{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:MULK2LXV3XQCNMZB7XO3WFU7G4","short_pith_number":"pith:MULK2LXV","canonical_record":{"source":{"id":"1706.09104","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2017-06-28T02:22:45Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"27149bccfb165a20e1aefedf14841a332682169c0e2bd3d82c4b18f9b4777c79","abstract_canon_sha256":"db25e1b48b8c0c35fd6175db92715c41ffc9b8158e4b7797c078754ed07ea743"},"schema_version":"1.0"},"canonical_sha256":"6516ad2ef5dde026b321fdddbb169f370bb5924308fce1fdac02ba4d12fb4f2d","source":{"kind":"arxiv","id":"1706.09104","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1706.09104","created_at":"2026-05-18T00:35:31Z"},{"alias_kind":"arxiv_version","alias_value":"1706.09104v1","created_at":"2026-05-18T00:35:31Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1706.09104","created_at":"2026-05-18T00:35:31Z"},{"alias_kind":"pith_short_12","alias_value":"MULK2LXV3XQC","created_at":"2026-05-18T12:31:31Z"},{"alias_kind":"pith_short_16","alias_value":"MULK2LXV3XQCNMZB","created_at":"2026-05-18T12:31:31Z"},{"alias_kind":"pith_short_8","alias_value":"MULK2LXV","created_at":"2026-05-18T12:31:31Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:MULK2LXV3XQCNMZB7XO3WFU7G4","target":"record","payload":{"canonical_record":{"source":{"id":"1706.09104","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2017-06-28T02:22:45Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"27149bccfb165a20e1aefedf14841a332682169c0e2bd3d82c4b18f9b4777c79","abstract_canon_sha256":"db25e1b48b8c0c35fd6175db92715c41ffc9b8158e4b7797c078754ed07ea743"},"schema_version":"1.0"},"canonical_sha256":"6516ad2ef5dde026b321fdddbb169f370bb5924308fce1fdac02ba4d12fb4f2d","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:35:31.109451Z","signature_b64":"BZJ6rVwfcJjWkIwy3ZPJfQqjsoZLpGHjxj9/OB/aryE3m9jAvsq7/AARYFE4uSpo724YZvtEPU/XUI+vV1d9AA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6516ad2ef5dde026b321fdddbb169f370bb5924308fce1fdac02ba4d12fb4f2d","last_reissued_at":"2026-05-18T00:35:31.108993Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:35:31.108993Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1706.09104","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":"2026-05-18T00:35:31Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"3MCz2qmcu62UwBO90cBABebj2/Dn7MKQyBSmZCA/xRTOIlmSPAoXi9p9WQKQn+ySuxW1XZMQUmm5uH7sEmaaDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-05T10:23:55.015454Z"},"content_sha256":"1e860ab9ce6aba7d44f875f94bce03e2ef53a1d2a5c29da1d7a21a53a8441d13","schema_version":"1.0","event_id":"sha256:1e860ab9ce6aba7d44f875f94bce03e2ef53a1d2a5c29da1d7a21a53a8441d13"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:MULK2LXV3XQCNMZB7XO3WFU7G4","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Theoretical study on the hyperfine interaction constants and the isotope shift factors for the $3s^2~^1 S_{ 0} ~-~ 3s3p~^{3,1}P^o_1$ transitions in Al$^+$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"physics.atom-ph","authors_text":"Jiguang Li, Luyou Xie, Tingxian Zhang, Zehuang Lu","submitted_at":"2017-06-28T02:22:45Z","abstract_excerpt":"We calculated the magnetic dipole and the electric quadrupole hyperfine interaction constants of 3s3p $^{3,1}P^o_1$ states and the isotope shift, including mass and field shift, factors for transitions from these two states to the ground state 3s$^2~^1S_0$ in Al$^+$ ions using the multiconfiguration Dirac-Hartree-Fock method. The effects of the electron correlations and the Breit interaction on these physical quantities were investigated in detail based on the active space approach. It is found that the CC and the higher-order correlations are considerable for evaluating the uncertainties of t"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1706.09104","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":"2026-05-18T00:35:31Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"O5s8JJ/wXbC5BbUIjls0V3bPcSXTeI1gBZJKgtb5GzrNjhbUy90KjlLTf/VAUL/l+lIxBu1i7IsX6aiC6k88Dg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-05T10:23:55.015814Z"},"content_sha256":"8e589e1f36e339b4451b1d38a3affb7587caa798719ab00ee4d3200cee541952","schema_version":"1.0","event_id":"sha256:8e589e1f36e339b4451b1d38a3affb7587caa798719ab00ee4d3200cee541952"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/MULK2LXV3XQCNMZB7XO3WFU7G4/bundle.json","state_url":"https://pith.science/pith/MULK2LXV3XQCNMZB7XO3WFU7G4/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/MULK2LXV3XQCNMZB7XO3WFU7G4/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":"2026-06-05T10:23:55Z","links":{"resolver":"https://pith.science/pith/MULK2LXV3XQCNMZB7XO3WFU7G4","bundle":"https://pith.science/pith/MULK2LXV3XQCNMZB7XO3WFU7G4/bundle.json","state":"https://pith.science/pith/MULK2LXV3XQCNMZB7XO3WFU7G4/state.json","well_known_bundle":"https://pith.science/.well-known/pith/MULK2LXV3XQCNMZB7XO3WFU7G4/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:MULK2LXV3XQCNMZB7XO3WFU7G4","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":"db25e1b48b8c0c35fd6175db92715c41ffc9b8158e4b7797c078754ed07ea743","cross_cats_sorted":["nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2017-06-28T02:22:45Z","title_canon_sha256":"27149bccfb165a20e1aefedf14841a332682169c0e2bd3d82c4b18f9b4777c79"},"schema_version":"1.0","source":{"id":"1706.09104","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1706.09104","created_at":"2026-05-18T00:35:31Z"},{"alias_kind":"arxiv_version","alias_value":"1706.09104v1","created_at":"2026-05-18T00:35:31Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1706.09104","created_at":"2026-05-18T00:35:31Z"},{"alias_kind":"pith_short_12","alias_value":"MULK2LXV3XQC","created_at":"2026-05-18T12:31:31Z"},{"alias_kind":"pith_short_16","alias_value":"MULK2LXV3XQCNMZB","created_at":"2026-05-18T12:31:31Z"},{"alias_kind":"pith_short_8","alias_value":"MULK2LXV","created_at":"2026-05-18T12:31:31Z"}],"graph_snapshots":[{"event_id":"sha256:8e589e1f36e339b4451b1d38a3affb7587caa798719ab00ee4d3200cee541952","target":"graph","created_at":"2026-05-18T00:35:31Z","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 calculated the magnetic dipole and the electric quadrupole hyperfine interaction constants of 3s3p $^{3,1}P^o_1$ states and the isotope shift, including mass and field shift, factors for transitions from these two states to the ground state 3s$^2~^1S_0$ in Al$^+$ ions using the multiconfiguration Dirac-Hartree-Fock method. The effects of the electron correlations and the Breit interaction on these physical quantities were investigated in detail based on the active space approach. It is found that the CC and the higher-order correlations are considerable for evaluating the uncertainties of t","authors_text":"Jiguang Li, Luyou Xie, Tingxian Zhang, Zehuang Lu","cross_cats":["nucl-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2017-06-28T02:22:45Z","title":"Theoretical study on the hyperfine interaction constants and the isotope shift factors for the $3s^2~^1 S_{ 0} ~-~ 3s3p~^{3,1}P^o_1$ transitions in Al$^+$"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1706.09104","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":"sha256:1e860ab9ce6aba7d44f875f94bce03e2ef53a1d2a5c29da1d7a21a53a8441d13","target":"record","created_at":"2026-05-18T00:35:31Z","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":"db25e1b48b8c0c35fd6175db92715c41ffc9b8158e4b7797c078754ed07ea743","cross_cats_sorted":["nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2017-06-28T02:22:45Z","title_canon_sha256":"27149bccfb165a20e1aefedf14841a332682169c0e2bd3d82c4b18f9b4777c79"},"schema_version":"1.0","source":{"id":"1706.09104","kind":"arxiv","version":1}},"canonical_sha256":"6516ad2ef5dde026b321fdddbb169f370bb5924308fce1fdac02ba4d12fb4f2d","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"6516ad2ef5dde026b321fdddbb169f370bb5924308fce1fdac02ba4d12fb4f2d","first_computed_at":"2026-05-18T00:35:31.108993Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:35:31.108993Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"BZJ6rVwfcJjWkIwy3ZPJfQqjsoZLpGHjxj9/OB/aryE3m9jAvsq7/AARYFE4uSpo724YZvtEPU/XUI+vV1d9AA==","signature_status":"signed_v1","signed_at":"2026-05-18T00:35:31.109451Z","signed_message":"canonical_sha256_bytes"},"source_id":"1706.09104","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:1e860ab9ce6aba7d44f875f94bce03e2ef53a1d2a5c29da1d7a21a53a8441d13","sha256:8e589e1f36e339b4451b1d38a3affb7587caa798719ab00ee4d3200cee541952"],"state_sha256":"30ee490693327c82fbfe4a002410e7ca64805978cd97da9f581b2988ef996837"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"9tQUIsC3Ic0aujvZrn5R2U8zg6b+LLv/NxYZj8YcTQrsnai/2slZOYeFWa1BSEIFk1U/AreegNQd4qVS1fjqDA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-05T10:23:55.017813Z","bundle_sha256":"403c9dc535257e386ad29702542175765c8b84191a6335ffa739fd19505819e6"}}