{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:GUWWT4HINRWI5PH53XGQXFV5TQ","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":"c3205d0b6a469af31fb6dbd8dd6b3f436772d403c10763dc146d11e2c5646748","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2012-01-25T09:45:57Z","title_canon_sha256":"a1271ea45060ff91bad7da0a3c357ee58717d08c66a06977981fd001eb022a80"},"schema_version":"1.0","source":{"id":"1201.5218","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1201.5218","created_at":"2026-05-18T03:10:00Z"},{"alias_kind":"arxiv_version","alias_value":"1201.5218v2","created_at":"2026-05-18T03:10:00Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1201.5218","created_at":"2026-05-18T03:10:00Z"},{"alias_kind":"pith_short_12","alias_value":"GUWWT4HINRWI","created_at":"2026-05-18T12:27:06Z"},{"alias_kind":"pith_short_16","alias_value":"GUWWT4HINRWI5PH5","created_at":"2026-05-18T12:27:06Z"},{"alias_kind":"pith_short_8","alias_value":"GUWWT4HI","created_at":"2026-05-18T12:27:06Z"}],"graph_snapshots":[{"event_id":"sha256:3161d5cf67403b42a471cc1f8948a1ac0898cf494aca76e4ac026c060f3bbc80","target":"graph","created_at":"2026-05-18T03:10:00Z","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"},"paper":{"abstract_excerpt":"When a linear chain of plasmonic nano-particles is exposed to a transverse DC magnetic field, the chain modes are elliptically polarized, in a single plane parallel to the chain axis; hence, a novel longitudinal plasmon-rotation is created. If, in addition, the chain geometry possesses longitudinal rotation, e.g. by using ellipsoidal particles that rotate in the same plane as the plasmon rotation, strong non-reciprocity is created. The structure possesses a new kind of chirality--the longitudinal chirality--and supports one-way guiding. Since all particles rotate in the same plane, the geometr","authors_text":"Ben Z. Steinberg, Yarden Mazor","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2012-01-25T09:45:57Z","title":"Longitudinal chirality, enhanced non-reciprocity, and nano-scale planar one-way guiding"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1201.5218","kind":"arxiv","version":2},"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":"sha256:38ecba15fb1e4115b1e137fa8df649a5d7602e73f8ff8e81ded15c65b27fe45c","target":"record","created_at":"2026-05-18T03:10:00Z","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":"c3205d0b6a469af31fb6dbd8dd6b3f436772d403c10763dc146d11e2c5646748","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2012-01-25T09:45:57Z","title_canon_sha256":"a1271ea45060ff91bad7da0a3c357ee58717d08c66a06977981fd001eb022a80"},"schema_version":"1.0","source":{"id":"1201.5218","kind":"arxiv","version":2}},"canonical_sha256":"352d69f0e86c6c8ebcfdddcd0b96bd9c1dc6db95371cf7d4c244af40de6e16c1","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"352d69f0e86c6c8ebcfdddcd0b96bd9c1dc6db95371cf7d4c244af40de6e16c1","first_computed_at":"2026-05-18T03:10:00.384493Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:10:00.384493Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"bChkjrQAXIb/dSqoJK29rlbpHfk0dkgZ5HAA3eiWHn9az5mcXXUescGLh9qOnr+LTXguK7nUaawz2aWnAMpBCA==","signature_status":"signed_v1","signed_at":"2026-05-18T03:10:00.385084Z","signed_message":"canonical_sha256_bytes"},"source_id":"1201.5218","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:38ecba15fb1e4115b1e137fa8df649a5d7602e73f8ff8e81ded15c65b27fe45c","sha256:3161d5cf67403b42a471cc1f8948a1ac0898cf494aca76e4ac026c060f3bbc80"],"state_sha256":"1c1276a2a9284802d1a4c9672f5bdeeecc7845ff45d88948cfc8c6c11e2efebd"}