Cargando…

Optimal CdS Buffer Thickness to Form High-Quality CdS/Cu(In,Ga)Se(2) Junctions in Solar Cells without Plasma Damage and Shunt Paths

[Image: see text] CdS has been known to be one of the best junction partners for Cu(In,Ga)Se(2) (CIGS) in CIGS solar cells. However, the use of thick CdS buffer decreases the short-circuit current density of CIGS solar cells. There are two obstacles that limit the use of ultrathin CdS. The first is...

Descripción completa

Detalles Bibliográficos
Autores principales: Cho, Kyung Soo, Jang, Jiseong, Park, Jeung-Hun, Lee, Doh-Kwon, Song, Soomin, Kim, Kihwan, Eo, Young-Joo, Yun, Jae Ho, Gwak, Jihye, Chung, Choong-Heui
Formato: Online Artículo Texto
Lenguaje:English
Publicado: American Chemical Society 2020
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7513370/
https://www.ncbi.nlm.nih.gov/pubmed/32984719
http://dx.doi.org/10.1021/acsomega.0c03268
_version_ 1783586371641802752
author Cho, Kyung Soo
Jang, Jiseong
Park, Jeung-Hun
Lee, Doh-Kwon
Song, Soomin
Kim, Kihwan
Eo, Young-Joo
Yun, Jae Ho
Gwak, Jihye
Chung, Choong-Heui
author_facet Cho, Kyung Soo
Jang, Jiseong
Park, Jeung-Hun
Lee, Doh-Kwon
Song, Soomin
Kim, Kihwan
Eo, Young-Joo
Yun, Jae Ho
Gwak, Jihye
Chung, Choong-Heui
author_sort Cho, Kyung Soo
collection PubMed
description [Image: see text] CdS has been known to be one of the best junction partners for Cu(In,Ga)Se(2) (CIGS) in CIGS solar cells. However, the use of thick CdS buffer decreases the short-circuit current density of CIGS solar cells. There are two obstacles that limit the use of ultrathin CdS. The first is plasma damage to CIGS during the preparation of transparent conducting windows and the second is a low shunt resistance due to the direct contact between the window and CIGS via pinholes in the thin CdS buffer. In other words, to avoid plasma damage and shunt paths, we may have to use a CdS buffer that is thicker than necessary to form a high-quality CdS/CIGS junction. This work aims to determine how thin the CdS buffer can be employed without sacrificing device performance while also eliminating the above two obstacles. We investigate the effect of CdS thickness on the performance of CIGS solar cells with silver nanowire-based window layers, which can eliminate both obstacles. An approximately 13 nm thick CdS buffer allows us to achieve high short-circuit current density and fill factor values. To attain an even high open-circuit voltage, an additional CdS buffer with a thickness of 13 nm is needed. The data from this study imply that an approximately 26 nm thick CdS buffer is sufficient to form a high-quality CdS/CIGS junction.
format Online
Article
Text
id pubmed-7513370
institution National Center for Biotechnology Information
language English
publishDate 2020
publisher American Chemical Society
record_format MEDLINE/PubMed
spelling pubmed-75133702020-09-25 Optimal CdS Buffer Thickness to Form High-Quality CdS/Cu(In,Ga)Se(2) Junctions in Solar Cells without Plasma Damage and Shunt Paths Cho, Kyung Soo Jang, Jiseong Park, Jeung-Hun Lee, Doh-Kwon Song, Soomin Kim, Kihwan Eo, Young-Joo Yun, Jae Ho Gwak, Jihye Chung, Choong-Heui ACS Omega [Image: see text] CdS has been known to be one of the best junction partners for Cu(In,Ga)Se(2) (CIGS) in CIGS solar cells. However, the use of thick CdS buffer decreases the short-circuit current density of CIGS solar cells. There are two obstacles that limit the use of ultrathin CdS. The first is plasma damage to CIGS during the preparation of transparent conducting windows and the second is a low shunt resistance due to the direct contact between the window and CIGS via pinholes in the thin CdS buffer. In other words, to avoid plasma damage and shunt paths, we may have to use a CdS buffer that is thicker than necessary to form a high-quality CdS/CIGS junction. This work aims to determine how thin the CdS buffer can be employed without sacrificing device performance while also eliminating the above two obstacles. We investigate the effect of CdS thickness on the performance of CIGS solar cells with silver nanowire-based window layers, which can eliminate both obstacles. An approximately 13 nm thick CdS buffer allows us to achieve high short-circuit current density and fill factor values. To attain an even high open-circuit voltage, an additional CdS buffer with a thickness of 13 nm is needed. The data from this study imply that an approximately 26 nm thick CdS buffer is sufficient to form a high-quality CdS/CIGS junction. American Chemical Society 2020-09-09 /pmc/articles/PMC7513370/ /pubmed/32984719 http://dx.doi.org/10.1021/acsomega.0c03268 Text en Copyright © 2020 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 Cho, Kyung Soo
Jang, Jiseong
Park, Jeung-Hun
Lee, Doh-Kwon
Song, Soomin
Kim, Kihwan
Eo, Young-Joo
Yun, Jae Ho
Gwak, Jihye
Chung, Choong-Heui
Optimal CdS Buffer Thickness to Form High-Quality CdS/Cu(In,Ga)Se(2) Junctions in Solar Cells without Plasma Damage and Shunt Paths
title Optimal CdS Buffer Thickness to Form High-Quality CdS/Cu(In,Ga)Se(2) Junctions in Solar Cells without Plasma Damage and Shunt Paths
title_full Optimal CdS Buffer Thickness to Form High-Quality CdS/Cu(In,Ga)Se(2) Junctions in Solar Cells without Plasma Damage and Shunt Paths
title_fullStr Optimal CdS Buffer Thickness to Form High-Quality CdS/Cu(In,Ga)Se(2) Junctions in Solar Cells without Plasma Damage and Shunt Paths
title_full_unstemmed Optimal CdS Buffer Thickness to Form High-Quality CdS/Cu(In,Ga)Se(2) Junctions in Solar Cells without Plasma Damage and Shunt Paths
title_short Optimal CdS Buffer Thickness to Form High-Quality CdS/Cu(In,Ga)Se(2) Junctions in Solar Cells without Plasma Damage and Shunt Paths
title_sort optimal cds buffer thickness to form high-quality cds/cu(in,ga)se(2) junctions in solar cells without plasma damage and shunt paths
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7513370/
https://www.ncbi.nlm.nih.gov/pubmed/32984719
http://dx.doi.org/10.1021/acsomega.0c03268
work_keys_str_mv AT chokyungsoo optimalcdsbufferthicknesstoformhighqualitycdscuingase2junctionsinsolarcellswithoutplasmadamageandshuntpaths
AT jangjiseong optimalcdsbufferthicknesstoformhighqualitycdscuingase2junctionsinsolarcellswithoutplasmadamageandshuntpaths
AT parkjeunghun optimalcdsbufferthicknesstoformhighqualitycdscuingase2junctionsinsolarcellswithoutplasmadamageandshuntpaths
AT leedohkwon optimalcdsbufferthicknesstoformhighqualitycdscuingase2junctionsinsolarcellswithoutplasmadamageandshuntpaths
AT songsoomin optimalcdsbufferthicknesstoformhighqualitycdscuingase2junctionsinsolarcellswithoutplasmadamageandshuntpaths
AT kimkihwan optimalcdsbufferthicknesstoformhighqualitycdscuingase2junctionsinsolarcellswithoutplasmadamageandshuntpaths
AT eoyoungjoo optimalcdsbufferthicknesstoformhighqualitycdscuingase2junctionsinsolarcellswithoutplasmadamageandshuntpaths
AT yunjaeho optimalcdsbufferthicknesstoformhighqualitycdscuingase2junctionsinsolarcellswithoutplasmadamageandshuntpaths
AT gwakjihye optimalcdsbufferthicknesstoformhighqualitycdscuingase2junctionsinsolarcellswithoutplasmadamageandshuntpaths
AT chungchoongheui optimalcdsbufferthicknesstoformhighqualitycdscuingase2junctionsinsolarcellswithoutplasmadamageandshuntpaths