{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2022:VIBAK5ZHSG6RA5XSN75YH56VZT","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":"a7984992b633716631c2b7d6dce70adf1d77686a83cf33525eae65a5d20c8ebe","cross_cats_sorted":["physics.soc-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nlin.AO","submitted_at":"2022-08-22T12:22:40Z","title_canon_sha256":"24143f3a6dafa015c40fa1660bba3fe01d896ad251fcdf2c95391fc14d807d3c"},"schema_version":"1.0","source":{"id":"2208.10237","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2208.10237","created_at":"2026-07-05T05:37:07Z"},{"alias_kind":"arxiv_version","alias_value":"2208.10237v2","created_at":"2026-07-05T05:37:07Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2208.10237","created_at":"2026-07-05T05:37:07Z"},{"alias_kind":"pith_short_12","alias_value":"VIBAK5ZHSG6R","created_at":"2026-07-05T05:37:07Z"},{"alias_kind":"pith_short_16","alias_value":"VIBAK5ZHSG6RA5XS","created_at":"2026-07-05T05:37:07Z"},{"alias_kind":"pith_short_8","alias_value":"VIBAK5ZH","created_at":"2026-07-05T05:37:07Z"}],"graph_snapshots":[{"event_id":"sha256:da79533b9104c4d7e6e5deca9a173819b5981fa431c32074a678c2368578c9c7","target":"graph","created_at":"2026-07-05T05:37:07Z","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/2208.10237/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Complex networks often possess communities defined based on network connectivity. When dynamics undergo in a network, one can also consider dynamical communities; i.e., a group of nodes displaying a similar dynamical process. We have investigated both analytically and numerically the development of dynamical community structure, where the community is referred to as a group of nodes synchronized in frequency, in networks of phase oscillators. We first demonstrate that using a few example networks, the community structure changes when network connectivity or interaction strength is varied. In p","authors_text":"Hiroshi Kori, Masaki Kato","cross_cats":["physics.soc-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nlin.AO","submitted_at":"2022-08-22T12:22:40Z","title":"Partial synchronization and community switching in phase-oscillator networks and its analysis based on a bidirectional, weighted chain of three oscillators"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2208.10237","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":"sha256:41800133fbe2511956d2f2506c1084c45a7effee3887fe344c123f6869c600cf","target":"record","created_at":"2026-07-05T05:37:07Z","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":"a7984992b633716631c2b7d6dce70adf1d77686a83cf33525eae65a5d20c8ebe","cross_cats_sorted":["physics.soc-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nlin.AO","submitted_at":"2022-08-22T12:22:40Z","title_canon_sha256":"24143f3a6dafa015c40fa1660bba3fe01d896ad251fcdf2c95391fc14d807d3c"},"schema_version":"1.0","source":{"id":"2208.10237","kind":"arxiv","version":2}},"canonical_sha256":"aa0205772791bd1076f26ffb83f7d5ccf58e3f10d89fac4dd2e973fe65f229c0","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"aa0205772791bd1076f26ffb83f7d5ccf58e3f10d89fac4dd2e973fe65f229c0","first_computed_at":"2026-07-05T05:37:07.502870Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T05:37:07.502870Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"9aQgVCR7Jrw6QYgQlrZLbespj6gLCpuvXlEm+9K5QvtS1SPo6THJvJU8ch684n45RsEeDe84fcd4lihuyzy5Bg==","signature_status":"signed_v1","signed_at":"2026-07-05T05:37:07.503405Z","signed_message":"canonical_sha256_bytes"},"source_id":"2208.10237","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:41800133fbe2511956d2f2506c1084c45a7effee3887fe344c123f6869c600cf","sha256:da79533b9104c4d7e6e5deca9a173819b5981fa431c32074a678c2368578c9c7"],"state_sha256":"52a0de2949c436632079ac1afc792ae2c5094064fa68b63437500257af8eeb07"}