{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2024:O2ISXXGNZPBWRBYVZKZ7F2U5FJ","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":"d9c9b481b54419d6be2928d3e461fc2497b504013d88000f45874fd6a84e9030","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.optics","submitted_at":"2024-03-13T13:52:26Z","title_canon_sha256":"19961089b0264379ba309a80705955730a1b3e73a020a7c5e45563af42d83127"},"schema_version":"1.0","source":{"id":"2403.08539","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2403.08539","created_at":"2026-07-05T08:25:01Z"},{"alias_kind":"arxiv_version","alias_value":"2403.08539v1","created_at":"2026-07-05T08:25:01Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2403.08539","created_at":"2026-07-05T08:25:01Z"},{"alias_kind":"pith_short_12","alias_value":"O2ISXXGNZPBW","created_at":"2026-07-05T08:25:01Z"},{"alias_kind":"pith_short_16","alias_value":"O2ISXXGNZPBWRBYV","created_at":"2026-07-05T08:25:01Z"},{"alias_kind":"pith_short_8","alias_value":"O2ISXXGN","created_at":"2026-07-05T08:25:01Z"}],"graph_snapshots":[{"event_id":"sha256:1afdb8e77270fa2b74f82461622967dd5d1daee035a217df16e49334a5e2ccef","target":"graph","created_at":"2026-07-05T08:25:01Z","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/2403.08539/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"The generation and focusing properties of higher-order polarized beams have attracted lots of interests due to its significant applications. In this paper,we derived the formula of transforming linear polarization into higher-order polarization, which is applicable to generating arbitrary order polarization. Based on the derived formula, the focusing properties of higher-order polarization by dielectric metasurface lens are studied , which exhibit an Abbe-limit-breaking feature for small numerical aperture, i.e., NA<0.6. When a binary phase (0 & {\\pi}) is further imposed on the aperture of met","authors_text":"Hanming Guo, Jinbing Hu, Songlin Zhuang, Xiang Yuan","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.optics","submitted_at":"2024-03-13T13:52:26Z","title":"Generation and high-resolution imaging of higher-order polarization via metasurface"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2403.08539","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:c27eeebec70db286edfcbaf4cda033097fe16c700e3b58b694554e309e746381","target":"record","created_at":"2026-07-05T08:25:01Z","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":"d9c9b481b54419d6be2928d3e461fc2497b504013d88000f45874fd6a84e9030","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.optics","submitted_at":"2024-03-13T13:52:26Z","title_canon_sha256":"19961089b0264379ba309a80705955730a1b3e73a020a7c5e45563af42d83127"},"schema_version":"1.0","source":{"id":"2403.08539","kind":"arxiv","version":1}},"canonical_sha256":"76912bdccdcbc3688715cab3f2ea9d2a521f0a4c4931bca682e7a6801a65fd9e","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"76912bdccdcbc3688715cab3f2ea9d2a521f0a4c4931bca682e7a6801a65fd9e","first_computed_at":"2026-07-05T08:25:01.757107Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T08:25:01.757107Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"ngl59tyK5eFJmPhvEh5bKQtwwT9/pnzO99dgpGYeaEQgWPB72cZoPi78so/yqynNvFi5w1LNAacYauEZPuZ+Cw==","signature_status":"signed_v1","signed_at":"2026-07-05T08:25:01.757532Z","signed_message":"canonical_sha256_bytes"},"source_id":"2403.08539","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:c27eeebec70db286edfcbaf4cda033097fe16c700e3b58b694554e309e746381","sha256:1afdb8e77270fa2b74f82461622967dd5d1daee035a217df16e49334a5e2ccef"],"state_sha256":"c50622c6357fc86cc425e150db753c697508e563190ec0275b78458fd090f9ad"}