{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2023:F24BIKQCNCJHC5ECFV7RZDBWS3","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":"22a3c25de132aa039c6cdbc40db1a77b0fa425e8f3f15c3b14b54fe4b3317fb2","cross_cats_sorted":["cond-mat.soft"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.optics","submitted_at":"2023-10-23T12:54:27Z","title_canon_sha256":"7efc7daf08c344a8354a549b4fec564cd854a0eb0f33686f744913bed0783776"},"schema_version":"1.0","source":{"id":"2310.18352","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2310.18352","created_at":"2026-07-05T08:14:01Z"},{"alias_kind":"arxiv_version","alias_value":"2310.18352v3","created_at":"2026-07-05T08:14:01Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2310.18352","created_at":"2026-07-05T08:14:01Z"},{"alias_kind":"pith_short_12","alias_value":"F24BIKQCNCJH","created_at":"2026-07-05T08:14:01Z"},{"alias_kind":"pith_short_16","alias_value":"F24BIKQCNCJHC5EC","created_at":"2026-07-05T08:14:01Z"},{"alias_kind":"pith_short_8","alias_value":"F24BIKQC","created_at":"2026-07-05T08:14:01Z"}],"graph_snapshots":[{"event_id":"sha256:93c751a673f5a33353547e267e50c71c5bae7d2d30ec0c75ff88a329fc7c0ef1","target":"graph","created_at":"2026-07-05T08:14:01Z","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/2310.18352/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"It has long been understood that dilute samples of chiral molecules such as rarefied gases should exhibit Rayleigh optical activity. We extend the existing theory by accounting for molecular dynamics and correlations, thus obtaining a more general theory of Rayleigh-Brillouin optical activity applicable to dense samples such as neat liquids.","authors_text":"Aidan S. Arnold, Duncan McArthur, Emmanouil I. Alexakis, Robert P. Cameron","cross_cats":["cond-mat.soft"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.optics","submitted_at":"2023-10-23T12:54:27Z","title":"Theory of Rayleigh-Brillouin optical activity light scattering applicable to chiral liquids"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2310.18352","kind":"arxiv","version":3},"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":"sha256:8cde9eb38fb1aaa1946401b405a69a879d00e9d4ed0b29c78b439145bd2c15c0","target":"record","created_at":"2026-07-05T08:14:01Z","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":"22a3c25de132aa039c6cdbc40db1a77b0fa425e8f3f15c3b14b54fe4b3317fb2","cross_cats_sorted":["cond-mat.soft"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.optics","submitted_at":"2023-10-23T12:54:27Z","title_canon_sha256":"7efc7daf08c344a8354a549b4fec564cd854a0eb0f33686f744913bed0783776"},"schema_version":"1.0","source":{"id":"2310.18352","kind":"arxiv","version":3}},"canonical_sha256":"2eb8142a0268927174822d7f1c8c3696dac679467f20bf3e85375fa82b95f1d3","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"2eb8142a0268927174822d7f1c8c3696dac679467f20bf3e85375fa82b95f1d3","first_computed_at":"2026-07-05T08:14:01.951943Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T08:14:01.951943Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"osiWqMiOYN9SzgcV8C/4Q88uCnjgDObBiZ8EcBzmovg3LIFBxyo5UonNK0SrbVByKFn+A7AURzqsbo/KQb3ODQ==","signature_status":"signed_v1","signed_at":"2026-07-05T08:14:01.952397Z","signed_message":"canonical_sha256_bytes"},"source_id":"2310.18352","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:8cde9eb38fb1aaa1946401b405a69a879d00e9d4ed0b29c78b439145bd2c15c0","sha256:93c751a673f5a33353547e267e50c71c5bae7d2d30ec0c75ff88a329fc7c0ef1"],"state_sha256":"b5127efe97f1ec4e9466638da3c3f6076c1c55e7be6679edb14ed20df2227e0b"}