Copper doping effect in the back surface field layer of CdTe thin film solar cells

被引:2
|
作者
Ahmad, Nur Irwany [1 ,2 ]
Kiong, Tiong Sieh [1 ,3 ]
Doroody, Camellia [1 ,3 ]
Rahman, Kazi Sajedur [4 ]
Norizan, Mohd Natashah [5 ]
Ahmad, Mohd Fairus [5 ]
Kar, Yap Boon [1 ]
Harif, Muhammad Najib [6 ]
Amin, Nowshad [7 ]
机构
[1] Univ Tenaga Nas, Energy Univ, Coll Engn, Jalan IKRAM UNITEN, Kajang 43000, Selangor, Malaysia
[2] Univ Malaysia Perlis, Fac Elect Engn & Technol, Arau 02600, Perlis, Malaysia
[3] Univ Tenaga Nas, The Energy Univ, Inst Sustainable Energy, Jalan IKRAM UNITEN, Kajang 43000, Selangor, Malaysia
[4] Univ Kebangsaan Malaysia, Solar Energy Res Inst, Bangi 43600, Selangor, Malaysia
[5] Univ Malaysia Perlis, Fac Elect Engn & Technol, Arau 02600, Perlis, Malaysia
[6] Univ Teknol MARA UiTM, Fac Appl Sci, Kuala Pilah 72000, Negeri Sembilan, Malaysia
[7] Amer Int Univ Bangladesh AIUB, Fac Engn, Dept Elect & Elect Engn, 408-1 Kuratoli Rd, Dhaka 1229, Bangladesh
关键词
Energy; Solar cell; Solar Cell Capacitance Simulator (SCAPS); Back surface field (BSF); Cadmium telluride (CdTe); Zinc telluride (ZnTe); Density functional theory (DFT);
D O I
10.1016/j.aej.2024.01.020
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
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 (eta). 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, eta = 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.
引用
收藏
页码:155 / 163
页数:9
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