{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2012:RRRKYDCY22KDPYPOKILQGCLEPK","short_pith_number":"pith:RRRKYDCY","canonical_record":{"source":{"id":"1205.5895","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2012-05-26T16:47:32Z","cross_cats_sorted":[],"title_canon_sha256":"cae5bea77fc3f89eafbb7dc650f86815f61ca869f760dc468ea2d8343e87e69e","abstract_canon_sha256":"5f71771c0da275c8b0416eb8c9c33802cb488884373e0b3b4ced61ef01c60a41"},"schema_version":"1.0"},"canonical_sha256":"8c62ac0c58d69437e1ee52170309647aa13fb5d94ec131056905a30330e616f4","source":{"kind":"arxiv","id":"1205.5895","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1205.5895","created_at":"2026-05-18T03:21:21Z"},{"alias_kind":"arxiv_version","alias_value":"1205.5895v2","created_at":"2026-05-18T03:21:21Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1205.5895","created_at":"2026-05-18T03:21:21Z"},{"alias_kind":"pith_short_12","alias_value":"RRRKYDCY22KD","created_at":"2026-05-18T12:27:20Z"},{"alias_kind":"pith_short_16","alias_value":"RRRKYDCY22KDPYPO","created_at":"2026-05-18T12:27:20Z"},{"alias_kind":"pith_short_8","alias_value":"RRRKYDCY","created_at":"2026-05-18T12:27:20Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2012:RRRKYDCY22KDPYPOKILQGCLEPK","target":"record","payload":{"canonical_record":{"source":{"id":"1205.5895","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2012-05-26T16:47:32Z","cross_cats_sorted":[],"title_canon_sha256":"cae5bea77fc3f89eafbb7dc650f86815f61ca869f760dc468ea2d8343e87e69e","abstract_canon_sha256":"5f71771c0da275c8b0416eb8c9c33802cb488884373e0b3b4ced61ef01c60a41"},"schema_version":"1.0"},"canonical_sha256":"8c62ac0c58d69437e1ee52170309647aa13fb5d94ec131056905a30330e616f4","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:21:21.671517Z","signature_b64":"wb+9uh7fjPCYrweKWeG4oJ6QwaTeaigtZeXD67X0d+FeTQ2K2HbdRinmpDaJKuCYbeNHM5IG3bYNyX1XmgtfDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8c62ac0c58d69437e1ee52170309647aa13fb5d94ec131056905a30330e616f4","last_reissued_at":"2026-05-18T03:21:21.670684Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:21:21.670684Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1205.5895","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T03:21:21Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"1vUP0WaQLwNq5FRbzQRi6/UOazM4ZRKFYLsUAS8Ce0K7xUagFP4PMBLuIGAij3BTNy5Yhv3gsN90Q2vD4LEJCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T16:20:40.361738Z"},"content_sha256":"66d42ade89ea4594e0becb3bb410f54803ab99d93ada215ab6137313d8b22809","schema_version":"1.0","event_id":"sha256:66d42ade89ea4594e0becb3bb410f54803ab99d93ada215ab6137313d8b22809"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2012:RRRKYDCY22KDPYPOKILQGCLEPK","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Study of the correlation effects in Yb^+ and implications for parity violation","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.atom-ph","authors_text":"M. G. Kozlov, M. S. Safronova, S. G. Porsev","submitted_at":"2012-05-26T16:47:32Z","abstract_excerpt":"Calculation of the energies, magnetic dipole hyperfine structure constants, E1 transition amplitudes between the low-lying states, and nuclear spin-dependent parity-nonconserving amplitudes for the ^2S_{1/2} - ^2D_{3/2,5/2} transitions in ^{171}Yb^+ ion is performed using two different approaches. First, we carried out many-body perturbation theory calculation considering Yb^+ as a monovalent system. Additional all-order calculations are carried out for selected properties. Second, we carried out configuration interaction calculation considering Yb as a 15-electron system and compared the resu"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1205.5895","kind":"arxiv","version":2},"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":"2026-05-18T03:21:21Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"WA+aR/U0TeO6VgTGNQrQ252pTsWer1K9BgcRyePs9kTZKn96jmOhwMe5z7XwaFt/AimDVFve6T3qth1iPfUYCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T16:20:40.362103Z"},"content_sha256":"2209524552be2c98697f691012788db249cad3ad51ff37695d86108f62c6f3c3","schema_version":"1.0","event_id":"sha256:2209524552be2c98697f691012788db249cad3ad51ff37695d86108f62c6f3c3"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/RRRKYDCY22KDPYPOKILQGCLEPK/bundle.json","state_url":"https://pith.science/pith/RRRKYDCY22KDPYPOKILQGCLEPK/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/RRRKYDCY22KDPYPOKILQGCLEPK/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":"2026-05-28T16:20:40Z","links":{"resolver":"https://pith.science/pith/RRRKYDCY22KDPYPOKILQGCLEPK","bundle":"https://pith.science/pith/RRRKYDCY22KDPYPOKILQGCLEPK/bundle.json","state":"https://pith.science/pith/RRRKYDCY22KDPYPOKILQGCLEPK/state.json","well_known_bundle":"https://pith.science/.well-known/pith/RRRKYDCY22KDPYPOKILQGCLEPK/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:RRRKYDCY22KDPYPOKILQGCLEPK","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":"5f71771c0da275c8b0416eb8c9c33802cb488884373e0b3b4ced61ef01c60a41","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2012-05-26T16:47:32Z","title_canon_sha256":"cae5bea77fc3f89eafbb7dc650f86815f61ca869f760dc468ea2d8343e87e69e"},"schema_version":"1.0","source":{"id":"1205.5895","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1205.5895","created_at":"2026-05-18T03:21:21Z"},{"alias_kind":"arxiv_version","alias_value":"1205.5895v2","created_at":"2026-05-18T03:21:21Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1205.5895","created_at":"2026-05-18T03:21:21Z"},{"alias_kind":"pith_short_12","alias_value":"RRRKYDCY22KD","created_at":"2026-05-18T12:27:20Z"},{"alias_kind":"pith_short_16","alias_value":"RRRKYDCY22KDPYPO","created_at":"2026-05-18T12:27:20Z"},{"alias_kind":"pith_short_8","alias_value":"RRRKYDCY","created_at":"2026-05-18T12:27:20Z"}],"graph_snapshots":[{"event_id":"sha256:2209524552be2c98697f691012788db249cad3ad51ff37695d86108f62c6f3c3","target":"graph","created_at":"2026-05-18T03:21:21Z","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":"Calculation of the energies, magnetic dipole hyperfine structure constants, E1 transition amplitudes between the low-lying states, and nuclear spin-dependent parity-nonconserving amplitudes for the ^2S_{1/2} - ^2D_{3/2,5/2} transitions in ^{171}Yb^+ ion is performed using two different approaches. First, we carried out many-body perturbation theory calculation considering Yb^+ as a monovalent system. Additional all-order calculations are carried out for selected properties. Second, we carried out configuration interaction calculation considering Yb as a 15-electron system and compared the resu","authors_text":"M. G. Kozlov, M. S. Safronova, S. G. Porsev","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2012-05-26T16:47:32Z","title":"Study of the correlation effects in Yb^+ and implications for parity violation"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1205.5895","kind":"arxiv","version":2},"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":"sha256:66d42ade89ea4594e0becb3bb410f54803ab99d93ada215ab6137313d8b22809","target":"record","created_at":"2026-05-18T03:21:21Z","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":"5f71771c0da275c8b0416eb8c9c33802cb488884373e0b3b4ced61ef01c60a41","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2012-05-26T16:47:32Z","title_canon_sha256":"cae5bea77fc3f89eafbb7dc650f86815f61ca869f760dc468ea2d8343e87e69e"},"schema_version":"1.0","source":{"id":"1205.5895","kind":"arxiv","version":2}},"canonical_sha256":"8c62ac0c58d69437e1ee52170309647aa13fb5d94ec131056905a30330e616f4","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"8c62ac0c58d69437e1ee52170309647aa13fb5d94ec131056905a30330e616f4","first_computed_at":"2026-05-18T03:21:21.670684Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:21:21.670684Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"wb+9uh7fjPCYrweKWeG4oJ6QwaTeaigtZeXD67X0d+FeTQ2K2HbdRinmpDaJKuCYbeNHM5IG3bYNyX1XmgtfDg==","signature_status":"signed_v1","signed_at":"2026-05-18T03:21:21.671517Z","signed_message":"canonical_sha256_bytes"},"source_id":"1205.5895","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:66d42ade89ea4594e0becb3bb410f54803ab99d93ada215ab6137313d8b22809","sha256:2209524552be2c98697f691012788db249cad3ad51ff37695d86108f62c6f3c3"],"state_sha256":"32d87e57eb98eb4106e2e40c961d0e7515a4b5c1db50107b300107d7d499a105"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"9U2k+jtVgtNOX+o/a6PrEhWea/wYJtK5LxJZKe2bu6/5b+Cu3b+VzynRAKFBlwEhsWFysrLX2eMio9QQUY0xBA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-28T16:20:40.364154Z","bundle_sha256":"35a077bc8327e87efa32a9b63af5e9881a612bb91d8b1be68ac77f75533e7d87"}}