Orientation dependence of electronic structure and optical gain of (11N)-oriented III-V-N quantum wells

A ten-band k ∙p Hamiltonian for III-V-N dilute nitride semiconductor quantum wells (QWs) grown on the (11N)-oriented substrates is presented. The energy dispersion curves, optical transition matrix elements, internal piezoelectric field, and optical gain of InGaAsN/GaAs on the (110), (111), (113)...

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Main Author: Fan, Weijun
Other Authors: School of Electrical and Electronic Engineering
Format: Article
Language:English
Published: 2013
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Online Access:https://hdl.handle.net/10356/96418
http://hdl.handle.net/10220/9931
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spelling sg-ntu-dr.10356-964182020-03-07T14:02:46Z Orientation dependence of electronic structure and optical gain of (11N)-oriented III-V-N quantum wells Fan, Weijun School of Electrical and Electronic Engineering DRNTU::Engineering::Electrical and electronic engineering A ten-band k ∙p Hamiltonian for III-V-N dilute nitride semiconductor quantum wells (QWs) grown on the (11N)-oriented substrates is presented. The energy dispersion curves, optical transition matrix elements, internal piezoelectric field, and optical gain of InGaAsN/GaAs on the (110), (111), (113), and (11∞)-oriented substrates are investigated including band-anti-crossing, strain, and piezoelectric field effects. The band structures and optical gain are sensitive to the substrate orientation. The fundamental transition energy is the largest for the (111)-oriented QW and the smallest for (11∞)-oriented QW. The absolute values of internal piezoelectric field in the well and barrier layers reach the maximum for the (111)-QW, and zero for the (110) and (11∞)-oriented QWs. There exists an injection current density turning point. When the injection current density is below the turning point, the (111)-oriented QW has the largest peak gain. At the larger injection current density, the (11∞)-oriented QW has the largest peak gain. Published version 2013-05-13T07:30:51Z 2019-12-06T19:30:24Z 2013-05-13T07:30:51Z 2019-12-06T19:30:24Z 2013 2013 Journal Article Fan, W. (2013). Orientation dependence of electronic structure and optical gain of (11N)-oriented III-V-N quantum wells. Journal of applied physics, 113(8). 00218979 https://hdl.handle.net/10356/96418 http://hdl.handle.net/10220/9931 10.1063/1.4793279 en Journal of applied physics © 2013 American Institute of Physics. This paper was published in Journal of Applied Physics and is made available as an electronic reprint (preprint) with permission of American Institute of Physics. The paper can be found at the following official DOI: http://dx.doi.org/10.1063/1.4793279. One print or electronic copy may be made for personal use only. Systematic or multiple reproduction, distribution to multiple locations via electronic or other means, duplication of any material in this paper for a fee or for commercial purposes, or modification of the content of the paper is prohibited and is subject to penalties under law. application/pdf
institution Nanyang Technological University
building NTU Library
country Singapore
collection DR-NTU
language English
topic DRNTU::Engineering::Electrical and electronic engineering
spellingShingle DRNTU::Engineering::Electrical and electronic engineering
Fan, Weijun
Orientation dependence of electronic structure and optical gain of (11N)-oriented III-V-N quantum wells
description A ten-band k ∙p Hamiltonian for III-V-N dilute nitride semiconductor quantum wells (QWs) grown on the (11N)-oriented substrates is presented. The energy dispersion curves, optical transition matrix elements, internal piezoelectric field, and optical gain of InGaAsN/GaAs on the (110), (111), (113), and (11∞)-oriented substrates are investigated including band-anti-crossing, strain, and piezoelectric field effects. The band structures and optical gain are sensitive to the substrate orientation. The fundamental transition energy is the largest for the (111)-oriented QW and the smallest for (11∞)-oriented QW. The absolute values of internal piezoelectric field in the well and barrier layers reach the maximum for the (111)-QW, and zero for the (110) and (11∞)-oriented QWs. There exists an injection current density turning point. When the injection current density is below the turning point, the (111)-oriented QW has the largest peak gain. At the larger injection current density, the (11∞)-oriented QW has the largest peak gain.
author2 School of Electrical and Electronic Engineering
author_facet School of Electrical and Electronic Engineering
Fan, Weijun
format Article
author Fan, Weijun
author_sort Fan, Weijun
title Orientation dependence of electronic structure and optical gain of (11N)-oriented III-V-N quantum wells
title_short Orientation dependence of electronic structure and optical gain of (11N)-oriented III-V-N quantum wells
title_full Orientation dependence of electronic structure and optical gain of (11N)-oriented III-V-N quantum wells
title_fullStr Orientation dependence of electronic structure and optical gain of (11N)-oriented III-V-N quantum wells
title_full_unstemmed Orientation dependence of electronic structure and optical gain of (11N)-oriented III-V-N quantum wells
title_sort orientation dependence of electronic structure and optical gain of (11n)-oriented iii-v-n quantum wells
publishDate 2013
url https://hdl.handle.net/10356/96418
http://hdl.handle.net/10220/9931
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