Delta-Doping in strained (Si) / (Ge) superlattices

buir.contributor.authorÇıracı, Salim
buir.contributor.orcidÇıracı, Salim|0000-0001-8023-9860
dc.citation.epage12731en_US
dc.citation.issueNumber17en_US
dc.citation.spage12728en_US
dc.citation.volumeNumber38en_US
dc.contributor.authorÇıracı, Salimen_US
dc.contributor.authorBatra, I. P.en_US
dc.contributor.authorTekman, E.en_US
dc.date.accessioned2016-02-08T10:57:19Z
dc.date.available2016-02-08T10:57:19Z
dc.date.issued1988en_US
dc.departmentDepartment of Physicsen_US
dc.description.abstractWe present a comparative study of the pseudomorphic (Si)6/(Ge)6 and -doped (Si)3(Sb)(Si)2/(Ge)6 superlattices using the self-consistent pseudopotential method. The strained (Si)6/(Ge)6 superlattice has the lowest conduction-band states of extended character, and the difference of energy between the direct and indirect band gap is 70 meV. Upon doping by Sb in the Si sublattice, a quasi-two-dimensional band confined to the Sb layer dips into the band gap. Furthermore, the average potential in the Ge sublattice rises relative to that of the Si side, which increases the band offset, and enhances the localization of the quantum well states. These results indicate that doping provides new means for controlling the electronic properties of strained superlattices. © 1988 The American Physical Society.en_US
dc.description.provenanceMade available in DSpace on 2016-02-08T10:57:19Z (GMT). No. of bitstreams: 1 bilkent-research-paper.pdf: 70227 bytes, checksum: 26e812c6f5156f83f0e77b261a471b5a (MD5) Previous issue date: 1988en
dc.identifier.doi10.1103/PhysRevB.38.12728en_US
dc.identifier.issn2469-9950
dc.identifier.urihttp://hdl.handle.net/11693/26265
dc.language.isoEnglishen_US
dc.publisherAmerican Physical Societyen_US
dc.relation.isversionofhttp://dx.doi.org/10.1103/PhysRevB.38.12728en_US
dc.source.titlePhysical Review Ben_US
dc.titleDelta-Doping in strained (Si) / (Ge) superlatticesen_US
dc.typeArticleen_US

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