\begin{document}$ {\gamma }_{\left\{100\right\}/\left\{010\right\}/\left\{001\right\}} $\end{document} = 1.76 J/m2. While the (110) and (111) lattices of ITO consist of In/Sn/O, in which the O atom percent on (110) and (111) lattices are 56 at.% and 25 at.% respectively. Besides, the calculated values of surface energy \begin{document}$ {\gamma }_{\left\{110\right\}/\left\{101\right\}/\left\{011\right\}} $\end{document} and \begin{document}$ {\gamma }_{\left\{111\right\}} $\end{document} are 1.07 and 0.89 J/m2, respectively. Combining the XPS measurement results and crystal structure of ITO, it can be understood that in the diffusion process of low-energy NHx ion/group into ITO film without preferred orientation, lots of In/Sn—O—N bonds are formed in the ITO lattices, which are rich in O and have lower surface energy \begin{document}$ \gamma $\end{document}. Then, after the low-energy NHx ion/group bombardment, the electrical properties of ITO film without preferred orientation are deteriorated seriously. On the contrary, because of the absence of O and the highest surface energy \begin{document}$ \gamma $\end{document}, it is hard for the low-energy NHx ion/group to diffuse into ITO (100) lattice. Then, after the low-energy NHx ion/group bombardment, the electrical properties of ITO film with (100) preferred orientation have little change. With all results, the ITO film with (100) preferred orientation can be an ideal candidate for transparent electrode in MAPbH3 perovskite solar cells."> - 必威体育下载

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    Zhao Shi-Ping, Zhang Xin, Liu Zhi-Hui, Wang Quan, Wang Hua-Lin, Jiang Wei-Wei, Liu Chao-Qian, Wang Nan, Liu Shi-Min, Cui Yun-Xian, Ma Yan-Ping, Ding Wan-Yu, Ju Dong-Ying
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    • Abstract views:5718
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    • Received Date:07 June 2020
    • Accepted Date:06 August 2020
    • Available Online:19 November 2020
    • Published Online:05 December 2020

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