{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2024:VBVWLOEHBPQPZG7GYU7ESMTH45","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":"62fce79dc6f358f92ba9f542b7756edbf8ea169ca5dd1eb6a58cea0357edd0f4","cross_cats_sorted":["physics.optics","quant-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.atom-ph","submitted_at":"2024-12-10T16:13:48Z","title_canon_sha256":"71340a18344decec5ce0ae45c9dd2b3332b4d01f14cdc5c3b394be7d2d3610ed"},"schema_version":"1.0","source":{"id":"2412.07632","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2412.07632","created_at":"2026-07-05T11:10:33Z"},{"alias_kind":"arxiv_version","alias_value":"2412.07632v2","created_at":"2026-07-05T11:10:33Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2412.07632","created_at":"2026-07-05T11:10:33Z"},{"alias_kind":"pith_short_12","alias_value":"VBVWLOEHBPQP","created_at":"2026-07-05T11:10:33Z"},{"alias_kind":"pith_short_16","alias_value":"VBVWLOEHBPQPZG7G","created_at":"2026-07-05T11:10:33Z"},{"alias_kind":"pith_short_8","alias_value":"VBVWLOEH","created_at":"2026-07-05T11:10:33Z"}],"graph_snapshots":[{"event_id":"sha256:1e05853f55dd29c45f2c9eb7014be7d323cb03339f3fbdd7fe0771e6d4e78e72","target":"graph","created_at":"2026-07-05T11:10:33Z","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/2412.07632/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"The development of novel radio frequency atomic receivers brings attention to the theoretical description of atom-light interactions in sophisticated, multilevel schemes. Of special interest, are the schemes where several interaction paths interfere with each other, bringing about the phase-sensitive measurement of detected radio fields. In the theoretical modeling of those cases, the common assumptions are often insufficient to determine the boundary detection parameters, such as receiving bandwidth or saturation point, critical for practical considerations of atomic sensing technology. This ","authors_text":"Bartosz Kasza, Micha{\\l} Parniak, Sebastian Bor\\'owka, Wojciech Wasilewski","cross_cats":["physics.optics","quant-ph"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.atom-ph","submitted_at":"2024-12-10T16:13:48Z","title":"Atomic-optical interferometry in fractured loops: a general solution for Rydberg radio frequency receivers"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2412.07632","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":"sha256:2eb2b62bc37a1ba54db76ae0a8f2808eb6e92583f969208e42d25458405c9d97","target":"record","created_at":"2026-07-05T11:10:33Z","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":"62fce79dc6f358f92ba9f542b7756edbf8ea169ca5dd1eb6a58cea0357edd0f4","cross_cats_sorted":["physics.optics","quant-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.atom-ph","submitted_at":"2024-12-10T16:13:48Z","title_canon_sha256":"71340a18344decec5ce0ae45c9dd2b3332b4d01f14cdc5c3b394be7d2d3610ed"},"schema_version":"1.0","source":{"id":"2412.07632","kind":"arxiv","version":2}},"canonical_sha256":"a86b65b8870be0fc9be6c53e493267e777bdb3c094d2a489dd2a9e200f2cf3ae","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"a86b65b8870be0fc9be6c53e493267e777bdb3c094d2a489dd2a9e200f2cf3ae","first_computed_at":"2026-07-05T11:10:33.675144Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T11:10:33.675144Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"MPU6kIuD6Q9erS2YIRkKf9pndCZd595BnMu5RSyvvmqTW52znPfnWY0O1qiu6zsD11DcP6rEf3YqiWrat3vUDA==","signature_status":"signed_v1","signed_at":"2026-07-05T11:10:33.675647Z","signed_message":"canonical_sha256_bytes"},"source_id":"2412.07632","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:2eb2b62bc37a1ba54db76ae0a8f2808eb6e92583f969208e42d25458405c9d97","sha256:1e05853f55dd29c45f2c9eb7014be7d323cb03339f3fbdd7fe0771e6d4e78e72"],"state_sha256":"42f5b69426ad1711c4ba715feeed2bc2623c94094b332c4dd07c9542aee36768"}