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ALD-Zn(x)Ti(y)O as Window Layer in Cu(In,Ga)Se(2) Solar Cells

[Image: see text] We report on the application of Zn(x)Ti(y)O deposited by atomic layer deposition (ALD) as buffer layer in thin film Cu(In,Ga)Se(2) (CIGS) solar cells to improve the photovoltaic device performance. State-of-the-art CIGS devices employ a CdS/ZnO layer stack sandwiched between the ab...

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Autores principales: Löckinger, Johannes, Nishiwaki, Shiro, Andres, Christian, Erni, Rolf, Rossell, Marta D., Romanyuk, Yaroslav E., Buecheler, Stephan, Tiwari, Ayodhya N.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: American Chemical Society 2018
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6302902/
https://www.ncbi.nlm.nih.gov/pubmed/30462473
http://dx.doi.org/10.1021/acsami.8b14490
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author Löckinger, Johannes
Nishiwaki, Shiro
Andres, Christian
Erni, Rolf
Rossell, Marta D.
Romanyuk, Yaroslav E.
Buecheler, Stephan
Tiwari, Ayodhya N.
author_facet Löckinger, Johannes
Nishiwaki, Shiro
Andres, Christian
Erni, Rolf
Rossell, Marta D.
Romanyuk, Yaroslav E.
Buecheler, Stephan
Tiwari, Ayodhya N.
author_sort Löckinger, Johannes
collection PubMed
description [Image: see text] We report on the application of Zn(x)Ti(y)O deposited by atomic layer deposition (ALD) as buffer layer in thin film Cu(In,Ga)Se(2) (CIGS) solar cells to improve the photovoltaic device performance. State-of-the-art CIGS devices employ a CdS/ZnO layer stack sandwiched between the absorber layer and the front contact. Replacing the sputter deposited ZnO with ALD-Zn(x)Ti(y)O allowed a reduction of the CdS layer thickness without adversely affecting open-circuit voltage (V(OC)). This leads to an increased photocurrent density with a device efficiency of up to 20.8% by minimizing the parasitic absorption losses commonly observed for CdS. ALD was chosen as method to deposit homogeneous layers of Zn(x)Ti(y)O with varying Ti content with a [Ti]/([Ti] + [Zn]) atomic fraction up to ∼0.35 at a relatively low temperature of 373 K. The Ti content influenced the absorption behavior of the Zn(x)Ti(y)O layer by increasing the optical bandgap >3.5 eV in the investigated range. Temperature-dependent current–voltage (I–V) measurements of solar cells were performed to investigate the photocurrent blocking behavior observed for high Ti content. Possible conduction band discontinuities introduced by Zn(x)Ti(y)O are discussed based on X-ray photoelectron spectroscopy (XPS) measurements.
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spelling pubmed-63029022019-11-21 ALD-Zn(x)Ti(y)O as Window Layer in Cu(In,Ga)Se(2) Solar Cells Löckinger, Johannes Nishiwaki, Shiro Andres, Christian Erni, Rolf Rossell, Marta D. Romanyuk, Yaroslav E. Buecheler, Stephan Tiwari, Ayodhya N. ACS Appl Mater Interfaces [Image: see text] We report on the application of Zn(x)Ti(y)O deposited by atomic layer deposition (ALD) as buffer layer in thin film Cu(In,Ga)Se(2) (CIGS) solar cells to improve the photovoltaic device performance. State-of-the-art CIGS devices employ a CdS/ZnO layer stack sandwiched between the absorber layer and the front contact. Replacing the sputter deposited ZnO with ALD-Zn(x)Ti(y)O allowed a reduction of the CdS layer thickness without adversely affecting open-circuit voltage (V(OC)). This leads to an increased photocurrent density with a device efficiency of up to 20.8% by minimizing the parasitic absorption losses commonly observed for CdS. ALD was chosen as method to deposit homogeneous layers of Zn(x)Ti(y)O with varying Ti content with a [Ti]/([Ti] + [Zn]) atomic fraction up to ∼0.35 at a relatively low temperature of 373 K. The Ti content influenced the absorption behavior of the Zn(x)Ti(y)O layer by increasing the optical bandgap >3.5 eV in the investigated range. Temperature-dependent current–voltage (I–V) measurements of solar cells were performed to investigate the photocurrent blocking behavior observed for high Ti content. Possible conduction band discontinuities introduced by Zn(x)Ti(y)O are discussed based on X-ray photoelectron spectroscopy (XPS) measurements. American Chemical Society 2018-11-21 2018-12-19 /pmc/articles/PMC6302902/ /pubmed/30462473 http://dx.doi.org/10.1021/acsami.8b14490 Text en Copyright © 2018 American Chemical Society This is an open access article published under an ACS AuthorChoice License (http://pubs.acs.org/page/policy/authorchoice_termsofuse.html) , which permits copying and redistribution of the article or any adaptations for non-commercial purposes.
spellingShingle Löckinger, Johannes
Nishiwaki, Shiro
Andres, Christian
Erni, Rolf
Rossell, Marta D.
Romanyuk, Yaroslav E.
Buecheler, Stephan
Tiwari, Ayodhya N.
ALD-Zn(x)Ti(y)O as Window Layer in Cu(In,Ga)Se(2) Solar Cells
title ALD-Zn(x)Ti(y)O as Window Layer in Cu(In,Ga)Se(2) Solar Cells
title_full ALD-Zn(x)Ti(y)O as Window Layer in Cu(In,Ga)Se(2) Solar Cells
title_fullStr ALD-Zn(x)Ti(y)O as Window Layer in Cu(In,Ga)Se(2) Solar Cells
title_full_unstemmed ALD-Zn(x)Ti(y)O as Window Layer in Cu(In,Ga)Se(2) Solar Cells
title_short ALD-Zn(x)Ti(y)O as Window Layer in Cu(In,Ga)Se(2) Solar Cells
title_sort ald-zn(x)ti(y)o as window layer in cu(in,ga)se(2) solar cells
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6302902/
https://www.ncbi.nlm.nih.gov/pubmed/30462473
http://dx.doi.org/10.1021/acsami.8b14490
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