Please use this identifier to cite or link to this item: http://dx.doi.org/10.25673/117835
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dc.contributor.authorCojocaru-Mirédin, Oana-
dc.contributor.authorHariskos, Dimitrios-
dc.contributor.authorHempel, Wolfram-
dc.contributor.authorKanevce, Ana-
dc.contributor.authorJin, Xiaowei-
dc.contributor.authorKeutgen, Jens-
dc.contributor.authorRaghuwanshi, Mohit-
dc.contributor.authorSchneider, Reinhard-
dc.contributor.authorScheer, Roland-
dc.contributor.authorGerthsen, Dagmar-
dc.contributor.authorWitte, Wolfram-
dc.date.accessioned2025-01-10T10:10:12Z-
dc.date.available2025-01-10T10:10:12Z-
dc.date.issued2024-
dc.identifier.urihttps://opendata.uni-halle.de//handle/1981185920/119795-
dc.identifier.urihttp://dx.doi.org/10.25673/117835-
dc.description.abstractThe design of a Cd-free and wider-bandgap buffer layer is stringent for future Cu(In,Ga)Se2 (CIGSe) thin-film solar cell applications. For that, an In2S3 buffer layer alloyed with a limited amount of O (well below 25 mol%) has been proposed as a pertinent alternative solution to CdS or Zn(O,S) buffers. However, the chemical stability of the In2S3/CIGSe heterointerface when O is added is not completely clear. Therefore, in this work, the buffer/absorber interface for a series of sputter-deposited In2S3 buffers with and without O is investigated. It is found that the solar cell with the highest open-circuit voltage is obtained for the O-free In2S3 buffer sputtered at 220 °C. This improved open-circuit voltage could be explained by the presence of a 20 nm-thick ordered vacancy compound (OVC) at the absorber surface. A much thinner OVC layer (5 nm) or even the absence of this layer is found for the cell with In2(O0.25S0.75)3 buffer layer where O is inserted. The volume fraction of the OVC layer is directly linked with the magnitude of Cu diffusion from the CIGSe surface into the In2(OxS1−x)3 buffer layer. The O addition strongly reduces the Cu diffusion inside the buffer layer up to complete suppression for very high O contents in the buffer. Finally, it is discussed that the presence of the OVC layer may lower the valence band maximum, thereby forming a hole barrier, suppressing charge carrier recombination at the In2(OxS1−x)3/CIGSe interface, which could result in an increased open-circuit voltage.eng
dc.language.isoeng-
dc.rights.urihttps://creativecommons.org/licenses/by-nc-nd/4.0/-
dc.subject.ddc530-
dc.titleOrdered vacancy compound formation at the interface of Cu(In,Ga)Se2 absorber with sputtered In2S3-based buffers : an atomic-scale perspectiveeng
dc.typeArticle-
local.versionTypepublishedVersion-
local.bibliographicCitation.journaltitleSolar RRL-
local.bibliographicCitation.volume8-
local.bibliographicCitation.issue23-
local.bibliographicCitation.pagestart1-
local.bibliographicCitation.pageend11-
local.bibliographicCitation.publishernameWiley-VCH-
local.bibliographicCitation.publisherplaceWeinheim-
local.bibliographicCitation.doi10.1002/solr.202400574-
local.openaccesstrue-
dc.identifier.ppn1914136640-
cbs.publication.displayform2024-
local.bibliographicCitation.year2024-
cbs.sru.importDate2025-01-10T10:09:38Z-
local.bibliographicCitationEnthalten in Solar RRL - Weinheim : Wiley-VCH, 2017-
local.accessrights.dnbfree-
Appears in Collections:Open Access Publikationen der MLU