为太阳能模拟器的空气质量过滤器制作 pbs 薄膜

Isom Hilmi, D. Y. Kusuma, H. Soetedjo, Q. Hidayah, Umi Salamah
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摘要

由于工业和民用需求的不断增长,太阳能电池板的产量也在持续增加。这也导致对太阳能模拟器测试工具的需求不断增加。太阳能模拟器是一种在实验室和工业规模上评估太阳能电池板性能的工具。太阳能模拟器的主要组件之一是空气质量过滤器(AMF)。AMF 的主要功能是从太阳能模拟器光源(如氙弧灯)中去除不需要的波段,使过滤后的光谱与太阳辐照光谱一致。AMF 可以通过在玻璃等透明基板上制作一层薄材料来实现。薄膜会以不同的方式吸收某些波段。本文报告了应用 AMF 的铬化铅锑薄膜的制作过程。薄膜的制作采用了热蒸发技术。由于具有可定制的光学特性,PbS 因其在不同光学设备中的多功能应用而闻名。不同数量(以克为单位)的 PbS 源粉末用于沉积 PbS 薄膜。然后使用紫外可见光谱法检测薄膜的光学特性。然后使用太阳能模拟器检测了有无使用薄膜作为光学滤光器的 Xe 弧光灯光的透射强度分布。从实验结果来看,使用 0.012 克 PbS 粉末源沉积的薄膜在透射强度分布方面是最佳的。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Fabrication of pbs films for air mass filter of solar simulator
The production of solar panels is continuously increasing due to increasing demands at industrial and residential levels. This also leads to an increasing demand for solar simulator testing tools. A solar simulator is a tool to assess a solar panel's performance in lab and industry scales. One of the main components of the solar simulator is the Air Mass Filter (AMF). The primary function of AMF is to remove unwanted wave bands from the solar simulator light source (e.g., Xe arc lamp) so that the filtered spectrum is commensurate to that of solar irradiation. An AMF can be produced by fabricating a thin material layer on a transparent substrate like glass. The film would absorb certain wave bands in different ways. This paper reports the fabrication of the chalcogenide PbS thin films for applying AMF. The thermal evaporation technique is used for the film fabrication. PbS is known for its versatility for applications in different optical devices due to its tailorable optical properties. Different amounts (in grams) of PbS source powders are used to deposit the PbS thin films. The optical properties of the films are then examined using UV-Vis spectroscopy. The distributions of the transmittance intensity of the Xe-arc-lamp light with and without the use of the films as an optical filter are then examined using a solar simulator. From the experiments, the film deposited using a 0.012 g PbS powder source is regarded as the optimum one regarding the transmittance intensity distribution.
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