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CH_3NH_3Cd_(0.875)Pb_(0.125)I_3 perovskite as potential photovoltaic materials
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摘要
The band structure, electronic and optical properties of the perovskite CH_3NH_3Cd_xPb_(1-x)I_3 are predicted using density functional theory.When Cd content is not over Pb content, the band gap of CH_3NH_3Cd_xPb_(1-x)I_3 is larger than that of CH_3NH_3PbI_3, and the smallest band gap appears in CH_3NH_3Cd_(0.875)Pb_(0.125)I_3 compound.In the wavelength range of 500-800 nm, the optical absorption coefficients of three kinds of composition CH_3NH_3Cd_xPb_(1-x)I_3(x=5,6,7) are much larger than those of CH_3NH_3PbI_3.Compared to CH_3NH_3PbI_3, the absorption coefficients of CH_3NH_3Cd_(0.875)Pb_(0.125)I_3 increase averagely 3.54 times in the visible light spectrum and the latter can absorb much more solar energy in infrared range than the former.The CH_3NH_3Cd_(0.875)Pb_(0.125)I_3 compound is exceptional candidates of photovoltaic materials.
The band structure, electronic and optical properties of the perovskite CH_3NH_3Cd_xPb_(1-x)I_3 are predicted using density functional theory.When Cd content is not over Pb content, the band gap of CH_3NH_3Cd_xPb_(1-x)I_3 is larger than that of CH_3NH_3PbI_3, and the smallest band gap appears in CH_3NH_3Cd_(0.875)Pb_(0.125)I_3 compound.In the wavelength range of 500-800 nm, the optical absorption coefficients of three kinds of composition CH_3NH_3Cd_xPb_(1-x)I_3(x=5,6,7) are much larger than those of CH_3NH_3PbI_3.Compared to CH_3NH_3PbI_3, the absorption coefficients of CH_3NH_3Cd_(0.875)Pb_(0.125)I_3 increase averagely 3.54 times in the visible light spectrum and the latter can absorb much more solar energy in infrared range than the former.The CH_3NH_3Cd_(0.875)Pb_(0.125)I_3 compound is exceptional candidates of photovoltaic materials.
引文
[1]Yuandi Zhang,Jing Feng,AIP Advances,2016,6,115208

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