{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2015:GZRJCETLKSUI5PCFLOWV43QE2Q","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":"0f14edf170467cde0d88fcc06e1977c3679fe49c2bee3050b56b11d647f25f12","cross_cats_sorted":["cond-mat.mes-hall","physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2015-11-13T21:02:08Z","title_canon_sha256":"b5a388d091e670ace91e3201d358612794b9b391241487a9301d020dcd0353c6"},"schema_version":"1.0","source":{"id":"1511.04456","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1511.04456","created_at":"2026-05-18T01:02:28Z"},{"alias_kind":"arxiv_version","alias_value":"1511.04456v2","created_at":"2026-05-18T01:02:28Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1511.04456","created_at":"2026-05-18T01:02:28Z"},{"alias_kind":"pith_short_12","alias_value":"GZRJCETLKSUI","created_at":"2026-05-18T12:29:22Z"},{"alias_kind":"pith_short_16","alias_value":"GZRJCETLKSUI5PCF","created_at":"2026-05-18T12:29:22Z"},{"alias_kind":"pith_short_8","alias_value":"GZRJCETL","created_at":"2026-05-18T12:29:22Z"}],"graph_snapshots":[{"event_id":"sha256:0f7240f085276cd423ff4db1db294da730bdb7b48b0868537d8c3d0867723430","target":"graph","created_at":"2026-05-18T01:02:28Z","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":"Single-crystal diamond cavity optomechanical devices are a promising example of a hybrid quantum system: by coupling mechanical resonances to both light and electron spins, they can enable new ways for photons to control solid state qubits. However, realizing cavity optomechanical devices from high quality diamond chips has been an outstanding challenge. Here we demonstrate single-crystal diamond cavity optomechanical devices that can enable photon-phonon-spin coupling. Cavity optomechanical coupling to $2\\,\\text{GHz}$ frequency ($f_\\text{m}$) mechanical resonances is observed. In room tempera","authors_text":"Behzad Khanaliloo, David P. Lake, J.P. Hadden, Matthew Mitchell, Paul E. Barclay, Tamiko Masuda","cross_cats":["cond-mat.mes-hall","physics.optics"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2015-11-13T21:02:08Z","title":"Single-crystal diamond low-dissipation cavity optomechanics"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1511.04456","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":"sha256:3bb9e4d943d722ecba7a6ffa5299179d0de862ae50b9c158413acd0b092a69be","target":"record","created_at":"2026-05-18T01:02:28Z","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":"0f14edf170467cde0d88fcc06e1977c3679fe49c2bee3050b56b11d647f25f12","cross_cats_sorted":["cond-mat.mes-hall","physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2015-11-13T21:02:08Z","title_canon_sha256":"b5a388d091e670ace91e3201d358612794b9b391241487a9301d020dcd0353c6"},"schema_version":"1.0","source":{"id":"1511.04456","kind":"arxiv","version":2}},"canonical_sha256":"366291126b54a88ebc455bad5e6e04d43d3de9b6c28c3e1f68933119677498b6","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"366291126b54a88ebc455bad5e6e04d43d3de9b6c28c3e1f68933119677498b6","first_computed_at":"2026-05-18T01:02:28.902012Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:02:28.902012Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"GdNiGHuQ4dG3Ckr0x8bXG1Q0qx1XHeoBG5nHJoofimp1wl/aSM+ioSvn0NCd7sajpHXhotZKYZywvoxjeABCCw==","signature_status":"signed_v1","signed_at":"2026-05-18T01:02:28.902557Z","signed_message":"canonical_sha256_bytes"},"source_id":"1511.04456","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:3bb9e4d943d722ecba7a6ffa5299179d0de862ae50b9c158413acd0b092a69be","sha256:0f7240f085276cd423ff4db1db294da730bdb7b48b0868537d8c3d0867723430"],"state_sha256":"561471355e382fbd20f0df28e6fa1c8e7e315bdba6e2c1b9021dbcd7af905899"}