{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2022:MV72NAOI4XEKB6L5GY25QM7PB3","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":"dece624d4c60dc6d4e80b0a2a62ab88cf01a54c0cc22091acf9207c7f552958b","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.atom-ph","submitted_at":"2022-12-06T20:09:11Z","title_canon_sha256":"5e5bfe3edf33fe52b4b046324e327e54e515e544defcfec6b0c360e88411e19f"},"schema_version":"1.0","source":{"id":"2212.03304","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2212.03304","created_at":"2026-07-05T06:57:20Z"},{"alias_kind":"arxiv_version","alias_value":"2212.03304v2","created_at":"2026-07-05T06:57:20Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2212.03304","created_at":"2026-07-05T06:57:20Z"},{"alias_kind":"pith_short_12","alias_value":"MV72NAOI4XEK","created_at":"2026-07-05T06:57:20Z"},{"alias_kind":"pith_short_16","alias_value":"MV72NAOI4XEKB6L5","created_at":"2026-07-05T06:57:20Z"},{"alias_kind":"pith_short_8","alias_value":"MV72NAOI","created_at":"2026-07-05T06:57:20Z"}],"graph_snapshots":[{"event_id":"sha256:aa9a911607fea46ad8586609d5e9d238ee39c3dc012b54256ed3d4ff2d407015","target":"graph","created_at":"2026-07-05T06:57:20Z","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/2212.03304/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Radio frequencies in the HF and VHF (3 MHz to 300 MHz) bands are challenging for Rydberg atom-based detection schemes, as resonant detection requires exciting the atoms to extremely high energy states. We demonstrate a method for detecting and measuring radio frequency (RF) carriers in the HF and VHF bands via a controlled Autler-Townes line splitting. Using a resonant, high-frequency (GHz) RF field, the absorption signal from Townes-Merrit sidebands created by a low frequency, non-resonant RF field can be enhanced. Notably, this technique uses a measurement of the optical frequency separation","authors_text":"Alexandra B. Artusio-Glimpse, Andrew P. Rotunno, Christopher L. Holloway, C. S. Adams, Maitreyi Jayaseelan, Matthew T. Simons, Nikunjkumar Prajapati, Robert M. Potvliege, Samuel Berweger","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.atom-ph","submitted_at":"2022-12-06T20:09:11Z","title":"Detection of HF and VHF Fields through Floquet Sideband Gaps by `Rabi Matching' Dressed Rydberg Atoms"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2212.03304","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":"sha256:3d4a7549c5326ddc6cf52782c36df50571e0bdb864ad5ccb4518079dbbd342e6","target":"record","created_at":"2026-07-05T06:57:20Z","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":"dece624d4c60dc6d4e80b0a2a62ab88cf01a54c0cc22091acf9207c7f552958b","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.atom-ph","submitted_at":"2022-12-06T20:09:11Z","title_canon_sha256":"5e5bfe3edf33fe52b4b046324e327e54e515e544defcfec6b0c360e88411e19f"},"schema_version":"1.0","source":{"id":"2212.03304","kind":"arxiv","version":2}},"canonical_sha256":"657fa681c8e5c8a0f97d3635d833ef0ed61552cc710ab6efa36447ef98198d01","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"657fa681c8e5c8a0f97d3635d833ef0ed61552cc710ab6efa36447ef98198d01","first_computed_at":"2026-07-05T06:57:20.453724Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T06:57:20.453724Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"EIizoYuwnGxkCCh+0y55UwOQfZVtDbSWsO+ShjIVB7tMvr8j8VTPAQGZSINM6Sp2JhxqW3PG8tFVyKUhKtJGCw==","signature_status":"signed_v1","signed_at":"2026-07-05T06:57:20.454222Z","signed_message":"canonical_sha256_bytes"},"source_id":"2212.03304","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:3d4a7549c5326ddc6cf52782c36df50571e0bdb864ad5ccb4518079dbbd342e6","sha256:aa9a911607fea46ad8586609d5e9d238ee39c3dc012b54256ed3d4ff2d407015"],"state_sha256":"55c3af9132ab4d6ded4ccea7b6d972951f6ded5472d068b2d62f8f8b10852f7c"}