钝化
非晶硅
材料科学
异质结
无定形固体
晶体硅
硅
氧化物
光电子学
纳米技术
化学
有机化学
图层(电子)
冶金
作者
Thomas Mueller,Stefan Schwertheim,W. R. Fahrner
出处
期刊:Conference record of the ... IEEE Photovoltaic Specialists Conference
日期:2008-05-01
卷期号:: 1-6
被引量:12
标识
DOI:10.1109/pvsc.2008.4922792
摘要
Wide-gap (highly transparent), hydrogenated amorphous silicon oxide (a-SiO x :H) layers are investigated for heterojunction solar cell applications: Intrinsic a-SiO x :H(i) films are formed in order to prove their applicability for surface passivating buffer layers sandwiched between the crystalline silicon (c-Si) and the doped amorphous layer used for the formation of the emitter and the back-surface-field in heterojunction cells. The a-SiO x :H films are processed by high frequency (70 MHz) plasma decomposition using silane (SiH 4 ), hydrogen (H 2 ), and carbon dioxide (CO 2 ) at the low deposition temperature of 155 °C. Quasi-steady-state photoconductance and transient photoconductance lifetime measurements have been carried out to determine the passivation quality of the intrinsic a-SiO x :H deposited on c-Si of different doping types and levels. A variation of the applied thickness of the grown a-SiO x :H films determines the impact on the performance of heterojunction solar cells. It will be demonstrated that excellent effective lifetimes as high as 4.7 ms on 1 Ωcm n-type float-zone (FZ) material (corresponding to a surface recombination velocity of 2.3 cm/s) and 14.2 ms on 130 Ωcm p-type FZ material (corresponding to a surface recombination velocity of 0.52 cm/s) can be achieved by surface passivation using our a-SiO x :H films. To validate the capability of the intrinsic and doped a-SiOx:H films separately, heterojunction solar cells consisting of (front to back) a-Si:H(p + )/a-Si:H(i)/c-Si(n)/a-Si:H(i)/a-Si:H(n + ), a-Si:H(p + )/a-SiO x :H(i)/c-Si(n)/a-SiO x :H(i)/a-Si:H(n + ), and the reversed doping sequence have been analyzed. By incorporating a-SiO x :H(i) to the a-Si:H(p)/c-Si structure we find a drastic increase of the open circuit voltage (up to 655 mV for p-type substrates and 695 mV for n-type substrates) and accordingly, a higher conversion efficiency than obtained with standard a-Si(i).
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