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A new method of determination of minority carrier diffusion length in the base region of silicon solar cells

机译:确定硅太阳能电池基极区中少数载流子扩散长度的新方法

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A new method of determination of the minority carrier diffusion length (L) in the base region of an n/sup +/-p-p/sup +/ silicon solar cell using the spectral response of the cell in a middle wavelength (/spl lambda/) range, e.g., 0.75>/spl lambda/>0.90 /spl mu/m is presented. In this method Q/sub int/ or if required Q/sub int//f where Q/sub int/ is the internal quantum efficiency of the cell and f=exp(/spl minus/(x/sub b//spl alpha//sub /spl lambda//))(L/sup 2//spl alpha//sub /spl lambda///sup 2//L/sup 2//spl alpha//sub /spl lambda///sup 2//spl minus/1), x/sub b/ being the distance of base region from the front surface, is plotted against the reciprocal absorption coefficient (/spl alpha//sub /spl lambda///sup /spl minus/1/ of silicon. The Q/sub int/ versus /spl alpha//sub /spl lambda///sup /spl minus/1/ or else Q/sub int//f versus /spl alpha//sub /spl lambda///sup /spl minus/1/, plot gives an intercept L/sub MW/ on the /spl alpha//sub /spl lambda///sup /spl minus/1/-axis and a unit intercept on the other axis. The intercept length L/sub MW/ is related to L through d/L and S/sub B/, where d is the thickness of the base region and S/sub B/ is the back surface recombination velocity of minority carriers. For d/L<2.5, L=L/sub MW/ and is independent of S/sub B/. However, for d/L>2.5, the true value of L which may be somewhat different from L/sub MW/ can be determined if S/sub B/ is known. While most existing long wavelength spectral response (LWSR) methods require d/L to be large (d/L<2.5) is such that tanh(d/L)/spl ap/1, this method has no such restriction on d/L. It is highly suitable for cells for which L is large but x/sub b/ is small. We have applied the MWSR and LWSR methods to a few n/sup +/-p-p/sup +/ silicon solar cells and have found that the former is much superior to the latter if d/L>2.5.
机译:一种确定n / sup +/- pp / sup + /硅太阳能电池基极区域中少数载流子扩散长度(L)的新方法,该方法利用电池在中间波长(/ spl lambda / )范围,例如0.75> / spl lambda /> 0.90 / spl mu / m。在此方法中Q / sub int /或如果需要的话Q / sub int // f,其中Q / sub int /是电池的内部量子效率,f = exp(/ spl负/(x / sub b // spl alpha // sub / spl lambda //))(L / sup 2 // spl alpha // sub / spl lambda /// sup 2 // L / sup 2 // spl alpha // sub / spl lambda /// sup 2 // spl减/ 1),x / sub b /是基础区域到前表面的距离,相对于相互吸收系数(/ spl alpha // sub / spl lambda /// sup / spl减/ 1 /硅.Q / sub int /与/ spl alpha // sub / spl lambda /// sup / spl减/ 1 /或Q / sub int // f与/ spl alpha // sub / spl lambda /// sup / spl minus / 1 /,图在/ spl alpha // sub / spl lambda //// sup / spl minus / 1 /-轴上给出了截距L / sub MW /,在另一个轴上给出了单位截距截距长度L / sub MW /与L到d / L和S / sub B /有关,其中d是基区的厚度,S / sub B /是少数载流子的背面复合速度。对于d / L <2.5,L = L / sub MW /并且独立于S / sub B / 。但是,对于d / L> 2.5,如果已知S / sub B /,则可以确定可能与L / sub MW /稍有不同的L的真实值。尽管大多数现有的长波长光谱响应(LWSR)方法要求d / L较大(d / L <2.5)使得tanh(d / L)/ spl ap / 1,但此方法对d / L没有此类限制。 L非常适合L大但x / sub b /小的电池。我们将MWSR和LWSR方法应用于少数n / sup +/- p-p / sup + /硅太阳能电池,并且发现如果d / L> 2.5,前者要比后者好得多。

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