Strain engineering of ferroelectric domains in KxNa1−xNbO3 epitaxial layers

dc.bibliographicCitation.journalTitleFrontiers in Materialseng
dc.bibliographicCitation.volume4
dc.contributor.authorSchwarzkopf, Jutta
dc.contributor.authorBraun, Dorothee
dc.contributor.authorHanke, Michael
dc.contributor.authorUecker, Reinhard
dc.contributor.authorSchmidbauer, Martin
dc.date.available2019-06-28T12:38:35Z
dc.date.issued2017
dc.description.abstractThe application of lattice strain through epitaxial growth of oxide films on lattice mismatched perovskite-like substrates strongly influences the structural properties of ferroelectric domains and their corresponding piezoelectric behavior. The formation of different ferroelectric phases can be understood by a strain-phase diagram, which is calculated within the framework of the Landau–Ginzburg–Devonshire theory. In this paper, we illustrate the opportunity of ferroelectric domain engineering in the KxNa1−xNbO3 lead-free material system. In particular, the following examples are discussed in detail: (i) Different substrates (NdGaO3, SrTiO3, DyScO3, TbScO3, and GdScO3) are used to systematically tune the incorporated epitaxial strain from compressive to tensile. This can be exploited to adjust the NaNbO3 thin film surface orientation and, concomitantly, the vector of electrical polarization, which rotates from mainly vertical to exclusive in-plane orientation. (ii) In ferroelectric NaNbO3, thin films grown on rare-earth scandate substrates, highly regular stripe domain patterns are observed. By using different film thicknesses, these can be tailored with regard to domain periodicity and vertical polarization component. (iii) A featured potassium concentration of x = 0.9 of KxNa1−xNbO3 thin films grown on (110) NdScO3 substrates favors the coexistence of two equivalent, monoclinic, but differently oriented ferroelectric phases. A complicated herringbone domain pattern is experimentally observed which consists of alternating MC and a1a2 domains. The coexistence of different types of ferroelectric domains leads to polarization discontinuities at the domain walls, potentially enabling high piezoelectric responses. In each of these examples, the experimental results are in excellent agreement with predictions based on the linear elasticity theory.eng
dc.description.versionpublishedVersioneng
dc.formatapplication/pdf
dc.identifier.urihttps://doi.org/10.34657/1662
dc.identifier.urihttps://oa.tib.eu/renate/handle/123456789/4091
dc.language.isoengeng
dc.publisherLausanne : Frontiers Mediaeng
dc.relation.doihttps://doi.org/10.3389/fmats.2017.00026
dc.rights.licenseCC BY 4.0 Unportedeng
dc.rights.urihttps://creativecommons.org/licenses/by/4.0/eng
dc.subject.ddc530eng
dc.subject.otherFerroelectric domainseng
dc.subject.otherKxNa1−xNbO3eng
dc.subject.otherthin filmseng
dc.subject.otherstrain engineeringeng
dc.subject.otherepitaxial growtheng
dc.subject.otherX-ray diffractioneng
dc.subject.otherpiezoresponse force microscopyeng
dc.subject.othermetal-organic chemical vapor depositioneng
dc.titleStrain engineering of ferroelectric domains in KxNa1−xNbO3 epitaxial layerseng
dc.typeArticleeng
dc.typeTexteng
tib.accessRightsopenAccesseng
wgl.contributorIKZeng
wgl.contributorPDIeng
wgl.subjectPhysikeng
wgl.subjectIngenieurwissenschafteneng
wgl.typeZeitschriftenartikeleng
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