Impact of Different Antireflection Layers on Cadmium Telluride (CdTe) Solar Cells: a PC1D Simulation Study

Author(s):  
Devendra KC ◽  
Deb Kumar Shah ◽  
Amer M. Alanazi ◽  
M. Shaheer Akhtar
MRS Advances ◽  
2018 ◽  
Vol 3 (41) ◽  
pp. 2441-2447 ◽  
Author(s):  
Ebin Bastola ◽  
Kamala Khanal Subedi ◽  
Khagendra P. Bhandari ◽  
Randy J. Ellingson

ABSTRACTThe cadmium telluride (CdTe) photovoltaic (PV) comprise an efficient and cost-effective technology for harvesting solar energy. However, device efficiency remains limited in part by low-open circuit voltage (VOC) and fill factor (FF) due to inefficient transport of photo-generated charge carriers. Given the deep valence band of CdTe, the use of copper/gold (Cu/Au) as a back contact serves primarily to narrow the width of the inherent Schottky junction evident in CdTe solar cells (in our laboratory, Cu/Au has been used as a standard back contact). For efficient transport of carriers to and into the back contact, a hole transport layer (HTL) is desired with valence band edge comparable to that of CdTe (∼ -5.9 eV). Here, we report solution-processed nanocrystal (NCs) based thin films as HTLs in CdTe solar cells. The earth abundant materials we discuss include iron pyrite (FeS2), nickel-alloyed iron pyrite (NixFe1-xS2), zinc copper sulfide (ZnxCu1-xS) nanocomposites, and perovskite-based films. The FeS2 and NixFe1-xS2 NCs are synthesized by a hot-injection route, and thin films are fabricated by drop-casting, and spin-coating techniques using colloidal NCs. ZnxCu1-xS thin films are fabricated by chemical bath deposition. These NC-based thin films are applied and studied as the HTLs in CdTe devices. On using these materials, the device performance can be increased up to 10% compared to the standard Cu/Au back contact. Here, we discuss the benefits, challenges, and opportunities for these back contact materials in CdTe photovoltaics.


2017 ◽  
Vol 5 (20) ◽  
pp. 4996-5004 ◽  
Author(s):  
Ebin Bastola ◽  
Khagendra P. Bhandari ◽  
Randy J. Ellingson

The solution-processed colloidal NixFe1−xS2 nanocrystal based thin films serve as the hole transport layers in cadmium telluride (CdTe) solar cells.


2017 ◽  
Vol 5 (10) ◽  
pp. 4904-4911 ◽  
Author(s):  
Jiajie Li ◽  
Yumin Zhang ◽  
Tangling Gao ◽  
Chang Hu ◽  
Tai Yao ◽  
...  

We demonstrate an innovative strategy for quantum dot-induced improved performance of cadmium telluride solar cells without a Cu buffer layer.


Molecules ◽  
2021 ◽  
Vol 26 (11) ◽  
pp. 3275
Author(s):  
Devendra KC ◽  
Deb Kumar Shah ◽  
M. Shaheer Akhtar ◽  
Mira Park ◽  
Chong Yeal Kim ◽  
...  

This paper numerically explores the possibility of ultrathin layering and high efficiency of graphene as a back surface field (BSF) based on a CdTe solar cell by Personal computer one-dimensional (PC1D) simulation. CdTe solar cells have been characterized and studied by varying the carrier lifetime, doping concentration, thickness, and bandgap of the graphene layer. With simulation results, the highest short-circuit current (Isc = 2.09 A), power conversion efficiency (h = 15%), and quantum efficiency (QE ~ 85%) were achieved at a carrier lifetime of 1 × 103 ms and a doping concentration of 1 × 1017 cm−3 of graphene as a BSF layer-based CdTe solar cell. The thickness of the graphene BSF layer (1 mm) was proven the ultrathin, optimal, and obtainable for the fabrication of high-performance CdTe solar cells, confirming the suitability of graphene material as a BSF. This simulation confirmed that a CdTe solar cell with the proposed graphene as the BSF layer might be highly efficient with optimized parameters for fabrication.


Author(s):  
Sandip S. Bista ◽  
Deng-Bing Li ◽  
Zhaoning Song ◽  
Rasha A. Awni ◽  
Suman Rijal ◽  
...  

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