{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:RUBJGQOLCLVXJXB6UHM7FWNUHO","short_pith_number":"pith:RUBJGQOL","canonical_record":{"source":{"id":"1607.03696","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2016-07-13T12:27:15Z","cross_cats_sorted":[],"title_canon_sha256":"fc9f44f7358007d442df7dc436256da854eb869cf4684c72b600f0b3f40c30c0","abstract_canon_sha256":"5a005e1d4b452235726176aadb6c31d6a989839e35650863b6a119e862e1ff15"},"schema_version":"1.0"},"canonical_sha256":"8d029341cb12eb74dc3ea1d9f2d9b43ba84cae40a577bbcdfd7bf7d94b569ddd","source":{"kind":"arxiv","id":"1607.03696","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1607.03696","created_at":"2026-05-18T00:39:02Z"},{"alias_kind":"arxiv_version","alias_value":"1607.03696v1","created_at":"2026-05-18T00:39:02Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1607.03696","created_at":"2026-05-18T00:39:02Z"},{"alias_kind":"pith_short_12","alias_value":"RUBJGQOLCLVX","created_at":"2026-05-18T12:30:41Z"},{"alias_kind":"pith_short_16","alias_value":"RUBJGQOLCLVXJXB6","created_at":"2026-05-18T12:30:41Z"},{"alias_kind":"pith_short_8","alias_value":"RUBJGQOL","created_at":"2026-05-18T12:30:41Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:RUBJGQOLCLVXJXB6UHM7FWNUHO","target":"record","payload":{"canonical_record":{"source":{"id":"1607.03696","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2016-07-13T12:27:15Z","cross_cats_sorted":[],"title_canon_sha256":"fc9f44f7358007d442df7dc436256da854eb869cf4684c72b600f0b3f40c30c0","abstract_canon_sha256":"5a005e1d4b452235726176aadb6c31d6a989839e35650863b6a119e862e1ff15"},"schema_version":"1.0"},"canonical_sha256":"8d029341cb12eb74dc3ea1d9f2d9b43ba84cae40a577bbcdfd7bf7d94b569ddd","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:39:02.539230Z","signature_b64":"slN3AhJPEx9ewx9hN1mh8WxYG+VWrHKj1cVuVT7nrXWWn4SdJ69lZIkLq+DZWIdqlEXpnJDULsSEuiqe/VsnBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8d029341cb12eb74dc3ea1d9f2d9b43ba84cae40a577bbcdfd7bf7d94b569ddd","last_reissued_at":"2026-05-18T00:39:02.538664Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:39:02.538664Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1607.03696","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":"2026-05-18T00:39:02Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"sfg/haX4O6EylcTIO5Wu03ecO0GvFYH65frT7B/rnDUd539gKVHt7lXsmmfqmR3cgZKqXcsPD1jWSOKBqyF5AQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-24T19:11:46.705088Z"},"content_sha256":"79df49f090e0becfdb5ea13097d65b1eda8af367d3a71195d7b55f3d9897add8","schema_version":"1.0","event_id":"sha256:79df49f090e0becfdb5ea13097d65b1eda8af367d3a71195d7b55f3d9897add8"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:RUBJGQOLCLVXJXB6UHM7FWNUHO","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"From Kardar-Parisi-Zhang scaling to explosive desynchronization in arrays of limit-cycle oscillators","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.stat-mech","authors_text":"Aditi Mitra, Florian Marquardt, Roland Lauter","submitted_at":"2016-07-13T12:27:15Z","abstract_excerpt":"We study the synchronization physics of 1D and 2D oscillator lattices subject to noise and predict a dynamical transition that leads to a sudden drastic increase of phase diffusion. Our analysis is based on the widely applicable Kuramoto-Sakaguchi model, with local couplings between oscillators. For smooth phase fields, the time evolution can initially be described by a surface growth model, the Kardar-Parisi-Zhang (KPZ) theory. We delineate the regime in which one can indeed observe the universal KPZ scaling in 1D lattices. For larger couplings, both in 1D and 2D, we observe a stochastic dyna"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1607.03696","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":"2026-05-18T00:39:02Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"+PRCiEERkDj7MAvvF6bv51Zv7KPE0dlDINp/SRH5IP3kh3PcQ0zG12Jgolp2WTD/Ov9mhTQ0kE5LrrmE+Uy7AA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-24T19:11:46.705440Z"},"content_sha256":"dfbafd032f795e15e87b497dd9f0ad742c886df8f2a905e8b40533e539e6e601","schema_version":"1.0","event_id":"sha256:dfbafd032f795e15e87b497dd9f0ad742c886df8f2a905e8b40533e539e6e601"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/RUBJGQOLCLVXJXB6UHM7FWNUHO/bundle.json","state_url":"https://pith.science/pith/RUBJGQOLCLVXJXB6UHM7FWNUHO/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/RUBJGQOLCLVXJXB6UHM7FWNUHO/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":"2026-06-24T19:11:46Z","links":{"resolver":"https://pith.science/pith/RUBJGQOLCLVXJXB6UHM7FWNUHO","bundle":"https://pith.science/pith/RUBJGQOLCLVXJXB6UHM7FWNUHO/bundle.json","state":"https://pith.science/pith/RUBJGQOLCLVXJXB6UHM7FWNUHO/state.json","well_known_bundle":"https://pith.science/.well-known/pith/RUBJGQOLCLVXJXB6UHM7FWNUHO/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:RUBJGQOLCLVXJXB6UHM7FWNUHO","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":"5a005e1d4b452235726176aadb6c31d6a989839e35650863b6a119e862e1ff15","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2016-07-13T12:27:15Z","title_canon_sha256":"fc9f44f7358007d442df7dc436256da854eb869cf4684c72b600f0b3f40c30c0"},"schema_version":"1.0","source":{"id":"1607.03696","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1607.03696","created_at":"2026-05-18T00:39:02Z"},{"alias_kind":"arxiv_version","alias_value":"1607.03696v1","created_at":"2026-05-18T00:39:02Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1607.03696","created_at":"2026-05-18T00:39:02Z"},{"alias_kind":"pith_short_12","alias_value":"RUBJGQOLCLVX","created_at":"2026-05-18T12:30:41Z"},{"alias_kind":"pith_short_16","alias_value":"RUBJGQOLCLVXJXB6","created_at":"2026-05-18T12:30:41Z"},{"alias_kind":"pith_short_8","alias_value":"RUBJGQOL","created_at":"2026-05-18T12:30:41Z"}],"graph_snapshots":[{"event_id":"sha256:dfbafd032f795e15e87b497dd9f0ad742c886df8f2a905e8b40533e539e6e601","target":"graph","created_at":"2026-05-18T00:39:02Z","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 study the synchronization physics of 1D and 2D oscillator lattices subject to noise and predict a dynamical transition that leads to a sudden drastic increase of phase diffusion. Our analysis is based on the widely applicable Kuramoto-Sakaguchi model, with local couplings between oscillators. For smooth phase fields, the time evolution can initially be described by a surface growth model, the Kardar-Parisi-Zhang (KPZ) theory. We delineate the regime in which one can indeed observe the universal KPZ scaling in 1D lattices. For larger couplings, both in 1D and 2D, we observe a stochastic dyna","authors_text":"Aditi Mitra, Florian Marquardt, Roland Lauter","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2016-07-13T12:27:15Z","title":"From Kardar-Parisi-Zhang scaling to explosive desynchronization in arrays of limit-cycle oscillators"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1607.03696","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":"sha256:79df49f090e0becfdb5ea13097d65b1eda8af367d3a71195d7b55f3d9897add8","target":"record","created_at":"2026-05-18T00:39:02Z","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":"5a005e1d4b452235726176aadb6c31d6a989839e35650863b6a119e862e1ff15","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2016-07-13T12:27:15Z","title_canon_sha256":"fc9f44f7358007d442df7dc436256da854eb869cf4684c72b600f0b3f40c30c0"},"schema_version":"1.0","source":{"id":"1607.03696","kind":"arxiv","version":1}},"canonical_sha256":"8d029341cb12eb74dc3ea1d9f2d9b43ba84cae40a577bbcdfd7bf7d94b569ddd","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"8d029341cb12eb74dc3ea1d9f2d9b43ba84cae40a577bbcdfd7bf7d94b569ddd","first_computed_at":"2026-05-18T00:39:02.538664Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:39:02.538664Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"slN3AhJPEx9ewx9hN1mh8WxYG+VWrHKj1cVuVT7nrXWWn4SdJ69lZIkLq+DZWIdqlEXpnJDULsSEuiqe/VsnBg==","signature_status":"signed_v1","signed_at":"2026-05-18T00:39:02.539230Z","signed_message":"canonical_sha256_bytes"},"source_id":"1607.03696","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:79df49f090e0becfdb5ea13097d65b1eda8af367d3a71195d7b55f3d9897add8","sha256:dfbafd032f795e15e87b497dd9f0ad742c886df8f2a905e8b40533e539e6e601"],"state_sha256":"38a0c4cef99ce817487ac90861700882025c234f652d13e6a8b3bc611289a54f"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ltsPQ0wuHoYR4CKnzqbKEe033X6/4T2e64lGdKGV2wfUF/lBr9q3amQwcPKUSJt2D9zVJJPpY0J6CUDUnn3DAQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-24T19:11:46.707409Z","bundle_sha256":"d348dcaefcc5aae877c6f165c3477c1a669e8c45bf7209ce4691755b48b80f4c"}}