{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:UKSAL2IVEV4EMFLKSCSSKNCVPH","short_pith_number":"pith:UKSAL2IV","schema_version":"1.0","canonical_sha256":"a2a405e915257846156a90a525345579cec23b311b989ff1d3e3db02532e4d90","source":{"kind":"arxiv","id":"1408.1823","version":1},"attestation_state":"computed","paper":{"title":"Experimental study of ionization yield of liquid xenon for electron recoils in the energy range 2.8 - 80 keV","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"physics.ins-det","authors_text":"A.A. Burenkov, A.G. Kovalenko, A.I. Bolozdynya, A.K. Karelin, A.M. Konovalov, A.S. Kobyakin, A.V. Etenko, A.V. Khromov, A.V. Kuchenkov, A.V. Kumpan, D.A. Egorov, D.G. Rudik, D.Yu. Akimov, I.S. Alexandrov, M.A. Gulin, M.A. Kirsanov, R.I. Nikolaev, S.G. Klimanov, S.V. Ivakhin, V.A. Belov, V.A. Kaplin, V.N. Stekhanov, V.V. Afanasyev, V.V. Sosnovtsev, Yu.A. Melikyan, Yu.V. Efremenko","submitted_at":"2014-08-08T11:35:36Z","abstract_excerpt":"We present the results of the first experimental study of ionization yield of electron recoils with energies below 100 keV produced in liquid xenon by the isotopes: 37Ar, 83mKr, 241Am, 129Xe, 131Xe. It is confirmed by a direct measurement with 37Ar isotope (2.82 keV) that the ionization yield is growing up with the energy decrease in the energy range below ~ 10 keV accordingly to the NEST predictions. Decay time of scintillation at 2.82 keV is measured to be 25 +/- 3 ns at the electric field of 3.75 kV/cm."},"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":"1408.1823","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.ins-det","submitted_at":"2014-08-08T11:35:36Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"cafff8f5b9d23d46cdd266f8e4175150176beab08cc04c8b078140e4fc52b0ee","abstract_canon_sha256":"66f2920a9fe753849a4fd801b1eb2255a50bd431ecf9a539b1bf6ca4374eadc9"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:42:22.565089Z","signature_b64":"hqBkMeXp85J6zSAWvs9IMa9LMjLrSJ/ZBa6rfhs6sqWOrqydsPac3V0UNYjjKroJYNKdWGozaeF/sv4siSP5Cg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a2a405e915257846156a90a525345579cec23b311b989ff1d3e3db02532e4d90","last_reissued_at":"2026-05-18T01:42:22.564367Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:42:22.564367Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Experimental study of ionization yield of liquid xenon for electron recoils in the energy range 2.8 - 80 keV","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"physics.ins-det","authors_text":"A.A. Burenkov, A.G. Kovalenko, A.I. Bolozdynya, A.K. Karelin, A.M. Konovalov, A.S. Kobyakin, A.V. Etenko, A.V. Khromov, A.V. Kuchenkov, A.V. Kumpan, D.A. Egorov, D.G. Rudik, D.Yu. Akimov, I.S. Alexandrov, M.A. Gulin, M.A. Kirsanov, R.I. Nikolaev, S.G. Klimanov, S.V. Ivakhin, V.A. Belov, V.A. Kaplin, V.N. Stekhanov, V.V. Afanasyev, V.V. Sosnovtsev, Yu.A. Melikyan, Yu.V. Efremenko","submitted_at":"2014-08-08T11:35:36Z","abstract_excerpt":"We present the results of the first experimental study of ionization yield of electron recoils with energies below 100 keV produced in liquid xenon by the isotopes: 37Ar, 83mKr, 241Am, 129Xe, 131Xe. It is confirmed by a direct measurement with 37Ar isotope (2.82 keV) that the ionization yield is growing up with the energy decrease in the energy range below ~ 10 keV accordingly to the NEST predictions. Decay time of scintillation at 2.82 keV is measured to be 25 +/- 3 ns at the electric field of 3.75 kV/cm."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1408.1823","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":"1408.1823","created_at":"2026-05-18T01:42:22.564497+00:00"},{"alias_kind":"arxiv_version","alias_value":"1408.1823v1","created_at":"2026-05-18T01:42:22.564497+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1408.1823","created_at":"2026-05-18T01:42:22.564497+00:00"},{"alias_kind":"pith_short_12","alias_value":"UKSAL2IVEV4E","created_at":"2026-05-18T12:28:52.271510+00:00"},{"alias_kind":"pith_short_16","alias_value":"UKSAL2IVEV4EMFLK","created_at":"2026-05-18T12:28:52.271510+00:00"},{"alias_kind":"pith_short_8","alias_value":"UKSAL2IV","created_at":"2026-05-18T12:28:52.271510+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/UKSAL2IVEV4EMFLKSCSSKNCVPH","json":"https://pith.science/pith/UKSAL2IVEV4EMFLKSCSSKNCVPH.json","graph_json":"https://pith.science/api/pith-number/UKSAL2IVEV4EMFLKSCSSKNCVPH/graph.json","events_json":"https://pith.science/api/pith-number/UKSAL2IVEV4EMFLKSCSSKNCVPH/events.json","paper":"https://pith.science/paper/UKSAL2IV"},"agent_actions":{"view_html":"https://pith.science/pith/UKSAL2IVEV4EMFLKSCSSKNCVPH","download_json":"https://pith.science/pith/UKSAL2IVEV4EMFLKSCSSKNCVPH.json","view_paper":"https://pith.science/paper/UKSAL2IV","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1408.1823&json=true","fetch_graph":"https://pith.science/api/pith-number/UKSAL2IVEV4EMFLKSCSSKNCVPH/graph.json","fetch_events":"https://pith.science/api/pith-number/UKSAL2IVEV4EMFLKSCSSKNCVPH/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/UKSAL2IVEV4EMFLKSCSSKNCVPH/action/timestamp_anchor","attest_storage":"https://pith.science/pith/UKSAL2IVEV4EMFLKSCSSKNCVPH/action/storage_attestation","attest_author":"https://pith.science/pith/UKSAL2IVEV4EMFLKSCSSKNCVPH/action/author_attestation","sign_citation":"https://pith.science/pith/UKSAL2IVEV4EMFLKSCSSKNCVPH/action/citation_signature","submit_replication":"https://pith.science/pith/UKSAL2IVEV4EMFLKSCSSKNCVPH/action/replication_record"}},"created_at":"2026-05-18T01:42:22.564497+00:00","updated_at":"2026-05-18T01:42:22.564497+00:00"}