Prospects of Zinc Sulphide as an alternative buffer layer for CZTS solar cells from numerical analysis

Author(s):  
F. Haque ◽  
N.A. Khan ◽  
K.S. Rahman ◽  
M.A. Islam ◽  
M. M. Alam ◽  
...  
Optik ◽  
2020 ◽  
Vol 204 ◽  
pp. 164155
Author(s):  
Benzetta Abd El Halim ◽  
Abderrezek Mahfoud ◽  
Djeghlal Mohammed Elamine

2021 ◽  
Vol 2128 (1) ◽  
pp. 012009
Author(s):  
Hassan Ismail Abdalmageed ◽  
Mostafa Fedawy ◽  
Moustafa H. Aly

Abstract This article uses computational models to evaluate the potential of copper-indium-gallium-diselenide (CIGS) thin film solar cells. The use of cadmium sulphide (CdS) renders the solar cell environmentally hazardous. A zinc sulphide (ZnS) that is non-toxic and has a large bandgap is studied as a potential replacement for cadmium sulphide in CIGS-based solar cells. The present research focuses on the impact of the CIGS-based solar cell bandgap absorber layer by increasing the absorber layer thickness (0.1-2 μm) using the solar cell simulator simulation tool SCAPS. The basic simulation produces 18.2 % efficiency with a CdS buffer layer, which is 9.95% better than the previously published work. The Simulated efficiency is 22.16% for the CIGS solar cell using ZnS. The simulation of solar cell characteristics of how the thickness of the absorber layer, the gallium grading (efficiency ranges up to 22.25 %) is demonstrated, showing the effect of buffer layer (ZnS) on the current of short-circuit density (JSC), open-circuit voltage (Voc), fill factor (FF), and efficiency (η) of the solar cell.


Pramana ◽  
2020 ◽  
Vol 94 (1) ◽  
Author(s):  
G L MBOPDA TCHEUM ◽  
A TEYOU NGOUPO ◽  
S OUÉDRAOGO ◽  
N GUIRDJEBAYE ◽  
J M B NDJAKA

2003 ◽  
Vol 762 ◽  
Author(s):  
Jianhua Zhu ◽  
Vikram L. Dalal

AbstractWe report on the growth and properties of microcrystalline Si:H and (Si,Ge):H solar cells on stainless steel substrates. The solar cells were grown using a remote, low pressure ECR plasma system. In order to crystallize (Si,Ge), much higher hydrogen dilution (∼40:1) had to be used compared to the case for mc-Si:H, where a dilution of 10:1 was adequate for crystallization. The solar cell structure was of the p+nn+ type, with light entering the p+ layer. It was found that it was advantageous to use a thin a-Si:H buffer layer at the back of the cells in order to reduce shunt density and improve the performance of the cells. A graded gap buffer layer was used at the p+n interface so as to improve the open-circuit voltage and fill factor. The open circuit voltage and fill factor decreased as the Ge content increased. Quantum efficiency measurements indicated that the device was indeed microcrystalline and followed the absorption characteristics of crystalline ( Si,Ge). As the Ge content increased, quantum efficiency in the infrared increased. X-ray measurements of films indicated grain sizes of ∼ 10nm. EDAX measurements were used to measure the Ge content in the films and devices. Capacitance measurements at low frequencies ( ~100 Hz and 1 kHz) indicated that the base layer was indeed behaving as a crystalline material, with classical C(V) curves. The defect density varied between 1x1016 to 2x1017/cm3, with higher defects indicated as the Ge concentration increased.


Author(s):  
Xingyun Liu ◽  
Zitong Feng ◽  
Yuxia Sun ◽  
Mingzhu Su ◽  
Ying Liu ◽  
...  

Author(s):  
Zhiqin Ying ◽  
Xi Yang ◽  
Jingming Zheng ◽  
Yudong Zhu ◽  
Jingwei Xiu ◽  
...  

A charge-transfer induced BCP:Ag complex is employed as a multifunctional buffer layer for efficient inverted semi-transparent perovskite solar cells.


2010 ◽  
Vol 23 (3) ◽  
pp. 313-316 ◽  
Author(s):  
Ryo Morioka ◽  
Kei Yasui ◽  
Masaki Ozawa ◽  
Keisuke Odoi ◽  
Hisashi Ichikawa ◽  
...  

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