The importance of back contact modification in Cu2ZnSnSe4 solar cells: The role of a thin MoO2 layer

dc.contributor.authorLópez-Marino, Simon
dc.contributor.authorEspindola Rodriguez, Moises
dc.contributor.authorSánchez González, Yudania
dc.contributor.authorAlcobé i Ollé, Xavier
dc.contributor.authorOliva Cuyàs, Francesc
dc.contributor.authorXie, Haibing
dc.contributor.authorNeuschitzer, Markus
dc.contributor.authorGiraldo Muñoz, Sergio
dc.contributor.authorPlacidi, Marcel
dc.contributor.authorCaballero, Raquel
dc.contributor.authorIzquierdo Roca, Victor
dc.contributor.authorPérez Rodríguez, Alejandro
dc.contributor.authorSaucedo Silva, Edgardo
dc.date.accessioned2019-02-19T17:42:20Z
dc.date.available2019-02-19T17:42:20Z
dc.date.issued2016-06-23
dc.date.updated2019-02-19T17:42:20Z
dc.description.abstractCu2ZnSn(SxSe1−x)4 (CZTSSe) photovoltaic absorbers could be the earth-abundant and low toxicity replacement for the already commercialized CuIn1−xGaxSe2 (CIGS) thin film technology. In order to make this possible, specific research efforts applied to the bulk, front and back interfaces must be performed with the aim of improving CZTSSe performance. In this paper the importance of back contact modification to obtain high efficiency Cu2ZnSnSe4 (CZTSe) solar cells and to increase a paramount and limiting parameter such as VOC is highlighted. Several Mo configurations (monolayer, bi-layer and tri-layer) with different electrical and morphological properties are investigated in CZTSe solar cells. An optimum tri-layer configuration in order to minimize overselenization of the back contact during thermal annealing while keeping reasonable electrical features is defined. Additionally, a thin intermediate MoO2 layer that results in a very effective barrier against selenization and innovative way to efficiently assist in the CZTSe absorber sintering is introduced. The use of this layer enhances grain growth and subsequently the efficiency of solar cells increases via major VOC and FF improvement. An efficiency increase from 7.2% to 9.5% is obtained using a Mo tri-layer with a 20nm intermediate MoO2 layer.
dc.format.extent14 p.
dc.format.mimetypeapplication/pdf
dc.identifier.idgrec665292
dc.identifier.issn2211-2855
dc.identifier.urihttps://hdl.handle.net/2445/128476
dc.language.isoeng
dc.publisherElsevier
dc.relation.isformatofVersió postprint del document publicat a: https://doi.org/10.1016/j.nanoen.2016.06.034
dc.relation.ispartofNano Energy, 2016, vol. 26, p. 708-721
dc.relation.projectIDinfo:eu-repo/grantAgreement/EC/FP7/316488/EU//KESTCELLS
dc.relation.urihttps://doi.org/10.1016/j.nanoen.2016.06.034
dc.rightscc-by-nc-nd (c) Elsevier, 2016
dc.rights.accessRightsinfo:eu-repo/semantics/openAccess
dc.rights.urihttp://creativecommons.org/licenses/by-nc-nd/3.0/es
dc.sourceArticles publicats en revistes (Enginyeria Electrònica i Biomèdica)
dc.subject.classificationCèl·lules solars
dc.subject.classificationPel·lícules fines
dc.subject.classificationFotoelectricitat
dc.subject.classificationEspectroscòpia Raman
dc.subject.otherSolar cells
dc.subject.otherThin films
dc.subject.otherPhotoelectricity
dc.subject.otherRaman spectroscopy
dc.titleThe importance of back contact modification in Cu2ZnSnSe4 solar cells: The role of a thin MoO2 layer
dc.typeinfo:eu-repo/semantics/article
dc.typeinfo:eu-repo/semantics/acceptedVersion

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