{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:TZTUG4EMHJSZRGZFUYH7JDWAWD","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":"d4edb18bb94361c8f589fce4a98f03c5a1e55e515751bb0ddd0b7ae2d143df90","cross_cats_sorted":["cond-mat.mes-hall","physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2018-10-12T19:47:44Z","title_canon_sha256":"dfafcb19ae654db0751649b06ada09b98c13c114d653c28c99a286f280ee5cdf"},"schema_version":"1.0","source":{"id":"1810.05701","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1810.05701","created_at":"2026-05-17T23:59:57Z"},{"alias_kind":"arxiv_version","alias_value":"1810.05701v1","created_at":"2026-05-17T23:59:57Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1810.05701","created_at":"2026-05-17T23:59:57Z"},{"alias_kind":"pith_short_12","alias_value":"TZTUG4EMHJSZ","created_at":"2026-05-18T12:32:56Z"},{"alias_kind":"pith_short_16","alias_value":"TZTUG4EMHJSZRGZF","created_at":"2026-05-18T12:32:56Z"},{"alias_kind":"pith_short_8","alias_value":"TZTUG4EM","created_at":"2026-05-18T12:32:56Z"}],"graph_snapshots":[{"event_id":"sha256:7928da0803fcab2b8790ff604293f37e5872d6fbbed09cc234050aab92551988","target":"graph","created_at":"2026-05-17T23:59:57Z","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":"The integration of quantum emitters with integrated photonics enables complex quantum photonic circuits that are necessary for photonic implementation of quantum simulators, computers, and networks. Thin-film lithium niobate is an ideal material substrate for quantum photonics because it can tightly confine light in small waveguides and has a strong electro-optic effect that can switch and modulate single photons at low power and high speed. However, lithium niobite lacks efficient single-photon emitters, which are essential for scalable quantum photonic circuits. We demonstrate deterministic ","authors_text":"Aziz Karasahin, Boris Desiatov, Chang-Min Lee, Christopher J. K. Richardson, Edo Waks, Je-Hyung Kim, Marko Lon\\v{c}ar, Mustafa Atabey Buyukkaya, Richard P. Leavitt, Shahriar Aghaeimeibodi","cross_cats":["cond-mat.mes-hall","physics.optics"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2018-10-12T19:47:44Z","title":"Integration of Quantum Emitters with Lithium Niobate Photonics"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1810.05701","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:a812805f82db510dc2bfaa3030fc7a524193e7fa3cecbdf41943ea476789a140","target":"record","created_at":"2026-05-17T23:59:57Z","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":"d4edb18bb94361c8f589fce4a98f03c5a1e55e515751bb0ddd0b7ae2d143df90","cross_cats_sorted":["cond-mat.mes-hall","physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2018-10-12T19:47:44Z","title_canon_sha256":"dfafcb19ae654db0751649b06ada09b98c13c114d653c28c99a286f280ee5cdf"},"schema_version":"1.0","source":{"id":"1810.05701","kind":"arxiv","version":1}},"canonical_sha256":"9e6743708c3a65989b25a60ff48ec0b0f1a37269b589be8e5732eeaf04b074d3","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"9e6743708c3a65989b25a60ff48ec0b0f1a37269b589be8e5732eeaf04b074d3","first_computed_at":"2026-05-17T23:59:57.548605Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-17T23:59:57.548605Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"/63qNsmiBJNWnEJpsKzhV5U+9XXDdEAlZgwWFZy4se4DwZ9zrNnwbgvtc9uCwBbnQglxSYrvayznW3JqRJ23Cw==","signature_status":"signed_v1","signed_at":"2026-05-17T23:59:57.549101Z","signed_message":"canonical_sha256_bytes"},"source_id":"1810.05701","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:a812805f82db510dc2bfaa3030fc7a524193e7fa3cecbdf41943ea476789a140","sha256:7928da0803fcab2b8790ff604293f37e5872d6fbbed09cc234050aab92551988"],"state_sha256":"bfb3af968a8c7d98e7bff032ff990e306122f9d2e2cb2d3f7837fee871a1cbf6"}