Selective lasing of InGaAs quantum-wire array on a V-grooved GaAs substrate by distributed optical feedback

1999 ◽  
Vol 11 (12) ◽  
pp. 1530-1532 ◽  
Author(s):  
T. Toda ◽  
F. Reinhardt ◽  
E. Martinet ◽  
E. Kapon ◽  
Y. Nakano
1991 ◽  
Vol 240 ◽  
Author(s):  
H. Kanbe ◽  
A. Chavez-Pirson ◽  
M. Kumagai ◽  
H. Saito ◽  
T. Fukui

ABSTRACTThe optical properties of a quantum wire array which was successfully realized in a 4-nm-thick (GaAs)1/2 (AlAs)1/2 fractional-layer superlattice (FLS) are described. The FLS sample was grown by metalorganic chemical vapor deposition on a (001) vicinal GaAs substrate tilted 2 ° towards [110]. The nominal cross sectional size of the GaAs wires is 4×4 nm. Optical anisotropy in absorption, refractive index and photoluminescence was clearly observed by polarization spectroscopy at room temperature as well as lower temperatures.


1997 ◽  
Vol 9 (1) ◽  
pp. 2-4 ◽  
Author(s):  
Tae-Geun Kim ◽  
Kyung-Hyun Park ◽  
Eun Kyu Kim ◽  
Suk-Ki Min ◽  
Jung-Ho Park

2002 ◽  
Vol 514 (1-3) ◽  
pp. 100-107 ◽  
Author(s):  
K. Yoo ◽  
S.J. Tang ◽  
P.T. Sprunger ◽  
I. Benito ◽  
J. Ortega ◽  
...  

2007 ◽  
Vol 76 (7) ◽  
pp. 074705 ◽  
Author(s):  
Hiroshi Tsukahara ◽  
Tsuneya Ando

1990 ◽  
Vol 209 ◽  
Author(s):  
D. M. Hwang ◽  
T. S. Ravi ◽  
R. Bhat ◽  
S. Simhony ◽  
C. Y. Chen ◽  
...  

ABSTRACTExtended regions of hexagonal zinc sulfide (wurtzite) structure are found to exist in AlGaAs grown by low-pressure OMCVD at 750°C. The specimen was prepared on a (001) GaAs substrate patterned with [110]-orientedV-grooves, intended for a quantum wire laser structure. A high density of planar faults was observed to originate in theAl0.66Ga0.34As cladding layers near the inner corners of the V-grooves and propagate towards the surface along the {111} planes. Many of these faults are stacking faults and microtwins. However, there also exhibit extended regions of hexagonal structure, revealed in electron diffraction patterns and high resolution lattice images. The hexagonal phase shares the same close-packed layers with the cubic phase, i.e., (0001)hexagonal // {111}cubic. The mechanism for the formation of hexagonal structure in this specimen is not yet fully understood.


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