Room temperature yellow InGaAlP quantum dot laser

被引:3
|
作者
Ledentsov, N. N. [1 ]
Shchukin, V. A. [1 ]
Shernyakov, Yu M. [2 ]
Kulagina, M. M. [3 ]
Payusov, A. S. [2 ]
Gordeev, N. Yu [2 ]
Maximov, M., V [2 ]
Zhukov, A. E. [2 ]
Karachinsky, L. Ya [4 ]
Denneulin, T. [5 ,6 ]
Cherkashin, N. [6 ]
机构
[1] VI Syst GmbH, Hardenbergstr 7, D-10623 Berlin, Germany
[2] St Petersburg Acad Univ, Khlopin St 8-3, St Petersburg 195220, Russia
[3] Ioffe Inst, Politekhnicheskaya 26, St Petersburg 194021, Russia
[4] ITMO Univ, Kronverksky Pr 49, St Petersburg 197101, Russia
[5] Peter Grunberg Inst PGI 5, Wilhelm Johnen Str, D-52425 Julich, Germany
[6] CEMES CNRS, 29 Rue Jeanne Marvig,BP 94347, F-31055 Toulouse 4, France
基金
俄罗斯基础研究基金会;
关键词
DIODES; OPERATION;
D O I
10.1016/j.sse.2019.03.009
中图分类号
TM [电工技术]; TN [电子技术、通信技术];
学科分类号
0808 ; 0809 ;
摘要
We report simulation of the conduction band alignment in tensile-strained GaP-enriched barrier structures and experimental results on injection lasing in the green-orange spectral range (558-605 nm) in (AlxGa1-x)(0.5)In0.5P-GaAs diodes containing such barriers. The wafers were grown by metal-organic vapor phase epitaxy side-by-side on (8 1 1)A, (2 1 1)A and (3 2 2)A GaAs substrates, which surface orientations were strongly tilted towards the [ 1 1 1]A direction with respect to the (1 0 0) plane. Four sheets of GaP-rich quantum barrier insertions were applied to suppress the leakage of non-equilibrium electrons from the gain medium. Two types of the gain medium were applied. In one case 4-fold stacked tensile-strained (In, Ga) P insertions were used. Experimental data shows that self-organized vertically-correlated quantum dots (QDs) are formed on (2 1 1)A- and (3 2 2)A-oriented substrates, while corrugated quantum wires are formed on the (8 1 1)A surface. In the other case a short-period superlattice (SPSL) composed of 16-fold stacked quasi-lattice-matched 1.4 nm-thick In0.5Ga0.5P layers separated by 4 nm-thick (Al0.6Ga0.4)(0.5)In0.5P layers was applied. Laser diodes with 4-fold stacked QDs having a threshold current densities of similar to 7-10 kA/cm(2) at room temperature were realized for both (2 1 1)A and (3 2 2)A surface orientations at cavity lengths of similar to 1 mm. Emission wavelength at room temperature was similar to 599-603 nm. Threshold current density for the stimulated emission was as low as similar to 1 kA/cm(2). For (8 1 1)A-grown structures no room temperature lasing was observed. SPSL structures demonstrated lasing only at low temperatures < 200 K. The shortest wavelength (558 nm, 90 K) in combination with the highest operation temperature (150 K) was realized for (3 2 2)A-oriented substrates in agreement with theoretical predictions.
引用
收藏
页码:129 / 138
页数:10
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