Matthew Zervos, Ioannis Paschos, Pavlos Savvidis, Nikoletta Florini, Konstantinos Koutsokostas, Philomela Komninou, Nektarios N. Lathiotakis, P. M. Levendis and Sarantos Marinakis
{"title":"High crystal quality and purity Cu2O by consecutive in situ annealing and thermal oxidation of Cu under H2 and O2 at elevated temperatures†","authors":"Matthew Zervos, Ioannis Paschos, Pavlos Savvidis, Nikoletta Florini, Konstantinos Koutsokostas, Philomela Komninou, Nektarios N. Lathiotakis, P. M. Levendis and Sarantos Marinakis","doi":"10.1039/D4CE01276C","DOIUrl":null,"url":null,"abstract":"<p >Cu<small><sub>2</sub></small>O has been obtained <em>via</em> the thermal oxidation of Cu foils with a maximum thickness of 120 μm under Ar and O<small><sub>2</sub></small> at 1020 °C for 30 min. Care was taken to suppress the oxidation of Cu during the temperature ramp by using H<small><sub>2</sub></small> prior to admitting O<small><sub>2</sub></small> at 1020 °C. We suggest that the ruby red Cu<small><sub>2</sub></small>O crystals are obtained in this way by strain-driven grain growth and consist of ∼500 μm grains that have a cubic crystal structure. More importantly we find that the crystal quality and purity of the Cu<small><sub>2</sub></small>O is improved significantly by pre-annealing the Cu under Ar and H<small><sub>2</sub></small> at 1000 °C and 10 mbar for up to 180 min. The Cu<small><sub>2</sub></small>O exhibited photoluminescence at 6.5 K with a maximum at 2.01 eV corresponding to the direct energy gap in very good agreement with density functional theory calculations of the electronic band structure. No emission due to recombination of bound excitons to copper vacancies V<small><sub>Cu</sub></small> and single V<small><sub>O</sub></small> or double charged V<small><sub>O</sub></small> oxygen vacancies was observed consistent with high crystal quality Cu<small><sub>2</sub></small>O. We find that the Cu<small><sub>2</sub></small>O crystals obtained in this way are p-type and the highest mobility measured at room temperature was <em>μ</em><small><sub>p</sub></small> = 82 cm V<small><sup>−1</sup></small> s<small><sup>−1</sup></small> with a carrier density of 7.3 × 10 cm<small><sup>3</sup></small>.</p>","PeriodicalId":70,"journal":{"name":"CrystEngComm","volume":" 13","pages":" 1977-1985"},"PeriodicalIF":2.6000,"publicationDate":"2025-02-25","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://pubs.rsc.org/en/content/articlepdf/2025/ce/d4ce01276c?page=search","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"CrystEngComm","FirstCategoryId":"92","ListUrlMain":"https://pubs.rsc.org/en/content/articlelanding/2025/ce/d4ce01276c","RegionNum":3,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"CHEMISTRY, MULTIDISCIPLINARY","Score":null,"Total":0}
引用次数: 0
Abstract
Cu2O has been obtained via the thermal oxidation of Cu foils with a maximum thickness of 120 μm under Ar and O2 at 1020 °C for 30 min. Care was taken to suppress the oxidation of Cu during the temperature ramp by using H2 prior to admitting O2 at 1020 °C. We suggest that the ruby red Cu2O crystals are obtained in this way by strain-driven grain growth and consist of ∼500 μm grains that have a cubic crystal structure. More importantly we find that the crystal quality and purity of the Cu2O is improved significantly by pre-annealing the Cu under Ar and H2 at 1000 °C and 10 mbar for up to 180 min. The Cu2O exhibited photoluminescence at 6.5 K with a maximum at 2.01 eV corresponding to the direct energy gap in very good agreement with density functional theory calculations of the electronic band structure. No emission due to recombination of bound excitons to copper vacancies VCu and single VO or double charged VO oxygen vacancies was observed consistent with high crystal quality Cu2O. We find that the Cu2O crystals obtained in this way are p-type and the highest mobility measured at room temperature was μp = 82 cm V−1 s−1 with a carrier density of 7.3 × 10 cm3.