Gas‐source molecular beam epitaxy of wide‐band‐gap Zn1−xHgxSe (x=0–0.14)

1995 ◽  
Vol 66 (24) ◽  
pp. 3337-3339 ◽  
Author(s):  
K. Hara ◽  
H. Machimura ◽  
M. Usui ◽  
H. Munekata ◽  
H. Kukimoto ◽  
...  
2005 ◽  
Vol 86 (19) ◽  
pp. 192911 ◽  
Author(s):  
Hiroshi Tanaka ◽  
Shigeo Fujita ◽  
Shizuo Fujita

2001 ◽  
Vol 223 (4) ◽  
pp. 461-465 ◽  
Author(s):  
E. Tournié ◽  
F. Vigué ◽  
M. Laügt ◽  
J.-P. Faurie

2007 ◽  
Vol 42 (1-6) ◽  
pp. 129-133 ◽  
Author(s):  
A. El-Shaer ◽  
A. Bakin ◽  
M. Al-Suleiman ◽  
S. Ivanov ◽  
A. Che Mofor ◽  
...  

1995 ◽  
Vol 66 (25) ◽  
pp. 3462-3464 ◽  
Author(s):  
B. J. Wu ◽  
J. M. DePuydt ◽  
G. M. Haugen ◽  
G. E. Höfler ◽  
M. A. Haase ◽  
...  

1991 ◽  
Vol 59 (10) ◽  
pp. 1206-1208 ◽  
Author(s):  
Maria J. S. P. Brasil ◽  
Maria C. Tamargo ◽  
R. E. Nahory ◽  
H. L. Gilchrist ◽  
R. J. Martin

1996 ◽  
Vol 74 (S1) ◽  
pp. 104-107
Author(s):  
Z. Pang ◽  
P. Mascher ◽  
J. G. Simmons ◽  
D. A. Thompson

In our investigations, Au, Al, Ni, Pt, Ti, and combinations thereof were deposited on InP and InGaAs by e-beam evaporation to form Schottky contacts. The Schottky-barrier heights of these diodes determined by forward I–V and (or) reverse C–V measurements lie between 0.38–0.48 eV. To increase the Schottky-barrier height, a strained GaxIn1−xP layer was inserted between the electrode metal(s) and the semiconductor. This material, which has a band-gap larger than InP, was grown by gas-source molecular beam epitaxy. The Schottky-barrier heights, which generally depend on the gallium fraction, x, and the thickness of the strained GaxIn1−xP layer, increase and are in the range of 0.56–0.65 eV in different contact schemes.


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