{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:LLLGTUYWXEGRD3L34IAYDPDSEX","short_pith_number":"pith:LLLGTUYW","canonical_record":{"source":{"id":"1409.5943","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2014-09-21T06:02:13Z","cross_cats_sorted":["nlin.PS"],"title_canon_sha256":"b8b68e49c9c2ef146294b740beb0cc6d02609c6efac1d3f40cc1744bbf10620a","abstract_canon_sha256":"ab5c54cfaf9c519c7df3c7253d4ea355177377bec98ab37cfa37bda56c75b284"},"schema_version":"1.0"},"canonical_sha256":"5ad669d316b90d11ed7be20181bc7225ed7bd12af931bc1e54f8f7638ef59229","source":{"kind":"arxiv","id":"1409.5943","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1409.5943","created_at":"2026-05-18T02:41:16Z"},{"alias_kind":"arxiv_version","alias_value":"1409.5943v3","created_at":"2026-05-18T02:41:16Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1409.5943","created_at":"2026-05-18T02:41:16Z"},{"alias_kind":"pith_short_12","alias_value":"LLLGTUYWXEGR","created_at":"2026-05-18T12:28:38Z"},{"alias_kind":"pith_short_16","alias_value":"LLLGTUYWXEGRD3L3","created_at":"2026-05-18T12:28:38Z"},{"alias_kind":"pith_short_8","alias_value":"LLLGTUYW","created_at":"2026-05-18T12:28:38Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:LLLGTUYWXEGRD3L34IAYDPDSEX","target":"record","payload":{"canonical_record":{"source":{"id":"1409.5943","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2014-09-21T06:02:13Z","cross_cats_sorted":["nlin.PS"],"title_canon_sha256":"b8b68e49c9c2ef146294b740beb0cc6d02609c6efac1d3f40cc1744bbf10620a","abstract_canon_sha256":"ab5c54cfaf9c519c7df3c7253d4ea355177377bec98ab37cfa37bda56c75b284"},"schema_version":"1.0"},"canonical_sha256":"5ad669d316b90d11ed7be20181bc7225ed7bd12af931bc1e54f8f7638ef59229","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:41:16.638664Z","signature_b64":"KlTgJUAbrz6276efivMOLw8TGvnLm/+II9d+MeUOFlB2tKzLONfFCSlp1RFS0BFyAyb46DvQtLnb/SL0vbFtAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5ad669d316b90d11ed7be20181bc7225ed7bd12af931bc1e54f8f7638ef59229","last_reissued_at":"2026-05-18T02:41:16.638113Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:41:16.638113Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1409.5943","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:41:16Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"e0jN2r8DfQdktrHInvJ6oXw9K65iWZx9wB0nuQWHCkfbCb8ypeoiptrl9GD0sPdvsVWhdPxcHq6fRv2t9RhzAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T19:25:12.233888Z"},"content_sha256":"b7f36a424c905ddcd460d1980157b84ad3867bd8e4f1f01551fb147b93a7ed39","schema_version":"1.0","event_id":"sha256:b7f36a424c905ddcd460d1980157b84ad3867bd8e4f1f01551fb147b93a7ed39"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:LLLGTUYWXEGRD3L34IAYDPDSEX","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Soliton Formation in Whispering-Gallery-Mode Resonators via Input Phase Modulation","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nlin.PS"],"primary_cat":"physics.optics","authors_text":"Ali Adibi, Ali A. Eftekhar, Hossein Taheri, Kurt Wiesenfeld","submitted_at":"2014-09-21T06:02:13Z","abstract_excerpt":"We propose a method for soliton formation in whispering-gallery-mode (WGM) resonators through input phase modulation. Our numerical simulations of a variant of the Lugiato-Lefever equation suggest that modulating the input phase at a frequency equal to the resonator free-spectral-range and at modest modulation depths provides a deterministic route towards soliton formation in WGM resonators without undergoing a chaotic phase. We show that the generated solitonic state is sustained when the modulation is turned off adiabatically. Our results support parametric seeding as a powerful means of con"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1409.5943","kind":"arxiv","version":3},"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":"2026-05-18T02:41:16Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"zPci0wGBmN5cHrUiK29W0wYTTBLnZ7SPgkgylLZ1bdmX1E+uj1iLQHrdPBuOPr0LO37q3Lc/9zxGMpim3tOvBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T19:25:12.234581Z"},"content_sha256":"d091f90268c880012d9674ad97ec94a7046339e5b3235a859a3fb688d8871952","schema_version":"1.0","event_id":"sha256:d091f90268c880012d9674ad97ec94a7046339e5b3235a859a3fb688d8871952"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/LLLGTUYWXEGRD3L34IAYDPDSEX/bundle.json","state_url":"https://pith.science/pith/LLLGTUYWXEGRD3L34IAYDPDSEX/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/LLLGTUYWXEGRD3L34IAYDPDSEX/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":"2026-05-27T19:25:12Z","links":{"resolver":"https://pith.science/pith/LLLGTUYWXEGRD3L34IAYDPDSEX","bundle":"https://pith.science/pith/LLLGTUYWXEGRD3L34IAYDPDSEX/bundle.json","state":"https://pith.science/pith/LLLGTUYWXEGRD3L34IAYDPDSEX/state.json","well_known_bundle":"https://pith.science/.well-known/pith/LLLGTUYWXEGRD3L34IAYDPDSEX/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:LLLGTUYWXEGRD3L34IAYDPDSEX","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":"ab5c54cfaf9c519c7df3c7253d4ea355177377bec98ab37cfa37bda56c75b284","cross_cats_sorted":["nlin.PS"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2014-09-21T06:02:13Z","title_canon_sha256":"b8b68e49c9c2ef146294b740beb0cc6d02609c6efac1d3f40cc1744bbf10620a"},"schema_version":"1.0","source":{"id":"1409.5943","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1409.5943","created_at":"2026-05-18T02:41:16Z"},{"alias_kind":"arxiv_version","alias_value":"1409.5943v3","created_at":"2026-05-18T02:41:16Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1409.5943","created_at":"2026-05-18T02:41:16Z"},{"alias_kind":"pith_short_12","alias_value":"LLLGTUYWXEGR","created_at":"2026-05-18T12:28:38Z"},{"alias_kind":"pith_short_16","alias_value":"LLLGTUYWXEGRD3L3","created_at":"2026-05-18T12:28:38Z"},{"alias_kind":"pith_short_8","alias_value":"LLLGTUYW","created_at":"2026-05-18T12:28:38Z"}],"graph_snapshots":[{"event_id":"sha256:d091f90268c880012d9674ad97ec94a7046339e5b3235a859a3fb688d8871952","target":"graph","created_at":"2026-05-18T02:41:16Z","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 propose a method for soliton formation in whispering-gallery-mode (WGM) resonators through input phase modulation. Our numerical simulations of a variant of the Lugiato-Lefever equation suggest that modulating the input phase at a frequency equal to the resonator free-spectral-range and at modest modulation depths provides a deterministic route towards soliton formation in WGM resonators without undergoing a chaotic phase. We show that the generated solitonic state is sustained when the modulation is turned off adiabatically. Our results support parametric seeding as a powerful means of con","authors_text":"Ali Adibi, Ali A. Eftekhar, Hossein Taheri, Kurt Wiesenfeld","cross_cats":["nlin.PS"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2014-09-21T06:02:13Z","title":"Soliton Formation in Whispering-Gallery-Mode Resonators via Input Phase Modulation"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1409.5943","kind":"arxiv","version":3},"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:b7f36a424c905ddcd460d1980157b84ad3867bd8e4f1f01551fb147b93a7ed39","target":"record","created_at":"2026-05-18T02:41:16Z","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":"ab5c54cfaf9c519c7df3c7253d4ea355177377bec98ab37cfa37bda56c75b284","cross_cats_sorted":["nlin.PS"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2014-09-21T06:02:13Z","title_canon_sha256":"b8b68e49c9c2ef146294b740beb0cc6d02609c6efac1d3f40cc1744bbf10620a"},"schema_version":"1.0","source":{"id":"1409.5943","kind":"arxiv","version":3}},"canonical_sha256":"5ad669d316b90d11ed7be20181bc7225ed7bd12af931bc1e54f8f7638ef59229","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"5ad669d316b90d11ed7be20181bc7225ed7bd12af931bc1e54f8f7638ef59229","first_computed_at":"2026-05-18T02:41:16.638113Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:41:16.638113Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"KlTgJUAbrz6276efivMOLw8TGvnLm/+II9d+MeUOFlB2tKzLONfFCSlp1RFS0BFyAyb46DvQtLnb/SL0vbFtAw==","signature_status":"signed_v1","signed_at":"2026-05-18T02:41:16.638664Z","signed_message":"canonical_sha256_bytes"},"source_id":"1409.5943","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:b7f36a424c905ddcd460d1980157b84ad3867bd8e4f1f01551fb147b93a7ed39","sha256:d091f90268c880012d9674ad97ec94a7046339e5b3235a859a3fb688d8871952"],"state_sha256":"f989b6514d5cdf40df1d474969b69b5eae099c0be35c2bbd58cad9840afcaedd"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ywcu39Bko0UYqndpJaTLdZJYjDO95WK3O6KL2UHv8UOoaYeJcRA9VG5J3jjKM/8UC05qGf/LkxEaua5vB0mwCQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-27T19:25:12.237583Z","bundle_sha256":"ed63c21e94d13791ec292be76e63b9c4b7dedc745934e09160722ea2b08a08af"}}