{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2022:5XAWBB5JZZIXTWFILMZX2EPQBM","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":"cac6ee5a2bddb5e56e040ad47b99da79f52ed680f49b705e42a648b927b16b0c","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.optics","submitted_at":"2022-12-16T13:04:28Z","title_canon_sha256":"c0e555e2e745dc2d3e441fb834295533e140e2e09256c26bca5d06a8f0e7401e"},"schema_version":"1.0","source":{"id":"2212.08457","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2212.08457","created_at":"2026-07-05T06:57:38Z"},{"alias_kind":"arxiv_version","alias_value":"2212.08457v2","created_at":"2026-07-05T06:57:38Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2212.08457","created_at":"2026-07-05T06:57:38Z"},{"alias_kind":"pith_short_12","alias_value":"5XAWBB5JZZIX","created_at":"2026-07-05T06:57:38Z"},{"alias_kind":"pith_short_16","alias_value":"5XAWBB5JZZIXTWFI","created_at":"2026-07-05T06:57:38Z"},{"alias_kind":"pith_short_8","alias_value":"5XAWBB5J","created_at":"2026-07-05T06:57:38Z"}],"graph_snapshots":[{"event_id":"sha256:b00062622b8745cc692d8a7d5319d6baa60b9930331698e5605ab91a27cc6193","target":"graph","created_at":"2026-07-05T06:57:38Z","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/2212.08457/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"The phenomena of magneto-optical polarization rotation and circular magnetic dichroism are well known in the Faraday configuration. We present another effect, an odd magneto-optical linear dichroism, arising in nanostructures with polarization-dependent mode Q-factors. It reveals itself as the magneto-optical modulation of light intensity for the two opposite magnetization directions in the Faraday configuration. The effect was demonstrated on a magnetophotonic crystal with a cavity mode, the polarization-dependent Q-factor of which is due to oblique incidence. For a polarization angle of 60{\\","authors_text":"Daria Ignatyeva, Sergey Lyashko, Tatiana Mikhailova, Vladimir Belotelov, Vladimir Berzhansky","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.optics","submitted_at":"2022-12-16T13:04:28Z","title":"Odd Magneto-Optical Linear Dichroism in a Magnetophotonic Crystal"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2212.08457","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":"sha256:9fa13c2cf54209a5ce3da2212fa6777250db791238176f190da69dd99480e5c7","target":"record","created_at":"2026-07-05T06:57:38Z","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":"cac6ee5a2bddb5e56e040ad47b99da79f52ed680f49b705e42a648b927b16b0c","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.optics","submitted_at":"2022-12-16T13:04:28Z","title_canon_sha256":"c0e555e2e745dc2d3e441fb834295533e140e2e09256c26bca5d06a8f0e7401e"},"schema_version":"1.0","source":{"id":"2212.08457","kind":"arxiv","version":2}},"canonical_sha256":"edc16087a9ce5179d8a85b337d11f00b3df2523c72f3545826b513825518ca9e","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"edc16087a9ce5179d8a85b337d11f00b3df2523c72f3545826b513825518ca9e","first_computed_at":"2026-07-05T06:57:38.505824Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T06:57:38.505824Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Im/ikcuemk3fuPUiSP7+HzblEjL7rJnfymERpcYUHvVcNKN7L3DFk6pnIYKc3EAqCX2McKFtrzfQsTDwb42uDQ==","signature_status":"signed_v1","signed_at":"2026-07-05T06:57:38.506377Z","signed_message":"canonical_sha256_bytes"},"source_id":"2212.08457","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:9fa13c2cf54209a5ce3da2212fa6777250db791238176f190da69dd99480e5c7","sha256:b00062622b8745cc692d8a7d5319d6baa60b9930331698e5605ab91a27cc6193"],"state_sha256":"f11982f1f8e476fe006d83db1c3d49126906d98b58735b82eaef8fe33924d20e"}