Optimization of the Epitaxial Growth of Undoped GaN Waveguides in GaN-Based Laser Diodes Evaluated by Photoluminescence

dc.bibliographicCitation.firstPage5138
dc.bibliographicCitation.issue9
dc.bibliographicCitation.lastPage5143
dc.bibliographicCitation.volume49
dc.contributor.authorNetzel, C.
dc.contributor.authorHoffmann, V.
dc.contributor.authorEinfeldt, S.
dc.contributor.authorWeyers, M.
dc.date.accessioned2022-09-02T07:26:24Z
dc.date.available2022-09-02T07:26:24Z
dc.date.issued2020
dc.description.abstractNon-intentionally doped c-plane GaN layers are generally employed as p-side waveguide layers in violet/blue-emitting laser diodes. The recombination and diffusion of charge carriers in the p-side GaN waveguide influence the injection efficiency of holes into the InGaN quantum wells of these devices. In this study, the non-radiative recombination and the diffusivity in the [000-1] direction for charge carriers in such GaN layers are investigated by the photoluminescence of buried InGaN quantum wells, in addition to the GaN photoluminescence. The vertical charge carrier diffusion length and the diffusion constant in GaN were determined by evaluating the intensity from InGaN quantum wells in different depths below a top GaN layer. Additionally, the intensity from the buried InGaN quantum wells was found to be more sensitive to variations in the non-radiative recombination rate in the GaN layer than the intensity from the GaN itself. The study enables conclusions to be drawn on how the growth of a p-side GaN waveguide layer has to be optimized: (1) The charge carrier diffusivity in the [000-1] direction at device operation temperature is limited by phonon scattering and can be only slightly improved by material quality. (2) The use of TMGa (trimethylgallium) instead of TEGa (triethylgallium) as a precursor for the growth of GaN lowers the background silicon doping level and is advantageous for a large hole diffusion length. (3) Small growth rates below 0.5 μm/h when using TMGa or below 0.12 μm/h when using TEGa enhance non-radiative recombination. (4) A V/III gas ratio of 2200 or more is needed for low non-radiative recombination rates in GaN.eng
dc.description.versionpublishedVersioneng
dc.identifier.urihttps://oa.tib.eu/renate/handle/123456789/10168
dc.identifier.urihttp://dx.doi.org/10.34657/9206
dc.language.isoengeng
dc.publisherWarrendale, Pa : TMS
dc.relation.doihttps://doi.org/10.1007/s11664-020-08159-x
dc.relation.essn1543-186X
dc.relation.ispartofseriesJournal of electronic materials : JEM ; a publication of the Minerals, Metals & Materials Society (TMS) and the Institute of Electrical and Electronics Engineers (IEEE) 49 (2020), Nr. 9
dc.rights.licenseCC BY 4.0 Unported
dc.rights.urihttps://creativecommons.org/licenses/by/4.0/
dc.subjectcharge carrier diffusioneng
dc.subjectGallium nitrideeng
dc.subjectMOVPE growtheng
dc.subjectphotoluminescenceeng
dc.subjectKonferenzschriftger
dc.subject.ddc670
dc.titleOptimization of the Epitaxial Growth of Undoped GaN Waveguides in GaN-Based Laser Diodes Evaluated by Photoluminescenceeng
dc.typearticleeng
dc.typeTexteng
dcterms.bibliographicCitation.journalTitleJournal of electronic materials : JEM ; a publication of the Minerals, Metals & Materials Society (TMS) and the Institute of Electrical and Electronics Engineers (IEEE)
tib.accessRightsopenAccesseng
tib.relation.conference18th Conference on Defects-Recognition, Imaging and Physics in Semiconductors (DRIP XVIII), 8.-12. September 2019, Berlin, Germany
wgl.contributorFBH
wgl.subjectPhysikger
wgl.typeZeitschriftenartikelger
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