{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2026:2YEWU4WT2VKQ2V4BX7FGDPUULL","short_pith_number":"pith:2YEWU4WT","canonical_record":{"source":{"id":"2605.29321","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2026-05-28T03:50:50Z","cross_cats_sorted":["quant-ph"],"title_canon_sha256":"d2e2d6b51a655cdcf7b34b007842936db9ae5f2a61f17b37720d3f19e02af0d4","abstract_canon_sha256":"7420184fae672162a304137dc2475d63099a82ced5b76f1851239e53bee816df"},"schema_version":"1.0"},"canonical_sha256":"d6096a72d3d5550d5781bfca61be945ac343b8687df45644e8dd80137eeed5e7","source":{"kind":"arxiv","id":"2605.29321","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2605.29321","created_at":"2026-05-29T01:05:32Z"},{"alias_kind":"arxiv_version","alias_value":"2605.29321v1","created_at":"2026-05-29T01:05:32Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2605.29321","created_at":"2026-05-29T01:05:32Z"},{"alias_kind":"pith_short_12","alias_value":"2YEWU4WT2VKQ","created_at":"2026-05-29T01:05:32Z"},{"alias_kind":"pith_short_16","alias_value":"2YEWU4WT2VKQ2V4B","created_at":"2026-05-29T01:05:32Z"},{"alias_kind":"pith_short_8","alias_value":"2YEWU4WT","created_at":"2026-05-29T01:05:32Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2026:2YEWU4WT2VKQ2V4BX7FGDPUULL","target":"record","payload":{"canonical_record":{"source":{"id":"2605.29321","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2026-05-28T03:50:50Z","cross_cats_sorted":["quant-ph"],"title_canon_sha256":"d2e2d6b51a655cdcf7b34b007842936db9ae5f2a61f17b37720d3f19e02af0d4","abstract_canon_sha256":"7420184fae672162a304137dc2475d63099a82ced5b76f1851239e53bee816df"},"schema_version":"1.0"},"canonical_sha256":"d6096a72d3d5550d5781bfca61be945ac343b8687df45644e8dd80137eeed5e7","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-29T01:05:32.612115Z","signature_b64":"tqv/1pT3xZCuIv3zBxdzF3VoWI/xrzqeMANtzpjFfZSi5fFer2ALFZ9JR+IRHy6fKKl+0d+OLOo/dz9pV3OOCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d6096a72d3d5550d5781bfca61be945ac343b8687df45644e8dd80137eeed5e7","last_reissued_at":"2026-05-29T01:05:32.611345Z","signature_status":"signed_v1","first_computed_at":"2026-05-29T01:05:32.611345Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2605.29321","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":"2026-05-29T01:05:32Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"RGf2Se595y1mDcRnxubGYBuVYHFnvGnZmJfwpDbH6zkcHnPaD8gDiu45qLIKJh/p7thkR+ocQV16hkAAvIxJBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-06T01:12:48.520780Z"},"content_sha256":"ed9eca1ac6cca3d878c658f19125a85bd3219183cae04ef1f189fa7db0fe1d97","schema_version":"1.0","event_id":"sha256:ed9eca1ac6cca3d878c658f19125a85bd3219183cae04ef1f189fa7db0fe1d97"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2026:2YEWU4WT2VKQ2V4BX7FGDPUULL","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Quantum and classical noise characteristics of parametrically driven cavity solitons in dispersive Kerr resonators","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["quant-ph"],"primary_cat":"physics.optics","authors_text":"Miro Erkintalo, Sophie S. Shamailov","submitted_at":"2026-05-28T03:50:50Z","abstract_excerpt":"Temporal cavity solitons generated in monochromatically driven dispersive Kerr resonators offer an attractive avenue for on-chip optical frequency comb generation. Key to many of their applications is to understand how noise -- both technical and quantum -- affects the soliton states, which has accordingly been extensively investigated. Here, we report on a comprehensive theoretical study that elucidates how technical and quantum fluctuations impact a new type of soliton structure that has very recently been predicted and observed in dispersive Kerr resonators under conditions of bichromatic d"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2605.29321","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2605.29321/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2026-05-29T01:05:32Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"SoUeJi1Rv1OcP19tU1fQgufXtzjlveVP48+9v/YhOYSiRC3JKStPRdXYmstt2RyAeyZkVDwtwBeOwfKN35+LCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-06T01:12:48.521282Z"},"content_sha256":"8b245172d8353982624887af37af0e34cde8af1f03464d1345dcfaa1ddae1f75","schema_version":"1.0","event_id":"sha256:8b245172d8353982624887af37af0e34cde8af1f03464d1345dcfaa1ddae1f75"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/2YEWU4WT2VKQ2V4BX7FGDPUULL/bundle.json","state_url":"https://pith.science/pith/2YEWU4WT2VKQ2V4BX7FGDPUULL/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/2YEWU4WT2VKQ2V4BX7FGDPUULL/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":"2026-08-06T01:12:48Z","links":{"resolver":"https://pith.science/pith/2YEWU4WT2VKQ2V4BX7FGDPUULL","bundle":"https://pith.science/pith/2YEWU4WT2VKQ2V4BX7FGDPUULL/bundle.json","state":"https://pith.science/pith/2YEWU4WT2VKQ2V4BX7FGDPUULL/state.json","well_known_bundle":"https://pith.science/.well-known/pith/2YEWU4WT2VKQ2V4BX7FGDPUULL/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2026:2YEWU4WT2VKQ2V4BX7FGDPUULL","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":"7420184fae672162a304137dc2475d63099a82ced5b76f1851239e53bee816df","cross_cats_sorted":["quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2026-05-28T03:50:50Z","title_canon_sha256":"d2e2d6b51a655cdcf7b34b007842936db9ae5f2a61f17b37720d3f19e02af0d4"},"schema_version":"1.0","source":{"id":"2605.29321","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2605.29321","created_at":"2026-05-29T01:05:32Z"},{"alias_kind":"arxiv_version","alias_value":"2605.29321v1","created_at":"2026-05-29T01:05:32Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2605.29321","created_at":"2026-05-29T01:05:32Z"},{"alias_kind":"pith_short_12","alias_value":"2YEWU4WT2VKQ","created_at":"2026-05-29T01:05:32Z"},{"alias_kind":"pith_short_16","alias_value":"2YEWU4WT2VKQ2V4B","created_at":"2026-05-29T01:05:32Z"},{"alias_kind":"pith_short_8","alias_value":"2YEWU4WT","created_at":"2026-05-29T01:05:32Z"}],"graph_snapshots":[{"event_id":"sha256:8b245172d8353982624887af37af0e34cde8af1f03464d1345dcfaa1ddae1f75","target":"graph","created_at":"2026-05-29T01:05:32Z","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/2605.29321/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Temporal cavity solitons generated in monochromatically driven dispersive Kerr resonators offer an attractive avenue for on-chip optical frequency comb generation. Key to many of their applications is to understand how noise -- both technical and quantum -- affects the soliton states, which has accordingly been extensively investigated. Here, we report on a comprehensive theoretical study that elucidates how technical and quantum fluctuations impact a new type of soliton structure that has very recently been predicted and observed in dispersive Kerr resonators under conditions of bichromatic d","authors_text":"Miro Erkintalo, Sophie S. Shamailov","cross_cats":["quant-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2026-05-28T03:50:50Z","title":"Quantum and classical noise characteristics of parametrically driven cavity solitons in dispersive Kerr resonators"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2605.29321","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:ed9eca1ac6cca3d878c658f19125a85bd3219183cae04ef1f189fa7db0fe1d97","target":"record","created_at":"2026-05-29T01:05:32Z","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":"7420184fae672162a304137dc2475d63099a82ced5b76f1851239e53bee816df","cross_cats_sorted":["quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2026-05-28T03:50:50Z","title_canon_sha256":"d2e2d6b51a655cdcf7b34b007842936db9ae5f2a61f17b37720d3f19e02af0d4"},"schema_version":"1.0","source":{"id":"2605.29321","kind":"arxiv","version":1}},"canonical_sha256":"d6096a72d3d5550d5781bfca61be945ac343b8687df45644e8dd80137eeed5e7","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"d6096a72d3d5550d5781bfca61be945ac343b8687df45644e8dd80137eeed5e7","first_computed_at":"2026-05-29T01:05:32.611345Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-29T01:05:32.611345Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"tqv/1pT3xZCuIv3zBxdzF3VoWI/xrzqeMANtzpjFfZSi5fFer2ALFZ9JR+IRHy6fKKl+0d+OLOo/dz9pV3OOCA==","signature_status":"signed_v1","signed_at":"2026-05-29T01:05:32.612115Z","signed_message":"canonical_sha256_bytes"},"source_id":"2605.29321","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:ed9eca1ac6cca3d878c658f19125a85bd3219183cae04ef1f189fa7db0fe1d97","sha256:8b245172d8353982624887af37af0e34cde8af1f03464d1345dcfaa1ddae1f75"],"state_sha256":"3bfe771160d603dc4590faf72542c2fa47c4fe5357b282168b92d2c24492b225"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"CHYfCG600DNcDEfWx7q0AIYZTGZqnRVkT1dJH2i6CLjYJEz5QOMKGdTCYj78iVX7yFqyKl+W8y3kEsHGd+SiDw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-06T01:12:48.525404Z","bundle_sha256":"78c5263136429ddcc519ab2cd94ac20b9028acee7aeeea3ec9d3c8b711d897bc"}}