Novel aspects in thin film silicon solar cells-amorphous, microcrystalline and nanocrystalline silicon

Abstract The improvement of photodegradation of a-Si:H has been studied on the basis of controlling the subsurface reaction and gaseous phase reaction. We found that higher deposition temperature, hydrogen dilution and triode method are effective to reduce the SiH2 density in the film and to suppress the photodegradation of solar cells. These results are explained in terms of the hydrogen elimination reaction in the subsurface region and the contribution of the higher silane radicals to the film growth. The high-rate deposition of μc-Si:H was obtained by means of a high-pressure method and further improvement in deposition rate and the film quality was achieved in combination with the locally high-density plasma, which enables effective dissociation of source gases without thermal damage. It was also found that the deposition pressure is crucial to improve the film quality for device. This technique was successfully applied to the solar cells and an efficiency of 7.9% was obtained at a deposition rate of 3.1 nm/s. The potential application of nanocrystalline silicon is also discussed.

[1]  A. Matsuda,et al.  High-rate growth of microcrystalline silicon films using a high-density SiH4/H2 glow-discharge plasma , 2004 .

[2]  A. Matsuda Formation kinetics and control of microcrystallite in μc-Si:H from glow discharge plasma , 1983 .

[3]  S. Tsuda,et al.  The Influence of the Si-H2 Bond on the Light-Induced Effect in a-Si Films and a-Si Solar Cells , 1989 .

[4]  A. Matsuda,et al.  High Rate Deposition of Microcrystalline Silicon Using Conventional Plasma-Enhanced Chemical Vapor Deposition , 1998 .

[5]  Michio Kondo,et al.  Effects of Substrate Surface Morphology on Microcrystalline Silicon Solar Cells , 2001 .

[6]  Reinhard Carius,et al.  Improvement of grain size and deposition rate of microcrystalline silicon by use of very high frequency glow discharge , 1994 .

[7]  R. Hayashi,et al.  Gas-phase diagnosis and high-rate growth of stable a-Si:H , 1999 .

[8]  A. Matsuda PLASMA AND SURFACE REACTIONS FOR OBTAINING LOW DEFECT DENSITY AMORPHOUS SILICON AT HIGH GROWTH RATES , 1998 .

[9]  Zafar Iqbal,et al.  Raman scattering from hydrogenated microcrystalline and amorphous silicon , 1982 .

[10]  D. Carlson,et al.  AMORPHOUS SILICON SOLAR CELL , 1976 .

[11]  O. Leroy,et al.  Cross-Sections, Rate Constants and Transport Coefficients in Silane Plasma Chemistry , 1996 .

[12]  A. Matsuda,et al.  Passivation of oxygen-related donors in microcrystalline silicon by low temperature deposition , 2001 .

[13]  M. Hori,et al.  Roles of SiH3 and SiH2 Radicals in Particle Growth in rf Silane Plasmas , 1997 .

[14]  A. Matsuda,et al.  High rate growth of microcrystalline silicon at low temperatures , 2000 .

[15]  Ch. Hof,et al.  On the Way towards High-Efficiency Thin Film Silicon Solar Cells by the "Micromorph" Concept , 1996 .

[16]  H. Sakai,et al.  The Role of Hydrogen in the Staebler-Wronski Effect of a-Si:H , 1985 .

[17]  S. Yamasaki,et al.  Microscopic structure of defects in microcrystalline silicon , 2000 .

[18]  T. Ohmi,et al.  Ion energy, ion flux, and ion mass effects on low‐temperature silicon epitaxy using low‐energy ion bombardment process , 1996 .

[19]  S. Suzuki,et al.  Growth of device grade c-Si film at over 50 /s using PECVD , 2002 .

[20]  Diego Fischer,et al.  Microcrystalline silicon and micromorph tandem solar cells , 1999 .

[21]  A. Matsuda,et al.  Key Issue for the Fabrication of High-Efficiency Microcrystalline Silicon Thin-Film Solar Cells at Low Temperatures , 2002 .

[22]  A. Matsuda,et al.  Substrate dependence of initial growth of microcrystalline silicon in plasma‐enhanced chemical vapor deposition , 1996 .