{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2022:SNPPCYARA5GWCX2PAGUDRYK7DJ","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":"65206e247214cf9af493f3c279d362238c5550952789223e4a52a75f133e7c96","cross_cats_sorted":["cond-mat.mtrl-sci","physics.optics"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.str-el","submitted_at":"2022-11-14T10:04:47Z","title_canon_sha256":"087c90d517578532507a39d9efcad4f4dea57203114cec5aad7d799ba3e265fa"},"schema_version":"1.0","source":{"id":"2211.07247","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2211.07247","created_at":"2026-07-05T08:24:35Z"},{"alias_kind":"arxiv_version","alias_value":"2211.07247v1","created_at":"2026-07-05T08:24:35Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2211.07247","created_at":"2026-07-05T08:24:35Z"},{"alias_kind":"pith_short_12","alias_value":"SNPPCYARA5GW","created_at":"2026-07-05T08:24:35Z"},{"alias_kind":"pith_short_16","alias_value":"SNPPCYARA5GWCX2P","created_at":"2026-07-05T08:24:35Z"},{"alias_kind":"pith_short_8","alias_value":"SNPPCYAR","created_at":"2026-07-05T08:24:35Z"}],"graph_snapshots":[{"event_id":"sha256:4ca44ab10a307e4c122915898479c53386971a192ce7a2ea21764147499ce397","target":"graph","created_at":"2026-07-05T08:24:35Z","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/2211.07247/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Harnessing the enhanced light-matter coupling and quantum vacuum fluctuations resulting from mode volume compression in optical cavities is a promising route towards functionalizing quantum materials and realizing exotic states of matter. Here, we extend cavity quantum electrodynamical materials engineering to correlated magnetic systems, by demonstrating that a Fabry-P\\'erot cavity can be used to control the magnetic state of the proximate quantum spin liquid $\\alpha$-RuCl$_3$. Depending on specific cavity properties such as the mode frequency, photon occupation, and strength of the light-mat","authors_text":"Adithya Sriram, Angel Rubio, Emil Vinas Bostr\\\"om, Martin Claassen","cross_cats":["cond-mat.mtrl-sci","physics.optics"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.str-el","submitted_at":"2022-11-14T10:04:47Z","title":"Controlling the magnetic state of the proximate quantum spin liquid $\\alpha$-RuCl$_3$ with an optical cavity"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2211.07247","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:d05154bde3d34510a1dde0eb2ce9bc2b3c1f00fc0149e11c043df9e6b21629af","target":"record","created_at":"2026-07-05T08:24:35Z","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":"65206e247214cf9af493f3c279d362238c5550952789223e4a52a75f133e7c96","cross_cats_sorted":["cond-mat.mtrl-sci","physics.optics"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.str-el","submitted_at":"2022-11-14T10:04:47Z","title_canon_sha256":"087c90d517578532507a39d9efcad4f4dea57203114cec5aad7d799ba3e265fa"},"schema_version":"1.0","source":{"id":"2211.07247","kind":"arxiv","version":1}},"canonical_sha256":"935ef16011074d615f4f01a838e15f1a4c1225770512bce720987c316034ad6c","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"935ef16011074d615f4f01a838e15f1a4c1225770512bce720987c316034ad6c","first_computed_at":"2026-07-05T08:24:35.430648Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T08:24:35.430648Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Mfn2PLZ7hDz696WMkFHg0Fv2N84NH/P8WMtG/KY+0bNxWsEj/XERoai5AeOGzHYYASsCT8mA3PlAsRwBjJtJCA==","signature_status":"signed_v1","signed_at":"2026-07-05T08:24:35.431205Z","signed_message":"canonical_sha256_bytes"},"source_id":"2211.07247","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:d05154bde3d34510a1dde0eb2ce9bc2b3c1f00fc0149e11c043df9e6b21629af","sha256:4ca44ab10a307e4c122915898479c53386971a192ce7a2ea21764147499ce397"],"state_sha256":"4b499898c1d18174641fdec4d0d5fa3eb3d5228c21c54e5fdf28457776571b1a"}