{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:ELBATMALKGVGR4ELVHST25ND3F","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":"8e80d0239b7c3417451dba779cafbf89191e4012f3d29c4b786b3c033a305442","cross_cats_sorted":["cond-mat.mes-hall","physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.app-ph","submitted_at":"2018-10-23T21:54:35Z","title_canon_sha256":"1e4f8179acff018fea5fd5de9ab5a9612de61d3156755db64d74345f36ff6fd6"},"schema_version":"1.0","source":{"id":"1810.10106","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1810.10106","created_at":"2026-05-17T23:51:32Z"},{"alias_kind":"arxiv_version","alias_value":"1810.10106v1","created_at":"2026-05-17T23:51:32Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1810.10106","created_at":"2026-05-17T23:51:32Z"},{"alias_kind":"pith_short_12","alias_value":"ELBATMALKGVG","created_at":"2026-05-18T12:32:22Z"},{"alias_kind":"pith_short_16","alias_value":"ELBATMALKGVGR4EL","created_at":"2026-05-18T12:32:22Z"},{"alias_kind":"pith_short_8","alias_value":"ELBATMAL","created_at":"2026-05-18T12:32:22Z"}],"graph_snapshots":[{"event_id":"sha256:5a4c7dcd06e2a8722d8922b7fbf369ea3f3d18d39c72260fa46719fbfb2ee617","target":"graph","created_at":"2026-05-17T23:51:32Z","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":"We utilize an effective Hamiltonian formalism, within the Floquet scattering framework, to design a class of driving-induced non-reciprocal components with {\\it minimal} complexity. In the high driving-frequency limit, where our scheme is formally applicable, these designs demonstrate a leading order non-reciprocal performance which is inverse proportional to the driving frequency. Surprisingly, the optimal non-reciprocal behavior persists also in the slow driving regime. Our approach highlights the importance of physical loops in the design of these driven non-reciprocal components.","authors_text":"Huanan Li, Tsampikos Kottos","cross_cats":["cond-mat.mes-hall","physics.optics"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.app-ph","submitted_at":"2018-10-23T21:54:35Z","title":"Design algorithms of driving-induced nonreciprocal components"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1810.10106","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":"sha256:10f48e82c8c70cee37dd1f723d8c4e74978bc1c0a40ab1138049aaf4a5ed121c","target":"record","created_at":"2026-05-17T23:51:32Z","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":"8e80d0239b7c3417451dba779cafbf89191e4012f3d29c4b786b3c033a305442","cross_cats_sorted":["cond-mat.mes-hall","physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.app-ph","submitted_at":"2018-10-23T21:54:35Z","title_canon_sha256":"1e4f8179acff018fea5fd5de9ab5a9612de61d3156755db64d74345f36ff6fd6"},"schema_version":"1.0","source":{"id":"1810.10106","kind":"arxiv","version":1}},"canonical_sha256":"22c209b00b51aa68f08ba9e53d75a3d95b8d8779bf63d99d8118298f638b9b09","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"22c209b00b51aa68f08ba9e53d75a3d95b8d8779bf63d99d8118298f638b9b09","first_computed_at":"2026-05-17T23:51:32.972681Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-17T23:51:32.972681Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"i2SbpOEgetZ9QBtJF7yD4tSuXO4zwnmVGtZzMl7nA8zlhafWDeatk9iYXtKiadwLrSVZpA5Q4IJa909K4QAoCQ==","signature_status":"signed_v1","signed_at":"2026-05-17T23:51:32.973449Z","signed_message":"canonical_sha256_bytes"},"source_id":"1810.10106","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:10f48e82c8c70cee37dd1f723d8c4e74978bc1c0a40ab1138049aaf4a5ed121c","sha256:5a4c7dcd06e2a8722d8922b7fbf369ea3f3d18d39c72260fa46719fbfb2ee617"],"state_sha256":"d51fdeb16696fabfdabc76ee9aaa2198c731722865ce3685bfabd7b73e2508bd"}