Studies of Performance of Cs2TiI6-XBrX (Where x=0 to 6)-Based Mixed Halide Perovskite Solar Cell with CdS Electron Transport Layer

被引:3
作者
Chakraborty, Kunal [1 ]
Medikondu, Nageswara Rao [2 ]
Duraisamy, Kumutha [3 ]
Soliman, Naglaa F. [4 ]
El-Shafai, Walid [5 ,6 ]
Lavadiya, Sunil [7 ]
Paul, Samrat [1 ]
Das, Sudipta [8 ]
机构
[1] North Eastern Hill Univ, Dept Energy Engn, Adv Mat Res & Energy Applicat Lab, Shillong 793022, India
[2] Koneru Lakshmaiah Educ Fdn, Dept Mech Engn, Vaddeswaram 522302, India
[3] KarpagaVinayaga Coll Engn & Technol, Dept Biomed Engn, Chengalpattu 603308, India
[4] Princess Nourah Bint Abdulrahman Univ, Coll Comp & Informat Sci, Dept Informat Technol, POB 84428, Riyadh 11671, Saudi Arabia
[5] Prince Sultan Univ, Comp Sci Dept, Secur Engn Lab, Riyadh 11586, Saudi Arabia
[6] Menoufia Univ, Fac Elect Engn, Dept Elect & Elect Commun Engn, Menoufia 32952, Egypt
[7] Marwadi Univ, Dept Informat & Commun Technol, Rajkot 360003, India
[8] IMPS Coll Engn & Technol, Dept Elect & Commun Engn, Malda 732103, India
关键词
perovskite; solar cell; diffusion; efficiency; SIMULATION;
D O I
10.3390/mi14020447
中图分类号
O65 [分析化学];
学科分类号
070302 ; 081704 ;
摘要
The present research work represents the numerical study of the device performance of a lead-free Cs2TiI6-XBrX-based mixed halide perovskite solar cell (PSC), where x = 1 to 5. The open circuit voltage (V-OC) and short circuit current (J(SC)) in a generic TCO/electron transport layer (ETL)/absorbing layer/hole transfer layer (HTL) structure are the key parameters for analyzing the device performance. The entire simulation was conducted by a SCAPS-1D (solar cell capacitance simulator- one dimensional) simulator. An alternative FTO/CdS/Cs2TiI6-XBrX/CuSCN/Ag solar cell architecture has been used and resulted in an optimized absorbing layer thickness at 0.5 mu m thickness for the Cs2TiBr6, Cs2TiI1Br5, Cs2TiI2Br4, Cs2TiI3Br3 and Cs2TiI4Br2 absorbing materials and at 1.0 mu m and 0.4 mu m thickness for the Cs2TiI5Br1 and Cs2TiI6 absorbing materials. The device temperature was optimized at 40 degrees C for the Cs2TiBr6, Cs2TiI1Br5 and Cs2TiI2Br4 absorbing layers and at 20 degrees C for the Cs2TiI3Br3, Cs2TiI4Br2, Cs2TiI5Br1 and Cs2TiI6 absorbing layers. The defect density was optimized at 10(10) (cm(-3)) for all the active layers.
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页数:11
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