{"id":"W3201832447","doi":"10.1021/acs.nanolett.1c02853","title":"The Effect of Photoinduced Surface Oxygen Vacancies on the Charge Carrier Dynamics in TiO<sub>2</sub> Films","year":2021,"lang":"en","type":"article","venue":"Nano Letters","topic":"Electronic and Structural Properties of Oxides","field":"Materials Science","cited_by":59,"is_retracted":false,"has_abstract":true,"ca_institutions":"McGill University; École de Technologie Supérieure; Université du Québec à Montréal","funders":"Engineering and Physical Sciences Research Council; Ministerio de Educación y Formación Profesional; Fonds de recherche du Québec – Nature et technologies; Deutsche Forschungsgemeinschaft; European Commission; Natural Sciences and Engineering Research Council of Canada; École de technologie supérieure","keywords":"Chemical physics; Vacancy defect; Materials science; Charge carrier; Semiconductor; Electron; Nucleation; Nanotechnology; Dynamics (music); Oxygen; Oxide; Titanium dioxide; Condensed matter physics; Chemistry; Optoelectronics; Physics","routes":{"ca_aff":true,"ca_fund":true,"ca_venue":false,"about_ca":false,"invisible_to_affiliation_only":false},"retraction":null,"screen":null,"direct_labels":[],"prediction":{"model_version":"metacan-v3-hybrid-931329e0061c","candidate_categories":[],"consensus_categories":[],"category_scores_codex":[0.00008890145,0.0002314303,0.000134832,0.00011122,0.00020653,0.0002471223,0.0002583688,0.0002971304,0.001391372],"category_scores_gemma":[0.000354222,0.000137799,0.0001095604,0.0001470234,0.0002854496,0.0003547123,0.0001084271,0.0004558635,0.000122773],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.0003872112,"about_ca_system_score_gemma":0.0001252479,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.001664619,"about_ca_topic_score_gemma":0.001967243,"domain_scores_codex":[0.9999295,0.000005834491,0.000003225402,0.00001853939,0.00002243192,0.00002045085],"domain_scores_gemma":[0.9997868,0.0001003741,0.00005737854,0.00001165769,0.00002655672,0.00001725697],"domain_codex":null,"domain_gemma":null,"domain_candidate":null,"domain_consensus":null,"study_design_codex":"bench_or_experimental","study_design_gemma":"bench_or_experimental","study_design_scores_codex":[0.0001316136,0.00004569123,0.0006310133,0.0000697593,0.0000108753,0.00009755051,0.0001188381,0.0003259909,0.9949361,0.0001566596,0.0001293189,0.003346392],"study_design_scores_gemma":[0.00001303522,0.000244668,0.01122036,0.000006773097,0.00001152741,0.00008439032,0.000135357,0.006036727,0.9811995,0.00006452553,0.0009710335,0.00001206863],"study_design_candidate":"bench_or_experimental","study_design_consensus":"bench_or_experimental","genre_codex":"empirical","genre_gemma":"empirical","genre_scores_codex":[0.9986162,0.0003666306,0.0003361479,0.00005165286,0.00001642593,0.00000661311,0.00008705317,0.00002206408,0.0004971509],"genre_scores_gemma":[0.9989595,0.0002377635,0.0002842816,0.00002520233,0.000005864634,0.000008985061,0.00004701707,0.000009885021,0.0004214002],"genre_candidate":"empirical","genre_consensus":"empirical","teacher_disagreement_score":0.001664619,"threshold_uncertainty_score":0.004654646,"prediction_status":"machine_predicted_unvalidated"},"machine_scores":{"provisional":true,"baseline":true,"maturity_gate_passed":false,"score_opus":0.006082207451351753,"score_gpt":0.1979090601590869,"score_spread":0.1918268527077351,"validation_status":"score_only:v0-immature-baseline","note":"Baseline scores from an immature model (maturity gate not passed). Scores rank; they never assert a category."}}