{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2022:3VTMVG2QORZ3LRSO6ZBV3RNCJD","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":"286f060296773d60886bb2cb331ca2830f1b878bc32b57715a4254bc0e3ba457","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2022-06-16T06:00:00Z","title_canon_sha256":"1b3dab908e24a9deebb5edc9b1a229200018b6857f8271686a5990635f6f2cea"},"schema_version":"1.0","source":{"id":"2206.07935","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2206.07935","created_at":"2026-07-05T04:32:20Z"},{"alias_kind":"arxiv_version","alias_value":"2206.07935v1","created_at":"2026-07-05T04:32:20Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2206.07935","created_at":"2026-07-05T04:32:20Z"},{"alias_kind":"pith_short_12","alias_value":"3VTMVG2QORZ3","created_at":"2026-07-05T04:32:20Z"},{"alias_kind":"pith_short_16","alias_value":"3VTMVG2QORZ3LRSO","created_at":"2026-07-05T04:32:20Z"},{"alias_kind":"pith_short_8","alias_value":"3VTMVG2Q","created_at":"2026-07-05T04:32:20Z"}],"graph_snapshots":[{"event_id":"sha256:437e4934dbddf9b0a43e32258c56e5b45ae59df6886d7781c596ad3753f71465","target":"graph","created_at":"2026-07-05T04:32:20Z","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/2206.07935/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"The realization of high-Q resonances in a silicon metasurface with various broken-symmetry blocks is reported. Theoretical analysis reveals that the sharp resonances in the metasurfaces originate from symmetry-protected bound states in the continuum (BIC) and the magnetic dipole dominates these peculiar states. A smaller size of the defect in the broken-symmetry block gives rise to the resonance with a larger Q factor. Importantly, this relationship can be tuned by changing the structural parameter, resulting from the modulation of the topological configuration of BICs. Consequently, a Q facto","authors_text":"C. Fang, G. Han, J. Zhao, Q. Yang, Q. Yuan, X. Gan, Y. Hao, Y. Liu, Y. Shao","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2022-06-16T06:00:00Z","title":"High-Q Resonances Governed by the Quasi-Bound States in the Continuum in All-Dielectric Metasurfaces"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2206.07935","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:caa76757ac70c3cdb6d78315b9e066cce9a782deff77d355ea8b87a3433a067b","target":"record","created_at":"2026-07-05T04:32:20Z","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":"286f060296773d60886bb2cb331ca2830f1b878bc32b57715a4254bc0e3ba457","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2022-06-16T06:00:00Z","title_canon_sha256":"1b3dab908e24a9deebb5edc9b1a229200018b6857f8271686a5990635f6f2cea"},"schema_version":"1.0","source":{"id":"2206.07935","kind":"arxiv","version":1}},"canonical_sha256":"dd66ca9b507473b5c64ef6435dc5a248d5437f5f689d6ec8e68971d76b00d7ab","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"dd66ca9b507473b5c64ef6435dc5a248d5437f5f689d6ec8e68971d76b00d7ab","first_computed_at":"2026-07-05T04:32:20.166926Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T04:32:20.166926Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"pSU4Umzz/kCivYPrDfredAEcQ7ygWUZp1/CmcBDvplahHMlPUKYImzn4ftN889ms/HBM7QOny4PDf5wYT/1DCg==","signature_status":"signed_v1","signed_at":"2026-07-05T04:32:20.167327Z","signed_message":"canonical_sha256_bytes"},"source_id":"2206.07935","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:caa76757ac70c3cdb6d78315b9e066cce9a782deff77d355ea8b87a3433a067b","sha256:437e4934dbddf9b0a43e32258c56e5b45ae59df6886d7781c596ad3753f71465"],"state_sha256":"4cf9f53e74c10079a6a32b73ca7595c72ef0b5d1c5e3650f0b5bd02f76691742"}