Determination of energy-band offsets between GaN and AlN using excitonic luminescence transition in AlGaN alloys

dc.citation.epage013705-4en_US
dc.citation.issueNumber1en_US
dc.citation.spage013705-1en_US
dc.citation.volumeNumber99en_US
dc.contributor.authorWestmeyer, A. N.en_US
dc.contributor.authorMahajan, S.en_US
dc.contributor.authorBajaj, K. K.en_US
dc.contributor.authorLin J. Y.en_US
dc.contributor.authorJiang, H. X.en_US
dc.contributor.authorKoleske, D. D.en_US
dc.contributor.authorSenger, R. T.en_US
dc.date.accessioned2016-02-08T10:20:28Z
dc.date.available2016-02-08T10:20:28Z
dc.date.issued2006en_US
dc.departmentDepartment of Physicsen_US
dc.description.abstractWe report the determination of the energy-band offsets between GaN and AlN using the linewidth (full width at half maximum) of an extremely sharp excitonic luminescence transition in Alx Ga1-x N alloy with x=0.18 at 10 K. Our sample was grown on C -plane sapphire substrate by metal-organic chemical-vapor deposition at 1050 °C. The observed value of the excitonic linewidth of 17 meV is the smallest ever reported in literature. On subtracting a typical value of the excitonic linewidth in high-quality GaN, namely, 4.0 meV, we obtain a value of 13.0 meV, which we attribute to compositional disorder. This value is considerably smaller than that calculated using a delocalized exciton model [S. M. Lee and K. K. Bajaj, J. Appl. Phys. 73, 1788 (1993)]. The excitons are known to be strongly localized by defects and/or the potential fluctuations in this alloy system. We have simulated this localization assuming that the hole, being much more massive than the electron, is completely immobile, i.e., the hole mass is treated as infinite. Assuming that the excitonic line broadening is caused entirely by the potential fluctuations experienced by the conduction electron, the value of the conduction-band offset between GaN and AlN is determined to be about 57% of the total-band-gap discontinuity. Using our model we have calculated the variation of the excitonic linewidth as a function of Al composition in our samples with higher Al content larger than 18% and have compared it with the experimental data. We also compare our value of the conduction-band offset with those recently proposed by several other groups using different techniques.en_US
dc.description.provenanceMade available in DSpace on 2016-02-08T10:20:28Z (GMT). No. of bitstreams: 1 bilkent-research-paper.pdf: 70227 bytes, checksum: 26e812c6f5156f83f0e77b261a471b5a (MD5) Previous issue date: 2006en
dc.identifier.doi10.1063/1.2158492en_US
dc.identifier.eissn1520-8850
dc.identifier.issn0021-8979
dc.identifier.urihttp://hdl.handle.net/11693/23868
dc.language.isoEnglishen_US
dc.publisherAmerican Institute of Physicsen_US
dc.publisherA I P Publishing LLCen_US
dc.relation.isversionofhttp://dx.doi.org/10.1063/1.2158492en_US
dc.source.titleJournal of Applied Physicsen_US
dc.subjectDelocalized exciton modelen_US
dc.subjectEnergy-band offsetsen_US
dc.subjectExcitonic luminescence transitionen_US
dc.subjectPotential fluctuationsen_US
dc.subjectAluminum nitrideen_US
dc.subjectElectronsen_US
dc.subjectExcitonsen_US
dc.subjectGallium nitrideen_US
dc.subjectLuminescenceen_US
dc.subjectMetallorganic chemical vapor depositionen_US
dc.subjectBand structureen_US
dc.titleDetermination of energy-band offsets between GaN and AlN using excitonic luminescence transition in AlGaN alloysen_US
dc.typeArticleen_US

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