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...
Saved in:
Main Authors: | , , , , , , , , |
---|---|
Other Authors: | |
Format: | Article |
Published: |
Elsevier B.V.
2025
|
Subjects: | |
Tags: |
Add Tag
No Tags, Be the first to tag this record!
|
id |
my.uniten.dspace-36856 |
---|---|
record_format |
dspace |
spelling |
my.uniten.dspace-368562025-03-03T15:45:14Z Copper doping effect in the back surface field layer of CdTe thin film solar cells 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. 57200991933 57216824752 56905467200 56348138800 57226822517 55779469900 58072938600 22634024000 7102424614 Cadmium sulfide Capacitance Carrier lifetime Conversion efficiency Copper Copper compounds Density functional theory Electric network analysis Energy gap II-VI semiconductors Ohmic contacts Open circuit voltage Semiconductor doping Thermionic emission Thin film solar cells Thin films Zinc compounds Back surface field Backsurface field Cadmium telluride Cell capacitance Density functional theory Density-functional-theory Energy Solar cell capacitance simulator Zinc telluride Zinc tellurides Cadmium telluride 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 (?). 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, ? = 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 Final 2025-03-03T07:45:14Z 2025-03-03T07:45:14Z 2024 Article 10.1016/j.aej.2024.01.020 2-s2.0-85182634692 https://www.scopus.com/inward/record.uri?eid=2-s2.0-85182634692&doi=10.1016%2fj.aej.2024.01.020&partnerID=40&md5=4610a8037e4bb9a52822e11a39a21a69 https://irepository.uniten.edu.my/handle/123456789/36856 88 155 163 All Open Access; Gold Open Access Elsevier B.V. Scopus |
institution |
Universiti Tenaga Nasional |
building |
UNITEN Library |
collection |
Institutional Repository |
continent |
Asia |
country |
Malaysia |
content_provider |
Universiti Tenaga Nasional |
content_source |
UNITEN Institutional Repository |
url_provider |
http://dspace.uniten.edu.my/ |
topic |
Cadmium sulfide Capacitance Carrier lifetime Conversion efficiency Copper Copper compounds Density functional theory Electric network analysis Energy gap II-VI semiconductors Ohmic contacts Open circuit voltage Semiconductor doping Thermionic emission Thin film solar cells Thin films Zinc compounds Back surface field Backsurface field Cadmium telluride Cell capacitance Density functional theory Density-functional-theory Energy Solar cell capacitance simulator Zinc telluride Zinc tellurides Cadmium telluride |
spellingShingle |
Cadmium sulfide Capacitance Carrier lifetime Conversion efficiency Copper Copper compounds Density functional theory Electric network analysis Energy gap II-VI semiconductors Ohmic contacts Open circuit voltage Semiconductor doping Thermionic emission Thin film solar cells Thin films Zinc compounds Back surface field Backsurface field Cadmium telluride Cell capacitance Density functional theory Density-functional-theory Energy Solar cell capacitance simulator Zinc telluride Zinc tellurides Cadmium telluride 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 |
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 (?). 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, ? = 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 |
author2 |
57200991933 |
author_facet |
57200991933 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. |
format |
Article |
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. |
author_sort |
Ahmad N.I. |
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 |
publisher |
Elsevier B.V. |
publishDate |
2025 |
_version_ |
1825816034503819264 |
score |
13.244413 |