{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:HXJ5EIEZHGCQT4C2KHTUQ3O2GO","short_pith_number":"pith:HXJ5EIEZ","schema_version":"1.0","canonical_sha256":"3dd3d22099398509f05a51e7486dda339f39874fe8eaa7bb6f3ad757d7916626","source":{"kind":"arxiv","id":"1208.1522","version":1},"attestation_state":"computed","paper":{"title":"Comment on \"Experimental Studies of Os^-: Observation of a Bound-Bound Electric Dipole Transition in an Atomic Negative Ion\"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.atom-ph","authors_text":"Alfred Z. Msezane, Filmon Kiros, Kelvin Suggs, Zineb Felfli","submitted_at":"2012-08-07T20:50:49Z","abstract_excerpt":"Bilodeau and Haugan [1], using Infrared laser photodetachment spectroscopy, measured the binding energies (BEs) of the ground state (4Fe9/2) and the excited state (4Fe7/2) of the Os^- ion to be 1.07780(12) eV and 0.553(3) eV, respectively. These values are consistent with those calculated using Relativistic Configuration Interaction (RCI) calculations [2]. Here we have calculated the BEs for the ground state and the two excited states of the Os^- ion using our recent complex angular momentum (CAM) methodology [3] and obtained the BEs of 1.910, 1.230 and 0.224 eV, respectively (see Figure). We "},"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":"1208.1522","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2012-08-07T20:50:49Z","cross_cats_sorted":[],"title_canon_sha256":"fcb45c978d0b47464cd74e92ea95caa0b39ff6164220481087012104d7c07c9b","abstract_canon_sha256":"0cdada269cc997ba65025a5c92891526831d44ff0a08f2c37b76422272818cc7"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:49:11.346594Z","signature_b64":"3iToanV4XtxvABwZBR9+Q2wBw8kDtkMmMCRHpKnzrn8SxX4aCTyJTjZF2K0qzRl3NVGgcNHYdIxdUcLEOBNoDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3dd3d22099398509f05a51e7486dda339f39874fe8eaa7bb6f3ad757d7916626","last_reissued_at":"2026-05-18T03:49:11.345951Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:49:11.345951Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Comment on \"Experimental Studies of Os^-: Observation of a Bound-Bound Electric Dipole Transition in an Atomic Negative Ion\"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.atom-ph","authors_text":"Alfred Z. Msezane, Filmon Kiros, Kelvin Suggs, Zineb Felfli","submitted_at":"2012-08-07T20:50:49Z","abstract_excerpt":"Bilodeau and Haugan [1], using Infrared laser photodetachment spectroscopy, measured the binding energies (BEs) of the ground state (4Fe9/2) and the excited state (4Fe7/2) of the Os^- ion to be 1.07780(12) eV and 0.553(3) eV, respectively. These values are consistent with those calculated using Relativistic Configuration Interaction (RCI) calculations [2]. Here we have calculated the BEs for the ground state and the two excited states of the Os^- ion using our recent complex angular momentum (CAM) methodology [3] and obtained the BEs of 1.910, 1.230 and 0.224 eV, respectively (see Figure). We "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1208.1522","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1208.1522","created_at":"2026-05-18T03:49:11.346040+00:00"},{"alias_kind":"arxiv_version","alias_value":"1208.1522v1","created_at":"2026-05-18T03:49:11.346040+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1208.1522","created_at":"2026-05-18T03:49:11.346040+00:00"},{"alias_kind":"pith_short_12","alias_value":"HXJ5EIEZHGCQ","created_at":"2026-05-18T12:27:09.501522+00:00"},{"alias_kind":"pith_short_16","alias_value":"HXJ5EIEZHGCQT4C2","created_at":"2026-05-18T12:27:09.501522+00:00"},{"alias_kind":"pith_short_8","alias_value":"HXJ5EIEZ","created_at":"2026-05-18T12:27:09.501522+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/HXJ5EIEZHGCQT4C2KHTUQ3O2GO","json":"https://pith.science/pith/HXJ5EIEZHGCQT4C2KHTUQ3O2GO.json","graph_json":"https://pith.science/api/pith-number/HXJ5EIEZHGCQT4C2KHTUQ3O2GO/graph.json","events_json":"https://pith.science/api/pith-number/HXJ5EIEZHGCQT4C2KHTUQ3O2GO/events.json","paper":"https://pith.science/paper/HXJ5EIEZ"},"agent_actions":{"view_html":"https://pith.science/pith/HXJ5EIEZHGCQT4C2KHTUQ3O2GO","download_json":"https://pith.science/pith/HXJ5EIEZHGCQT4C2KHTUQ3O2GO.json","view_paper":"https://pith.science/paper/HXJ5EIEZ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1208.1522&json=true","fetch_graph":"https://pith.science/api/pith-number/HXJ5EIEZHGCQT4C2KHTUQ3O2GO/graph.json","fetch_events":"https://pith.science/api/pith-number/HXJ5EIEZHGCQT4C2KHTUQ3O2GO/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/HXJ5EIEZHGCQT4C2KHTUQ3O2GO/action/timestamp_anchor","attest_storage":"https://pith.science/pith/HXJ5EIEZHGCQT4C2KHTUQ3O2GO/action/storage_attestation","attest_author":"https://pith.science/pith/HXJ5EIEZHGCQT4C2KHTUQ3O2GO/action/author_attestation","sign_citation":"https://pith.science/pith/HXJ5EIEZHGCQT4C2KHTUQ3O2GO/action/citation_signature","submit_replication":"https://pith.science/pith/HXJ5EIEZHGCQT4C2KHTUQ3O2GO/action/replication_record"}},"created_at":"2026-05-18T03:49:11.346040+00:00","updated_at":"2026-05-18T03:49:11.346040+00:00"}