Effect of Cd1-xZnxS Window Layer Incorporation in CdTe Solar Cell by Numerical Simulation
| dc.contributor.author | Das, N. K. | |
| dc.contributor.author | Sengupta, A. K. | |
| dc.contributor.author | Dey, Mrinmoy | |
| dc.contributor.author | Rahman, K. S. | |
| dc.contributor.author | Matin, M. A. | |
| dc.contributor.author | Amin, N. | |
| dc.date.accessioned | 2026-07-06T21:26:45Z | |
| dc.date.available | 2026-07-06T21:26:45Z | |
| dc.date.issued | 7-Feb-2019 | |
| dc.description.abstract | CdTe is a very potential binary semiconductor | |
| dc.description.abstract | material for solar photovoltaic application due to its superior | |
| dc.description.abstract | optoelectronic properties. The overall performances of | |
| dc.description.abstract | incorporating Cd1-xZnxS window layer in lieu of CdS layer in | |
| dc.description.abstract | CdTe solar cell were investigated by SCAPS-1D simulator. The | |
| dc.description.abstract | Cd1-xZnxS is an alloy of CdS and ZnS which increase band gap of | |
| dc.description.abstract | window layer from 2.42 eV to 3.7 eV as a function of x (from x=0 | |
| dc.description.abstract | to 1). The spectral response of the design Cd1-xZnxS/CdTe cell | |
| dc.description.abstract | improves in blue region which implies the big improvement of | |
| dc.description.abstract | short circuit current density Jsc. In addition, in the traditional | |
| dc.description.abstract | back contact of CdTe cell a small positive conduction band (ΔEC | |
| dc.description.abstract | <0.3 eV) offset is necessary to reduce the forward current J0 as | |
| dc.description.abstract | well as the recombination losses at the back contact. To achieve | |
| dc.description.abstract | this goal a highly doped ZnTe:Cu extra layer was used as an | |
| dc.description.abstract | electron reflector (ER) above back contact. Furthermore, this ER | |
| dc.description.abstract | interface allows electron tunnelling by reducing the barrier | |
| dc.description.abstract | height of the valence band which in turn leads to an | |
| dc.description.abstract | improvement of open circuit voltage and fill factor. The | |
| dc.description.abstract | performance of the proposed cell was examined by varying | |
| dc.description.abstract | thickness and doping concentration of transparent conducting | |
| dc.description.abstract | oxide (TCO) layer, window layer, absorber layer and finally ER | |
| dc.description.abstract | layer. The simulated results of the proposed cell had shown that | |
| dc.description.abstract | the open circuit voltage (Voc) overcame the 1-volt barrier of CdTe | |
| dc.description.abstract | cell with energy conversion efficiencies of 19.93 %. | |
| dc.identifier.other | http://103.99.128.19:8080/jspui/handle/123456789/298 | |
| dc.identifier.uri | http://103.99.128.19:8080/xmlui/handle/123456789/298 | |
| dc.publisher | Faculty of Electrical and Computer Engineering, CUET | |
| dc.source | CUET Digital Repository | |
| dc.subject | Cd1-xZnxS window layer | |
| dc.subject | CdTe Solar cell | |
| dc.subject | Cu electron reflector | |
| dc.title | Effect of Cd1-xZnxS Window Layer Incorporation in CdTe Solar Cell by Numerical Simulation | |
| dc.title.alternative | International Conference on Electrical, Computer and Communication Engineering (ECCE-2019) |
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