Strain Effect in Polycrystalline Films of Indium Antimonide and Gallium Antimonide

Author(s):  
I. I. Fal’ko
Physica ◽  
1954 ◽  
Vol 20 (7-12) ◽  
pp. 1073-1076 ◽  
Author(s):  
R.G. Breckenridge ◽  
R.F. Blunt ◽  
W.R. Hosler ◽  
H.P.R. Frederikse ◽  
J.H. Becker ◽  
...  

Physica ◽  
1954 ◽  
Vol 3 (7-12) ◽  
pp. 1073-1076
Author(s):  
R BRECKENRIDGE ◽  
R BLUNT ◽  
W HOSLER ◽  
H FREDERIKSE ◽  
J BECKER ◽  
...  

2011 ◽  
Vol 1351 ◽  
Author(s):  
Takehiro Onishi ◽  
Andrew J. Lohn ◽  
Elane Coleman ◽  
Gary S. Tompa ◽  
Nobuhiko P. Kobayashi

ABSTRACTWe describe an ex-situ monitoring technique for a small amount (∼30 mono-layers) of erbium monoantimonide (ErSb) deposited on an indium antimonide (InSb) epitaxial layer prepared on InSb(100) substrates by metal organic chemical vapor deposition (MOCVD). Our objective is to improve thermoelectric properties of nanocomposites that employ nanometer size semi-metallic ErSb particles (ErSb nanoparticles) embedded in ternary group III-V compound semiconductor host materials such as indium gallium antimonide (InGaSb) and indium antimonide arsenide (InSbAs). The formation of ErSb nanoparticles embedded in a host material is spontaneous and needs to be carefully controlled to tune the size and volume density of the ErSb nanoparticles. We used an ex-situ monitoring technique based on glancing-angle infrared-absorption, reflection absorption infra-red spectroscopy (RAIRS), to study the formation of ErSb nanoparticles to correlate the amount of delivered ErSb and surface morphology of the surface of InSb covered with ErSb.


1973 ◽  
Vol 37 ◽  
pp. 639-649 ◽  
Author(s):  
H. Filler ◽  
C.K. So ◽  
R.C. Whited ◽  
B.J. Parsons

1957 ◽  
Vol 5 (5) ◽  
pp. 265-274 ◽  
Author(s):  
Fred H Eisen ◽  
C.Ernest Birchenall

Deformation under certain conditions causes twinning in silicon, germanium, gallium antimonide, indium antimonide and zinc blende which have the A 4 crystal structure. In material beneath hardness impressions formed at elevated temperatures a flow stress is superimposed upon hydrostatic compression; under these circumstances deformation twins form at temperatures between 0⋅44 and 0⋅74 of the absolute melting-points. Twins of the {111} type and, except in the case of zinc blende, of {123} type have been observed. Minor boundaries of thick growth twins may be {123} planes which also form boundary faces of etch pits. The only coherent interface possible between a {111} twin and matrix is a {111} plane; it is shown that among semi-coherent boundaries a {123} plane gives the best fit. The translational shears for twinning have been determined: for (111) twinning the shear is 0⋅4084 a in the [11 ¯ 2] direction with ( ¯ 110) as the shear plane; for (123) twinning the shear is 0⋅6552 a in [41 ¯ 2] direction with (1 ¯ 21) as the shear plane; where a is the parameter of the A 4 unit cell.


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