以TiO2和季硫系Cu2FeSnS4为电荷传输通道的cspbbr3基钙钛矿太阳能电池的光伏性能:通过SCAPS-1D研究解锁>26%的效率

Eli Danladi , Wadai Mutah , Peverga R. Jubu , Kehinde A. Ogunmoye , Zakari L. Abubakar , Dennis A. Bala , Nicholas N. Tasie , Adamu Idris , Francis Aungwa , Matthew I. Amanyi , Eghwubare Akpoguma , Ndinaobong I. Noah , Fabian Ezema
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引用次数: 0

摘要

铯基钙钛矿太阳能电池(PSCs)由于其高稳定性和低成本在光伏领域受到了极大的研究兴趣,但与有机-无机卤化物太阳能电池相比,其性能受到低产量的挑战。在本研究中,利用一维太阳能电池电容模拟(scpps - 1d)工具研究了具有不同空穴传输层(HTLs)的铯溴化铅(CsPbBr3)基PSC的光伏(PV)性能,这些空穴传输层包括硫氰酸铜(CuSCN)、碘化铜(CuI)、掺镁铜铬氧化物(Mg-CuCrO2)、氧化铜(II)、硫化铜锑(CuSbS2)、硫化铜铁锡(CFTS)和硫化铜钡锡(CBTS)。最佳器件配置为ITO/TiO2/CsPbBr3/CFTS/Au,功率转换效率(PCE)为12.665%,填充因子(FF)为80.435%,电流密度(Jsc)为17.595 mA/cm2,光电电压(Voc)为0.895 V。通过改变电子传递层(ETL)的厚度、ETL和吸收剂的掺杂浓度、吸收剂的缺陷密度、吸收剂的厚度和HTL的厚度对优化构型进行了进一步的研究,得到了0.01 μm、1020 cm−3、1012 cm−3、1014 cm−2、0.5 μm和1.2 μm的优化值。利用优化后的数据进行适当的模拟,TiO2和CFTS作为电荷输运通道时,PCE为26.032%,FF为81.006%,Jsc为34.908 mA/cm2, Voc为0.921 V。结果表明,与未优化装置相比,PCE提高了~ 2.06倍,FF提高了~ 1.01倍,Jsc提高了~ 1.98倍,Voc提高了~ 1.03倍。此外,还研究了温度、金属功函数、串联电阻和分流电阻的影响,发现温度升高会引起载流子浓度的变化,导致复合率高,也会对饱和电流产生影响,而串联电阻增加会导致器件性能下降,这是由于变色造成的。低分流电阻,通过提供限制电流流动的替代通路,导致器件输出损失。该模拟和验证结果显示了CsPbBr3吸收剂的真正潜力,为光伏行业开发更便宜、高性能的设备创造了一条主要的研究途径。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Photovoltaic performance of CsPbBr3-based perovskite solar cell with TiO2 and quaternary chalcogenide Cu2FeSnS4 as charge transport channels: Unlocking >26% efficiency via SCAPS-1D investigation
Cesium-based perovskite solar cells (PSCs) have received tremendous research interest in the domain of photovoltaic due their high stability and low cost, but their performances are challenged with low output when compared to their organic-inorganic halide counterpart. In this research work, the one-dimensional solar cell capacitance simulation (SCAPS-1D) tool was used to investigate the photovoltaic (PV) performance of cesium lead bromide (CsPbBr3)-based PSC with different hole transport layers (HTLs), which include copper(I) thiocyanate (CuSCN), copper(I) iodide (CuI), magnesium-doped copper chromium oxide (Mg-CuCrO2), copper (II) oxide (CuO), copper antimony sulfide (CuSbS2), copper iron tin sulfide (CFTS), and copper barium tin sulfide (CBTS). The best device configuration was ITO/TiO2/CsPbBr3/CFTS/Au, which gave a power conversion efficiency (PCE) of 12.665%, fill factor (FF) of 80.435%, current density (Jsc) of 17.595 mA/cm2, and photo voltage (Voc) of 0.895 V. Further study was carried out on the optimized configuration by varying the thickness of electron transport layer (ETL), doping concentration of ETL and absorber, defect density of the absorber, thickness of absorber, and thickness of HTL to obtain 0.01 μm, 1020 cm−3, 1012 cm−3, 1014 cm−2, 0.5 μm, and 1.2 μm as optimized values. After proper simulation with the optimized data, a PCE of 26.032%, FF of 81.006%, Jsc of 34.908 mA/cm2, Voc of 0.921 V were obtained with TiO2 and CFTS as charge transport channels. This shows an enhancement of ∼2.06 times in PCE, ∼1.01 times in FF, ∼1.98 times in Jsc, and ∼1.03 times in Voc over the unoptimized device. Additionally, the influence of temperature, metal work function, series resistance, and shunt resistance was also studied, and it was found that the rise in temperature causes a shift in the concentration of carriers, giving rise to high rate of recombination which also results in influence on the saturation current, while an increase in series resistance results in a decrease in the device performance, which is attributed to discoloration. Low shunt resistance, results in losses in device output by giving an alternative pathway that limits the flow of current. This simulation alongside the validated results shows the real potential of CsPbBr3 absorber, creating a major research pathway for the PV industry to develop less expensive and high-performing devices.
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