31.474(44.359) % -限制中获得的效率最高 \\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\ mathbf {n }^+(\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\ mathbf {p }^+)-\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\ mathbf {p }(\\\\\\\\

H. van Cong, K. C. Ho-Huynh Thi, P. Blaise, R. Brouzet, O. Henri-Rousseau
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引用次数: 0

摘要

在我们最近的工作[1,2]中,基于:(1)重(轻)掺杂和施主(受体)d(a)尺寸对总载流子-少数饱和电流密度JoI(II)≡JEn(p)o + JBp(n)o, JEn(p)o(JBp(n)o),分别注入到n+(p+) - p(n)结太阳能电池的重掺杂施主(受体)-GaAs发射体-轻掺杂施主(施主)-Si基区HD[d(a)-Si]ERLD[a(d)Si]BR中,(2)有效的高斯施主密度谱来确定JEn(p)o,(3)利用两个实验点,分别考察了光伏转换因子nI(II)、短路电流密度JscI(II)、填充因子FI(II)、效率ηI(II)。然后,在300K下,n+(p+)−p(n)结太阳能电池的效率最高,达到31%(30.65%)。在本工作中,基于这种处理方法,采用W = 15 μm, NSb(In) = 1019 (1020) cm−3和S = 100 (cm/ S)等物理条件,根据高透明HD[Sb(In)-GaAs]ER,然后对LD[In(Sb)]进行NIn(Sb) = 1018 (1017)cm−3的处理。物理学报,ISSN: 2706-8862 http://www.scirea.org/journal/Physics July 26, 2022卷,第4期,August https://doi.org/10.54647/physics14475
本文章由计算机程序翻译,如有差异,请以英文原文为准。
31.474 (44.359) %- Limiting Highest Efficiencies obtained in the \\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\mathbf{n}^+(\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\mathbf{p}^+)-\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\mathbf{p}(\\\\\\\\
In our recent works [1, 2], by basing on: (1) the effects of heavy(light) doping and donor (acceptor), d(a), size , which affect the total carrier-minority saturation current density JoI(II) ≡ JEn(p)o + JBp(n)o, JEn(p)o(JBp(n)o), being injected respectively into the heavily doped donor (acceptor)-GaAs emitter-lightly doped acceptor (donor)-Si base regions, HD[d(a)-Si]ERLD[a(d)Si]BR, of n+(p+) − p(n) junction solar cells, respectively, (2) an effective Gaussian donor-density profile to determine JEn(p)o , and (3) the use of two experimental points, we investigated the photovoltaic conversion factor nI(II), short circuit current density JscI(II), fill factor FI(II) , and finally efficiency ηI(II) . Then, the limiting highest efficiencies, 31% (30.65%), were obtained in n+(p+) − p(n) junction solar cells at 300K. In the present work, by basing on such a treatment method, and using the physical conditions such as: W = 15 μm, NSb(In) = 1019 (1020) cm−3 and S = 100 (cm/s ) , according to the highly transparent HD[Sb(In)-GaAs]ER, and then NIn(Sb) = 1018 (1017)cm−3 for LD[In(Sb)SCIREA Journal of Physics ISSN: 2706-8862 http://www.scirea.org/journal/Physics July 26, 2022 Volume 7, Issue 4, August 2022 https://doi.org/10.54647/physics14475
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