a0fa9648c00a4fc7e5d4647f5027","first_computed_at":"2026-07-05T00:23:04.490794Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T00:23:04.490794Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"+IR1cgAblG0vBZZFdKU3JRSp99IbHzx1n9pXZ69CdG6cOokM7palBRl3K+K1y1gIh8BIGa0fJrs8T3ECAeGCCA==","signature_status":"signed_v1","signed_at":"2026-07-05T00:23:04.491260Z","signed_message":"canonical_sha256_bytes"},"source_id":"1904.12174","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:bf62ffc2bff9f2b886c8a24eeb1aaaff9dac69eddfbc4828a48e417dd93a5781","sha256:503bf280dbb9dfb2a6a36f6559a92240bc9343bcb4647d491540d73452977999"],"state_sha256":"35655a629bd7ba5f68aa416d41367ac948eb0f7b1cd1ab16f88729953d1c752f"}