Strong light-matter coupling in bulk GaN-microcavities with double dielectric mirrors fabricated by two different methods

被引:5
|
作者
Reveret, F. [1 ,2 ]
Bejtka, K. [3 ,4 ]
Edwards, P. R. [4 ]
Chenot, S. [3 ]
Sellers, I. R. [3 ]
Disseix, P. [1 ,2 ]
Vasson, A. [1 ,2 ]
Leymarie, J. [1 ,2 ]
Duboz, J. Y. [3 ]
Leroux, M. [3 ]
Semond, F. [3 ]
Martin, R. W. [4 ]
机构
[1] Univ Clermont Ferrand, Clermont Univ, LASMEA, F-63000 Clermont Ferrand, France
[2] CNRS, UMR 6602, LASMEA, F-63177 Clermont Ferrand, France
[3] CRHEA CNRS, F-06560 Valbonne, France
[4] Univ Strathclyde, SUPA, Dept Phys, Glasgow G4 0NG, Lanark, Scotland
基金
英国工程与自然科学研究理事会;
关键词
SEMICONDUCTOR MICROCAVITIES; LASER;
D O I
10.1063/1.3477450
中图分类号
O59 [应用物理学];
学科分类号
摘要
Two routes for the fabrication of bulk GaN microcavities embedded between two dielectric mirrors are described, and the optical properties of the microcavities thus obtained are compared. In both cases, the GaN active layer is grown by molecular beam epitaxy on (111) Si, allowing use of selective etching to remove the substrate. In the first case, a three period Al(0.2)Ga(0.8)N / AlN Bragg mirror followed by a lambda/2 GaN cavity are grown directly on the Si. In the second case, a crack-free 2,mu m thick GaN layer is grown, and progressively thinned to a final thickness of lambda. Both devices work in the strong coupling regime at low temperature, as evidenced by angle-dependent reflectivity or transmission experiments. However, strong light-matter coupling in emission at room temperature is observed only for the second one. This is related to the poor optoelectronic quality of the active layer of the first device, due to its growth only 250 nm above the Si substrate and its related high defect density. The reflectivity spectra of the microcavities are well accounted for by using transfer matrix calculations. (C) 2010 American Institute of Physics. [doi:10.1063/1.3477450]
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页数:6
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