{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:JLLLAHSX7GKFT2TDQABT7UINHN","short_pith_number":"pith:JLLLAHSX","schema_version":"1.0","canonical_sha256":"4ad6b01e57f99459ea6380033fd10d3b41ce6a4a190790c46440c6180cd60734","source":{"kind":"arxiv","id":"1609.02183","version":1},"attestation_state":"computed","paper":{"title":"Experimental radiative lifetimes for highly excited states and calculated oscillator strengths for lines of astrophysical interest in singly ionized cobalt (Co II)","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.atom-ph"],"primary_cat":"astro-ph.SR","authors_text":"H. Hartman, H. Lundberg, H. Nilsson, L. Engstrom, P. Palmeri, P. Quinet, V. Fivet","submitted_at":"2016-09-07T20:43:59Z","abstract_excerpt":"This work reports new experimental radiative lifetimes and calculated oscillator strengths for transitions of astrophysical interest in singly ionized cobalt. More precisely, nineteen radiative lifetimes in Co+ have been measured with the time-resolved laser-induced fluorescence technique using one- and two-step excitations. Out of these, seven belonging to the high lying 3d$^7$($^4$F)4d configuration in the energy range 90697 - 93738 cm$^{-1}$ are new, and the other twelve from th3d$^7$($^4$F)F)4p configuration with energies between 45972 and 49328 cm$^{-1}$1 are compared with previous measur"},"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":"1609.02183","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"astro-ph.SR","submitted_at":"2016-09-07T20:43:59Z","cross_cats_sorted":["physics.atom-ph"],"title_canon_sha256":"9109e6c61ba0e9cb4dec764bb8e01e0e7297badef407e8e370a644ac0146535c","abstract_canon_sha256":"59d3a99f8c956aa79bf97aabad846c9a17439fd7cf6792c309e5139e4930ff1b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:03:37.508265Z","signature_b64":"Bk+v2TzwoSlFIhQZpIEvyUNialsWON/twn638ou4OVjOCjxFKuEY+2uVEcK/YObHZADsYRs7Jm3O/TXA0EexDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4ad6b01e57f99459ea6380033fd10d3b41ce6a4a190790c46440c6180cd60734","last_reissued_at":"2026-05-18T01:03:37.507581Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:03:37.507581Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Experimental radiative lifetimes for highly excited states and calculated oscillator strengths for lines of astrophysical interest in singly ionized cobalt (Co II)","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.atom-ph"],"primary_cat":"astro-ph.SR","authors_text":"H. Hartman, H. Lundberg, H. Nilsson, L. Engstrom, P. Palmeri, P. Quinet, V. Fivet","submitted_at":"2016-09-07T20:43:59Z","abstract_excerpt":"This work reports new experimental radiative lifetimes and calculated oscillator strengths for transitions of astrophysical interest in singly ionized cobalt. More precisely, nineteen radiative lifetimes in Co+ have been measured with the time-resolved laser-induced fluorescence technique using one- and two-step excitations. Out of these, seven belonging to the high lying 3d$^7$($^4$F)4d configuration in the energy range 90697 - 93738 cm$^{-1}$ are new, and the other twelve from th3d$^7$($^4$F)F)4p configuration with energies between 45972 and 49328 cm$^{-1}$1 are compared with previous measur"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1609.02183","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":"1609.02183","created_at":"2026-05-18T01:03:37.507671+00:00"},{"alias_kind":"arxiv_version","alias_value":"1609.02183v1","created_at":"2026-05-18T01:03:37.507671+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1609.02183","created_at":"2026-05-18T01:03:37.507671+00:00"},{"alias_kind":"pith_short_12","alias_value":"JLLLAHSX7GKF","created_at":"2026-05-18T12:30:25.849896+00:00"},{"alias_kind":"pith_short_16","alias_value":"JLLLAHSX7GKFT2TD","created_at":"2026-05-18T12:30:25.849896+00:00"},{"alias_kind":"pith_short_8","alias_value":"JLLLAHSX","created_at":"2026-05-18T12:30:25.849896+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/JLLLAHSX7GKFT2TDQABT7UINHN","json":"https://pith.science/pith/JLLLAHSX7GKFT2TDQABT7UINHN.json","graph_json":"https://pith.science/api/pith-number/JLLLAHSX7GKFT2TDQABT7UINHN/graph.json","events_json":"https://pith.science/api/pith-number/JLLLAHSX7GKFT2TDQABT7UINHN/events.json","paper":"https://pith.science/paper/JLLLAHSX"},"agent_actions":{"view_html":"https://pith.science/pith/JLLLAHSX7GKFT2TDQABT7UINHN","download_json":"https://pith.science/pith/JLLLAHSX7GKFT2TDQABT7UINHN.json","view_paper":"https://pith.science/paper/JLLLAHSX","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1609.02183&json=true","fetch_graph":"https://pith.science/api/pith-number/JLLLAHSX7GKFT2TDQABT7UINHN/graph.json","fetch_events":"https://pith.science/api/pith-number/JLLLAHSX7GKFT2TDQABT7UINHN/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/JLLLAHSX7GKFT2TDQABT7UINHN/action/timestamp_anchor","attest_storage":"https://pith.science/pith/JLLLAHSX7GKFT2TDQABT7UINHN/action/storage_attestation","attest_author":"https://pith.science/pith/JLLLAHSX7GKFT2TDQABT7UINHN/action/author_attestation","sign_citation":"https://pith.science/pith/JLLLAHSX7GKFT2TDQABT7UINHN/action/citation_signature","submit_replication":"https://pith.science/pith/JLLLAHSX7GKFT2TDQABT7UINHN/action/replication_record"}},"created_at":"2026-05-18T01:03:37.507671+00:00","updated_at":"2026-05-18T01:03:37.507671+00:00"}