{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2026:AWPYWQLZHOZU5NH6S6AUIGPQKC","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":"5bb507fca508dfacc0e421480791ea9e1120f0ed5d075f86a6a7443270c235c1","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2026-02-20T09:57:25Z","title_canon_sha256":"36ae9033a52d7b497cd545c0dc37a87609cf16dedc7fac2a4fceff910a497f41"},"schema_version":"1.0","source":{"id":"2602.18110","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2602.18110","created_at":"2026-05-20T01:05:09Z"},{"alias_kind":"arxiv_version","alias_value":"2602.18110v2","created_at":"2026-05-20T01:05:09Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2602.18110","created_at":"2026-05-20T01:05:09Z"},{"alias_kind":"pith_short_12","alias_value":"AWPYWQLZHOZU","created_at":"2026-05-20T01:05:09Z"},{"alias_kind":"pith_short_16","alias_value":"AWPYWQLZHOZU5NH6","created_at":"2026-05-20T01:05:09Z"},{"alias_kind":"pith_short_8","alias_value":"AWPYWQLZ","created_at":"2026-05-20T01:05:09Z"}],"graph_snapshots":[{"event_id":"sha256:ca708c9b5de2e8e687cba8dc1383ae486c81fc1fcc5abae348a098e937f0d340","target":"graph","created_at":"2026-05-20T01:05:09Z","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/2602.18110/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Reservoir computing leverages nonlinear dynamics of physical systems to process temporal information with minimal training cost. Here, we demonstrate that cavity solitons sustained in a fiber optical cavity provide an optical platform for photonic reservoir computing. Our methodology exploits the use of a phase-modulated drive laser to encode the input, while the reservoir states are accessed through frequency-resolved readout. Numerical simulations indicate that the emission of Kelly waves enriches the dynamics and enhances performance for machine learning tasks. We evaluate the performance o","authors_text":"Alessandro Lupo, Amir Arsalan Arabieh, Serge Massar, Simon-Pierre Gorza","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2026-02-20T09:57:25Z","title":"Cavity Solitons as a Nonlinear Substrate for Photonic Neuromorphic Computing"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2602.18110","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":"sha256:7e325f9947b35a7aa55d5a669554dcd545f0768a39c6c885b9152fefdb850232","target":"record","created_at":"2026-05-20T01:05:09Z","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":"5bb507fca508dfacc0e421480791ea9e1120f0ed5d075f86a6a7443270c235c1","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2026-02-20T09:57:25Z","title_canon_sha256":"36ae9033a52d7b497cd545c0dc37a87609cf16dedc7fac2a4fceff910a497f41"},"schema_version":"1.0","source":{"id":"2602.18110","kind":"arxiv","version":2}},"canonical_sha256":"059f8b41793bb34eb4fe97814419f050a358d67bef61c7118e925df6be500cd1","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"059f8b41793bb34eb4fe97814419f050a358d67bef61c7118e925df6be500cd1","first_computed_at":"2026-05-20T01:05:09.676909Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-20T01:05:09.676909Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"fzJG0K7pbCdPzEYK/zYVpdM8vhsP3Nu3FXpoR+y15IpqGSqNlDPvZA/XDlzEYc+02N9hsVRaX/1xKyxVS9+GCg==","signature_status":"signed_v1","signed_at":"2026-05-20T01:05:09.677915Z","signed_message":"canonical_sha256_bytes"},"source_id":"2602.18110","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:7e325f9947b35a7aa55d5a669554dcd545f0768a39c6c885b9152fefdb850232","sha256:ca708c9b5de2e8e687cba8dc1383ae486c81fc1fcc5abae348a098e937f0d340"],"state_sha256":"6500add6a839eb6cd4df078bf5bf91f72966a31b4465860ae5598e20404a410a"}