Copper doping effect in the back surface field layer of CdTe thin film solar cells
In this work, the Solar Cell Capacitance Simulator (SCAPS-1D) is employed to evaluate the characteristics of CdTe thin films with ZnTe as the Back Surface Field (BSF) layer and estimate the effective copper doping ratio at both the atomic scale and the device operational response perspective. The el...
Published in: | Alexandria Engineering Journal |
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Elsevier B.V.
2024
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2-s2.0-85182634692 Ahmad N.I.; Kiong T.S.; Doroody C.; Rahman K.S.; Norizan M.N.; Ahmad M.F.; Kar Y.B.; Harif M.N.; Amin N. Copper doping effect in the back surface field layer of CdTe thin film solar cells 2024 Alexandria Engineering Journal 88 10.1016/j.aej.2024.01.020 https://www.scopus.com/inward/record.uri?eid=2-s2.0-85182634692&doi=10.1016%2fj.aej.2024.01.020&partnerID=40&md5=4610a8037e4bb9a52822e11a39a21a69 In this work, the Solar Cell Capacitance Simulator (SCAPS-1D) is employed to evaluate the characteristics of CdTe thin films with ZnTe as the Back Surface Field (BSF) layer and estimate the effective copper doping ratio at both the atomic scale and the device operational response perspective. The electrical characteristics of ZnTe, at varying levels of copper doping, were derived using density functional theory (DFT) by applying the generalized gradient approximation (GGA) and Hubbard U corrections (DFT+U). The performance of ZnTe with different Cu concentrations as a BSF layer was evaluated by analysing the values of four key parameters that are open circuit voltage (VOC), short circuit current density (JSC), fill factor (FF), and conversion efficiency (η). The results indicate that an increase in Cu concentration from 0% to 3%, 6%, 10%, and 12% resulted in a reduction of the energy band gap. Specifically, the energy band gap decreased from 2.24 eV to 2.10 eV, 1.98 eV, 1.92 eV, and 1.88 eV, respectively. Optimal Cu doping promotes the favourable shift in the valence band maxima (VBM) and formation of p + -ZnTe, lowering thermionic emission and improving carrier lifetime, which results in an improved ohmic contact, η = 18.73% for 10% of Cu content. Excessive doping in contrast degraded the overall device performance by forming an unmatched carrier band offset at the front interface with CdS, increasing the acceptor type defect and CdTe compensation rate. Overall, the findings suggest that incorporating a controlled level of Cu, which in this case is around 10%, promotes the efficiency and stability of the proposed CdTe device configuration to a certain extent. © 2024 The Authors Elsevier B.V. 11100168 English Article All Open Access; Gold Open Access |
author |
Ahmad N.I.; Kiong T.S.; Doroody C.; Rahman K.S.; Norizan M.N.; Ahmad M.F.; Kar Y.B.; Harif M.N.; Amin N. |
spellingShingle |
Ahmad N.I.; Kiong T.S.; Doroody C.; Rahman K.S.; Norizan M.N.; Ahmad M.F.; Kar Y.B.; Harif M.N.; Amin N. Copper doping effect in the back surface field layer of CdTe thin film solar cells |
author_facet |
Ahmad N.I.; Kiong T.S.; Doroody C.; Rahman K.S.; Norizan M.N.; Ahmad M.F.; Kar Y.B.; Harif M.N.; Amin N. |
author_sort |
Ahmad N.I.; Kiong T.S.; Doroody C.; Rahman K.S.; Norizan M.N.; Ahmad M.F.; Kar Y.B.; Harif M.N.; Amin N. |
title |
Copper doping effect in the back surface field layer of CdTe thin film solar cells |
title_short |
Copper doping effect in the back surface field layer of CdTe thin film solar cells |
title_full |
Copper doping effect in the back surface field layer of CdTe thin film solar cells |
title_fullStr |
Copper doping effect in the back surface field layer of CdTe thin film solar cells |
title_full_unstemmed |
Copper doping effect in the back surface field layer of CdTe thin film solar cells |
title_sort |
Copper doping effect in the back surface field layer of CdTe thin film solar cells |
publishDate |
2024 |
container_title |
Alexandria Engineering Journal |
container_volume |
88 |
container_issue |
|
doi_str_mv |
10.1016/j.aej.2024.01.020 |
url |
https://www.scopus.com/inward/record.uri?eid=2-s2.0-85182634692&doi=10.1016%2fj.aej.2024.01.020&partnerID=40&md5=4610a8037e4bb9a52822e11a39a21a69 |
description |
In this work, the Solar Cell Capacitance Simulator (SCAPS-1D) is employed to evaluate the characteristics of CdTe thin films with ZnTe as the Back Surface Field (BSF) layer and estimate the effective copper doping ratio at both the atomic scale and the device operational response perspective. The electrical characteristics of ZnTe, at varying levels of copper doping, were derived using density functional theory (DFT) by applying the generalized gradient approximation (GGA) and Hubbard U corrections (DFT+U). The performance of ZnTe with different Cu concentrations as a BSF layer was evaluated by analysing the values of four key parameters that are open circuit voltage (VOC), short circuit current density (JSC), fill factor (FF), and conversion efficiency (η). The results indicate that an increase in Cu concentration from 0% to 3%, 6%, 10%, and 12% resulted in a reduction of the energy band gap. Specifically, the energy band gap decreased from 2.24 eV to 2.10 eV, 1.98 eV, 1.92 eV, and 1.88 eV, respectively. Optimal Cu doping promotes the favourable shift in the valence band maxima (VBM) and formation of p + -ZnTe, lowering thermionic emission and improving carrier lifetime, which results in an improved ohmic contact, η = 18.73% for 10% of Cu content. Excessive doping in contrast degraded the overall device performance by forming an unmatched carrier band offset at the front interface with CdS, increasing the acceptor type defect and CdTe compensation rate. Overall, the findings suggest that incorporating a controlled level of Cu, which in this case is around 10%, promotes the efficiency and stability of the proposed CdTe device configuration to a certain extent. © 2024 The Authors |
publisher |
Elsevier B.V. |
issn |
11100168 |
language |
English |
format |
Article |
accesstype |
All Open Access; Gold Open Access |
record_format |
scopus |
collection |
Scopus |
_version_ |
1809677883818377216 |