{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2025:MSW4BE4ZO34OZSDOK56YTQNPYI","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":"987c9d87eb5b59fc201c9287fbdb57ac0eaadec9fbdcd80e80009dcdce21c946","cross_cats_sorted":["cond-mat.mes-hall"],"license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","primary_cat":"physics.optics","submitted_at":"2025-09-05T02:40:46Z","title_canon_sha256":"4f028ba61c25920274c2a5e111a4b4f076eb88738560458642df9e51ba71d203"},"schema_version":"1.0","source":{"id":"2509.04760","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2509.04760","created_at":"2026-06-19T16:12:14Z"},{"alias_kind":"arxiv_version","alias_value":"2509.04760v2","created_at":"2026-06-19T16:12:14Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2509.04760","created_at":"2026-06-19T16:12:14Z"},{"alias_kind":"pith_short_12","alias_value":"MSW4BE4ZO34O","created_at":"2026-06-19T16:12:14Z"},{"alias_kind":"pith_short_16","alias_value":"MSW4BE4ZO34OZSDO","created_at":"2026-06-19T16:12:14Z"},{"alias_kind":"pith_short_8","alias_value":"MSW4BE4Z","created_at":"2026-06-19T16:12:14Z"}],"graph_snapshots":[{"event_id":"sha256:75c166b1db0a1d9348643f06a1d36843ec1e056955573f7c8b2d8c20747dab81","target":"graph","created_at":"2026-06-19T16:12:14Z","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/2509.04760/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Photoluminescent color centers in diamond and hexagonal boron nitride (hBN) are powerful nanoscale solid-state quantum sensors that are explored in a plethora of quantum technologies. Methods for integrating them into macroscopic structures that improve their sensitivity and enable their large-scale deployment are highly sought after. Here, we demonstrate cavity-enhanced photoluminescence (PL) of fluorescent nanodiamonds (FNDs) and hBN nanoparticles (NPs) embedded in polymer-based thin-film optical cavities on the centimeter scale. The cavity resonances efficiently modulate the spectral PL pea","authors_text":"Daniel E. G\\'omez, Daniel J. Tibben, David A. Broadway, Jean-Philippe Tetienne, Philipp Reineck, Roy Styles","cross_cats":["cond-mat.mes-hall"],"headline":"","license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","primary_cat":"physics.optics","submitted_at":"2025-09-05T02:40:46Z","title":"A scalable method for cavity-enhanced solid-state quantum sensors"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2509.04760","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:e3446d5e720e4d61b3121fdfc1675a8e2ffd3e1ac8d5328059aa084f44c3f2b0","target":"record","created_at":"2026-06-19T16:12:14Z","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":"987c9d87eb5b59fc201c9287fbdb57ac0eaadec9fbdcd80e80009dcdce21c946","cross_cats_sorted":["cond-mat.mes-hall"],"license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","primary_cat":"physics.optics","submitted_at":"2025-09-05T02:40:46Z","title_canon_sha256":"4f028ba61c25920274c2a5e111a4b4f076eb88738560458642df9e51ba71d203"},"schema_version":"1.0","source":{"id":"2509.04760","kind":"arxiv","version":2}},"canonical_sha256":"64adc0939976f8ecc86e577d89c1afc2165e4d9266198fb3f53f193946e2010a","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"64adc0939976f8ecc86e577d89c1afc2165e4d9266198fb3f53f193946e2010a","first_computed_at":"2026-06-19T16:12:14.977994Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-06-19T16:12:14.977994Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"4rZrXEjczVYITNgIF6IFRwZ26kTBJ25nE5oU1ZNVhBYnJypEwdqEgSl72+PyEUjLscjpe2mMlAcvheanUCC8CA==","signature_status":"signed_v1","signed_at":"2026-06-19T16:12:14.978367Z","signed_message":"canonical_sha256_bytes"},"source_id":"2509.04760","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:e3446d5e720e4d61b3121fdfc1675a8e2ffd3e1ac8d5328059aa084f44c3f2b0","sha256:75c166b1db0a1d9348643f06a1d36843ec1e056955573f7c8b2d8c20747dab81"],"state_sha256":"8ba36cdd803a69e874146a106867e7bdf8772b6b1ffd167bee1a14d1c3c960f8"}