{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:3NGLBOWCRZRFVDE55JOLC4WBVL","short_pith_number":"pith:3NGLBOWC","schema_version":"1.0","canonical_sha256":"db4cb0bac28e625a8c9dea5cb172c1aaf3bd0002532be32ea4b6bb2093e75110","source":{"kind":"arxiv","id":"1706.04832","version":1},"attestation_state":"computed","paper":{"title":"Single photoionization of the Zn II ion in the photon energy range 17.5 to 90.0 eV: experiment and theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.atom-ph","authors_text":"A. Antill\\'on, A. L. D. Kilcoyne, A. M. Covington, A. M. Ju\\'arez, A. Morales-Mori, B. M. McLaughlin, D. Calabrese, E. M. Hern\\'andez, G. Hinojosa, J. S. Thompson, O. Windelius, V. T. Davis","submitted_at":"2017-06-14T17:30:44Z","abstract_excerpt":"Measurements of the single photoionization cross section of Cu-like Zn$^+$ ions are reported in the energy (wavelength) range 17.5 eV (709 \\AA) to 90 eV (138 \\AA). The measurements on this {\\it trans}-Fe element were performed at the Advanced Light Source synchrotron radiation facility in Berkeley, California at a photon energy resolution of 17 meV using the photon-ion merged-beams end-station. Below 30 eV the spectrum is dominated by excitation autoionizing resonance states. The experimental results are compared with large-scale photoionization cross-section calculations performed using a Dir"},"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":"1706.04832","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2017-06-14T17:30:44Z","cross_cats_sorted":[],"title_canon_sha256":"fe0fef03482cf966e6e7dedd20ccc5acbc6d9793282037d189ffdebb78eccf3f","abstract_canon_sha256":"eba7700227a7d0b49e4ecc43d574f9b7c5db03d6987302aa848c7be8ff6c1bca"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:39:31.491580Z","signature_b64":"ht37ll3xmH3kKA0nD1FWCmfv6WCBBakN2H+Nk8+BOb9D/M3/lVNlVilStBf9PgGEXRRJB20MSU/fiBb5kr/9BQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"db4cb0bac28e625a8c9dea5cb172c1aaf3bd0002532be32ea4b6bb2093e75110","last_reissued_at":"2026-05-18T00:39:31.491058Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:39:31.491058Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Single photoionization of the Zn II ion in the photon energy range 17.5 to 90.0 eV: experiment and theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.atom-ph","authors_text":"A. Antill\\'on, A. L. D. Kilcoyne, A. M. Covington, A. M. Ju\\'arez, A. Morales-Mori, B. M. McLaughlin, D. Calabrese, E. M. Hern\\'andez, G. Hinojosa, J. S. Thompson, O. Windelius, V. T. Davis","submitted_at":"2017-06-14T17:30:44Z","abstract_excerpt":"Measurements of the single photoionization cross section of Cu-like Zn$^+$ ions are reported in the energy (wavelength) range 17.5 eV (709 \\AA) to 90 eV (138 \\AA). The measurements on this {\\it trans}-Fe element were performed at the Advanced Light Source synchrotron radiation facility in Berkeley, California at a photon energy resolution of 17 meV using the photon-ion merged-beams end-station. Below 30 eV the spectrum is dominated by excitation autoionizing resonance states. The experimental results are compared with large-scale photoionization cross-section calculations performed using a Dir"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1706.04832","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":"1706.04832","created_at":"2026-05-18T00:39:31.491137+00:00"},{"alias_kind":"arxiv_version","alias_value":"1706.04832v1","created_at":"2026-05-18T00:39:31.491137+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1706.04832","created_at":"2026-05-18T00:39:31.491137+00:00"},{"alias_kind":"pith_short_12","alias_value":"3NGLBOWCRZRF","created_at":"2026-05-18T12:30:58.224056+00:00"},{"alias_kind":"pith_short_16","alias_value":"3NGLBOWCRZRFVDE5","created_at":"2026-05-18T12:30:58.224056+00:00"},{"alias_kind":"pith_short_8","alias_value":"3NGLBOWC","created_at":"2026-05-18T12:30:58.224056+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/3NGLBOWCRZRFVDE55JOLC4WBVL","json":"https://pith.science/pith/3NGLBOWCRZRFVDE55JOLC4WBVL.json","graph_json":"https://pith.science/api/pith-number/3NGLBOWCRZRFVDE55JOLC4WBVL/graph.json","events_json":"https://pith.science/api/pith-number/3NGLBOWCRZRFVDE55JOLC4WBVL/events.json","paper":"https://pith.science/paper/3NGLBOWC"},"agent_actions":{"view_html":"https://pith.science/pith/3NGLBOWCRZRFVDE55JOLC4WBVL","download_json":"https://pith.science/pith/3NGLBOWCRZRFVDE55JOLC4WBVL.json","view_paper":"https://pith.science/paper/3NGLBOWC","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1706.04832&json=true","fetch_graph":"https://pith.science/api/pith-number/3NGLBOWCRZRFVDE55JOLC4WBVL/graph.json","fetch_events":"https://pith.science/api/pith-number/3NGLBOWCRZRFVDE55JOLC4WBVL/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/3NGLBOWCRZRFVDE55JOLC4WBVL/action/timestamp_anchor","attest_storage":"https://pith.science/pith/3NGLBOWCRZRFVDE55JOLC4WBVL/action/storage_attestation","attest_author":"https://pith.science/pith/3NGLBOWCRZRFVDE55JOLC4WBVL/action/author_attestation","sign_citation":"https://pith.science/pith/3NGLBOWCRZRFVDE55JOLC4WBVL/action/citation_signature","submit_replication":"https://pith.science/pith/3NGLBOWCRZRFVDE55JOLC4WBVL/action/replication_record"}},"created_at":"2026-05-18T00:39:31.491137+00:00","updated_at":"2026-05-18T00:39:31.491137+00:00"}