Interface analysis of ultrathin SiO2 layers between c‐Si substrates and phosphorus‐doped poly‐Si by theoretical surface potential analysis using the injection‐dependent lifetime

钝化 材料科学 多晶硅 兴奋剂 薄脆饼 氧化物 载流子寿命 掺杂剂 太阳能电池 晶体硅 光电子学 氧化硅 分析化学(期刊) 图层(电子) 纳米技术 化学 冶金 薄膜晶体管 氮化硅 色谱法
作者
Sung‐Jin Choi,Ji-Min Baek,Taejun Kim,Kwan Hong Min,Myeong Sang Jeong,Hee‐eun Song,Min Gu Kang,Donghwan Kim,Yoonmook Kang,Hae‐Seok Lee,Jae‐Min Myoung,Sungeun Park
出处
期刊:Progress in Photovoltaics [Wiley]
卷期号:29 (1): 32-46 被引量:9
标识
DOI:10.1002/pip.3338
摘要

Abstract Passivated contact structures are often representative of tunnel oxide passivated contact (TOPCon) and polycrystalline silicon on oxide (POLO) solar cells. These passivated contact technologies in silicon solar cells have experienced great strides in efficiency. However, characteristics analysis of poly‐Si/SiO 2 applied to TOPCon and POLO solar cells as a carrier‐selective and passivated contact is still challenging because the silicon oxide film is very thin (<1.5 nm), poly‐Si and silicon oxide properties change during thermal treatment for passivation effects, and dopant diffusion from poly‐Si layer to the silicon wafer occurs. In this study, the interfacial analysis was performed by applying an algorithm based on the extended Shockley–Read–Hall (SRH) theory to the P‐doped poly‐Si/SiO 2 /c‐Si structure. Quantitative parameters of the P‐doped poly‐Si/SiO 2 /c‐Si interface were extracted by fitting the measured and simulated lifetime curves with algorithms, such as D it (interface trap density) and Q f (fixed charge), from which we were able to elucidate the passivation effect of the interface. The interface analysis method using this algorithm is meaningful in that it can quantify the passivation characteristics of TOPCon with very thin silicon oxide film. The interface characteristics were also analyzed using the injection‐dependent lifetime after thermal treatment of P‐doped poly‐Si/SiO 2 /c‐Si samples for passivation effect. After the 850°C thermal treatment, the following best passivation effects were verified, namely, ψ s = 0.248 eV, D it = 1.0 × 10 11 cm −2 ·eV −1 , Q f = 2.4 × 10 12 cm −2 , and J 02 = 370 pA·cm −2 . Through the analysis model using carrier lifetime theory, we investigated quantitatively the passivation properties of P‐doped poly‐Si/SiO 2 /c‐Si.
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