Ga(As,P) strained-layer superlattices: A ternary semiconductor with independently adjustable band gap and lattice constant

Author(s):  
P. L. Gourley
1989 ◽  
Author(s):  
H. Okumura ◽  
K. Miki ◽  
S. Misawa ◽  
K. Sakamoto ◽  
T. Sakamoto ◽  
...  

1985 ◽  
Vol 47 (5) ◽  
pp. 492-494 ◽  
Author(s):  
E. D. Jones ◽  
H. Ackermann ◽  
J. E. Schirber ◽  
T. J. Drummond ◽  
L. R. Dawson ◽  
...  

Author(s):  
S. Chadda ◽  
A. K. Datye ◽  
L. R. Dawson

III-V alloy devices are being considered for applications as infrared detectors, by several research groups due to processing advantages over II-VI alloy devices. InAs0.4Sb0.6 has the lowest band gap at 77 K among all III-V compounds, which corresponds to a cut off wavelength of 9 μm. The use of strained layer superlattices (SLS) was first proposed by Osbourn for lowering the band gap and achieving absorption at wavelengths greater than 12 μm at 77 K. A schematic diagram of the device is shown in figure 1. It was grown by Molecular Beam Epitaxy (MBE) at 425 °C and it consists of a p-n junction embedded in a InAs0.15Sb0.85/InSb SLS with layers of equal (110 Å) thickness. The n and p type dopants were S (PbS) and Be respectively. The active device SLS was grown on a composition graded strain relief buffer on the (100) face of an InSb substrate. The samples were sliced, thinned, polished, dimpled and ion milled for making cross-section Transmission Electron Microscope (TEM) samples.


1987 ◽  
Vol 48 (C5) ◽  
pp. C5-321-C5-327 ◽  
Author(s):  
H. BRUGGER ◽  
G. ABSTREITER

2007 ◽  
Vol 91 (4) ◽  
pp. 043514 ◽  
Author(s):  
J. B. Rodriguez ◽  
E. Plis ◽  
G. Bishop ◽  
Y. D. Sharma ◽  
H. Kim ◽  
...  

1998 ◽  
Vol 184-185 ◽  
pp. 728-731 ◽  
Author(s):  
I.V. Bradley ◽  
J.P. Creasey ◽  
K.P. O'Donnell

1987 ◽  
Vol 103 ◽  
Author(s):  
William C. Johnson

ABSTRACTUsing recent results from the thermodynamics of stressed solids, two-phase coexistence in a simple binary strained-layer superlattice is examined. We show that for a given temperature and overall composition of the superlattice, there can exist more than one linearly stable, equilibrium thermodynamic state. That is, there may exist several combinations of relative thickness of the phases and corresponding phase compositions that minimize the free energy of the system. The equilibrium state observed experimentally can, therefore, be influenced by the processing path.


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