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First-principles investigation on the electronic structures of CdSe(x)S(1−x) and simulation of CdTe solar cell with a CdSe(x)S(1−x) window layer by SCAPS
The short-circuit current density (J(SC)) of CdTe solar cells both in the short and long wavelength regions can be effectively enhanced by using CdS/CdSe as the composite window layer. CdS/CdSe composite layers would interdiffuse to form the CdSe(x)S(1−x) ternary layer during the high temperature de...
Autores principales: | , , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
The Royal Society of Chemistry
2022
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9364174/ https://www.ncbi.nlm.nih.gov/pubmed/36043063 http://dx.doi.org/10.1039/d2ra03053e |
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author | He, Xu Li, Chunxiu Wu, Lili Hao, Xia Zhang, Jingquan Feng, Lianghuan Tang, Peng Du, Zheng |
author_facet | He, Xu Li, Chunxiu Wu, Lili Hao, Xia Zhang, Jingquan Feng, Lianghuan Tang, Peng Du, Zheng |
author_sort | He, Xu |
collection | PubMed |
description | The short-circuit current density (J(SC)) of CdTe solar cells both in the short and long wavelength regions can be effectively enhanced by using CdS/CdSe as the composite window layer. CdS/CdSe composite layers would interdiffuse to form the CdSe(x)S(1−x) ternary layer during the high temperature deposition process of CdTe films. In this paper, the electronic properties of CdSe(x)S(1−x) (0 ≤ x ≤ 1) ternary alloys are investigated by first-principles calculation based on the density functional theory (DFT) and the performance of CdS/CdSe/CdTe devices are modeled by SCAPS to reveal why CdS/CdSe complex layers have good effects. The calculation results show that the position of the valence band of CdSe(x)S(1−x) moves towards the vacuum level as the doping concentration of Se increases and the band gap becomes narrow. According to device modeling, the highest conversion efficiency of 20.34% could be achieved through adjusting the conduction band offset (CBO) of theCdSe(x)S(1−x)/CdTe interface to about 0.11 eV while the Se concentration x approaches 0.75. Further investigations suggest a 50–120 nm thickness of CdSe(x)S(1−x) (x = 0.75) would obtain better device performance. It means that solar cells with a CdSe(x)S(1−x)/CdTe structure need a suitable Se content and thickness of CdSe(x)S(1−x). These results can provide theoretical guidance for the design and fabrication of high efficiency CdTe solar cells. |
format | Online Article Text |
id | pubmed-9364174 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2022 |
publisher | The Royal Society of Chemistry |
record_format | MEDLINE/PubMed |
spelling | pubmed-93641742022-08-29 First-principles investigation on the electronic structures of CdSe(x)S(1−x) and simulation of CdTe solar cell with a CdSe(x)S(1−x) window layer by SCAPS He, Xu Li, Chunxiu Wu, Lili Hao, Xia Zhang, Jingquan Feng, Lianghuan Tang, Peng Du, Zheng RSC Adv Chemistry The short-circuit current density (J(SC)) of CdTe solar cells both in the short and long wavelength regions can be effectively enhanced by using CdS/CdSe as the composite window layer. CdS/CdSe composite layers would interdiffuse to form the CdSe(x)S(1−x) ternary layer during the high temperature deposition process of CdTe films. In this paper, the electronic properties of CdSe(x)S(1−x) (0 ≤ x ≤ 1) ternary alloys are investigated by first-principles calculation based on the density functional theory (DFT) and the performance of CdS/CdSe/CdTe devices are modeled by SCAPS to reveal why CdS/CdSe complex layers have good effects. The calculation results show that the position of the valence band of CdSe(x)S(1−x) moves towards the vacuum level as the doping concentration of Se increases and the band gap becomes narrow. According to device modeling, the highest conversion efficiency of 20.34% could be achieved through adjusting the conduction band offset (CBO) of theCdSe(x)S(1−x)/CdTe interface to about 0.11 eV while the Se concentration x approaches 0.75. Further investigations suggest a 50–120 nm thickness of CdSe(x)S(1−x) (x = 0.75) would obtain better device performance. It means that solar cells with a CdSe(x)S(1−x)/CdTe structure need a suitable Se content and thickness of CdSe(x)S(1−x). These results can provide theoretical guidance for the design and fabrication of high efficiency CdTe solar cells. The Royal Society of Chemistry 2022-08-10 /pmc/articles/PMC9364174/ /pubmed/36043063 http://dx.doi.org/10.1039/d2ra03053e Text en This journal is © The Royal Society of Chemistry https://creativecommons.org/licenses/by-nc/3.0/ |
spellingShingle | Chemistry He, Xu Li, Chunxiu Wu, Lili Hao, Xia Zhang, Jingquan Feng, Lianghuan Tang, Peng Du, Zheng First-principles investigation on the electronic structures of CdSe(x)S(1−x) and simulation of CdTe solar cell with a CdSe(x)S(1−x) window layer by SCAPS |
title | First-principles investigation on the electronic structures of CdSe(x)S(1−x) and simulation of CdTe solar cell with a CdSe(x)S(1−x) window layer by SCAPS |
title_full | First-principles investigation on the electronic structures of CdSe(x)S(1−x) and simulation of CdTe solar cell with a CdSe(x)S(1−x) window layer by SCAPS |
title_fullStr | First-principles investigation on the electronic structures of CdSe(x)S(1−x) and simulation of CdTe solar cell with a CdSe(x)S(1−x) window layer by SCAPS |
title_full_unstemmed | First-principles investigation on the electronic structures of CdSe(x)S(1−x) and simulation of CdTe solar cell with a CdSe(x)S(1−x) window layer by SCAPS |
title_short | First-principles investigation on the electronic structures of CdSe(x)S(1−x) and simulation of CdTe solar cell with a CdSe(x)S(1−x) window layer by SCAPS |
title_sort | first-principles investigation on the electronic structures of cdse(x)s(1−x) and simulation of cdte solar cell with a cdse(x)s(1−x) window layer by scaps |
topic | Chemistry |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9364174/ https://www.ncbi.nlm.nih.gov/pubmed/36043063 http://dx.doi.org/10.1039/d2ra03053e |
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