{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:QPGDRA4CAW62FB7PYCWYQB5HTY","short_pith_number":"pith:QPGDRA4C","canonical_record":{"source":{"id":"1401.2284","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2014-01-10T11:12:20Z","cross_cats_sorted":["quant-ph"],"title_canon_sha256":"5e650c8778c9d9d72fc8495478c3b6f47970b267e509de3dba932bba5f6d811f","abstract_canon_sha256":"d3cf4da6b06e1f7ce465f6689876a9260e7077bc1809016d1e9f35bd31b084eb"},"schema_version":"1.0"},"canonical_sha256":"83cc38838205bda287efc0ad8807a79e3b517f90f9db1dff6080b835bacf13df","source":{"kind":"arxiv","id":"1401.2284","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1401.2284","created_at":"2026-05-18T02:55:05Z"},{"alias_kind":"arxiv_version","alias_value":"1401.2284v3","created_at":"2026-05-18T02:55:05Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1401.2284","created_at":"2026-05-18T02:55:05Z"},{"alias_kind":"pith_short_12","alias_value":"QPGDRA4CAW62","created_at":"2026-05-18T12:28:46Z"},{"alias_kind":"pith_short_16","alias_value":"QPGDRA4CAW62FB7P","created_at":"2026-05-18T12:28:46Z"},{"alias_kind":"pith_short_8","alias_value":"QPGDRA4C","created_at":"2026-05-18T12:28:46Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:QPGDRA4CAW62FB7PYCWYQB5HTY","target":"record","payload":{"canonical_record":{"source":{"id":"1401.2284","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2014-01-10T11:12:20Z","cross_cats_sorted":["quant-ph"],"title_canon_sha256":"5e650c8778c9d9d72fc8495478c3b6f47970b267e509de3dba932bba5f6d811f","abstract_canon_sha256":"d3cf4da6b06e1f7ce465f6689876a9260e7077bc1809016d1e9f35bd31b084eb"},"schema_version":"1.0"},"canonical_sha256":"83cc38838205bda287efc0ad8807a79e3b517f90f9db1dff6080b835bacf13df","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:55:05.549214Z","signature_b64":"wwr2Z+yyrD9RDM22S9UWur5RVtkWOiBE1pinVUE7y6lgNAVQfN7yDIh9h4z02j09pCuiYLxrbhDM0m36qCDHCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"83cc38838205bda287efc0ad8807a79e3b517f90f9db1dff6080b835bacf13df","last_reissued_at":"2026-05-18T02:55:05.548603Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:55:05.548603Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1401.2284","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:55:05Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"oqoxBL5YsBaCQXwg3zY/lsodMwVE3AwkZQW84+RaUO44zuRV+0kLf+Y3+AW8l+RGf+5ZcyZvg1XwQ5f/sMaiAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-20T04:38:04.479617Z"},"content_sha256":"f8b6c0800c28b050cddbb871a89ec22d21f5b8ae60b173e3222d347304ab138c","schema_version":"1.0","event_id":"sha256:f8b6c0800c28b050cddbb871a89ec22d21f5b8ae60b173e3222d347304ab138c"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:QPGDRA4CAW62FB7PYCWYQB5HTY","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Electron Electric Dipole Moment and Hyperfine Interaction Constants for ThO","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["quant-ph"],"primary_cat":"physics.atom-ph","authors_text":"Malaya K. Nayak, Timo Fleig","submitted_at":"2014-01-10T11:12:20Z","abstract_excerpt":"A recently implemented relativistic four-component configuration interaction approach to study ${\\cal{P}}$- and ${\\cal{T}}$-odd interaction constants in atoms and molecules is employed to determine the electron electric dipole moment effective electric field in the $\\Omega=1$ first excited state of the ThO molecule. We obtain a value of $E_{\\text{eff}} = 75.6 \\left[\\frac{\\rm GV}{\\rm cm}\\right]$ with an estimated error bar of $3\\%$ and $10\\%$ smaller than a previously reported result [arXiv:1308.0414 [physics.atom-ph]]. Using the same wavefunction model we obtain an excitation energy of $T_v^{\\"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1401.2284","kind":"arxiv","version":3},"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":"2026-05-18T02:55:05Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"EJJlnzjp7WOTEyqh2828rEC2mj7zlcZ1Ao1LmcxasoWyXlwxMim0v3Z5g+AnWolL2/yGls56+mD7flMXI/JUDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-20T04:38:04.480377Z"},"content_sha256":"f3b4979dd54197e50ad0639d237ab8461483c0d217155c43d5ec3b07572a0f40","schema_version":"1.0","event_id":"sha256:f3b4979dd54197e50ad0639d237ab8461483c0d217155c43d5ec3b07572a0f40"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/QPGDRA4CAW62FB7PYCWYQB5HTY/bundle.json","state_url":"https://pith.science/pith/QPGDRA4CAW62FB7PYCWYQB5HTY/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/QPGDRA4CAW62FB7PYCWYQB5HTY/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":"2026-05-20T04:38:04Z","links":{"resolver":"https://pith.science/pith/QPGDRA4CAW62FB7PYCWYQB5HTY","bundle":"https://pith.science/pith/QPGDRA4CAW62FB7PYCWYQB5HTY/bundle.json","state":"https://pith.science/pith/QPGDRA4CAW62FB7PYCWYQB5HTY/state.json","well_known_bundle":"https://pith.science/.well-known/pith/QPGDRA4CAW62FB7PYCWYQB5HTY/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:QPGDRA4CAW62FB7PYCWYQB5HTY","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":"d3cf4da6b06e1f7ce465f6689876a9260e7077bc1809016d1e9f35bd31b084eb","cross_cats_sorted":["quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2014-01-10T11:12:20Z","title_canon_sha256":"5e650c8778c9d9d72fc8495478c3b6f47970b267e509de3dba932bba5f6d811f"},"schema_version":"1.0","source":{"id":"1401.2284","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1401.2284","created_at":"2026-05-18T02:55:05Z"},{"alias_kind":"arxiv_version","alias_value":"1401.2284v3","created_at":"2026-05-18T02:55:05Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1401.2284","created_at":"2026-05-18T02:55:05Z"},{"alias_kind":"pith_short_12","alias_value":"QPGDRA4CAW62","created_at":"2026-05-18T12:28:46Z"},{"alias_kind":"pith_short_16","alias_value":"QPGDRA4CAW62FB7P","created_at":"2026-05-18T12:28:46Z"},{"alias_kind":"pith_short_8","alias_value":"QPGDRA4C","created_at":"2026-05-18T12:28:46Z"}],"graph_snapshots":[{"event_id":"sha256:f3b4979dd54197e50ad0639d237ab8461483c0d217155c43d5ec3b07572a0f40","target":"graph","created_at":"2026-05-18T02:55:05Z","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":"A recently implemented relativistic four-component configuration interaction approach to study ${\\cal{P}}$- and ${\\cal{T}}$-odd interaction constants in atoms and molecules is employed to determine the electron electric dipole moment effective electric field in the $\\Omega=1$ first excited state of the ThO molecule. We obtain a value of $E_{\\text{eff}} = 75.6 \\left[\\frac{\\rm GV}{\\rm cm}\\right]$ with an estimated error bar of $3\\%$ and $10\\%$ smaller than a previously reported result [arXiv:1308.0414 [physics.atom-ph]]. Using the same wavefunction model we obtain an excitation energy of $T_v^{\\","authors_text":"Malaya K. Nayak, Timo Fleig","cross_cats":["quant-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2014-01-10T11:12:20Z","title":"Electron Electric Dipole Moment and Hyperfine Interaction Constants for ThO"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1401.2284","kind":"arxiv","version":3},"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:f8b6c0800c28b050cddbb871a89ec22d21f5b8ae60b173e3222d347304ab138c","target":"record","created_at":"2026-05-18T02:55:05Z","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":"d3cf4da6b06e1f7ce465f6689876a9260e7077bc1809016d1e9f35bd31b084eb","cross_cats_sorted":["quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2014-01-10T11:12:20Z","title_canon_sha256":"5e650c8778c9d9d72fc8495478c3b6f47970b267e509de3dba932bba5f6d811f"},"schema_version":"1.0","source":{"id":"1401.2284","kind":"arxiv","version":3}},"canonical_sha256":"83cc38838205bda287efc0ad8807a79e3b517f90f9db1dff6080b835bacf13df","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"83cc38838205bda287efc0ad8807a79e3b517f90f9db1dff6080b835bacf13df","first_computed_at":"2026-05-18T02:55:05.548603Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:55:05.548603Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"wwr2Z+yyrD9RDM22S9UWur5RVtkWOiBE1pinVUE7y6lgNAVQfN7yDIh9h4z02j09pCuiYLxrbhDM0m36qCDHCA==","signature_status":"signed_v1","signed_at":"2026-05-18T02:55:05.549214Z","signed_message":"canonical_sha256_bytes"},"source_id":"1401.2284","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:f8b6c0800c28b050cddbb871a89ec22d21f5b8ae60b173e3222d347304ab138c","sha256:f3b4979dd54197e50ad0639d237ab8461483c0d217155c43d5ec3b07572a0f40"],"state_sha256":"1c93d49643ac777134ec0f04443616c8d282ea13a2e00679a1c6d71cbfba636f"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"db8BhIATFrAVOzN0wECFZzGT8NH11qD3XposzM7O+Cc92SA8WXkHJd5JR3RTFbtShgl0cmYCLhnrJwHstRUlBA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-20T04:38:04.484274Z","bundle_sha256":"97c929daac1c23da7299db31d9182ce6122b67eb3b891e4c1b0cbcbc3237a358"}}