mose2 layer
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2021 ◽  
pp. 163301
Author(s):  
Sung-Tae Kim ◽  
Vishwa Bhatt ◽  
Ye-Chan Kim ◽  
Ho-Jung Jeong ◽  
Ju-Hyung Yun ◽  
...  
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Coatings ◽  
2021 ◽  
Vol 11 (8) ◽  
pp. 930
Author(s):  
Fazliyana Za’abar ◽  
Yulisa Yusoff ◽  
Hassan Mohamed ◽  
Siti Abdullah ◽  
Ahmad Mahmood Zuhdi ◽  
...  

The influence of Molybdenum diselenide (MoSe2) as an interfacial layer between Cu(In,Ga)Se2 (CIGS) absorber layer and Molybdenum (Mo) back contact in a conventional CIGS thin-film solar cell was investigated numerically using SCAPS-1D (a Solar Cell Capacitance Simulator). Using graded bandgap profile of the absorber layer that consist of both back grading (BG) and front grading (FG), which is defined as double grading (DG), attribution to the variation in Ga content was studied. The key focus of this study is to explore the combinatorial effects of MoSe2 contact layer and Ga grading of the absorber to suppress carrier losses due to back contact recombination and resistance that usually occur in case of standard Mo thin films. Thickness, bandgap energy, electron affinity and carrier concentration of the MoSe2 layer were all varied to determine the best configuration for incorporating into the CIGS solar cell structure. A bandgap grading profile that offers optimum functionality in the proposed configuration with additional MoSe2 layer has also been investigated. From the overall results, CIGS solar cells with thin MoSe2 layer and high acceptor doping concentration have been found to outperform the devices without MoSe2 layer, with an increase in efficiency from 20.19% to 23.30%. The introduction of bandgap grading in the front and back interfaces of the absorber layer further improves both open-circuit voltage (VOC) and short-circuit current density (JSC), most likely due to the additional quasi-electric field beneficial for carrier collection and reduced back surface and bulk recombination. A maximum power conversion efficiency (PCE) of 28.06%, fill factor (FF) of 81.89%, JSC of 39.45 mA/cm2, and VOC of 0.868 V were achieved by optimizing the properties of MoSe2 layer and bandgap grading configuration of the absorber layer. This study provides an insight into the different possibilities for designing higher efficiency CIGS solar cell structure through the manipulation of naturally formed MoSe2 layer and absorber bandgap engineering that can be experimentally replicated.


2020 ◽  
Vol 381 ◽  
pp. 363-373 ◽  
Author(s):  
Weiheng Chen ◽  
Ru Qiao ◽  
Changsheng Song ◽  
Leihong Zhao ◽  
Zhong-Jie Jiang ◽  
...  

2014 ◽  
Vol 570 ◽  
pp. 166-171 ◽  
Author(s):  
Yi-Cheng Lin ◽  
Ming -Tsung Shen ◽  
Yung-Lin Chen ◽  
Hung-Ru Hsu ◽  
Cheng-Han Wu

2007 ◽  
Vol 124-126 ◽  
pp. 983-986 ◽  
Author(s):  
Ki Hyun Kim ◽  
Se Jin Ahn ◽  
Byung Tae Ahn ◽  
Kyung Hoon Yoon

To make a dense CIGS absorber layer, spray deposited CIGS films were annealed in the two-zone RTP furnace in Se atmosphere. More Se supply by increasing Se evaporation temperature or by increasing the flow rate of carrier gas resulted in the larger CIGS grains. However, a thick MoSe2 layer was formed between CIGS and Mo, as the Se supply increased, results in partial detachment of CIGS/MoSe2/Mo layers from the glass substrate. From the result, it was found that the short heat- treatment with high Se vapor pressure is better than the long heat-treatment with low Se vapor pressure. The large CIGS grains without peeling off, can be obtained from the following conditions; Se evaporation temperature of 450oC, substrate temperature of 550oC, annealing time of 5 min, and flow rate of carrier gas of 30 sccm.


2003 ◽  
Vol 431-432 ◽  
pp. 398-402 ◽  
Author(s):  
R. Würz ◽  
D. Fuertes Marrón ◽  
A. Meeder ◽  
A. Rumberg ◽  
S.M. Babu ◽  
...  

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