Stranski-Krastanov Growth of InAs Quantum Dots with Narrow Size Distribution

2000 ◽  
Vol 39 (Part 2, No. 12A) ◽  
pp. L1245-L1248 ◽  
Author(s):  
Koichi Yamaguchi ◽  
Kunihiko Yujobo ◽  
Toshiyuki Kaizu
2008 ◽  
Vol 17 (1) ◽  
pp. 323-327 ◽  
Author(s):  
Huang She-Song ◽  
Niu Zhi-Chuan ◽  
Zhan Feng ◽  
Ni Hai-Qiao ◽  
Zhao Huan ◽  
...  

2007 ◽  
Vol 18 (S1) ◽  
pp. 191-194 ◽  
Author(s):  
S. I. Jung ◽  
H. Y. Yeo ◽  
I. Yun ◽  
J. Y. Leem ◽  
I. K. Han ◽  
...  

2000 ◽  
Vol 62 (11) ◽  
pp. 7213-7218 ◽  
Author(s):  
H. Kissel ◽  
U. Müller ◽  
C. Walther ◽  
W. T. Masselink ◽  
Yu. I. Mazur ◽  
...  

2017 ◽  
Vol 32 (5) ◽  
pp. 055013 ◽  
Author(s):  
H Xie ◽  
R Prioli ◽  
G Torelly ◽  
H Liu ◽  
A M Fischer ◽  
...  

2019 ◽  
Vol 126 (2) ◽  
pp. 024301 ◽  
Author(s):  
Francesco Basso Basset ◽  
Sergio Bietti ◽  
Artur Tuktamyshev ◽  
Stefano Vichi ◽  
Emiliano Bonera ◽  
...  

2007 ◽  
Vol 31 ◽  
pp. 132-134
Author(s):  
P. Boonpeng ◽  
S. Panyakeow ◽  
S. Ratanathammaphan

InAs quantum dots (QDs) have been grown by solid-source molecular beam epitaxy on different InxGa1-xAs (0 ≤ x ≤ 0.3) to investigate the effect of In-mole-fraction and thickness of InGaAs insertion layer (IL) on the structural and optical properties of the QDs. The density of QDs directly grown on GaAs is 1×1010 cm-2, and increase to 1.4-1.8×1010 cm-2 on InGaAs layers which depend on the In-mole-fraction and thickness of InGaAs layers. The effects of In-mole-fraction and thickness of InGaAs insertion layer on optical properties of the QDs are studied by photoluminescence (PL). The FWHM of PL spectrum corresponds to the size distribution of the QDs.


2005 ◽  
Vol 44 (4A) ◽  
pp. 2037-2040 ◽  
Author(s):  
Chang-Myung Lee ◽  
Suk-Ho Choi ◽  
Sam-Kyu Noh ◽  
Joo In Lee ◽  
Jin-Soo Kim ◽  
...  

1995 ◽  
Vol 417 ◽  
Author(s):  
J.-L. Lazzari ◽  
R. Klann ◽  
A. Mazuelas ◽  
A. Trampert ◽  
M. Wassermeier ◽  
...  

AbstractWe study the growth of InAs/AlxGa1-xAs/GaAs heterostructures as well as their structural and optical properties. Structurally coherent InAs islands with a narrow size distribution are found to be formed only in a very narrow range of InAs coverage. In striking contrast, the photoluminescence band in the 1.15–1.35 eV spectral range, which is commonly attributed to the emission from InAs quantum dots, is present for all of our structures, regardless the presence or absence of InAs islands and their strain state. Moreover, for constant InAs coverage this PL band follows not the Γ gap but the L gap of the AlxGa1-xAs barrier. This latter result is in disagreement with effective mass calculations for three-dimensionally confined excitons.


2005 ◽  
Vol 483 (1-2) ◽  
pp. 158-163 ◽  
Author(s):  
Z.M. Zhao ◽  
O. Hul'ko ◽  
H.J. Kim ◽  
J. Liu ◽  
B. Shi ◽  
...  

2010 ◽  
Vol 18 (3) ◽  
Author(s):  
S. Sengupta ◽  
S.Y. Shah ◽  
N. Halder ◽  
S. Chakrabarti

AbstractEpitaxially grown self-assembled InAs quantum dots (QDs) have found applications in optoelectronics. Efforts are being made to obtain efficient quantum-dot lasers operating at longer telecommunication wavelengths, specifically 1.3 μm and 1.55 μm. This requires narrow emission linewidth from the quantum dots at these wavelengths. In InAs/GaAs single layer quantum dot (SQD) structure, higher InAs monolayer coverage for the QDs gives rise to larger dots emitting at longer wavelengths but results in inhomogeneous dot-size distribution. The bilayer quantum dot (BQD) can be used as an alternative to SQDs, which can emit at longer wavelengths (1.229 μm at 8 K) with significantly narrow linewidth (∼16.7 meV). Here, we compare the properties of single layer and bilayer quantum dots grown with higher InAs monolayer coverage. In the BQD structure, only the top QD layer is covered with increased (3.2 ML) InAs monolayer coverage. The emission line width of our BQD sample is found to be insensitive towards post growth treatments.


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