{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:KPOO5RO6Z5TD5B4BAHZO26SL3F","short_pith_number":"pith:KPOO5RO6","canonical_record":{"source":{"id":"1703.01349","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2017-03-03T21:56:06Z","cross_cats_sorted":[],"title_canon_sha256":"effecaa7a13b93af585573f493c825f687cdbc00abc097a93146b0ce64b1086f","abstract_canon_sha256":"a09cc80218567d5272d093d50da3fd5d043d9327611d9d00e5c23947b9c01cc1"},"schema_version":"1.0"},"canonical_sha256":"53dceec5decf663e878101f2ed7a4bd943fe80999117616f9a97130187cc7175","source":{"kind":"arxiv","id":"1703.01349","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1703.01349","created_at":"2026-05-18T00:40:07Z"},{"alias_kind":"arxiv_version","alias_value":"1703.01349v2","created_at":"2026-05-18T00:40:07Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1703.01349","created_at":"2026-05-18T00:40:07Z"},{"alias_kind":"pith_short_12","alias_value":"KPOO5RO6Z5TD","created_at":"2026-05-18T12:31:24Z"},{"alias_kind":"pith_short_16","alias_value":"KPOO5RO6Z5TD5B4B","created_at":"2026-05-18T12:31:24Z"},{"alias_kind":"pith_short_8","alias_value":"KPOO5RO6","created_at":"2026-05-18T12:31:24Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:KPOO5RO6Z5TD5B4BAHZO26SL3F","target":"record","payload":{"canonical_record":{"source":{"id":"1703.01349","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2017-03-03T21:56:06Z","cross_cats_sorted":[],"title_canon_sha256":"effecaa7a13b93af585573f493c825f687cdbc00abc097a93146b0ce64b1086f","abstract_canon_sha256":"a09cc80218567d5272d093d50da3fd5d043d9327611d9d00e5c23947b9c01cc1"},"schema_version":"1.0"},"canonical_sha256":"53dceec5decf663e878101f2ed7a4bd943fe80999117616f9a97130187cc7175","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:40:07.001387Z","signature_b64":"bR5T0j0nSTp4iGjVzk9sUKxHIcYDTPfPqaFiHpTkhAP03CYHfyiMmuPB+XB7Foug4DLmnyLIxxm8zJXSk4iHAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"53dceec5decf663e878101f2ed7a4bd943fe80999117616f9a97130187cc7175","last_reissued_at":"2026-05-18T00:40:07.000859Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:40:07.000859Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1703.01349","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":"2026-05-18T00:40:07Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"lptyo+eiJhQ70CBEyYsAYtnINBHaackD59skWVPOo6ftxLsp1rUKf+0uqo9GxZcZ7+M4C53s3qWWVhtYyIoGBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T18:53:52.909964Z"},"content_sha256":"fd18e97b865a21c0f752d7b91715e553d11a0eda4c2d8afd69ca7790601c7713","schema_version":"1.0","event_id":"sha256:fd18e97b865a21c0f752d7b91715e553d11a0eda4c2d8afd69ca7790601c7713"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:KPOO5RO6Z5TD5B4BAHZO26SL3F","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"A theoretical study of the g-factor of the 6s6p 3P0 state of mercury","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.atom-ph","authors_text":"M.S. Safronova, S.G. Porsev, U.I. Safronova","submitted_at":"2017-03-03T21:56:06Z","abstract_excerpt":"We calculate the g-factor of the 6s6p 3P0 state of 199 and 201 mercury isotopes using a relativistic high-precision all-order method that combines the configuration interaction and the coupled-cluster approaches. Our values $g(199Hg) = -0.9485(49)*10^{-3}$ and $g(201Hg) = -0.3504(18)*10^{-3}$ are in agreement with the experimental measurements within the 0.5% theoretical uncertainty. We also calculate the hyperfine quenching rate of the 6s6p 3P0 state in 199Hg and 201Hg and determine its lifetime to be 1.3 and 1.9 s, respectively."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1703.01349","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":"2026-05-18T00:40:07Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"g/bE1zEHgtK21cLr6/1liubDPZmfM9arvD6AIGF/lic9KWIqsCzV8vNICDSwqOiTYTm/shEMuTOZFb1QRF4eAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T18:53:52.910674Z"},"content_sha256":"95d644e01faec39115977d1879a9c826731f26d5d2b9b9902177f012e3008287","schema_version":"1.0","event_id":"sha256:95d644e01faec39115977d1879a9c826731f26d5d2b9b9902177f012e3008287"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/KPOO5RO6Z5TD5B4BAHZO26SL3F/bundle.json","state_url":"https://pith.science/pith/KPOO5RO6Z5TD5B4BAHZO26SL3F/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/KPOO5RO6Z5TD5B4BAHZO26SL3F/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":"2026-05-25T18:53:52Z","links":{"resolver":"https://pith.science/pith/KPOO5RO6Z5TD5B4BAHZO26SL3F","bundle":"https://pith.science/pith/KPOO5RO6Z5TD5B4BAHZO26SL3F/bundle.json","state":"https://pith.science/pith/KPOO5RO6Z5TD5B4BAHZO26SL3F/state.json","well_known_bundle":"https://pith.science/.well-known/pith/KPOO5RO6Z5TD5B4BAHZO26SL3F/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:KPOO5RO6Z5TD5B4BAHZO26SL3F","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":"a09cc80218567d5272d093d50da3fd5d043d9327611d9d00e5c23947b9c01cc1","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2017-03-03T21:56:06Z","title_canon_sha256":"effecaa7a13b93af585573f493c825f687cdbc00abc097a93146b0ce64b1086f"},"schema_version":"1.0","source":{"id":"1703.01349","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1703.01349","created_at":"2026-05-18T00:40:07Z"},{"alias_kind":"arxiv_version","alias_value":"1703.01349v2","created_at":"2026-05-18T00:40:07Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1703.01349","created_at":"2026-05-18T00:40:07Z"},{"alias_kind":"pith_short_12","alias_value":"KPOO5RO6Z5TD","created_at":"2026-05-18T12:31:24Z"},{"alias_kind":"pith_short_16","alias_value":"KPOO5RO6Z5TD5B4B","created_at":"2026-05-18T12:31:24Z"},{"alias_kind":"pith_short_8","alias_value":"KPOO5RO6","created_at":"2026-05-18T12:31:24Z"}],"graph_snapshots":[{"event_id":"sha256:95d644e01faec39115977d1879a9c826731f26d5d2b9b9902177f012e3008287","target":"graph","created_at":"2026-05-18T00:40:07Z","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 calculate the g-factor of the 6s6p 3P0 state of 199 and 201 mercury isotopes using a relativistic high-precision all-order method that combines the configuration interaction and the coupled-cluster approaches. Our values $g(199Hg) = -0.9485(49)*10^{-3}$ and $g(201Hg) = -0.3504(18)*10^{-3}$ are in agreement with the experimental measurements within the 0.5% theoretical uncertainty. We also calculate the hyperfine quenching rate of the 6s6p 3P0 state in 199Hg and 201Hg and determine its lifetime to be 1.3 and 1.9 s, respectively.","authors_text":"M.S. Safronova, S.G. Porsev, U.I. Safronova","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2017-03-03T21:56:06Z","title":"A theoretical study of the g-factor of the 6s6p 3P0 state of mercury"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1703.01349","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:fd18e97b865a21c0f752d7b91715e553d11a0eda4c2d8afd69ca7790601c7713","target":"record","created_at":"2026-05-18T00:40:07Z","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":"a09cc80218567d5272d093d50da3fd5d043d9327611d9d00e5c23947b9c01cc1","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2017-03-03T21:56:06Z","title_canon_sha256":"effecaa7a13b93af585573f493c825f687cdbc00abc097a93146b0ce64b1086f"},"schema_version":"1.0","source":{"id":"1703.01349","kind":"arxiv","version":2}},"canonical_sha256":"53dceec5decf663e878101f2ed7a4bd943fe80999117616f9a97130187cc7175","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"53dceec5decf663e878101f2ed7a4bd943fe80999117616f9a97130187cc7175","first_computed_at":"2026-05-18T00:40:07.000859Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:40:07.000859Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"bR5T0j0nSTp4iGjVzk9sUKxHIcYDTPfPqaFiHpTkhAP03CYHfyiMmuPB+XB7Foug4DLmnyLIxxm8zJXSk4iHAA==","signature_status":"signed_v1","signed_at":"2026-05-18T00:40:07.001387Z","signed_message":"canonical_sha256_bytes"},"source_id":"1703.01349","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:fd18e97b865a21c0f752d7b91715e553d11a0eda4c2d8afd69ca7790601c7713","sha256:95d644e01faec39115977d1879a9c826731f26d5d2b9b9902177f012e3008287"],"state_sha256":"d21d277c7504e1f3d8c707ae960575c021e1b8105c8593d877aa0508229d689e"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"lf0HEDXYuIN+nTXMMNcoSW0QX570yn/wF/Fxiwsozct4LJEnDTGHcEz0h6PI2lD1zarQzdN7f0+W0/5vFqPBCQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-25T18:53:52.914971Z","bundle_sha256":"1f5e6a20bb5aa189d70cde6b4bea4317d3ae5411dce5e407b18345430b4f7d80"}}