{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:5JEB3LBNJ4QRGY2LLEJQBBBGSS","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":"2652036c2ae72d267989970b7e652058b361a0241b313960b41143916b7dfa12","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2016-07-20T18:25:48Z","title_canon_sha256":"e457748c368c5eaa639c7ca78e36e0f33a66af16384899cda9caa85eceedd99b"},"schema_version":"1.0","source":{"id":"1607.06052","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1607.06052","created_at":"2026-05-18T01:00:34Z"},{"alias_kind":"arxiv_version","alias_value":"1607.06052v1","created_at":"2026-05-18T01:00:34Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1607.06052","created_at":"2026-05-18T01:00:34Z"},{"alias_kind":"pith_short_12","alias_value":"5JEB3LBNJ4QR","created_at":"2026-05-18T12:30:01Z"},{"alias_kind":"pith_short_16","alias_value":"5JEB3LBNJ4QRGY2L","created_at":"2026-05-18T12:30:01Z"},{"alias_kind":"pith_short_8","alias_value":"5JEB3LBN","created_at":"2026-05-18T12:30:01Z"}],"graph_snapshots":[{"event_id":"sha256:df2680db9e1245c2eee85c52586deb6e2ff89a9ef2ca1e16e7536edbfe3189b0","target":"graph","created_at":"2026-05-18T01:00:34Z","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":"Device figures of merit are commonly employed to assess bulk material properties for a particular device class, yet these properties ultimately originate in the linear and nonlinear susceptibilities of the material which are not independent of each other. In this work, we calculate the electro-optic device figure of merit based on the half-wave voltage and linear loss, which is important for phase modulators and serves as the simplest example of the approach. This figure of merit is then related back to the microscopic properties in the context of a dye-doped polymer, and its fundamental limit","authors_text":"Mark G. Kuzyk, Rick Lytel, Sean Mossman","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2016-07-20T18:25:48Z","title":"Fundamental limits on the electro-optic device figure of merit"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1607.06052","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":"sha256:4b18f2963805f5921545657854358383a75a1056cc0407dd44a228bed1f7cd93","target":"record","created_at":"2026-05-18T01:00:34Z","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":"2652036c2ae72d267989970b7e652058b361a0241b313960b41143916b7dfa12","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2016-07-20T18:25:48Z","title_canon_sha256":"e457748c368c5eaa639c7ca78e36e0f33a66af16384899cda9caa85eceedd99b"},"schema_version":"1.0","source":{"id":"1607.06052","kind":"arxiv","version":1}},"canonical_sha256":"ea481dac2d4f2113634b59130084269497f7b7fe326d98f7bf9fc691fa44b1a9","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"ea481dac2d4f2113634b59130084269497f7b7fe326d98f7bf9fc691fa44b1a9","first_computed_at":"2026-05-18T01:00:34.100615Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:00:34.100615Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"VZGJTZBu/kzwUeoxODRieASitkMWfoZwCTiFT8VtJmwAfs0OvvHOaNVE67V2aKVgx/xF67twKWRaMTqsUjVfCg==","signature_status":"signed_v1","signed_at":"2026-05-18T01:00:34.101140Z","signed_message":"canonical_sha256_bytes"},"source_id":"1607.06052","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:4b18f2963805f5921545657854358383a75a1056cc0407dd44a228bed1f7cd93","sha256:df2680db9e1245c2eee85c52586deb6e2ff89a9ef2ca1e16e7536edbfe3189b0"],"state_sha256":"e3a611e5e07e79ad99afaaf89b11100adefa184b816e065e69d9f468e062cafb"}