{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:J42P53DLUL3OBQ2HXC4FN24EP6","short_pith_number":"pith:J42P53DL","canonical_record":{"source":{"id":"1601.02690","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2016-01-11T23:33:00Z","cross_cats_sorted":[],"title_canon_sha256":"6df9eab7008eaabf156f61b5b35a1d27f4f7b26eb666fdc2c458b3dba1ed2d36","abstract_canon_sha256":"9ec2419be70470fc9cb4d4fd03ba9016b400b191e4a96ed8181722615c601078"},"schema_version":"1.0"},"canonical_sha256":"4f34feec6ba2f6e0c347b8b856eb847fa7d7f2fb7fae9336c3dc8e2664198c48","source":{"kind":"arxiv","id":"1601.02690","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1601.02690","created_at":"2026-05-18T01:19:25Z"},{"alias_kind":"arxiv_version","alias_value":"1601.02690v1","created_at":"2026-05-18T01:19:25Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1601.02690","created_at":"2026-05-18T01:19:25Z"},{"alias_kind":"pith_short_12","alias_value":"J42P53DLUL3O","created_at":"2026-05-18T12:30:22Z"},{"alias_kind":"pith_short_16","alias_value":"J42P53DLUL3OBQ2H","created_at":"2026-05-18T12:30:22Z"},{"alias_kind":"pith_short_8","alias_value":"J42P53DL","created_at":"2026-05-18T12:30:22Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:J42P53DLUL3OBQ2HXC4FN24EP6","target":"record","payload":{"canonical_record":{"source":{"id":"1601.02690","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2016-01-11T23:33:00Z","cross_cats_sorted":[],"title_canon_sha256":"6df9eab7008eaabf156f61b5b35a1d27f4f7b26eb666fdc2c458b3dba1ed2d36","abstract_canon_sha256":"9ec2419be70470fc9cb4d4fd03ba9016b400b191e4a96ed8181722615c601078"},"schema_version":"1.0"},"canonical_sha256":"4f34feec6ba2f6e0c347b8b856eb847fa7d7f2fb7fae9336c3dc8e2664198c48","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:19:25.056293Z","signature_b64":"m3W5M65wC5iKdv3Y5hn5Diy8olcIQwgGjfiu+/jtUVMXDqDiHPHc4SorjHu6RHw/mr3ZKtDOmbC+spG7JXqCDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4f34feec6ba2f6e0c347b8b856eb847fa7d7f2fb7fae9336c3dc8e2664198c48","last_reissued_at":"2026-05-18T01:19:25.055608Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:19:25.055608Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1601.02690","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:19:25Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"QPW5f1MkpZZi3TRAeJInzs9Y8Mu7YMR4JBvBBjTl/AhZrFEhahuFZajDMX3H80B/0HE/iMSYNoVCbwz5cdaNBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T10:06:42.916426Z"},"content_sha256":"7d039f15a7578c4ca54cb6ed3af0e8662a8d76eb01472482d2169a542f013cf1","schema_version":"1.0","event_id":"sha256:7d039f15a7578c4ca54cb6ed3af0e8662a8d76eb01472482d2169a542f013cf1"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:J42P53DLUL3OBQ2HXC4FN24EP6","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Measurement scheme and analysis for weak ground state hyperfine transition moments through two-pathway coherent control","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.atom-ph","authors_text":"D. S. Elliott, J. Choi","submitted_at":"2016-01-11T23:33:00Z","abstract_excerpt":"We report our detailed analysis of a table-top system for the measurement of the weak-force-induced electric dipole moment of a ground state hyperfine transition carried out in an atomic beam geometry. We describe an experimental configuration of conductors for application of orthogonal r.f. and static electric fields, with cavity enhancement of the r.f. field amplitude, that allows confinement of the r.f. field to a region in which the static fields are uniform and well-characterized. We carry out detailed numerical simulations of the field modes, and analyze the expected magnitude of statist"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1601.02690","kind":"arxiv","version":1},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:19:25Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"eMEjtD09Sug1Vc652MLgC/TMGhQ0NmWyjIk2hP8xy6LaoSiR1y19GgGDak7q5aNjHCLCHEKb3TdnA/pPqkV9Dg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T10:06:42.916894Z"},"content_sha256":"ec29d5f9497b85cbdd68cd39c7f21db79a4c779e60de903be077c50f78065443","schema_version":"1.0","event_id":"sha256:ec29d5f9497b85cbdd68cd39c7f21db79a4c779e60de903be077c50f78065443"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/J42P53DLUL3OBQ2HXC4FN24EP6/bundle.json","state_url":"https://pith.science/pith/J42P53DLUL3OBQ2HXC4FN24EP6/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/J42P53DLUL3OBQ2HXC4FN24EP6/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-05-25T10:06:42Z","links":{"resolver":"https://pith.science/pith/J42P53DLUL3OBQ2HXC4FN24EP6","bundle":"https://pith.science/pith/J42P53DLUL3OBQ2HXC4FN24EP6/bundle.json","state":"https://pith.science/pith/J42P53DLUL3OBQ2HXC4FN24EP6/state.json","well_known_bundle":"https://pith.science/.well-known/pith/J42P53DLUL3OBQ2HXC4FN24EP6/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:J42P53DLUL3OBQ2HXC4FN24EP6","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":"9ec2419be70470fc9cb4d4fd03ba9016b400b191e4a96ed8181722615c601078","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2016-01-11T23:33:00Z","title_canon_sha256":"6df9eab7008eaabf156f61b5b35a1d27f4f7b26eb666fdc2c458b3dba1ed2d36"},"schema_version":"1.0","source":{"id":"1601.02690","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1601.02690","created_at":"2026-05-18T01:19:25Z"},{"alias_kind":"arxiv_version","alias_value":"1601.02690v1","created_at":"2026-05-18T01:19:25Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1601.02690","created_at":"2026-05-18T01:19:25Z"},{"alias_kind":"pith_short_12","alias_value":"J42P53DLUL3O","created_at":"2026-05-18T12:30:22Z"},{"alias_kind":"pith_short_16","alias_value":"J42P53DLUL3OBQ2H","created_at":"2026-05-18T12:30:22Z"},{"alias_kind":"pith_short_8","alias_value":"J42P53DL","created_at":"2026-05-18T12:30:22Z"}],"graph_snapshots":[{"event_id":"sha256:ec29d5f9497b85cbdd68cd39c7f21db79a4c779e60de903be077c50f78065443","target":"graph","created_at":"2026-05-18T01:19:25Z","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 report our detailed analysis of a table-top system for the measurement of the weak-force-induced electric dipole moment of a ground state hyperfine transition carried out in an atomic beam geometry. We describe an experimental configuration of conductors for application of orthogonal r.f. and static electric fields, with cavity enhancement of the r.f. field amplitude, that allows confinement of the r.f. field to a region in which the static fields are uniform and well-characterized. We carry out detailed numerical simulations of the field modes, and analyze the expected magnitude of statist","authors_text":"D. S. Elliott, J. Choi","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2016-01-11T23:33:00Z","title":"Measurement scheme and analysis for weak ground state hyperfine transition moments through two-pathway coherent control"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1601.02690","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":"sha256:7d039f15a7578c4ca54cb6ed3af0e8662a8d76eb01472482d2169a542f013cf1","target":"record","created_at":"2026-05-18T01:19:25Z","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":"9ec2419be70470fc9cb4d4fd03ba9016b400b191e4a96ed8181722615c601078","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2016-01-11T23:33:00Z","title_canon_sha256":"6df9eab7008eaabf156f61b5b35a1d27f4f7b26eb666fdc2c458b3dba1ed2d36"},"schema_version":"1.0","source":{"id":"1601.02690","kind":"arxiv","version":1}},"canonical_sha256":"4f34feec6ba2f6e0c347b8b856eb847fa7d7f2fb7fae9336c3dc8e2664198c48","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"4f34feec6ba2f6e0c347b8b856eb847fa7d7f2fb7fae9336c3dc8e2664198c48","first_computed_at":"2026-05-18T01:19:25.055608Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:19:25.055608Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"m3W5M65wC5iKdv3Y5hn5Diy8olcIQwgGjfiu+/jtUVMXDqDiHPHc4SorjHu6RHw/mr3ZKtDOmbC+spG7JXqCDA==","signature_status":"signed_v1","signed_at":"2026-05-18T01:19:25.056293Z","signed_message":"canonical_sha256_bytes"},"source_id":"1601.02690","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:7d039f15a7578c4ca54cb6ed3af0e8662a8d76eb01472482d2169a542f013cf1","sha256:ec29d5f9497b85cbdd68cd39c7f21db79a4c779e60de903be077c50f78065443"],"state_sha256":"4b35ea5f0e77140d0cfe1d998484e6f71033362b7e2617a4f5f22eef5790f302"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"8ZyZsBlVQBb14xsDFNhRpwyen/CcT9Lgre9ja2MD/yX5tqdNzcrOHHIbm5NEAuVxwn4dGRBYVVjhPEueWZirBQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-25T10:06:42.919797Z","bundle_sha256":"a9a44725304ca9d43e8a6cd66d2937a1d4fc0bdb13bec1f57c54783a6e2192c7"}}