首页> 外文期刊>Coatings >Numerical Insights into the Influence of Electrical Properties of n-CdS Buffer Layer on the Performance of SLG/Mo/p-Absorber/n-CdS/n-ZnO/Ag Configured Thin Film Photovoltaic Devices
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Numerical Insights into the Influence of Electrical Properties of n-CdS Buffer Layer on the Performance of SLG/Mo/p-Absorber/n-CdS/n-ZnO/Ag Configured Thin Film Photovoltaic Devices

机译:N-CDS缓冲层电性能对SLG / MO / P吸收器/ N-CDS / N-ZnO / AG配置薄膜光伏器件性能影响的数值见解

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A CdS thin film buffer layer has been widely used as conventional n-type heterojunction partner both in established and emerging thin film photovoltaic devices. In this study, we perform numerical simulation to elucidate the influence of electrical properties of the CdS buffer layer, essentially in terms of carrier mobility and carrier concentration on the performance of SLG/Mo/p-Absorber/n-CdS/n-ZnO/Ag configured thin film photovoltaic devices, by using the Solar Cell Capacitance Simulator (SCAPS-1D). A wide range of p-type absorber layers with a band gap from 0.9 to 1.7 eV and electron affinity from 3.7 to 4.7 eV have been considered in this simulation study. For an ideal absorber layer (no defect), the carrier mobility and carrier concentration of CdS buffer layer do not significantly alter the maximum attainable efficiency. Generally, it was revealed that for an absorber layer with a conduction band offset (CBO) that is more than 0.3 eV, Jsc is strongly dependent on the carrier mobility and carrier concentration of the CdS buffer layer, whereas Voc is predominantly dependent on the back contact barrier height. However, as the bulk defect density of the absorber layer is increased from 1014 to 1018 cm?3, a CdS buffer layer with higher carrier mobility and carrier concentration is an imperative requirement to a yield device with higher conversion efficiency and a larger band gap-CBO window for realization of a functional device. Most tellingly, simulation outcomes from this study reveal that electrical properties of the CdS buffer layer play a decisive role in determining the progress of emerging p-type photo-absorber layer materials, particularly during the embryonic device development stage.
机译:CDS薄膜缓冲层已广泛用作建立和出现的薄膜光伏器件中的常规N型异质结合作伙伴。在本研究中,我们进行数值模拟以阐明CDS缓冲层的电特性的影响,基本上就载流子迁移率和载波浓度而言,SLG / MO / P吸收器/ N-CDS / N-ZnO /的性能/ AG配置的薄膜光伏器件,通过使用太阳能电池电容模拟器(SCAPS-1D)。在该模拟研究中考虑了从0.9至1.7eV和3.7至4.7eV的带隙的各种P型吸收层,并从3.7至4.7eV中考虑了来自3.7至4.7eV的电子亲和力。对于理想的吸收层(无缺陷),Cds缓冲层的载流子迁移率和载体浓度不会显着改变最大可达到的效率。通常,据揭示,对于具有大于0.3eV的传导带偏移(CBO)的吸收层,JSC强烈取决于CDS缓冲层的载流子迁移率和载体浓度,而VOC主要取决于背面接触屏障高度。然而,随着吸收层的块缺陷密度从1014增加到1018cm?3,具有较高载流子迁移率和载流子浓度的Cds缓冲层是对具有更高转换效率和更大频带隙的产量装置的必要要求。用于实现功能设备的CBO窗口。最据说,来自该研究的模拟结果表明CDS缓冲层的电性能在确定新出现的P型光吸收层材料的进展中起决定性的作用,特别是在胚胎器件开发阶段。

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