ChemInform Abstract: MOLECULAR STRUCTURE OF 1,2-BIS(TRIFLUOROMETHYL)DITHIETE BY VAPOR PHASE ELECTRON DIFFRACTION

1976 ◽  
Vol 7 (18) ◽  
pp. no-no
Author(s):  
J. LAWRENCE HENCHER ◽  
QUANG SHEN ◽  
DENNIS G. TUCK
1974 ◽  
Vol 52 (23) ◽  
pp. 3936-3940 ◽  
Author(s):  
Gerald Barbe ◽  
J. Lawrence Hencher ◽  
Quang Shen ◽  
Dennis G. Tuck

The molecular structure of trimethylindium has been redetermined by vapor phase electron diffraction. The independent structural parameters assuming three-fold axial symmetry based on the rg distances and their estimated uncertainties (2σ) are r(InC) = 209.3 ± 0.6 pm, r(CH) = 114 ± 3 pm, and < HCIn = 112.7 ± 0.8°. A slight nonplanarity (3.0 ± 2.5°) was attributed to a shrinkage effect in [Formula: see text] of 0.4 pm. The analysis was insensitive to the rotational position of the methyl groups relative to the InC3 frame. The root mean square amplitudes were not accurate due to a problem with the indium phase factor.


1976 ◽  
Vol 98 (4) ◽  
pp. 899-902 ◽  
Author(s):  
J. Lawrence Hencher ◽  
Quang Shen ◽  
Dennis G. Tuck

Author(s):  
S. McKernan ◽  
C. B. Carter ◽  
D. Bour ◽  
J. R. Shealy

The growth of ternary III-V semiconductors by organo-metallic vapor phase epitaxy (OMVPE) is widely practiced. It has been generally assumed that the resulting structure is the same as that of the corresponding binary semiconductors, but with the two different cation or anion species randomly distributed on their appropriate sublattice sites. Recently several different ternary semiconductors including AlxGa1-xAs, Gaxln-1-xAs and Gaxln1-xP1-6 have been observed in ordered states. A common feature of these ordered compounds is that they contain a relatively high density of defects. This is evident in electron diffraction patterns from these materials where streaks, which are typically parallel to the growth direction, are associated with the extra reflections arising from the ordering. However, where the (Ga,ln)P epilayer is reasonably well ordered the streaking is extremely faint, and the intensity of the ordered spot at 1/2(111) is much greater than that at 1/2(111). In these cases it is possible to image relatively clearly many of the defects found in the ordered structure.


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