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首页> 外文期刊>Optical and quantum electronics >Influence of P~+-ZnTe back surface contact on photovoltaic performance of ZnTe based solar cells
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Influence of P~+-ZnTe back surface contact on photovoltaic performance of ZnTe based solar cells

机译:P〜+ -ZnTe背面接触对ZnTe基太阳能电池光伏性能的影响

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In order to improve photovoltaic performance of solar cells based on ZnTe thin films two device structures have been proposed and its photovoltaic parameters have been numerically simulated using Solar Cell Capacitance Simulator software. The first one is the ZnO/CdS/ZnTe conventional structure and the second one is the ZnO/CdS/ZnTe/P+-ZnTe structure with a P+-ZnTe layer inserted at the back surface of ZnTe active layer to produce a back surface field effect which could reduce back carrier recombination and thus increase the photovoltaic conversion efficiency of cells. The effect of ZnO, CdS and ZnTe layer thicknesses and the P+-ZnTe added layer and its thickness have been optimized for producing maximum working parameters such as: open-circuit voltage V-oc, short-circuit current density J(sc), fill factor FF, photovoltaic conversion efficiency eta. The solar cell with ZnTe/P+-ZnTe junction showed remarkably higher conversion efficiency over the conventional solar cell based on ZnTe layer and the conversion efficiency of the ZnO/CdS/ZnTe/P+-ZnTe solar cell was found to be dependent on ZnTe and P+-ZnTe layer thicknesses. The optimization of ZnTe, CdS and ZnTe layers and the inserting of P+-ZnTe back surface layer results in an enhancement of the energy conversion efficiency since its maximum has increased from 10% for ZnO, CdS and ZnTe layer thicknesses of 0.05, 0.08 and 2 A mu m, respectively to 13.37% when ZnO, CdS, ZnTe and P+-ZnTe layer thicknesses are closed to 0.03, 0.03, 0.5 and 0.1 A mu m, respectively. Furthermore, the highest calculated output parameters have been J(sc) = 9.35 mA/cm(2), V-oc = 1.81 V, eta = 13.37% and FF = 79.05% achieved with ZnO, CdS, ZnTe, and P+-ZnTe layer thicknesses about 0.03, 0.03, 0.5 and 0.1 A mu m, respectively. Finally, the spectral response in the long-wavelength region for ZnO/CdS/ZnTe solar cells has decreased at the increase of back surface recombination velocity. However, it has exhibited a red shift and showed no dependence of back surface recombination velocity for ZnO/CdS/ZnTe/P + -ZnTe solar cells.
机译:为了提高基于ZnTe薄膜的太阳能电池的光伏性能,提出了两种器件结构,并使用太阳能电池电容模拟器软件对其光伏参数进行了数值模拟。第一个是ZnO / CdS / ZnTe常规结构,第二个是ZnO / CdS / ZnTe / P + -ZnTe结构,在ZnTe有源层的背面插入P + -ZnTe层以产生背面场效应这可以减少反向载流子复合,从而提高电池的光电转换效率。 ZnO,CdS和ZnTe层厚度以及P + -ZnTe添加层及其厚度的影响已得到优化,以产生最大的工作参数,例如:开路电压V-oc,短路电流密度J(sc),填充因子FF,光电转换效率η。具有ZnTe / P + -ZnTe结的太阳能电池显示出比基于ZnTe层的常规太阳能电池明显更高的转换效率,并且发现ZnO / CdS / ZnTe / P + -ZnTe太阳能电池的转换效率取决于ZnTe和P + -ZnTe层的厚度。 ZnTe,CdS和ZnTe层的优化以及P + -ZnTe背面层的插入可提高能量转换效率,因为对于ZnO,CdS和ZnTe层,其厚度分别为0.05、0.08和2时,最大值从10%增加当ZnO,CdS,ZnTe和P + -ZnTe层的厚度分别接近0.03、0.03、0.5和0.1 Aμm时,μm分别达到13.37%。此外,使用ZnO,CdS,ZnTe和P + -ZnTe实现的最高计算输出参数为J(sc)= 9.35 mA / cm(2),V-oc = 1.81 V,eta = 13.37%和FF = 79.05%层的厚度分别约为0.03、0.03、0.5和0.1μm。最后,随着背表面复合速度的增加,ZnO / CdS / ZnTe太阳能电池在长波长区域的光谱响应降低。但是,对于ZnO / CdS / ZnTe / P + -ZnTe太阳能电池,它表现出红移并且不依赖于背面复合速度。

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