{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2022:R2YTCTCNH4OE3VJSQ3D2TXN6VL","short_pith_number":"pith:R2YTCTCN","canonical_record":{"source":{"id":"2205.08258","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2022-05-17T11:59:35Z","cross_cats_sorted":[],"title_canon_sha256":"08ddbe3863665234cd9b76a78bf479da0b2a4ef9f45517b2be9a75aa63fc2f8e","abstract_canon_sha256":"1f1e0bf3aad98b4bfa3a4537b84f8d916cf80a8f9307a97b101c9e312e64c653"},"schema_version":"1.0"},"canonical_sha256":"8eb1314c4d3f1c4dd53286c7a9ddbeaadb67aa0947a5fedc9eb7c3d688d7c6e9","source":{"kind":"arxiv","id":"2205.08258","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2205.08258","created_at":"2026-07-05T04:46:54Z"},{"alias_kind":"arxiv_version","alias_value":"2205.08258v1","created_at":"2026-07-05T04:46:54Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2205.08258","created_at":"2026-07-05T04:46:54Z"},{"alias_kind":"pith_short_12","alias_value":"R2YTCTCNH4OE","created_at":"2026-07-05T04:46:54Z"},{"alias_kind":"pith_short_16","alias_value":"R2YTCTCNH4OE3VJS","created_at":"2026-07-05T04:46:54Z"},{"alias_kind":"pith_short_8","alias_value":"R2YTCTCN","created_at":"2026-07-05T04:46:54Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2022:R2YTCTCNH4OE3VJSQ3D2TXN6VL","target":"record","payload":{"canonical_record":{"source":{"id":"2205.08258","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2022-05-17T11:59:35Z","cross_cats_sorted":[],"title_canon_sha256":"08ddbe3863665234cd9b76a78bf479da0b2a4ef9f45517b2be9a75aa63fc2f8e","abstract_canon_sha256":"1f1e0bf3aad98b4bfa3a4537b84f8d916cf80a8f9307a97b101c9e312e64c653"},"schema_version":"1.0"},"canonical_sha256":"8eb1314c4d3f1c4dd53286c7a9ddbeaadb67aa0947a5fedc9eb7c3d688d7c6e9","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T04:46:54.170451Z","signature_b64":"NtFFaA/NFPsmz1v4XAz7mDfUiUZGvkgc7vxJ7P1MxVBqAC0w3tlvCiHV07x102YYVLqdVTRUvwxYCc30J6h0BA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8eb1314c4d3f1c4dd53286c7a9ddbeaadb67aa0947a5fedc9eb7c3d688d7c6e9","last_reissued_at":"2026-07-05T04:46:54.170064Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T04:46:54.170064Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2205.08258","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-05T04:46:54Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"gqmRynYuDR7D/FECuXinP9zukNla4GXTldxKva08RDgrvMZAIaiGLKPh73BdJz6NdlnTTZjySC0Yb8/u/ifKAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-06T11:11:26.261629Z"},"content_sha256":"5a91172e15248f4e8e1a88a5b263c9ea2ab8bad18816c3efe85b4a28701afdbe","schema_version":"1.0","event_id":"sha256:5a91172e15248f4e8e1a88a5b263c9ea2ab8bad18816c3efe85b4a28701afdbe"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2022:R2YTCTCNH4OE3VJSQ3D2TXN6VL","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Polarization manipulation of giant photonic spin Hall effect using wave-guiding effect","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.optics","authors_text":"Kyoungsik Kim, Monu Nath Baitha","submitted_at":"2022-05-17T11:59:35Z","abstract_excerpt":"In plasmonic systems, the enhanced photonic spin Hall effect (PSHE) was previously possible only for horizontal polarization. By employing the wave-guiding surface plasmon resonance (WG-SPR) effect, we report a giant photonic spin Hall effect (G-PSHE) of reflected light for both horizontal and vertical polarization waves. We investigated the polarization-manipulated G-PSHE in the Kretschmann configuration with an additional glass dielectric layer. This additional dielectric layer allowed us to achieve millimeter-scale (more than 2 mm to sub-millimeter) G-PSHE. We achieved polarization manipula"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2205.08258","kind":"arxiv","version":1},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2205.08258/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-05T04:46:54Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ANyA+K2zOdhmLW6jlwwE8Q0FLVpvM+8g6Wro8KoqNsAZuJkZBPfYhHPydj2xIzjHlPKAW2dxrKbQBLCmm67xAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-06T11:11:26.262001Z"},"content_sha256":"9b9a0efe43be840ae4c8ceeb04df74408ec4d0b43f8215ed070df178ed3a722d","schema_version":"1.0","event_id":"sha256:9b9a0efe43be840ae4c8ceeb04df74408ec4d0b43f8215ed070df178ed3a722d"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/R2YTCTCNH4OE3VJSQ3D2TXN6VL/bundle.json","state_url":"https://pith.science/pith/R2YTCTCNH4OE3VJSQ3D2TXN6VL/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/R2YTCTCNH4OE3VJSQ3D2TXN6VL/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-07-06T11:11:26Z","links":{"resolver":"https://pith.science/pith/R2YTCTCNH4OE3VJSQ3D2TXN6VL","bundle":"https://pith.science/pith/R2YTCTCNH4OE3VJSQ3D2TXN6VL/bundle.json","state":"https://pith.science/pith/R2YTCTCNH4OE3VJSQ3D2TXN6VL/state.json","well_known_bundle":"https://pith.science/.well-known/pith/R2YTCTCNH4OE3VJSQ3D2TXN6VL/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2022:R2YTCTCNH4OE3VJSQ3D2TXN6VL","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":"1f1e0bf3aad98b4bfa3a4537b84f8d916cf80a8f9307a97b101c9e312e64c653","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2022-05-17T11:59:35Z","title_canon_sha256":"08ddbe3863665234cd9b76a78bf479da0b2a4ef9f45517b2be9a75aa63fc2f8e"},"schema_version":"1.0","source":{"id":"2205.08258","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2205.08258","created_at":"2026-07-05T04:46:54Z"},{"alias_kind":"arxiv_version","alias_value":"2205.08258v1","created_at":"2026-07-05T04:46:54Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2205.08258","created_at":"2026-07-05T04:46:54Z"},{"alias_kind":"pith_short_12","alias_value":"R2YTCTCNH4OE","created_at":"2026-07-05T04:46:54Z"},{"alias_kind":"pith_short_16","alias_value":"R2YTCTCNH4OE3VJS","created_at":"2026-07-05T04:46:54Z"},{"alias_kind":"pith_short_8","alias_value":"R2YTCTCN","created_at":"2026-07-05T04:46:54Z"}],"graph_snapshots":[{"event_id":"sha256:9b9a0efe43be840ae4c8ceeb04df74408ec4d0b43f8215ed070df178ed3a722d","target":"graph","created_at":"2026-07-05T04:46:54Z","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/2205.08258/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"In plasmonic systems, the enhanced photonic spin Hall effect (PSHE) was previously possible only for horizontal polarization. By employing the wave-guiding surface plasmon resonance (WG-SPR) effect, we report a giant photonic spin Hall effect (G-PSHE) of reflected light for both horizontal and vertical polarization waves. We investigated the polarization-manipulated G-PSHE in the Kretschmann configuration with an additional glass dielectric layer. This additional dielectric layer allowed us to achieve millimeter-scale (more than 2 mm to sub-millimeter) G-PSHE. We achieved polarization manipula","authors_text":"Kyoungsik Kim, Monu Nath Baitha","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2022-05-17T11:59:35Z","title":"Polarization manipulation of giant photonic spin Hall effect using wave-guiding effect"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2205.08258","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":"sha256:5a91172e15248f4e8e1a88a5b263c9ea2ab8bad18816c3efe85b4a28701afdbe","target":"record","created_at":"2026-07-05T04:46:54Z","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":"1f1e0bf3aad98b4bfa3a4537b84f8d916cf80a8f9307a97b101c9e312e64c653","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2022-05-17T11:59:35Z","title_canon_sha256":"08ddbe3863665234cd9b76a78bf479da0b2a4ef9f45517b2be9a75aa63fc2f8e"},"schema_version":"1.0","source":{"id":"2205.08258","kind":"arxiv","version":1}},"canonical_sha256":"8eb1314c4d3f1c4dd53286c7a9ddbeaadb67aa0947a5fedc9eb7c3d688d7c6e9","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"8eb1314c4d3f1c4dd53286c7a9ddbeaadb67aa0947a5fedc9eb7c3d688d7c6e9","first_computed_at":"2026-07-05T04:46:54.170064Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T04:46:54.170064Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"NtFFaA/NFPsmz1v4XAz7mDfUiUZGvkgc7vxJ7P1MxVBqAC0w3tlvCiHV07x102YYVLqdVTRUvwxYCc30J6h0BA==","signature_status":"signed_v1","signed_at":"2026-07-05T04:46:54.170451Z","signed_message":"canonical_sha256_bytes"},"source_id":"2205.08258","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:5a91172e15248f4e8e1a88a5b263c9ea2ab8bad18816c3efe85b4a28701afdbe","sha256:9b9a0efe43be840ae4c8ceeb04df74408ec4d0b43f8215ed070df178ed3a722d"],"state_sha256":"eb85dc37744eb201f4af282c35640e3af59cab5cc735918159606e35190c3ec4"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"amWH0LpOm+Lg3geR25kccIl9MY7iMjSNwVGTq2FFxHRMYXLfSqelNrFTrJyDRcJTLBNrU3RAokgxEzugILcBBQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-07-06T11:11:26.263979Z","bundle_sha256":"6d712c53d9b576dbf33abe61fd5eab222024b7bad28bda119ce65816774400d1"}}