Selective epitaxial growth of GaAs on Si with strained short-period superlattices by molecular beam epitaxy under atomic hydrogen irradiation

Author(s):  
Takuto Tsuji ◽  
Hiroo Yonezu ◽  
Naoki Ohshima



1992 ◽  
Vol 60-61 ◽  
pp. 553-558 ◽  
Author(s):  
R.K. Soni ◽  
H. Asahi ◽  
S. Emura ◽  
T. Watanabe ◽  
K. Asami ◽  
...  


1993 ◽  
Vol 325 ◽  
Author(s):  
X. C. Liu ◽  
S. Q. Gu ◽  
E. E. Reuter ◽  
S. G. Bishop ◽  
A. C. Chen ◽  
...  

AbstractSpontaneously laterally ordered (GaP)2/(InP)2 short period superlattices (SPS) grown by Molecular Beam Epitaxy (MBE) on nominal (100) GaAs substrates have been studied by photoluminescence (PL) spectroscopy. The samples studied included SPS comprising 110 pairs of (GaP)2/(InP)2 (total thickness σ90 nm) and multiquantum well structures in which quantum wells comprising 12 pairs of (GaP)2/(InP)2 SPS layers (thickness σ10 nm) are alternated with lattice-matched GaInP random alloy barrier layers. The 5K PL spectra include a σ1760 meV nearband edge band, and a much broader, lower energy (σ1670 meV) luminescence band that exhibits an unusual fatiguing behavior; its intensity diminishes monotonically during continuous illumination by the exciting light. This fatigued PL state is metastable at low temperatures. In the quantum well structure, although the relative intensity of the lower energy band is significantly weaker in comparison to the higher one, the fatiguing behavior still exists. However the fatiguing rate is slower in quantum well structures than that observed in the thick SPS film.



1991 ◽  
Vol 59 (14) ◽  
pp. 1735-1736 ◽  
Author(s):  
K. Aketagawa ◽  
T. Tatsumi ◽  
J. Sakai


1995 ◽  
Vol 399 ◽  
Author(s):  
M. Shima ◽  
L. Salamanca-Riba ◽  
G. Springholz ◽  
G. Bauer

ABSTRACTMolecular beam epitaxy was used to grow EuTe(x)/PbTe(y) short period superlattices with x=1-4 EuTe(111) monolayers alternating with y≈3x PbTe monolayers. The superlattices were characterized by transmission electron microscopy and high resolution x-ray diffraction. Regions with double periodicity were observed coexisting with areas of nominal periodicity. The sample with x=3.5 and y=9, for example, contains regions with double periodicity of x=7 and y=17. X-ray diffraction measurements confirm the formation of the double periodicity in these samples by the appearance of weak satellites in between the satellites of the nominal periodicity. The double periodicity in the superlattice is believed to result from interdiffusion during the growth. A model for this process is presented.





1998 ◽  
Vol 73 (13) ◽  
pp. 1844-1846 ◽  
Author(s):  
A. G. Norman ◽  
S. P. Ahrenkiel ◽  
H. Moutinho ◽  
M. M. Al-Jassim ◽  
A. Mascarenhas ◽  
...  


2010 ◽  
Vol 96 (2) ◽  
pp. 021904 ◽  
Author(s):  
E. Luna ◽  
B. Satpati ◽  
J. B. Rodriguez ◽  
A. N. Baranov ◽  
E. Tournié ◽  
...  


1987 ◽  
Vol 26 (Part 2, No. 7) ◽  
pp. L1174-L1176 ◽  
Author(s):  
Akihiko Okamoto ◽  
Keiichi Ohata


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