{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2022:RB673L33QXYXAL6HNDVVLO7CEZ","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":"e98485874154d3fd00d10c782309b0ff43a662a8b0ed2b72170bfd3da24e8273","cross_cats_sorted":["physics.class-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nlin.CD","submitted_at":"2022-06-01T01:27:12Z","title_canon_sha256":"5905649eed31f89097d8fc394ff9b7093ebed4e72dfba63fb231bfc02cd49813"},"schema_version":"1.0","source":{"id":"2206.01089","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2206.01089","created_at":"2026-07-05T05:22:48Z"},{"alias_kind":"arxiv_version","alias_value":"2206.01089v1","created_at":"2026-07-05T05:22:48Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2206.01089","created_at":"2026-07-05T05:22:48Z"},{"alias_kind":"pith_short_12","alias_value":"RB673L33QXYX","created_at":"2026-07-05T05:22:48Z"},{"alias_kind":"pith_short_16","alias_value":"RB673L33QXYXAL6H","created_at":"2026-07-05T05:22:48Z"},{"alias_kind":"pith_short_8","alias_value":"RB673L33","created_at":"2026-07-05T05:22:48Z"}],"graph_snapshots":[{"event_id":"sha256:29de4dd1b4f28cf397fcaa34d17ba48d41874736cdce6b1963261b75991aa495","target":"graph","created_at":"2026-07-05T05:22:48Z","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/2206.01089/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Many nonlinear systems are described by eigenmodes with amplitude-dependent frequencies, interacting strongly whenever the frequencies become commensurate at internal resonances. Fast energy exchange via the resonances holds the key to rich dynamical behavior, such as time-varying relaxation rates and signatures of nonergodicity in thermal equilibrium, revealed in the recent experimental and theoretical studies of micro and nanomechanical resonators. However, a universal yet intuitive physical description for these diverse and sometimes contradictory experimental observations remains elusive. ","authors_text":"Daniel Lopez, Diego J. Perez-Morelo, Mingkang Wang, Vladimir A. Aksyuk","cross_cats":["physics.class-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nlin.CD","submitted_at":"2022-06-01T01:27:12Z","title":"Persistent nonlinear phase-locking and non-monotonic energy dissipation in micromechanical resonators"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2206.01089","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":"sha256:4ebe8466595ee360cbb47feacb1dd9772435b13388c07b9a705331c882dd7d50","target":"record","created_at":"2026-07-05T05:22:48Z","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":"e98485874154d3fd00d10c782309b0ff43a662a8b0ed2b72170bfd3da24e8273","cross_cats_sorted":["physics.class-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nlin.CD","submitted_at":"2022-06-01T01:27:12Z","title_canon_sha256":"5905649eed31f89097d8fc394ff9b7093ebed4e72dfba63fb231bfc02cd49813"},"schema_version":"1.0","source":{"id":"2206.01089","kind":"arxiv","version":1}},"canonical_sha256":"887dfdaf7b85f1702fc768eb55bbe22660adf036697eb12f50e8550d1faaeb62","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"887dfdaf7b85f1702fc768eb55bbe22660adf036697eb12f50e8550d1faaeb62","first_computed_at":"2026-07-05T05:22:48.004681Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T05:22:48.004681Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"xIR362ghQ9N6UuHQHBEdIbg1Bmz8wdu7iyLd/Btu7WZNIknc4yJET/5f6unefPvdV2t+JJwN5pMeTMvdEXp5Dg==","signature_status":"signed_v1","signed_at":"2026-07-05T05:22:48.005106Z","signed_message":"canonical_sha256_bytes"},"source_id":"2206.01089","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:4ebe8466595ee360cbb47feacb1dd9772435b13388c07b9a705331c882dd7d50","sha256:29de4dd1b4f28cf397fcaa34d17ba48d41874736cdce6b1963261b75991aa495"],"state_sha256":"7ac9c47f3f3ee631359e85f097b26e129fc6f6f1943838e35a5e6bb86f2d5e17"}