{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2025:3YEAL77B3ABLWZR6RN2GUHHPVF","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":"0b04a44c00ea3bf167e5eec8b8f0ce836cb733140ae29c8f798dac1bd12b1b51","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.optics","submitted_at":"2025-06-02T09:33:00Z","title_canon_sha256":"450a4ff202d1f5cbb8c1862fbf711c6c8f1bc67268e7bbbc048c2911eb382fda"},"schema_version":"1.0","source":{"id":"2506.01472","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2506.01472","created_at":"2026-05-29T02:05:34Z"},{"alias_kind":"arxiv_version","alias_value":"2506.01472v1","created_at":"2026-05-29T02:05:34Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2506.01472","created_at":"2026-05-29T02:05:34Z"},{"alias_kind":"pith_short_12","alias_value":"3YEAL77B3ABL","created_at":"2026-05-29T02:05:34Z"},{"alias_kind":"pith_short_16","alias_value":"3YEAL77B3ABLWZR6","created_at":"2026-05-29T02:05:34Z"},{"alias_kind":"pith_short_8","alias_value":"3YEAL77B","created_at":"2026-05-29T02:05:34Z"}],"graph_snapshots":[{"event_id":"sha256:ede9254ff515754168514356f0b7edabfda63c0bfe5d9467a9e5cbfb5995d805","target":"graph","created_at":"2026-05-29T02:05:34Z","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/2506.01472/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Photonic time crystals (PTCs) are spatially uniform media with periodic modulation in time, enabling momentum bandgaps and the parametric amplification of light. While their potential in optical systems is very promising, practical implementations require temporally modulating nanostructures of finite size, for which the physics is no longer governed by bulk properties but by resonant states, or quasinormal modes. Despite their importance, a quantitative theory describing the dynamics of these modes has been missing -- a gap we address here by developing a comprehensive resonant state theory f","authors_text":"Adri\\`a Can\\'os Valero, David Globosits, Egor A. Muljarov, Sergei Gladyshev, Stefan Rotter, Thomas Weiss","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.optics","submitted_at":"2025-06-02T09:33:00Z","title":"Resonant states of structured photonic time crystals"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2506.01472","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":"sha256:12576c877c687f92c82505482531d06d01b0ffc34509777a7b6d7f75e04b8aca","target":"record","created_at":"2026-05-29T02:05:34Z","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":"0b04a44c00ea3bf167e5eec8b8f0ce836cb733140ae29c8f798dac1bd12b1b51","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.optics","submitted_at":"2025-06-02T09:33:00Z","title_canon_sha256":"450a4ff202d1f5cbb8c1862fbf711c6c8f1bc67268e7bbbc048c2911eb382fda"},"schema_version":"1.0","source":{"id":"2506.01472","kind":"arxiv","version":1}},"canonical_sha256":"de0805ffe1d802bb663e8b746a1cefa95174d38da84ae8b9ac08ad8c5ccf165b","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"de0805ffe1d802bb663e8b746a1cefa95174d38da84ae8b9ac08ad8c5ccf165b","first_computed_at":"2026-05-29T02:05:34.961386Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-29T02:05:34.961386Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"9fowP+qlUXHmOZCMKWnhTq0nrRVYe4VnaddZVLKMW8311eptDixuiJ6q/8DrcfP/AHALK7sFNFrtfUYrTZUmAQ==","signature_status":"signed_v1","signed_at":"2026-05-29T02:05:34.961878Z","signed_message":"canonical_sha256_bytes"},"source_id":"2506.01472","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:12576c877c687f92c82505482531d06d01b0ffc34509777a7b6d7f75e04b8aca","sha256:ede9254ff515754168514356f0b7edabfda63c0bfe5d9467a9e5cbfb5995d805"],"state_sha256":"572866a1bf51a9cd101a61d368bc96d90cc809a1d0bf1a94de6be89cdb965670"}