{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2023:SWVCWQAR6ADSJKNHGUWDNSOCZE","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":"e751aee62b46c8ba15e65037a8e5b8d2b9547d4843dbaa0bd299c32df94e79a4","cross_cats_sorted":["cond-mat.mes-hall"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.optics","submitted_at":"2023-01-04T03:13:53Z","title_canon_sha256":"e66b94a66f7c019e2dc636a2ad5d4b8c821ac41fa24441ecbd5f5f404093cc9c"},"schema_version":"1.0","source":{"id":"2301.01418","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2301.01418","created_at":"2026-07-05T06:15:21Z"},{"alias_kind":"arxiv_version","alias_value":"2301.01418v2","created_at":"2026-07-05T06:15:21Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2301.01418","created_at":"2026-07-05T06:15:21Z"},{"alias_kind":"pith_short_12","alias_value":"SWVCWQAR6ADS","created_at":"2026-07-05T06:15:21Z"},{"alias_kind":"pith_short_16","alias_value":"SWVCWQAR6ADSJKNH","created_at":"2026-07-05T06:15:21Z"},{"alias_kind":"pith_short_8","alias_value":"SWVCWQAR","created_at":"2026-07-05T06:15:21Z"}],"graph_snapshots":[{"event_id":"sha256:796c0525421e3e61e078c96cb5089b70653ea3116cd01fe1238eeb9c4edf3f55","target":"graph","created_at":"2026-07-05T06:15:21Z","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/2301.01418/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We propose a magnetic laser in a subwavelength system consisting of a high-refractive-index dielectric cavity and an active medium formed by magnetic quantum emitters. Stimulated emissions of magnetic quantum emitters induced by their coherent interactions with quantized magnetic fields of a cavity are theoretically considered. The condition to archive such a magnetic laser is obtained. Numerical results show that magnetic lasers are feasible in some realistic systems, for example, a silicon disk of high-quality whispering gallery modes with embedded emitters. Furthermore, the competitions bet","authors_text":"Jun He, Ma-Long Hu, Xiao-Jing Du, Zhong-Jian Yang","cross_cats":["cond-mat.mes-hall"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.optics","submitted_at":"2023-01-04T03:13:53Z","title":"Magnetic light amplification by stimulated emission of radiation in subwavelength systems of a dielectric cavity and magnetic quantum emitters"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2301.01418","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:cacddda1f0337d1873767a34d043d6be585b3c321bee124f63499bec9130a6e0","target":"record","created_at":"2026-07-05T06:15:21Z","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":"e751aee62b46c8ba15e65037a8e5b8d2b9547d4843dbaa0bd299c32df94e79a4","cross_cats_sorted":["cond-mat.mes-hall"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.optics","submitted_at":"2023-01-04T03:13:53Z","title_canon_sha256":"e66b94a66f7c019e2dc636a2ad5d4b8c821ac41fa24441ecbd5f5f404093cc9c"},"schema_version":"1.0","source":{"id":"2301.01418","kind":"arxiv","version":2}},"canonical_sha256":"95aa2b4011f00724a9a7352c36c9c2c91d51a319bb26b28aa2b4fa26eb66570e","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"95aa2b4011f00724a9a7352c36c9c2c91d51a319bb26b28aa2b4fa26eb66570e","first_computed_at":"2026-07-05T06:15:21.409944Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T06:15:21.409944Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"1h8iO62ZfcEq5dIC2cp0EIBYRW+xKsSwAsI/cVwfB9dW5ps86RZxCuWRyaE6P0nzg84sKxNQ9f8aIICwdkdiCQ==","signature_status":"signed_v1","signed_at":"2026-07-05T06:15:21.410434Z","signed_message":"canonical_sha256_bytes"},"source_id":"2301.01418","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:cacddda1f0337d1873767a34d043d6be585b3c321bee124f63499bec9130a6e0","sha256:796c0525421e3e61e078c96cb5089b70653ea3116cd01fe1238eeb9c4edf3f55"],"state_sha256":"eb0319b4ca882f3c86d19c458fcd21449f0aa574f47c7027526055a68140eb8e"}