{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2021:TJD7HY5GC34M4I7XR5TXZCCWVX","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":"af83fad7e44960562a360f8dcb35b53ab23db94dbb75860a2be822021e164dd4","cross_cats_sorted":["cond-mat.mtrl-sci","physics.optics","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2021-11-29T19:51:27Z","title_canon_sha256":"21d442d4fcfe36c3f47c1a65a9f8e51be6f30ca1606b5005addbfa0f84d51f60"},"schema_version":"1.0","source":{"id":"2111.14921","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2111.14921","created_at":"2026-07-05T07:16:30Z"},{"alias_kind":"arxiv_version","alias_value":"2111.14921v1","created_at":"2026-07-05T07:16:30Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2111.14921","created_at":"2026-07-05T07:16:30Z"},{"alias_kind":"pith_short_12","alias_value":"TJD7HY5GC34M","created_at":"2026-07-05T07:16:30Z"},{"alias_kind":"pith_short_16","alias_value":"TJD7HY5GC34M4I7X","created_at":"2026-07-05T07:16:30Z"},{"alias_kind":"pith_short_8","alias_value":"TJD7HY5G","created_at":"2026-07-05T07:16:30Z"}],"graph_snapshots":[{"event_id":"sha256:ca3ac9b94fb567e852a37d02d482ada0b1ca09ae12bc3cd02cb88a18855d5003","target":"graph","created_at":"2026-07-05T07:16:30Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2111.14921/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Milled nanodiamonds containing nitrogen-vacancy (NV) centers provide an excellent platform for sensing applications as they are optically robust, have nanoscale quantum sensitivity, and form colloidal dispersions which enable bottom-up assembly techniques for device integration. However, variations in their size, shape, and surface chemistry limit the ability to position individual nanodiamonds and statistically study properties that affect their optical and quantum characteristics. Here, we present a scalable strategy to form ordered arrays of nanodiamonds using capillary-driven, template-ass","authors_text":"Cherie R. Kagan, Henry J. Shulevitz, Jun Xu, Lee C. Bassett, Raj N. Patel, Steven Neuhaus, Tzu-Yung Huang","cross_cats":["cond-mat.mtrl-sci","physics.optics","quant-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2021-11-29T19:51:27Z","title":"Template-Assisted Self Assembly of Fluorescent Nanodiamonds for Scalable Quantum Technologies"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2111.14921","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":"sha256:256581674d11da8dc771d417b3b316524534e1977e93afbad7eb793bc0f9d3d6","target":"record","created_at":"2026-07-05T07:16:30Z","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":"af83fad7e44960562a360f8dcb35b53ab23db94dbb75860a2be822021e164dd4","cross_cats_sorted":["cond-mat.mtrl-sci","physics.optics","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2021-11-29T19:51:27Z","title_canon_sha256":"21d442d4fcfe36c3f47c1a65a9f8e51be6f30ca1606b5005addbfa0f84d51f60"},"schema_version":"1.0","source":{"id":"2111.14921","kind":"arxiv","version":1}},"canonical_sha256":"9a47f3e3a616f8ce23f78f677c8856adda95d680fa89bbc0f0f0d785387c7296","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"9a47f3e3a616f8ce23f78f677c8856adda95d680fa89bbc0f0f0d785387c7296","first_computed_at":"2026-07-05T07:16:30.926880Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T07:16:30.926880Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"87aO2hRjlHiW0WVXEOYUbX+27BOsC6FwXGhQYOK0ZXjyXQijjSdorGPBk6dzBP/cm4Q20IMzlkiP+sQgf8ZTBw==","signature_status":"signed_v1","signed_at":"2026-07-05T07:16:30.927349Z","signed_message":"canonical_sha256_bytes"},"source_id":"2111.14921","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:256581674d11da8dc771d417b3b316524534e1977e93afbad7eb793bc0f9d3d6","sha256:ca3ac9b94fb567e852a37d02d482ada0b1ca09ae12bc3cd02cb88a18855d5003"],"state_sha256":"f6a36cb867e54a16ce073ceaa75f3892c4578004bae1f585109a95f2eaf1fdae"}