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Electron-Selective TiO(2) Contact for Cu(In,Ga)Se(2) Solar Cells

The non-toxic and wide bandgap material TiO(2) is explored as an n-type buffer layer on p-type Cu(In,Ga)Se(2) (CIGS) absorber layer for thin film solar cells. The amorphous TiO(2) thin film deposited by atomic layer deposition process at low temperatures shows conformal coverage on the CIGS absorber...

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Autores principales: Hsu, Weitse, Sutter-Fella, Carolin M., Hettick, Mark, Cheng, Lungteng, Chan, Shengwen, Chen, Yunfeng, Zeng, Yuping, Zheng, Maxwell, Wang, Hsin-Ping, Chiang, Chien-Chih, Javey, Ali
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group 2015
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4630620/
https://www.ncbi.nlm.nih.gov/pubmed/26526426
http://dx.doi.org/10.1038/srep16028
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author Hsu, Weitse
Sutter-Fella, Carolin M.
Hettick, Mark
Cheng, Lungteng
Chan, Shengwen
Chen, Yunfeng
Zeng, Yuping
Zheng, Maxwell
Wang, Hsin-Ping
Chiang, Chien-Chih
Javey, Ali
author_facet Hsu, Weitse
Sutter-Fella, Carolin M.
Hettick, Mark
Cheng, Lungteng
Chan, Shengwen
Chen, Yunfeng
Zeng, Yuping
Zheng, Maxwell
Wang, Hsin-Ping
Chiang, Chien-Chih
Javey, Ali
author_sort Hsu, Weitse
collection PubMed
description The non-toxic and wide bandgap material TiO(2) is explored as an n-type buffer layer on p-type Cu(In,Ga)Se(2) (CIGS) absorber layer for thin film solar cells. The amorphous TiO(2) thin film deposited by atomic layer deposition process at low temperatures shows conformal coverage on the CIGS absorber layer. Solar cells from non-vacuum deposited CIGS absorbers with TiO(2) buffer layer result in a high short-circuit current density of 38.9 mA/cm(2) as compared to 36.9 mA/cm(2) measured in the reference cell with CdS buffer layer, without compromising open-circuit voltage. The significant photocurrent gain, mainly in the UV part of the spectrum, can be attributed to the low parasitic absorption loss in the ultrathin TiO(2) layer (~10 nm) with a larger bandgap of 3.4 eV compared to 2.4 eV of the traditionally used CdS. Overall the solar cell conversion efficiency was improved from 9.5% to 9.9% by substituting the CdS by TiO(2) on an active cell area of 10.5 mm(2). Optimized TiO(2)/CIGS solar cells show excellent long-term stability. The results imply that TiO(2) is a promising buffer layer material for CIGS solar cells, avoiding the toxic CdS buffer layer with added performance advantage.
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spelling pubmed-46306202015-11-05 Electron-Selective TiO(2) Contact for Cu(In,Ga)Se(2) Solar Cells Hsu, Weitse Sutter-Fella, Carolin M. Hettick, Mark Cheng, Lungteng Chan, Shengwen Chen, Yunfeng Zeng, Yuping Zheng, Maxwell Wang, Hsin-Ping Chiang, Chien-Chih Javey, Ali Sci Rep Article The non-toxic and wide bandgap material TiO(2) is explored as an n-type buffer layer on p-type Cu(In,Ga)Se(2) (CIGS) absorber layer for thin film solar cells. The amorphous TiO(2) thin film deposited by atomic layer deposition process at low temperatures shows conformal coverage on the CIGS absorber layer. Solar cells from non-vacuum deposited CIGS absorbers with TiO(2) buffer layer result in a high short-circuit current density of 38.9 mA/cm(2) as compared to 36.9 mA/cm(2) measured in the reference cell with CdS buffer layer, without compromising open-circuit voltage. The significant photocurrent gain, mainly in the UV part of the spectrum, can be attributed to the low parasitic absorption loss in the ultrathin TiO(2) layer (~10 nm) with a larger bandgap of 3.4 eV compared to 2.4 eV of the traditionally used CdS. Overall the solar cell conversion efficiency was improved from 9.5% to 9.9% by substituting the CdS by TiO(2) on an active cell area of 10.5 mm(2). Optimized TiO(2)/CIGS solar cells show excellent long-term stability. The results imply that TiO(2) is a promising buffer layer material for CIGS solar cells, avoiding the toxic CdS buffer layer with added performance advantage. Nature Publishing Group 2015-11-03 /pmc/articles/PMC4630620/ /pubmed/26526426 http://dx.doi.org/10.1038/srep16028 Text en Copyright © 2015, Macmillan Publishers Limited http://creativecommons.org/licenses/by/4.0/ This work is licensed under a Creative Commons Attribution 4.0 International License. The images or other third party material in this article are included in the article’s Creative Commons license, unless indicated otherwise in the credit line; if the material is not included under the Creative Commons license, users will need to obtain permission from the license holder to reproduce the material. To view a copy of this license, visit http://creativecommons.org/licenses/by/4.0/
spellingShingle Article
Hsu, Weitse
Sutter-Fella, Carolin M.
Hettick, Mark
Cheng, Lungteng
Chan, Shengwen
Chen, Yunfeng
Zeng, Yuping
Zheng, Maxwell
Wang, Hsin-Ping
Chiang, Chien-Chih
Javey, Ali
Electron-Selective TiO(2) Contact for Cu(In,Ga)Se(2) Solar Cells
title Electron-Selective TiO(2) Contact for Cu(In,Ga)Se(2) Solar Cells
title_full Electron-Selective TiO(2) Contact for Cu(In,Ga)Se(2) Solar Cells
title_fullStr Electron-Selective TiO(2) Contact for Cu(In,Ga)Se(2) Solar Cells
title_full_unstemmed Electron-Selective TiO(2) Contact for Cu(In,Ga)Se(2) Solar Cells
title_short Electron-Selective TiO(2) Contact for Cu(In,Ga)Se(2) Solar Cells
title_sort electron-selective tio(2) contact for cu(in,ga)se(2) solar cells
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4630620/
https://www.ncbi.nlm.nih.gov/pubmed/26526426
http://dx.doi.org/10.1038/srep16028
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