{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2025:DSXNELSPZHKOOCB6WYJFEZKLVN","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":"f238d2e1fe276a5751cfe83b46faf13de114cddce0f9027f0424b3ab3c61fc87","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2025-08-29T13:37:13Z","title_canon_sha256":"25f68088d83a0664bb14176fe6ab9d0b935e657e3181470fd96053a2b4cca513"},"schema_version":"1.0","source":{"id":"2508.21626","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2508.21626","created_at":"2026-07-05T12:01:46Z"},{"alias_kind":"arxiv_version","alias_value":"2508.21626v1","created_at":"2026-07-05T12:01:46Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2508.21626","created_at":"2026-07-05T12:01:46Z"},{"alias_kind":"pith_short_12","alias_value":"DSXNELSPZHKO","created_at":"2026-07-05T12:01:46Z"},{"alias_kind":"pith_short_16","alias_value":"DSXNELSPZHKOOCB6","created_at":"2026-07-05T12:01:46Z"},{"alias_kind":"pith_short_8","alias_value":"DSXNELSP","created_at":"2026-07-05T12:01:46Z"}],"graph_snapshots":[{"event_id":"sha256:55cff5dc96305070859eb26f70de54aff5d4b9a0367dec72d26eb4c4ceee2b43","target":"graph","created_at":"2026-07-05T12:01:46Z","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/2508.21626/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"The ability to control topological properties of laser emission represents a fundamental advancement in photonic technology. Achieving topological laser in a single compact photonic structure is crucial for device integration and miniaturization but faces significant challenges for designing both the high-quality (high-Q) mode and radiative topological configurations. Recently, bound states in the continuum (BICs), as extraordinary states possessing both ultrahigh Q factors and polarization topological charges, have been demonstrated as a promising platform for compact topological lasers. Howe","authors_text":"Jiajun Wang, Jian Zi, Lei Shi, Xinhao Wang, Zhaochen Wu","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2025-08-29T13:37:13Z","title":"Vectorial microlasers with designable topological charges based on M\\\"{o}bius-like correspondence in quasi-BICs"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2508.21626","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":"sha256:93f67e598b8981ee678649b215a5ab428c8535a49d40d3a7a58e3b29666263cc","target":"record","created_at":"2026-07-05T12:01:46Z","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":"f238d2e1fe276a5751cfe83b46faf13de114cddce0f9027f0424b3ab3c61fc87","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2025-08-29T13:37:13Z","title_canon_sha256":"25f68088d83a0664bb14176fe6ab9d0b935e657e3181470fd96053a2b4cca513"},"schema_version":"1.0","source":{"id":"2508.21626","kind":"arxiv","version":1}},"canonical_sha256":"1caed22e4fc9d4e7083eb61252654bab7020b569166b64c321888d3b4b51d6d0","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"1caed22e4fc9d4e7083eb61252654bab7020b569166b64c321888d3b4b51d6d0","first_computed_at":"2026-07-05T12:01:46.838322Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T12:01:46.838322Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"ueRUCU3w+l3r3k6DJrHO/KDZXWovW5k3GCmR1ikbPSvjqxkB8edYurk3aarPltGZQCpNwgabsMarB4bYj6naDw==","signature_status":"signed_v1","signed_at":"2026-07-05T12:01:46.838850Z","signed_message":"canonical_sha256_bytes"},"source_id":"2508.21626","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:93f67e598b8981ee678649b215a5ab428c8535a49d40d3a7a58e3b29666263cc","sha256:55cff5dc96305070859eb26f70de54aff5d4b9a0367dec72d26eb4c4ceee2b43"],"state_sha256":"80001f42a03490494351f2ec13e775b5c4afe34fa60aa701ff99d94fbb58ac67"}