Optical Design and Calculation of Interlayer in Thin Film Silicon Tandem Solar Cells

2014 ◽  
Vol 34 (6) ◽  
pp. 0622006
Author(s):  
涂晔 Tu Ye ◽  
杨雯 Yang Wen ◽  
杨培志 Yang Peizhi ◽  
张力元 Zhang Liyuan ◽  
段良飞 Duan Liangfei
2009 ◽  
Vol 159-160 ◽  
pp. 44-47 ◽  
Author(s):  
Vlad Smirnov ◽  
Chandan Das ◽  
Thomas Melle ◽  
Andreas Lambertz ◽  
Markus Hülsbeck ◽  
...  

2014 ◽  
Vol 2 (30) ◽  
pp. 6140-6147 ◽  
Author(s):  
Peihua Wangyang ◽  
Yanchang Gan ◽  
Qingkang Wang ◽  
Xuesong Jiang

Micromorph tandem solar cells coated with a HP array layer were fabricated by UV NIL. The HP array layer could reduce the average reflectance of the solar cells from 7.7% to 1.8%. And a relative improvement of efficiency of up to 4.1% is observed as compared to the bare solar cells.


Author(s):  
Jin-Won Chung ◽  
Ji Eun Lee ◽  
Ji Hoon Jang ◽  
Jeong Chul Lee ◽  
Jun-Sik Cho ◽  
...  

MRS Advances ◽  
2018 ◽  
Vol 3 (52) ◽  
pp. 3111-3119 ◽  
Author(s):  
Ramez H. Ahangharnejhad ◽  
Zhaoning Song ◽  
Adam B. Phillips ◽  
Suneth C. Watthage ◽  
Zahrah S. Almutawah ◽  
...  

Abstract:Monolithic integrated thin film tandem solar cells consisting of a high bandgap perovskite top cell and a low bandgap thin film bottom cell are expected to reach higher power conversion efficiencies (PCEs) with lower manufacturing cost and environmental impacts than the market-dominant crystalline silicon photovoltaics. There have been several demonstrations of 4-terminal and 2-terminal perovskite tandem devices with CuInGaSe2 (CIGS) or CuInSe2 (CIS) and, similar to the other tandem structures, the optimization of this device relies on optimal choice for the perovskite bandgap and thickness. Therefore, further advancement will be enabled by tuning the perovskite absorber to maximize the photocurrent limited by the current match condition. Here, we systematically study the optical absorption and transmission of perovskite thin films with varying absorber band gap. Based on these results, we model the photocurrent generations in both perovskite and CIS subcells and estimate the performances of projected tandem devices by considering the ideally functioning perovskite and CIS device. Our results show that for perovskite layers with 500 nm thickness the optimal bandgap is around 1.6 eV. With these configurations, PCEs above 20% could be achieved by monolithically integrated perovskite/CIS tandem solar cells. Also by modelling the absorption at every layer we calculate the quantum efficiency at each subcell in addition to tracking optical losses.


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