Numerical analysis on ZnxCd1−xS/CdTe solar cells with different buffer layers, front and back contacts

Author(s):  
Md. Sharafat Hossain ◽  
M. M. Aliyu ◽  
M. A. Matin ◽  
T. Razykov ◽  
K. Sopian ◽  
...  
2019 ◽  
Vol 691 ◽  
pp. 137556 ◽  
Author(s):  
Francesco Bittau ◽  
Shridhar Jagdale ◽  
Christos Potamialis ◽  
Jake W. Bowers ◽  
John M. Walls ◽  
...  

MRS Advances ◽  
2019 ◽  
Vol 4 (16) ◽  
pp. 913-919 ◽  
Author(s):  
Fadhil K. Alfadhili ◽  
Adam B. Phillips ◽  
Geethika K. Liyanage ◽  
Jacob M. Gibbs ◽  
Manoj K. Jamarkattel ◽  
...  

ABSTRACTFormation of a low barrier back contact plays a critical role in improving the photoconversion efficiency of the CdTe solar cells. Incorporating a buffer layer to minimize the band bending at the back of the CdTe device can significantly lower the barrier for the hole current, improving open circuit voltage (VOC) and the fill factor. Over the past years, researchers have incorporated the both ZnTe and Te as buffer layers to improve CdTe device performance. Here we compare device performance using these two materials as buffer layers at the back of CdTe devices. We show that using Te in contact to CdTe results in higher performance than using ZnTe in contact to the CdTe. Low temperature current density-voltage measurements show that Te results is a lower barrier with CdTe than ZnTe, indicating that Te has better band alignment, resulting in less downward bending in the CdTe at the back interface, than ZnTe does.


Author(s):  
M. I. Hossain ◽  
P. Chelvanathan ◽  
M. M. Alam ◽  
M. Akhtaruzzaman ◽  
K. Sopian ◽  
...  

2019 ◽  
Vol 2 (8) ◽  
pp. 5419-5426 ◽  
Author(s):  
Geethika K. Liyanage ◽  
Adam B. Phillips ◽  
Fadhil K. Alfadhili ◽  
Randy J. Ellingson ◽  
Michael J. Heben

2005 ◽  
Vol 480-481 ◽  
pp. 224-229 ◽  
Author(s):  
C.S. Ferekides ◽  
R. Mamazza ◽  
U. Balasubramanian ◽  
D.L. Morel

MRS Advances ◽  
2016 ◽  
Vol 1 (14) ◽  
pp. 937-942 ◽  
Author(s):  
Y. G. Fedorenko ◽  
J. D. Major ◽  
A. Pressman ◽  
L. Phillips ◽  
K. Durose

ABSTRACTWe considered modification of the defect density of states in CdTe as influenced by a buffer layer in ZnO(ZnS, SnSe)/CdS/CdTe solar cells. Compared to the solar cells employing ZnO buffer layers, implementation of ZnSe and ZnS resulted in the lower net ionized acceptor concentration and the energy shift of the dominant deep trap levels to the midgap of CdTe. The results clearly indicated that the same defect was responsible for the inefficient doping and the formation of recombination centers in CdTe. This observation can be explained taking into account the effect of strain on the electronic properties of the grain boundary interface states in polycrystalline CdTe. In the conditions of strain, interaction of chlorine with the grain boundary point defects can be altered.


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