{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:MB27ETJEGMTVERCC2VUDVRGFUP","short_pith_number":"pith:MB27ETJE","canonical_record":{"source":{"id":"1401.0930","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2014-01-05T19:19:14Z","cross_cats_sorted":[],"title_canon_sha256":"4881377a7f5060b2d4a73e5e584f55bd8dd9d7f018d685e03c48380a6989bdc9","abstract_canon_sha256":"fa21cbba1eec1937fd459709584ad8b2e4e7b410100f187e6336bcb326519d96"},"schema_version":"1.0"},"canonical_sha256":"6075f24d243327524442d5683ac4c5a3d240b155432eaea3a60fa09110ef79c4","source":{"kind":"arxiv","id":"1401.0930","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1401.0930","created_at":"2026-05-18T03:03:11Z"},{"alias_kind":"arxiv_version","alias_value":"1401.0930v1","created_at":"2026-05-18T03:03:11Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1401.0930","created_at":"2026-05-18T03:03:11Z"},{"alias_kind":"pith_short_12","alias_value":"MB27ETJEGMTV","created_at":"2026-05-18T12:28:38Z"},{"alias_kind":"pith_short_16","alias_value":"MB27ETJEGMTVERCC","created_at":"2026-05-18T12:28:38Z"},{"alias_kind":"pith_short_8","alias_value":"MB27ETJE","created_at":"2026-05-18T12:28:38Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:MB27ETJEGMTVERCC2VUDVRGFUP","target":"record","payload":{"canonical_record":{"source":{"id":"1401.0930","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2014-01-05T19:19:14Z","cross_cats_sorted":[],"title_canon_sha256":"4881377a7f5060b2d4a73e5e584f55bd8dd9d7f018d685e03c48380a6989bdc9","abstract_canon_sha256":"fa21cbba1eec1937fd459709584ad8b2e4e7b410100f187e6336bcb326519d96"},"schema_version":"1.0"},"canonical_sha256":"6075f24d243327524442d5683ac4c5a3d240b155432eaea3a60fa09110ef79c4","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:03:11.503305Z","signature_b64":"66q5fYYAKNLkgmhRK1HRJ9iRPlfaQY6r51/sj9Lad7AXlmOe6dkx+h+eOaXi9OoQYt3j4PpQs9GR/+F7TZBODA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6075f24d243327524442d5683ac4c5a3d240b155432eaea3a60fa09110ef79c4","last_reissued_at":"2026-05-18T03:03:11.502686Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:03:11.502686Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1401.0930","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":"2026-05-18T03:03:11Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"dcK3r9lUFXherlood6ANRdnX6AsvAI4Q7eNHe/iyV7JvJHhlIkIJyMe4VF8oeEKvszITge4/Y1DunizsrkBiCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T22:32:01.911978Z"},"content_sha256":"f84e0f27bf581267f05166cee2b06ccb3f61f296dc225a6e1268f71c17632a7a","schema_version":"1.0","event_id":"sha256:f84e0f27bf581267f05166cee2b06ccb3f61f296dc225a6e1268f71c17632a7a"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:MB27ETJEGMTVERCC2VUDVRGFUP","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"On phase-locking of Kerr combs","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.optics","authors_text":"Aur\\'elien Coillet, Yanne K. Chembo","submitted_at":"2014-01-05T19:19:14Z","abstract_excerpt":"We theoretically investigate the phase-locking phenomena between the spectral components of Kerr optical frequency combs in the dynamical regime of Turing patterns. We show that these Turing patterns display a particularly strong and robust phase-locking, originating from a cascade of phase-locked triplets which asymptotically lead to a global phase-locking between the modes. The local and global phase-locking relationship defining the shape of the optical pulses are analytically determined. Our analysis also shows that solitons display a much weaker phase-locking which can be destroyed more e"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1401.0930","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":"2026-05-18T03:03:11Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"X34N5dX4LD7nM+WIruZxDKcm8NSVZdgSe5xNM8Ug2WQ9jcIMKG0SHcJi53prtoTe8WNhcWJcYZRocc5N1pySAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T22:32:01.912343Z"},"content_sha256":"14bc5c8808e61cd2907834272968628a8770ee783b802c2e87c920035ebd99eb","schema_version":"1.0","event_id":"sha256:14bc5c8808e61cd2907834272968628a8770ee783b802c2e87c920035ebd99eb"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/MB27ETJEGMTVERCC2VUDVRGFUP/bundle.json","state_url":"https://pith.science/pith/MB27ETJEGMTVERCC2VUDVRGFUP/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/MB27ETJEGMTVERCC2VUDVRGFUP/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":"2026-05-26T22:32:01Z","links":{"resolver":"https://pith.science/pith/MB27ETJEGMTVERCC2VUDVRGFUP","bundle":"https://pith.science/pith/MB27ETJEGMTVERCC2VUDVRGFUP/bundle.json","state":"https://pith.science/pith/MB27ETJEGMTVERCC2VUDVRGFUP/state.json","well_known_bundle":"https://pith.science/.well-known/pith/MB27ETJEGMTVERCC2VUDVRGFUP/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:MB27ETJEGMTVERCC2VUDVRGFUP","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":"fa21cbba1eec1937fd459709584ad8b2e4e7b410100f187e6336bcb326519d96","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2014-01-05T19:19:14Z","title_canon_sha256":"4881377a7f5060b2d4a73e5e584f55bd8dd9d7f018d685e03c48380a6989bdc9"},"schema_version":"1.0","source":{"id":"1401.0930","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1401.0930","created_at":"2026-05-18T03:03:11Z"},{"alias_kind":"arxiv_version","alias_value":"1401.0930v1","created_at":"2026-05-18T03:03:11Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1401.0930","created_at":"2026-05-18T03:03:11Z"},{"alias_kind":"pith_short_12","alias_value":"MB27ETJEGMTV","created_at":"2026-05-18T12:28:38Z"},{"alias_kind":"pith_short_16","alias_value":"MB27ETJEGMTVERCC","created_at":"2026-05-18T12:28:38Z"},{"alias_kind":"pith_short_8","alias_value":"MB27ETJE","created_at":"2026-05-18T12:28:38Z"}],"graph_snapshots":[{"event_id":"sha256:14bc5c8808e61cd2907834272968628a8770ee783b802c2e87c920035ebd99eb","target":"graph","created_at":"2026-05-18T03:03:11Z","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 theoretically investigate the phase-locking phenomena between the spectral components of Kerr optical frequency combs in the dynamical regime of Turing patterns. We show that these Turing patterns display a particularly strong and robust phase-locking, originating from a cascade of phase-locked triplets which asymptotically lead to a global phase-locking between the modes. The local and global phase-locking relationship defining the shape of the optical pulses are analytically determined. Our analysis also shows that solitons display a much weaker phase-locking which can be destroyed more e","authors_text":"Aur\\'elien Coillet, Yanne K. Chembo","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2014-01-05T19:19:14Z","title":"On phase-locking of Kerr combs"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1401.0930","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:f84e0f27bf581267f05166cee2b06ccb3f61f296dc225a6e1268f71c17632a7a","target":"record","created_at":"2026-05-18T03:03:11Z","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":"fa21cbba1eec1937fd459709584ad8b2e4e7b410100f187e6336bcb326519d96","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2014-01-05T19:19:14Z","title_canon_sha256":"4881377a7f5060b2d4a73e5e584f55bd8dd9d7f018d685e03c48380a6989bdc9"},"schema_version":"1.0","source":{"id":"1401.0930","kind":"arxiv","version":1}},"canonical_sha256":"6075f24d243327524442d5683ac4c5a3d240b155432eaea3a60fa09110ef79c4","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"6075f24d243327524442d5683ac4c5a3d240b155432eaea3a60fa09110ef79c4","first_computed_at":"2026-05-18T03:03:11.502686Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:03:11.502686Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"66q5fYYAKNLkgmhRK1HRJ9iRPlfaQY6r51/sj9Lad7AXlmOe6dkx+h+eOaXi9OoQYt3j4PpQs9GR/+F7TZBODA==","signature_status":"signed_v1","signed_at":"2026-05-18T03:03:11.503305Z","signed_message":"canonical_sha256_bytes"},"source_id":"1401.0930","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:f84e0f27bf581267f05166cee2b06ccb3f61f296dc225a6e1268f71c17632a7a","sha256:14bc5c8808e61cd2907834272968628a8770ee783b802c2e87c920035ebd99eb"],"state_sha256":"164538d808afa4bbf84acd3dd272c370cf4465656a8344bd16e822868fb5cf0c"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"93RWJXbNPDI13cL4rxk55LlZ+3Mm36l8b8H9FhqHI9BPO29fCHXOq8tRPRT1EmRNQ4ts0mB/RUc2m1HcJhVsBA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-26T22:32:01.915679Z","bundle_sha256":"70c2c6a4e6f39aab888676f27a17b31cda4fb2f274723c3acdd7a70b923c589c"}}