{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:UBGQJDFJVOIDAIQQTBRJFIWXCC","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":"728f5ae4d78c2e40c985856c165b956093180c5cc51f018ea661cf4759a0a6bb","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2017-11-16T11:19:45Z","title_canon_sha256":"01c2e17612f82d10592e2606308b27f798fcf475143306763673a25abcccf516"},"schema_version":"1.0","source":{"id":"1711.06028","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1711.06028","created_at":"2026-05-18T00:17:42Z"},{"alias_kind":"arxiv_version","alias_value":"1711.06028v1","created_at":"2026-05-18T00:17:42Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1711.06028","created_at":"2026-05-18T00:17:42Z"},{"alias_kind":"pith_short_12","alias_value":"UBGQJDFJVOID","created_at":"2026-05-18T12:31:46Z"},{"alias_kind":"pith_short_16","alias_value":"UBGQJDFJVOIDAIQQ","created_at":"2026-05-18T12:31:46Z"},{"alias_kind":"pith_short_8","alias_value":"UBGQJDFJ","created_at":"2026-05-18T12:31:46Z"}],"graph_snapshots":[{"event_id":"sha256:94017fb5e45e9c7f75717dd655f5955dd88f99a02a9c27ee00c3b1003bd85119","target":"graph","created_at":"2026-05-18T00:17:42Z","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"},"paper":{"abstract_excerpt":"We analyze nonlinear magneto-optical rotation (NMOR) in rubidium vapor subjected to continuously-scanned magnetic field. By varying magnetic-field sweep rate, a transition from traditionally-observed dispersive-like NMOR signals (low sweep rate) to oscillating signals (higher sweep rates) is demonstrated. The transient oscillatory behavior is studied versus light and magnetic-field parameters, revealing a strong dependence of the signals on magnetic-sweep rate and light intensity. The experimental results are supported with density-matrix calculations, which enable quantitative analysis of the","authors_text":"A. Rybak, M. Florkowski, R. S. Grewal, S. Pustelny","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2017-11-16T11:19:45Z","title":"Transient dynamics of nonlinear magneto-optical rotation"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1711.06028","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:f00a7460ea60255bfc182c178d4317c96cf1fce71f34adb738d612436dfed28f","target":"record","created_at":"2026-05-18T00:17:42Z","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":"728f5ae4d78c2e40c985856c165b956093180c5cc51f018ea661cf4759a0a6bb","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2017-11-16T11:19:45Z","title_canon_sha256":"01c2e17612f82d10592e2606308b27f798fcf475143306763673a25abcccf516"},"schema_version":"1.0","source":{"id":"1711.06028","kind":"arxiv","version":1}},"canonical_sha256":"a04d048ca9ab90302210986292a2d7109627cc79bd4c2f5c24222cc67494b111","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"a04d048ca9ab90302210986292a2d7109627cc79bd4c2f5c24222cc67494b111","first_computed_at":"2026-05-18T00:17:42.320309Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:17:42.320309Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"jN//9TPS1haj3VaKiTKmdC+4KxjZd9sMdpvT7GtqoGG3L6yROH/NFV1iVH6ikyWZAPmmDJx8yjFFF6DOt8JWCA==","signature_status":"signed_v1","signed_at":"2026-05-18T00:17:42.321024Z","signed_message":"canonical_sha256_bytes"},"source_id":"1711.06028","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:f00a7460ea60255bfc182c178d4317c96cf1fce71f34adb738d612436dfed28f","sha256:94017fb5e45e9c7f75717dd655f5955dd88f99a02a9c27ee00c3b1003bd85119"],"state_sha256":"14cde3b47df84bf1ffcf7b874e5105c2b45479392710aa9b1b50e7deb53f61af"}