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晶体分数和掺杂浓度对异质结太阳能电池n型掺杂微晶硅:氢背表面场层的影响

Crystalline Fraction and Doping Concentration Effect on Heterojunction Solar Cells n-Doped µc-Si:H Back Surface Field Layer.

作者信息

Kim Sangho, Shin Chonghoon, Balaji Nagarajan, Yi Junsin

出版信息

J Nanosci Nanotechnol. 2015 Mar;15(3):2294-9. doi: 10.1166/jnn.2015.10242.

Abstract

The back surface field (BSF) plays a vital role for high efficiency in the Heterojunction Intrinsic Thin (HIT) film solar cell. This paper investigated the effect of crystalline volume fraction (Xc) and 1% hydrogen diluted phosphine (PH3) gas doping concentration of the n-type µc-Si:H back surface file (BSF) layer. Initially, the thickness of the n-type µc-Si:H BSF layer was optimized. With increase in Xc from 6% to 59%, the open circuit voltage (Voc) increased from 573 mV to 696 mV, and the fill factor (FF) also increased from 59% to 71%. In the long wavelengths region (≥ 950 nm), the QE of the solar cells decreased over the optimized Xc of the n-doped micro BSF layer, due to the defects of a film. In the second part of this paper, the effect of high conductivity n-type µc-Si:H BSF layer with optimized thickness on the performance of HIT solar cells was investigated, by doping gas ratio variation. Even though Xc decreased, conductivity was increased, with increasing PH3 doping concentration. Under the optimized condition, a n-µc-Si:H BSF layer has a dark conductivity of 2.59 S/cm, activation energy of 0.0519 eV, and X, of 52%. The conversion efficiency of 18.9% was achieved with a Voc of 706 mV, fill factor of 72%, and short circuit current density of 37.1 mW·cm(-2).

摘要

背表面场(BSF)在异质结本征薄膜(HIT)太阳能电池的高效性能中起着至关重要的作用。本文研究了n型微晶硅氢化薄膜(µc-Si:H)背表面场(BSF)层的晶体体积分数(Xc)和1%氢气稀释磷化氢(PH3)气体掺杂浓度的影响。首先,对n型µc-Si:H BSF层的厚度进行了优化。随着Xc从6%增加到59%,开路电压(Voc)从573 mV增加到696 mV,填充因子(FF)也从59%增加到71%。在长波长区域(≥950 nm),由于薄膜缺陷,太阳能电池的量子效率(QE)在n掺杂微BSF层的优化Xc之上降低。在本文的第二部分,通过改变掺杂气体比例,研究了具有优化厚度的高电导率n型µc-Si:H BSF层对HIT太阳能电池性能的影响。尽管Xc降低,但随着PH3掺杂浓度的增加,电导率增加。在优化条件下,n-µc-Si:H BSF层的暗电导率为2.59 S/cm,激活能为0.0519 eV,X为52%。实现了18.9%的转换效率,Voc为706 mV,填充因子为72%,短路电流密度为37.1 mW·cm(-2)。

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