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dc.contributor.authorKe, M. L.en
dc.contributor.authorChen, X.en
dc.contributor.authorZervos, Matthewen
dc.contributor.authorNawaz, R.en
dc.contributor.authorElliott, M.en
dc.contributor.authorWestwood, D. I.en
dc.contributor.authorBlood, P.en
dc.contributor.authorGodfrey, M. J.en
dc.contributor.authorWilliams, R. H.en
dc.creatorKe, M. L.en
dc.creatorChen, X.en
dc.creatorZervos, Matthewen
dc.creatorNawaz, R.en
dc.creatorElliott, M.en
dc.creatorWestwood, D. I.en
dc.creatorBlood, P.en
dc.creatorGodfrey, M. J.en
dc.creatorWilliams, R. H.en
dc.date.accessioned2019-05-06T12:23:51Z
dc.date.available2019-05-06T12:23:51Z
dc.date.issued1996
dc.identifier.urihttp://gnosis.library.ucy.ac.cy/handle/7/48471
dc.description.abstractWe report here an investigation of selectively delta-doped strained InGaAs/GaAs quantum wells. Electronic structures of the systems were calculated by self-consistently solving the Schrödinger and Poisson equations and the calculations revealed a systematic variation of the band structure as the delta sheet moved away from the center of the well to the edge and finally to the barrier. The results were found to be in agreement with our photoluminescence (PL) measurements. For center-doped samples, band-gap renormalization was found to be strong from the PL data, and our realistic random-phase approximation calculation for the heavily doped sample is in excellent agreement with the PL data. The radiative lifetimes were measured to be around 450 ps for all the samples, and surprisingly they vary very little from sample to sample although the wave-function overlap was considerably different for some samples. We also report Shubnikov-de Haas (SdH) measurements on the two barrier doped cases. For the heavily doped sample (A12132), two oscillation signals were detected and they were identified as two upper subbands. The measured electron densities were in very good agreement with the self-consistent calculation. Illumination did not make any difference to the measured densities. For the low-doped sample (A12025), however, the measured electron density before illumination is much smaller than the calculated, and illumination was found to make a large difference. © 1996 American Institute of Physics.en
dc.language.isoengen
dc.sourceJournal of Applied Physicsen
dc.subjectComputer simulationen
dc.subjectEnergy gapen
dc.subjectApproximation theoryen
dc.subjectDifferential equationsen
dc.subjectOptical propertiesen
dc.subjectSemiconductor dopingen
dc.subjectElectronic structureen
dc.subjectSemiconductor quantum wellsen
dc.subjectSemiconducting indium compoundsen
dc.subjectElectric propertiesen
dc.subjectBand gap renormalizationen
dc.subjectElectron density measurementen
dc.subjectIndium gallium arsenideen
dc.subjectPhotoluminescenceen
dc.subjectPoisson equationsen
dc.subjectRadiative lifetimesen
dc.subjectRandom phase approximationen
dc.subjectSchrodinger equationsen
dc.subjectSelectively delta doped strained quantum wellsen
dc.subjectSemiconducting gallium arsenideen
dc.subjectShubnikov-de Haas measurementsen
dc.titleOptical and electrical properties of selectively delta-doped strained InxGa1-xAs/GaAs quantum wellsen
dc.typeinfo:eu-repo/semantics/article
dc.identifier.doi10.1063/1.361133
dc.description.volume79
dc.description.startingpage2627
dc.description.endingpage2632
dc.author.facultyΠολυτεχνική Σχολή / Faculty of Engineering
dc.author.departmentΤμήμα Μηχανικών Μηχανολογίας και Κατασκευαστικής / Department of Mechanical and Manufacturing Engineering
dc.type.uhtypeArticleen
dc.contributor.orcidZervos, Matthew [0000-0002-6321-233X]
dc.description.totalnumpages2627-2632
dc.gnosis.orcid0000-0002-6321-233X


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