Analysis of Photovoltaic Characteristics of Carbon Nanotube Incorporated Perovskite Solar Cell with CNT Chirality Variation

M. Reza, S. M. Mominuzzaman
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引用次数: 1

Abstract

Perovskite solar cell with carbon nanotube (CNT) is the most current research interest in the field of photonics and renewable energy. Recently many researchers are trying to incorporate several types of CNTs in different layers of solar cell to enhance the efficiency. In this work the effect of CNT chirality for incorporating semiconductive CNT in active layer of perovskite solar cell is simulated to comprehend the optimization dependencies to attain better cell performance parameters. Also the efficiency of solar cell is increased for incorporating CNT in the active layer of solar cell. Single chiral semi-conductive single wall CNTs with diameter range from 0.28 nm to 1.04 nm as well as a cell structure is considered which consists of $\mathrm {C}\mathrm {H}_{3}\mathrm {N}\mathrm {H}_{3}\mathrm {P}\mathrm {b}\mathrm {I}_{3}$ active layer and Spiro-MeOTAD hole transport layer. Open circuit voltage, short circuit current density and absorption coefficient are determined for CNT chirality variation. To calculate fill factor and power conversion efficiency equivalent circuit parameters are extracted. Maximum open circuit voltage and fill factor are determined as 1.33 V and 0.79 for (4,3) chirality respectively. Also short circuit current density up to 25.44 mA/cm2 and efficiency to 21.84% can be maximized for (6,4) CNT chirality. Finally it is perceived that by changing CNT chirality efficiency can be increased by a range of about 74.7%.
碳纳米管掺杂钙钛矿太阳能电池手性变化的光伏特性分析
碳纳米管钙钛矿太阳能电池是当前光子学和可再生能源领域的研究热点。近年来,许多研究人员试图在太阳能电池的不同层中加入几种类型的碳纳米管以提高效率。本文模拟了碳纳米管手性对钙钛矿太阳能电池活性层中半导体碳纳米管的影响,以了解优化依赖关系,以获得更好的电池性能参数。在太阳能电池的有源层中掺入碳纳米管也提高了太阳能电池的效率。考虑了直径为0.28 nm ~ 1.04 nm的单手性半导电单壁碳纳米管以及由$\ mathm {C}\ mathm {H}_{3}\ mathm {N}\ mathm {H}_{3}}\ mathm {P}\ mathm {b}\ mathm {I}_{3}$活性层和Spiro-MeOTAD空穴传输层组成的细胞结构。确定了碳纳米管手性变化的开路电压、短路电流密度和吸收系数。为了计算填充系数和功率转换效率,提取了等效电路参数。(4,3)手性的最大开路电压和填充因子分别为1.33 V和0.79。此外,对于(6,4)碳纳米管手性,短路电流密度可达25.44 mA/cm2,效率可达21.84%。最后,通过改变碳纳米管的手性,可以将效率提高约74.7%。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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