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首页> 外文期刊>Solar Energy >Photoelectrical properties of pulsed laser deposited boron doped p-carbon-silicon and phosphorus doped n-carbon/p-silicon heterojunction solar cells
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Photoelectrical properties of pulsed laser deposited boron doped p-carbon-silicon and phosphorus doped n-carbon/p-silicon heterojunction solar cells

机译:脉冲激光沉积硼掺杂的p-碳/ n-硅和磷掺杂的n-碳/ p-硅异质结太阳能电池的光电性能

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This paper reports on the successful deposition of boron doped p-type (p-C:B) and phosphorus doped n-type (n-C:P) semiconducting carbon films and fabrication of p-C:B on n-type silicon (Si) substrate (p-C:B-Si) and n-C:P/p-Si cells by pulsed laser deposition at room temperature using graphite target. The B and P powder were respectively mixed with graphite powder in range from 1% to 20% of B by weight in the targets (Bwt.%) and 1-10% of P by weight in the targets (Pwt.%), and compressed into pellet targets. The B and P atoms incorporated in the films were determined by X-ray pho-toelectron spectroscopy to be in the range of 0.2-1.75 and 0.22-1.77 atomic percentages, respectively. The cells performances have been given under illumination ?-Ⅴ rectifying curve (AM 1.5, 100mW/cm~2, 25℃). The open circuit voltage (V_(oc)) and short circuit current density (J_(sc)) for p-C:B-Si are observed to vary from 230 to 250mV and 1.5 to 2.2mA/cm~2, respectively. While, for n-C:P/p-Si cells the V_(oc) and J_(sc) are observed to vary from 215 to 265mV and 7.5 to 10.5mA/cm~2, respectively. The p-G:B-Si cells fabricated using 3 Bwt.% shows highest energy conversion efficiency, η = 0.20% and fill factor, FF = 45%. While, the n-C:P/p-Si cell fabricated using 7 Pwt.% shows highest of η = 1.14% and fill factor, FF = 41%. The quantum efficiency of p-C:B-Si and n-C:P/p-Si cells are observed to improve with percentage of B and P, respectively. The contribution of quantum efficiency in the lower wavelength region (below 750 nm) may be due to the photon absorption by carbon layer and in the higher wavelength region is due to the Si substrates.
机译:本文报道了硼掺杂的p型(pC:B)和磷掺杂的n型(nC:P)半导体碳膜的成功沉积以及在n型硅(Si)衬底(pC: B / n-Si)和nC:P / p-Si电池通过使用石墨靶材在室温下通过脉冲激光沉积来实现。将B粉和P粉分别与靶粉中B的1重量%至20%(Bwt。%)和靶粉中P的1-10%重量(Pwt。%)的石墨粉混合,并且压缩成小球目标。通过X射线光电子能谱测定掺入膜中的B和P原子分别在0.2-1.75和0.22-1.77原子百分比的范围内。电池在α-Ⅴ照度校正曲线(AM 1.5,100mW / cm〜2,25℃)下给出了电池性能。 p-C:B / n-Si的开路电压(V_(oc))和短路电流密度(J_(sc))分别从230至250mV和1.5至2.2mA / cm〜2变化。而对于n-C:P / p-Si电池,V_(oc)和J_(sc)分别在215mV至265mV和7.5mV至10.5mA / cm〜2之间变化。使用3 Bwt。%制成的p-G:B / n-Si电池显示出最高的能量转换效率,η= 0.20%,填充系数,FF = 45%。而使用7 Pwt。%制成的n-C:P / p-Si电池显示最高的η= 1.14%和填充系数FF = 41%。观察到p-C:B / n-Si和n-C:P / p-Si电池的量子效率分别随B和P的百分比而提高。在较低波长区域(低于750 nm)中,量子效率的贡献可能归因于碳层对光子的吸收,而在较高波长区域中,归因于Si衬底。

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