{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2026:PLJWCKYAHHSCQ7EPYHRSPID2FA","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":"ae4651e935bed6c385b0cc719168ab04649d93dc72fb5534ba8b7b0634bdd705","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2026-02-07T16:08:47Z","title_canon_sha256":"9bfc63fccd3fdb02a1688453cbc49881e46419243abd320bdb06e41b3856c989"},"schema_version":"1.0","source":{"id":"2602.07600","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2602.07600","created_at":"2026-06-23T02:12:46Z"},{"alias_kind":"arxiv_version","alias_value":"2602.07600v2","created_at":"2026-06-23T02:12:46Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2602.07600","created_at":"2026-06-23T02:12:46Z"},{"alias_kind":"pith_short_12","alias_value":"PLJWCKYAHHSC","created_at":"2026-06-23T02:12:46Z"},{"alias_kind":"pith_short_16","alias_value":"PLJWCKYAHHSCQ7EP","created_at":"2026-06-23T02:12:46Z"},{"alias_kind":"pith_short_8","alias_value":"PLJWCKYA","created_at":"2026-06-23T02:12:46Z"}],"graph_snapshots":[{"event_id":"sha256:fba0952e4607384734916b71fa394df9620204d3044a2749f09a2702ff0bd16b","target":"graph","created_at":"2026-06-23T02:12:46Z","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/2602.07600/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Recent experiments have demonstrated the ability to manipulate nonlinear interactions via time modulation, giving rise to the so-called stroboscopic nonlinearity. To date, however, this phenomenon has not been subjected to a rigorous theoretical analysis. In this work, we clarify the physical mechanism underlying stroboscopic nonlinear dynamics based on time-nonlocal response and establish an effective time-independent model under suitable modulation conditions. The proposed model almost exactly reproduces the full time-dependent dynamics in the quasi-steady state and significantly outperforms","authors_text":"Haidong Li, Jiameng Zhang, Jiaxin Li, Jingjun Xu, Juan Wu, Mingjing Fan, Siyu Li, Xiaobin Peng, Xiaoqin Huang, Yi Hu, Yuhui Zhuang","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2026-02-07T16:08:47Z","title":"Time-independent theoretical framework for stroboscopic nonlinear dynamics based on time-nonlocal response"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2602.07600","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":"sha256:6a1eda31e74765d264c6ec1e820341e91de446c5856f536f79622580fc7d8bf1","target":"record","created_at":"2026-06-23T02:12:46Z","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":"ae4651e935bed6c385b0cc719168ab04649d93dc72fb5534ba8b7b0634bdd705","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2026-02-07T16:08:47Z","title_canon_sha256":"9bfc63fccd3fdb02a1688453cbc49881e46419243abd320bdb06e41b3856c989"},"schema_version":"1.0","source":{"id":"2602.07600","kind":"arxiv","version":2}},"canonical_sha256":"7ad3612b0039e4287c8fc1e327a07a281a716e3905a2f22a18ff1d40eda191fa","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"7ad3612b0039e4287c8fc1e327a07a281a716e3905a2f22a18ff1d40eda191fa","first_computed_at":"2026-06-23T02:12:46.632997Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-06-23T02:12:46.632997Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"x+7AuqwSnNsaj8jSmLSsSrJffUngf9NRwcO6PDq6U5AoevYi+t5W1y30eBfjH7fKg3JfD0t3FPwHqeuV5ok5Dg==","signature_status":"signed_v1","signed_at":"2026-06-23T02:12:46.633559Z","signed_message":"canonical_sha256_bytes"},"source_id":"2602.07600","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:6a1eda31e74765d264c6ec1e820341e91de446c5856f536f79622580fc7d8bf1","sha256:fba0952e4607384734916b71fa394df9620204d3044a2749f09a2702ff0bd16b"],"state_sha256":"44a8013536a8aaf4a8f0b7afa460e3f29a6fc9d2504bc0d0e1fc9bd9a85f772c"}