Modelling of Germanium-Based Perovskite Solar Cell for Different Hole Transport Materials and Defect Density

IF 0.5 Q4 OPTICS
Nurul Afiqah Buruhanutheen, Ahmad Sharmi Abdullah, Mohd Halim Irwan Ibrahim, Fauzan Ahmad, Mohd Haniff Ibrahim
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引用次数: 0

Abstract

The performance of four distinct materials (organic and inorganic) was simulated and analyzed as hole transport layer (HTL) in the design of germanium (Ge)-based Perovskite Solar Cell (PSC). A 1-dimensional numerical software (SCAPS 1-D) has been applied to simulate the HTL candidates: spiro-OMeTAD, PTAA, nickel oxide (NiO), and copper (I) thiocyanate (CuSCN), with tin (IV) dioxide (SnO2) as the electron transport layer (ETL). The thickness of the methylammonium germanium iodide (CH3NH3GeI3) absorber was varied from 300 nm to 1100 nm, and the highest simulated power conversion efficiency was achieved at a thickness of 800 nm for all HTL candidates. It was observed that the inorganic CuSCN outperformed its counterparts with a power conversion efficiency (PCE) of 25.38%. The effect of the perovskite absorber’s defect density was investigated, and ultimately, it was demonstrated that this value is disproportionately related to the PCE. A reduction of nearly 98% in PCE was recorded when the defect density increased from 1x1014 cm-3 to 1x1020 cm-3. Additionally, for a constant ETL thickness of 80 nm, it was revealed that the PCE would decrease slightly, ranging from 0.1% to 0.3%, with an increase in HTL thickness from 50 nm to 300 nm. Comparing the PCE of our current work with published reports further justifies its competitiveness. Full Text: PDF References W.R. Becquerel, "Becquerel Photovoltaic Effect in Binary Compounds", J. Chem. Phys. 32, 1505 (1960). CrossRef A. Kojima, K. Teshima, Y. Shirai, T. Miyasaka, "Organometal Halide Perovskites as Visible-Light Sensitizers for Photovoltaic Cells", J. Am. Chem. Soc. 131, 6050 (2009). CrossRef M.M. Salah, K.M. Hassan, M. Abouelatta, A. Shaker, "A comparative study of different ETMs in perovskite solar cell with inorganic copper iodide as HTM", Optik 178, 958 (2019). CrossRef S. Rai, B. Pandey, A. Garg, D. Dwivedi, "Hole transporting layer optimization for an efficient lead-free double perovskite solar cell by numerical simulation", Opt. Mater, 121, 111645 (2021). CrossRef H. Liangsheng, Z. Min, S. Yubao, M. Xinxia, W. Jiang, Z. Qunzhi, F, Zaiguo, L. Yihao, H. Guoyu, L. Tong, "Tin-based perovskite solar cells: Further improve the performance of the electron transport layer-free structure by device simulation", Sol. Energy, 230, 345 (2021). CrossRef K. Fatema, M. Arefin, "Enhancing the efficiency of Pb-based and Sn-based perovskite solar cell by applying different ETL and HTL using SCAPS-ID", Opt. Mater. 125, 112036 (2022). CrossRef P. Patel, "Device simulation of highly efficient eco-friendly CH3NH3SnI3 perovskite solar cell", Sci. Rep., 11, 3082 (2021). CrossRef P. Roy, Y. Raoui, A. Khare, "Design and simulation of efficient tin based perovskite solar cells through optimization of selective layers: Theoretical insights", Opt. Mater., 125, 112057 (2022). CrossRef A.I. Azmi, M.Y. Mohd Noor, M.H.I. Ibrahim, F. Ahmad, M.H. Ibrahim, "A Numerical Simulation of Transport Layer Thickness Effect in Tin-Based Perovskite Solar Cell", JJEE, 8, 355 (2022). CrossRef A.A. Kanoun, M.B. Kanoun, A.E. Merad, S. Goumri-Said, "Toward development of high-performance perovskite solar cells based on CH3NH3GeI3 using computational approach", Sol. Energy, 182, 237 (2019). CrossRef A. Hima, N. Lakhdar, "Enhancement of efficiency and stability of CH3NH3GeI3 solar cells with CuSbS2", Opt. Mater., 99, 109607 (2020). CrossRef S.T. Jan, M. Noman, "Influence of layer thickness, defect density, doping concentration, interface defects, work function, working temperature and reflecting coating on lead-free perovskite solar cell", Sol. Energy, 237, 29 (2022). CrossRef
不同空穴输运材料和缺陷密度下锗基钙钛矿太阳能电池的建模
在锗基钙钛矿太阳能电池(PSC)的设计中,模拟和分析了四种不同材料(有机和无机)作为空穴传输层(HTL)的性能。以二氧化锡(SnO2)为电子传递层(ETL),应用一维数值软件(SCAPS 1-D)模拟了HTL候选者:spiro-OMeTAD、PTAA、氧化镍(NiO)和硫氰酸铜(CuSCN)。甲基碘化锗(CH3NH3GeI3)吸收剂的厚度从300 nm变化到1100 nm,所有HTL候选材料的模拟功率转换效率在800 nm时达到最高。结果表明,无机CuSCN的功率转换效率(PCE)为25.38%,优于同类材料。研究了钙钛矿吸收剂缺陷密度的影响,最终证明缺陷密度值与PCE不成比例地相关,当缺陷密度从1x1014 cm-3增加到1x1020 cm-3时,PCE下降了近98%。此外,当ETL厚度为80 nm时,随着HTL厚度从50 nm增加到300 nm, PCE会略有下降,幅度在0.1% ~ 0.3%之间。将我们目前工作的个人支出与已发表的报告进行比较,进一步证明了其竞争力。W.R. Becquerel,“二元化合物中的贝克勒尔光电效应”,化学学报。物理学32,1505(1960)。引用本文:A. Kojima, K. Teshima, Y. Shirai, T. Miyasaka,“有机金属卤化物钙钛矿在光伏电池可见光敏化中的应用”,J. Am。化学。社会学报,131,6050(2009)。CrossRef M.M. Salah, K.M. Hassan, M. Abouelatta, A. Shaker,“无机氯化铜作为HTM的钙钛矿太阳能电池中不同etm的比较研究”,光学学报,178,958(2019)。陈晓明,陈晓明,陈晓明,“基于量子力学的无铅双钙钛矿太阳能电池的空穴传输层优化研究”,光子学报,2011,31(11):1245 - 1245(2021)。CrossRef胡良生,闵志明,邵玉宝,孟新霞,姜伟,朱群智,F,再国,李义浩,洪国宇,仝亮,“锡基钙钛矿太阳能电池:通过器件模拟进一步提高电子传输无层结构的性能”,太阳能学报,230,345(2021)。CrossRef K. Fatema, M. Arefin,“基于SCAPS-ID的pb基和sn基钙钛矿太阳能电池的效率提高”,光电工程,125,112036(2022)。CrossRef P. Patel,“高效环保CH3NH3SnI3钙钛矿太阳能电池的器件模拟”,Sci。众议员,11,3082(2021)。CrossRef P. Roy, Y. Raoui, A. Khare,“通过优化选择层的高效锡基钙钛矿太阳能电池的设计和模拟:理论见解”,光学学报。生物工程学报,125,112057(2022)。[CrossRef] A.I. Azmi, M.Y. Mohd Noor, M.H.I. Ibrahim, F. Ahmad, M.H. Ibrahim,“锡基钙钛矿太阳能电池输运层厚度效应的数值模拟”,中国机械工程,8,355(2022)。A.A. Kanoun, M.B. Kanoun, A.E. Merad, S. Goumri-Said,“基于CH3NH3GeI3的高性能钙钛矿太阳能电池的计算方法研究”,太阳能,182,237(2019)。CrossRef A. Hima, N. Lakhdar,“利用CuSbS2提高CH3NH3GeI3太阳能电池的效率和稳定性”,光电学报。浙江农业学报,1999,109607(2020)。[10]王晓明,杨晓明,“无铅钙钛矿太阳能电池的制备及其性能研究”,材料工程,2003,24(6):444 - 444。CrossRef
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