Growth and characteristics of InAsSb epilayers with a cutoff wavelength of 4.8 μm prepared by one-step liquid phase epitaxy

Rare Metals ◽  
2009 ◽  
Vol 28 (4) ◽  
pp. 313-316 ◽  
Author(s):  
Yuzhu Gao ◽  
Xiuying Gong ◽  
Weizheng Fang ◽  
Ishida Akihiro
1999 ◽  
Vol 587 ◽  
Author(s):  
H. Yokoi ◽  
T. Mizumoto

AbstractSelective area growth of magnetic garnet crystals was studied by liquid-phase epitaxy. The garnet layers grown on Ti-masked substrates were analyzed under a scanning electron microscope, and by X-ray diffraction measurements, energy-dispersive X-ray analysis and reflection high-energy electron diffraction. Narrow stripes in the Ti mask were designed to form waveguides by one-step growth. The light waves could be guided within the waveguide fabricated by selective area liquid-phase epitaxy.


Author(s):  
Guangwei Qu ◽  
Lizhong Hu ◽  
Xiuping Liang ◽  
Heqiu Zhang ◽  
Yu Zhao

1989 ◽  
Vol 161 ◽  
Author(s):  
Dipankar Chandra ◽  
Michael W. Goodwin

ABSTRACTA comprehensive study of all materials parameters influencing metal-insulator-semiconductor (MIS) properties of n-type HgCdTe films grown by liquid phase epitaxy from tellurium rich melts was conducted. When the epitaxy process was optimized to grow films free of inclusions and terracing, the first indications of the MIS properties to be expected could be obtained from the temperature dependence of the Hall electron mobility.Films displaying an anomalous dependence of the Hall mobility on temperature yielded non-classical low frequency MIS properties with little or no measurable ‘dark’ storage times (< 2×10−6 second). The MIS performance of these films appeared relatively independent of other materials parameters; remaining, for example, virtually unaffected by the film dislocation density changing between 5×104 and 2 × 106/cm2.Films displaying a classical dependence of the Hall mobility on temperature yielded drastically improved classical high frequency MIS properties. For these films, the MIS performance appeared almost exclusively dependent on dislocation density levels as long as the donor density remained lower than 1×1015/cm3. The dark storage time of classical films increased continuously with decreasing dislocation density levels, rising to 100µsec for a dislocation density level of 1 × 105/cm2 for materials with a 77°K cutoff wavelength of 10.5 µm. A simple monotonic relationship could be established between the MIS performance parameters and the dislocation density over the entire measurement span: from 5×104 to 2.5×106/cm2.


1989 ◽  
Vol 66 (5) ◽  
pp. 2225-2227 ◽  
Author(s):  
Guotong Du ◽  
Xiaoyu Ma ◽  
Zheng Zou ◽  
Xiaobo Zhang ◽  
Dingsan Gao

2004 ◽  
Vol 40 (4) ◽  
pp. 3045-3047 ◽  
Author(s):  
J.-H. Park ◽  
H. Takagi ◽  
J.-K. Cho ◽  
K. Nishimura ◽  
H. Uchida ◽  
...  

1987 ◽  
Vol 91 ◽  
Author(s):  
H.-P. Trah ◽  
M.I. Alonso ◽  
M. Konuma ◽  
E. Bauser ◽  
H. Cerva ◽  
...  

ABSTRACTSingle-crystal Si1−x Gex(O<×≲1) layers are grown by seeded growth on partially SiO2-masked Si-substrates, using a one-step liquid phase epitaxy (LPE) process. The seed regions are stripe- and hole-shaped windows in the oxide, having linear dimensions between 1.5 and 100 μm. The windows extend in different orientation on (111) and (100) orientated substrates. Lateral overgrowth over the oxide-masked areas is achieved up to 70 μm in <110>-directions. X-ray diffraction and Raman scattering show that the epitaxial islands are homogeneous and of excellent crystal quality. In the regions of lateral overgrowth the dislocation density is reduced considerably as shown by defect-etching and cross section transmission electron microscopy.


1979 ◽  
Vol 35 (6) ◽  
pp. 441-443 ◽  
Author(s):  
A. Doi ◽  
T. Fukuzawa ◽  
M. Nakamura ◽  
R. Ito ◽  
K. Aiki

Author(s):  
N.A. Bert ◽  
A.O. Kosogov

The very thin (<100 Å) InGaAsP layers were grown not only by molecular beam epitaxy and metal-organic chemical vapor deposition but recently also by simple liquid phase epitaxy (LPE) technique. Characterization of their thickness, interfase abruptness and lattice defects is important and requires TEM methods to be used.The samples were InGaAsP/InGaP double heterostructures grown on (111)A GaAs substrate. The exact growth conditions are described in Ref.1. The salient points are that the quarternary layers were being grown at 750°C during a fast movement of substrate and a convection caused in the melt by that movement was eliminated. TEM cross-section specimens were prepared by means of conventional procedure. The studies were conducted in EM 420T and JEM 4000EX instruments.The (200) dark-field cross-sectional imaging is the most appropriate TEM technique to distinguish between individual layers in 111-v semiconductor heterostructures.


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