{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2019:5FXCZ2YXQSXLAUXG4BT5YUT3ZI","short_pith_number":"pith:5FXCZ2YX","canonical_record":{"source":{"id":"1908.03722","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2019-08-10T10:20:58Z","cross_cats_sorted":[],"title_canon_sha256":"f8e386b475184fec66a88a22aea00d82ab910ddf76a4e95f9cf82dc655cd76e6","abstract_canon_sha256":"6f4633c5f8a6b8f541ce9d1bd15519d195096255ef83d1d04163844c54f2155e"},"schema_version":"1.0"},"canonical_sha256":"e96e2ceb1784aeb052e6e067dc527bca1752e35a542d39f6b8114d77fbca676d","source":{"kind":"arxiv","id":"1908.03722","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1908.03722","created_at":"2026-07-04T23:53:17Z"},{"alias_kind":"arxiv_version","alias_value":"1908.03722v1","created_at":"2026-07-04T23:53:17Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1908.03722","created_at":"2026-07-04T23:53:17Z"},{"alias_kind":"pith_short_12","alias_value":"5FXCZ2YXQSXL","created_at":"2026-07-04T23:53:17Z"},{"alias_kind":"pith_short_16","alias_value":"5FXCZ2YXQSXLAUXG","created_at":"2026-07-04T23:53:17Z"},{"alias_kind":"pith_short_8","alias_value":"5FXCZ2YX","created_at":"2026-07-04T23:53:17Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2019:5FXCZ2YXQSXLAUXG4BT5YUT3ZI","target":"record","payload":{"canonical_record":{"source":{"id":"1908.03722","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2019-08-10T10:20:58Z","cross_cats_sorted":[],"title_canon_sha256":"f8e386b475184fec66a88a22aea00d82ab910ddf76a4e95f9cf82dc655cd76e6","abstract_canon_sha256":"6f4633c5f8a6b8f541ce9d1bd15519d195096255ef83d1d04163844c54f2155e"},"schema_version":"1.0"},"canonical_sha256":"e96e2ceb1784aeb052e6e067dc527bca1752e35a542d39f6b8114d77fbca676d","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T23:53:17.745392Z","signature_b64":"QSCvRUMex2YMbpPK0U03cdM/4y4VqiLppw/EI2VOlXw/lbVv1BDPh6plmmVP4VLKAPtLOh8y6x4sm3Nt4DJSCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e96e2ceb1784aeb052e6e067dc527bca1752e35a542d39f6b8114d77fbca676d","last_reissued_at":"2026-07-04T23:53:17.744975Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T23:53:17.744975Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1908.03722","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":"2026-07-04T23:53:17Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"OkXswIM+AiIIR3a/3ZCv3wvGI5cCixI61O/Yz2uXGPudMfyc5YyH5wD+xEN3smD+VRrZGJz9IP06i0VdtrfTBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-16T06:11:34.310069Z"},"content_sha256":"8fada7d5604519f6cd54a663c987caa884c4799516abaa7c6b4ddd2dab940fb6","schema_version":"1.0","event_id":"sha256:8fada7d5604519f6cd54a663c987caa884c4799516abaa7c6b4ddd2dab940fb6"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2019:5FXCZ2YXQSXLAUXG4BT5YUT3ZI","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Analysis of Electric Dipole Moment of $^{225}$Ra Atom using the Relativistic Normal Coupled-cluster Theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.atom-ph","authors_text":"B. K. Sahoo, R. Mitra, V. S. Prasannaa","submitted_at":"2019-08-10T10:20:58Z","abstract_excerpt":"In view of the large differences in the previous calculations of enhancement factors to the parity and time-reversal violating (P,T-odd) electric dipole moment (EDM) of $^{225}$Ra due to nuclear Schiff moment (NSM) and tensor-pseudotensor (T-PT) electron-nucleus (e-N) interactions between the relativistic coupled-cluster (RCC) theory and other many-body methods, we employ the relativistic normal coupled-cluster (RNCC) theory to explain the discrepancies. The normalization of the wave function in the RNCC theory becomes unity by construction. This feature removes the ambiguity associated with t"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1908.03722","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/1908.03722/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2026-07-04T23:53:17Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"azcY37ttgoHn1j1AEaW+9N3GsmgLHnuKeERwfLL0Q7/0ZjAuJyCO1ykcNFgyQu8h/6nquHKcIseyD3TpzXkFCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-16T06:11:34.310566Z"},"content_sha256":"0b9473e317e8b52d44230e65ef357678f8eb7f04428bef54637b57b499f03c97","schema_version":"1.0","event_id":"sha256:0b9473e317e8b52d44230e65ef357678f8eb7f04428bef54637b57b499f03c97"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/5FXCZ2YXQSXLAUXG4BT5YUT3ZI/bundle.json","state_url":"https://pith.science/pith/5FXCZ2YXQSXLAUXG4BT5YUT3ZI/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/5FXCZ2YXQSXLAUXG4BT5YUT3ZI/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":"2026-08-16T06:11:34Z","links":{"resolver":"https://pith.science/pith/5FXCZ2YXQSXLAUXG4BT5YUT3ZI","bundle":"https://pith.science/pith/5FXCZ2YXQSXLAUXG4BT5YUT3ZI/bundle.json","state":"https://pith.science/pith/5FXCZ2YXQSXLAUXG4BT5YUT3ZI/state.json","well_known_bundle":"https://pith.science/.well-known/pith/5FXCZ2YXQSXLAUXG4BT5YUT3ZI/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2019:5FXCZ2YXQSXLAUXG4BT5YUT3ZI","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":"6f4633c5f8a6b8f541ce9d1bd15519d195096255ef83d1d04163844c54f2155e","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2019-08-10T10:20:58Z","title_canon_sha256":"f8e386b475184fec66a88a22aea00d82ab910ddf76a4e95f9cf82dc655cd76e6"},"schema_version":"1.0","source":{"id":"1908.03722","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1908.03722","created_at":"2026-07-04T23:53:17Z"},{"alias_kind":"arxiv_version","alias_value":"1908.03722v1","created_at":"2026-07-04T23:53:17Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1908.03722","created_at":"2026-07-04T23:53:17Z"},{"alias_kind":"pith_short_12","alias_value":"5FXCZ2YXQSXL","created_at":"2026-07-04T23:53:17Z"},{"alias_kind":"pith_short_16","alias_value":"5FXCZ2YXQSXLAUXG","created_at":"2026-07-04T23:53:17Z"},{"alias_kind":"pith_short_8","alias_value":"5FXCZ2YX","created_at":"2026-07-04T23:53:17Z"}],"graph_snapshots":[{"event_id":"sha256:0b9473e317e8b52d44230e65ef357678f8eb7f04428bef54637b57b499f03c97","target":"graph","created_at":"2026-07-04T23:53:17Z","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/1908.03722/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"In view of the large differences in the previous calculations of enhancement factors to the parity and time-reversal violating (P,T-odd) electric dipole moment (EDM) of $^{225}$Ra due to nuclear Schiff moment (NSM) and tensor-pseudotensor (T-PT) electron-nucleus (e-N) interactions between the relativistic coupled-cluster (RCC) theory and other many-body methods, we employ the relativistic normal coupled-cluster (RNCC) theory to explain the discrepancies. The normalization of the wave function in the RNCC theory becomes unity by construction. This feature removes the ambiguity associated with t","authors_text":"B. K. Sahoo, R. Mitra, V. S. Prasannaa","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2019-08-10T10:20:58Z","title":"Analysis of Electric Dipole Moment of $^{225}$Ra Atom using the Relativistic Normal Coupled-cluster Theory"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1908.03722","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":"sha256:8fada7d5604519f6cd54a663c987caa884c4799516abaa7c6b4ddd2dab940fb6","target":"record","created_at":"2026-07-04T23:53:17Z","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":"6f4633c5f8a6b8f541ce9d1bd15519d195096255ef83d1d04163844c54f2155e","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2019-08-10T10:20:58Z","title_canon_sha256":"f8e386b475184fec66a88a22aea00d82ab910ddf76a4e95f9cf82dc655cd76e6"},"schema_version":"1.0","source":{"id":"1908.03722","kind":"arxiv","version":1}},"canonical_sha256":"e96e2ceb1784aeb052e6e067dc527bca1752e35a542d39f6b8114d77fbca676d","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"e96e2ceb1784aeb052e6e067dc527bca1752e35a542d39f6b8114d77fbca676d","first_computed_at":"2026-07-04T23:53:17.744975Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T23:53:17.744975Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"QSCvRUMex2YMbpPK0U03cdM/4y4VqiLppw/EI2VOlXw/lbVv1BDPh6plmmVP4VLKAPtLOh8y6x4sm3Nt4DJSCg==","signature_status":"signed_v1","signed_at":"2026-07-04T23:53:17.745392Z","signed_message":"canonical_sha256_bytes"},"source_id":"1908.03722","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:8fada7d5604519f6cd54a663c987caa884c4799516abaa7c6b4ddd2dab940fb6","sha256:0b9473e317e8b52d44230e65ef357678f8eb7f04428bef54637b57b499f03c97"],"state_sha256":"3b2ef55216da2b8db2e3bcc345a53ed889f05ef05d331e1340fcf52ff7f27281"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"oaHTgpzVHXHKDuDdKjHLp0CqXNfv3CDI6lQT03kGAwaOxFUmae2HO67EXxqhtPUXhJqMuAdSQM2jEO5tw1xXCw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-16T06:11:34.315348Z","bundle_sha256":"c5c805dd45e28b4e2f926405295ea7d565c79ab0f3e01f76b950a19246d366d8"}}