{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2019:TPJB72PSF64GKEOZE43ZBE6CVG","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":"8cda4e213890674ccdff24b0ec273be1a3b8d0824ed337502702fbc2602f58da","cross_cats_sorted":["physics.chem-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2019-08-20T22:01:28Z","title_canon_sha256":"80959a3734f42973fa04e87e50e142aee91d5d6b0f556bf15cd388e9929ed7bc"},"schema_version":"1.0","source":{"id":"1908.07627","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1908.07627","created_at":"2026-07-04T23:58:59Z"},{"alias_kind":"arxiv_version","alias_value":"1908.07627v1","created_at":"2026-07-04T23:58:59Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1908.07627","created_at":"2026-07-04T23:58:59Z"},{"alias_kind":"pith_short_12","alias_value":"TPJB72PSF64G","created_at":"2026-07-04T23:58:59Z"},{"alias_kind":"pith_short_16","alias_value":"TPJB72PSF64GKEOZ","created_at":"2026-07-04T23:58:59Z"},{"alias_kind":"pith_short_8","alias_value":"TPJB72PS","created_at":"2026-07-04T23:58:59Z"}],"graph_snapshots":[{"event_id":"sha256:6a3be10405689ba471e38361860d0d3b66ffe9c7f675dd9b59578d6d21e51eef","target":"graph","created_at":"2026-07-04T23:58:59Z","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/1908.07627/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Resonant mm-wave fields drive $n_0f(2) \\rightarrow (n_0 \\pm 1)g(2)$ transitions in a state-selected $n_0f(2)$ Rydberg gas of NO. This transformation produces a clear signature in the selected field ionization spectrum and dramatically increases the intensity of corresponding features in the spectrum of the $n_0f(2)$ Rydberg series observed in UV-UV double resonant transitions via the $A ~^2\\Sigma^+, ~N'=0$ state. Here, $n_0$ refers to the principal quantum number of an $f$ Rydberg state converging to the $N^+=2$ rotational state of NO$^+ X~ ^1\\Sigma^+$. Enhancement owing to transitions from $\\","authors_text":"Edward R. Grant, Fernanda Banic Viana Martins, James S. Keller","cross_cats":["physics.chem-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2019-08-20T22:01:28Z","title":"Control of molecular ultracold plasma relaxation dynamics by mm-wave Rydberg-Rydberg transitions"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1908.07627","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":"sha256:8b0738a47fa3d5c25af459f5decd335f361a6ba195e62a370606bc1566758778","target":"record","created_at":"2026-07-04T23:58:59Z","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":"8cda4e213890674ccdff24b0ec273be1a3b8d0824ed337502702fbc2602f58da","cross_cats_sorted":["physics.chem-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2019-08-20T22:01:28Z","title_canon_sha256":"80959a3734f42973fa04e87e50e142aee91d5d6b0f556bf15cd388e9929ed7bc"},"schema_version":"1.0","source":{"id":"1908.07627","kind":"arxiv","version":1}},"canonical_sha256":"9bd21fe9f22fb86511d927379093c2a9a380cc606f3090e7156f867196c89fa9","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"9bd21fe9f22fb86511d927379093c2a9a380cc606f3090e7156f867196c89fa9","first_computed_at":"2026-07-04T23:58:59.808151Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T23:58:59.808151Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"T3xCcFjPLKfwDQh7pp+nCK8z5EDpJjy2ILtNZTsUTOU5IgBE9K15U2v4Nj8i/yhruE3uhJObxdcKNkS7legrDA==","signature_status":"signed_v1","signed_at":"2026-07-04T23:58:59.808521Z","signed_message":"canonical_sha256_bytes"},"source_id":"1908.07627","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:8b0738a47fa3d5c25af459f5decd335f361a6ba195e62a370606bc1566758778","sha256:6a3be10405689ba471e38361860d0d3b66ffe9c7f675dd9b59578d6d21e51eef"],"state_sha256":"ba125b394386e1071b6ac9aebda236f1ac89f4147d4212a9e4628cc0964ef4f0"}