{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:RD4B4HG2TUTERO2T2TEEPUXDE2","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":"ac37f6bbdfce8fb45f67eaba565b4b66da723adf540365bf7abc34d1eaf00ec9","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2018-08-01T15:43:23Z","title_canon_sha256":"5562b88130c01d412d7263bdcd28abdcf892ba0c9871bc97c814b001b3e6d254"},"schema_version":"1.0","source":{"id":"1808.00384","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1808.00384","created_at":"2026-05-18T00:09:06Z"},{"alias_kind":"arxiv_version","alias_value":"1808.00384v1","created_at":"2026-05-18T00:09:06Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1808.00384","created_at":"2026-05-18T00:09:06Z"},{"alias_kind":"pith_short_12","alias_value":"RD4B4HG2TUTE","created_at":"2026-05-18T12:32:50Z"},{"alias_kind":"pith_short_16","alias_value":"RD4B4HG2TUTERO2T","created_at":"2026-05-18T12:32:50Z"},{"alias_kind":"pith_short_8","alias_value":"RD4B4HG2","created_at":"2026-05-18T12:32:50Z"}],"graph_snapshots":[{"event_id":"sha256:f66b51e6d558f6e0d4cbaa31cc9bd06b42f9cb0f3b0ed5ad698a937e58413484","target":"graph","created_at":"2026-05-18T00:09:06Z","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":"Precision measurements of parity non-conserving (PNC) interactions in atoms, molecules and ions can lead to the discovery of new physics beyond the standard model and understanding of weak-force induced interactions in the nucleus. In this paper, we propose and analyze a novel atomic parity violation measurement scheme for a forbidden transition where we combine a two-pathway coherent control mechanism with probe gain techniques. We detail a feasible experimental geometry for $6S_{1/2}\\rightarrow 7S_{1/2}$ transitions in a cesium vapor cell, and consider the statistical noise of such a measure","authors_text":"A. Damitz, D. S. Elliott, George Toh, J. Choi, R. T. Sutherland","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2018-08-01T15:43:23Z","title":"Gain measurement scheme for precise determination of atomic parity violation through two-pathway coherent control"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1808.00384","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:be084bebd01f3e6dbabbf221c6fdd4dbe979ff5b553be9da147d9fd02dd6012f","target":"record","created_at":"2026-05-18T00:09:06Z","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":"ac37f6bbdfce8fb45f67eaba565b4b66da723adf540365bf7abc34d1eaf00ec9","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2018-08-01T15:43:23Z","title_canon_sha256":"5562b88130c01d412d7263bdcd28abdcf892ba0c9871bc97c814b001b3e6d254"},"schema_version":"1.0","source":{"id":"1808.00384","kind":"arxiv","version":1}},"canonical_sha256":"88f81e1cda9d2648bb53d4c847d2e326b73c7666b24640c1c810ad5804751b4b","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"88f81e1cda9d2648bb53d4c847d2e326b73c7666b24640c1c810ad5804751b4b","first_computed_at":"2026-05-18T00:09:06.251245Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:09:06.251245Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"LGMTBTtmhjUvYV9z1BXrJf2qiCT6QUbxIfmxQN2ji84d1oA17wGfsTx1f1wETnRnN1fKXbfMjL6AKV3FtlGGCQ==","signature_status":"signed_v1","signed_at":"2026-05-18T00:09:06.252025Z","signed_message":"canonical_sha256_bytes"},"source_id":"1808.00384","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:be084bebd01f3e6dbabbf221c6fdd4dbe979ff5b553be9da147d9fd02dd6012f","sha256:f66b51e6d558f6e0d4cbaa31cc9bd06b42f9cb0f3b0ed5ad698a937e58413484"],"state_sha256":"9099c69e9f38858507d23b185b1aa0c163504eb3429f7d8e35c1ef20fd6f7687"}