{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2026:RLHTATHOKYC3AZORCN4ZV6L424","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":"7de9fcc16fce4e10fe9d93bf17ee068f2021d8d64e0529711ee67856dfb872ed","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.optics","submitted_at":"2026-06-16T14:55:10Z","title_canon_sha256":"efd3affd9b4be694565c0bf4f41ec38603f9d3a8324927e2ea218699bdfc92f8"},"schema_version":"1.0","source":{"id":"2606.18012","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2606.18012","created_at":"2026-06-19T16:10:45Z"},{"alias_kind":"arxiv_version","alias_value":"2606.18012v1","created_at":"2026-06-19T16:10:45Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2606.18012","created_at":"2026-06-19T16:10:45Z"},{"alias_kind":"pith_short_12","alias_value":"RLHTATHOKYC3","created_at":"2026-06-19T16:10:45Z"},{"alias_kind":"pith_short_16","alias_value":"RLHTATHOKYC3AZOR","created_at":"2026-06-19T16:10:45Z"},{"alias_kind":"pith_short_8","alias_value":"RLHTATHO","created_at":"2026-06-19T16:10:45Z"}],"graph_snapshots":[{"event_id":"sha256:0912a919b779c3b055ac161b962d9af4bcf2ca2b27221cd73fc27435e20e9a0c","target":"graph","created_at":"2026-06-19T16:10:45Z","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/2606.18012/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Many of the most powerful and elegant models in physics are grounded in symmetries. In electrodynamics, for example, geometric symmetries govern the observable effects of light-matter interactions. However, for man-made objects, exact symmetries are rarely met and tiny deviations are common. Nonetheless, even approximate symmetries keep many symmetry-derived rules effectively intact. However, as we will show here, this is not universally true. We demonstrate that an incremental violation of the symmetry of a carefully designed system can produce an optical response maximally different from the","authors_text":"Carsten Rockstuhl, Ivan Fernandez-Corbaton, Jan David Fischbach, Lukas Rebholz, Markus Nyman, Nikita Ustimenko","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.optics","submitted_at":"2026-06-16T14:55:10Z","title":"Broken-symmetry phenomena enhanced by quasi-bound states in the continuum"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2606.18012","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":"sha256:26e0dd8d2edf6c4eb0847e2c45a2ff504a149682a9630e8f753d8bc75061cc52","target":"record","created_at":"2026-06-19T16:10:45Z","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":"7de9fcc16fce4e10fe9d93bf17ee068f2021d8d64e0529711ee67856dfb872ed","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.optics","submitted_at":"2026-06-16T14:55:10Z","title_canon_sha256":"efd3affd9b4be694565c0bf4f41ec38603f9d3a8324927e2ea218699bdfc92f8"},"schema_version":"1.0","source":{"id":"2606.18012","kind":"arxiv","version":1}},"canonical_sha256":"8acf304cee5605b065d113799af97cd70635de7b7a2fd0833e8d5de2329d0b8e","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"8acf304cee5605b065d113799af97cd70635de7b7a2fd0833e8d5de2329d0b8e","first_computed_at":"2026-06-19T16:10:45.833445Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-06-19T16:10:45.833445Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"0OxgkOIgCIrSSmgN1eZBQBlt2YpS08kmghw40x9bql7J40TV4j6dY8bQkVrjqY0SAcKdCJ40uHjOjXV1eLFWAQ==","signature_status":"signed_v1","signed_at":"2026-06-19T16:10:45.833786Z","signed_message":"canonical_sha256_bytes"},"source_id":"2606.18012","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:26e0dd8d2edf6c4eb0847e2c45a2ff504a149682a9630e8f753d8bc75061cc52","sha256:0912a919b779c3b055ac161b962d9af4bcf2ca2b27221cd73fc27435e20e9a0c"],"state_sha256":"410579e7b1d37d15e9b4d6ca5c69ea9c169e33c965cfe1c6daa0df68ecef6dff"}