Effect of impurity in Cu 2 O nanowires on the degradation of methyl orange

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Effect of impurity in ­Cu2O nanowires on the degradation of methyl orange Zhipeng Xie1 · Yan Zhou1 · Linlin Guan1 · Sajjad Muhammad1 · Yuhan Jiang1 · Shuyu Zhang1 · Chunxin Yu1 · Yangjing Jiao1 · Shuangshuang Zhang1 · Yang Ren1 · Xiaowei Zhou1 · Zhu Liu1  Received: 4 October 2019 / Accepted: 14 January 2020 © Springer Science+Business Media, LLC, part of Springer Nature 2020

Abstract Effect of the impurity in ­Cu2O nanowire on the degradation of methyl orange under light irradiation in dark circumstances was investigated. Here, we present the fabrication of C ­ u2O nanowires at different temperatures (110, 130, 150, 170, and 190 °C) by a facile hydrothermal route. Meanwhile, at the synthesis temperature of 110–150 °C, the major impurity in ­Cu2O nanowires was ­Cu4O3, and a new Cu impurity was introduced in the ­Cu2O nanowires as the synthesis temperature increased from 170 to 190 °C. Overall, as the synthesis temperature increases from 110 to 190 °C, the total impurity decreases in ­Cu2O nanowires. The fast degradation rate in dark circumstances has been achieved in ­Cu2O nanowires for all synthesis temperatures, which can be attributed to the ­Cu2+ in the ­Cu4O3 impurity of ­Cu2O nanowires. This result shows that the ­Cu2O nanowires obtained at the synthesis temperature of 150 °C have the fastest degradation rate for both under light irradiation and in dark circumstances. It has been found that under light irradiation, the Cu impurity in C ­ u2O nanowires plays a vital role in the degradation of methyl orange. In the current scenario, different impurity contents influence the catalyst activity of ­Cu2O nanowires under the visible light or dark, respectively.

1 Introduction Semiconductor materials are widely used in the field of photocatalytic degradation due to their good electronic structure, light absorption properties, and charge transport properties [1, 2]. Among them, ­Cu2O is the most widely used in the field of photocatalytic degradation due to its narrow bandgap, broaden absorption of sunlight, non-toxicity, and environmental friendliness [3–12]. However, ­Cu2O is unstable due to photogenerated electrons can result in the self-decomposition of ­Cu2O [13]. To address this issue, a heterojunction or a Schottky junction with other semiconductors or metals

Zhipeng Xie and Yan Zhou have contributed equally. Electronic supplementary material  The online version of this article (https​://doi.org/10.1007/s1085​4-020-02914​-w) contains supplementary material, which is available to authorized users. * Zhu Liu [email protected] 1



Department of Physics, School of Physics and Astronomy, Yunnan University, Kunming 650091, Yunnan, People’s Republic of China

[14, 15] had been introduced in C ­ u2O for a facile electrons and holes separation. Recently, the preparation of cuprous oxide is mostly carried out by the hydrothermal method due to the adjustable morphology of C ­ u 2O, cost-effective, and simple preparation parameters to handle [16, 17]. However, it is difficult to obtained completely pure ­Cu2O during the