{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2026:WBPQRINY6RO4SUKC6DFWCM3YRU","short_pith_number":"pith:WBPQRINY","schema_version":"1.0","canonical_sha256":"b05f08a1b8f45dc95142f0cb6133788d305f5d69265037c30fe30143873ae029","source":{"kind":"arxiv","id":"2607.03175","version":1},"attestation_state":"computed","paper":{"title":"Calculation of the energy levels and hyperfine structure for Xe~II, Rn~II, and Og~II ions","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"physics.atom-ph","authors_text":"T. H. Dinh, V. A. Dzuba, V. V. Flambaum","submitted_at":"2026-07-03T10:24:18Z","abstract_excerpt":"Energy levels, Land\\'e $g$-factors, and hyperfine-structure constants are calculated for the singly ionized noble-gas atoms Xe II, Rn II, and Og II. The calculations are performed using the configuration-interaction method with perturbative treatment of high-lying configurations. Core polarization effects in the hyperfine interaction are included within the time-dependent Hartree-Fock method. Calculations for Xe II are used to test the accuracy of the approach by comparison with available experimental data. The agreement is at the level of about one percent for the energies and typically about"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"2607.03175","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.atom-ph","submitted_at":"2026-07-03T10:24:18Z","cross_cats_sorted":[],"title_canon_sha256":"6e0fd6766d065a6d55fb16e84b5b8fb98842c6fec341563d5eca43f20ab98b5b","abstract_canon_sha256":"7d948fb10081aa96f8cdd421d50a5aace2ca7a43de5670e25a32bf5eebd19c14"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-07T01:16:45.638579Z","signature_b64":"c01KwXzoNPEeWY5RAOq76/ebLda05skbVXIslIMBlDHMQvQYFoF9CrbKEAHTGRjQ4NF/7aMgKGBHAtHCtag+Bw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b05f08a1b8f45dc95142f0cb6133788d305f5d69265037c30fe30143873ae029","last_reissued_at":"2026-07-07T01:16:45.638097Z","signature_status":"signed_v1","first_computed_at":"2026-07-07T01:16:45.638097Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Calculation of the energy levels and hyperfine structure for Xe~II, Rn~II, and Og~II ions","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"physics.atom-ph","authors_text":"T. H. Dinh, V. A. Dzuba, V. V. Flambaum","submitted_at":"2026-07-03T10:24:18Z","abstract_excerpt":"Energy levels, Land\\'e $g$-factors, and hyperfine-structure constants are calculated for the singly ionized noble-gas atoms Xe II, Rn II, and Og II. The calculations are performed using the configuration-interaction method with perturbative treatment of high-lying configurations. Core polarization effects in the hyperfine interaction are included within the time-dependent Hartree-Fock method. Calculations for Xe II are used to test the accuracy of the approach by comparison with available experimental data. The agreement is at the level of about one percent for the energies and typically about"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2607.03175","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/2607.03175/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"},"aliases":[{"alias_kind":"arxiv","alias_value":"2607.03175","created_at":"2026-07-07T01:16:45.638169+00:00"},{"alias_kind":"arxiv_version","alias_value":"2607.03175v1","created_at":"2026-07-07T01:16:45.638169+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2607.03175","created_at":"2026-07-07T01:16:45.638169+00:00"},{"alias_kind":"pith_short_12","alias_value":"WBPQRINY6RO4","created_at":"2026-07-07T01:16:45.638169+00:00"},{"alias_kind":"pith_short_16","alias_value":"WBPQRINY6RO4SUKC","created_at":"2026-07-07T01:16:45.638169+00:00"},{"alias_kind":"pith_short_8","alias_value":"WBPQRINY","created_at":"2026-07-07T01:16:45.638169+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/WBPQRINY6RO4SUKC6DFWCM3YRU","json":"https://pith.science/pith/WBPQRINY6RO4SUKC6DFWCM3YRU.json","graph_json":"https://pith.science/api/pith-number/WBPQRINY6RO4SUKC6DFWCM3YRU/graph.json","events_json":"https://pith.science/api/pith-number/WBPQRINY6RO4SUKC6DFWCM3YRU/events.json","paper":"https://pith.science/paper/WBPQRINY"},"agent_actions":{"view_html":"https://pith.science/pith/WBPQRINY6RO4SUKC6DFWCM3YRU","download_json":"https://pith.science/pith/WBPQRINY6RO4SUKC6DFWCM3YRU.json","view_paper":"https://pith.science/paper/WBPQRINY","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2607.03175&json=true","fetch_graph":"https://pith.science/api/pith-number/WBPQRINY6RO4SUKC6DFWCM3YRU/graph.json","fetch_events":"https://pith.science/api/pith-number/WBPQRINY6RO4SUKC6DFWCM3YRU/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/WBPQRINY6RO4SUKC6DFWCM3YRU/action/timestamp_anchor","attest_storage":"https://pith.science/pith/WBPQRINY6RO4SUKC6DFWCM3YRU/action/storage_attestation","attest_author":"https://pith.science/pith/WBPQRINY6RO4SUKC6DFWCM3YRU/action/author_attestation","sign_citation":"https://pith.science/pith/WBPQRINY6RO4SUKC6DFWCM3YRU/action/citation_signature","submit_replication":"https://pith.science/pith/WBPQRINY6RO4SUKC6DFWCM3YRU/action/replication_record"}},"created_at":"2026-07-07T01:16:45.638169+00:00","updated_at":"2026-07-07T01:16:45.638169+00:00"}