Incorporation of rare earths into II-VI compounds during MBE growth: Optical and EXAFS studies of Sm-doped ZnTe

1998 ◽  
Vol 184-185 (1-2) ◽  
pp. 119-123
Author(s):  
D Wruck
Keyword(s):  
1998 ◽  
Vol 184-185 ◽  
pp. 119-123 ◽  
Author(s):  
D. Wruck ◽  
R. Boyn ◽  
L. Parthier ◽  
F. Henneberger
Keyword(s):  

Author(s):  
R. Rajesh ◽  
R. Droopad ◽  
C. H. Kuo ◽  
R. W. Carpenter ◽  
G. N. Maracas

Knowledge of material pseudodielectric functions at MBE growth temperatures is essential for achieving in-situ, real time growth control. This allows us to accurately monitor and control thicknesses of the layers during growth. Undesired effusion cell temperature fluctuations during growth can thus be compensated for in real-time by spectroscopic ellipsometry. The accuracy in determining pseudodielectric functions is increased if one does not require applying a structure model to correct for the presence of an unknown surface layer such as a native oxide. Performing these measurements in an MBE reactor on as-grown material gives us this advantage. Thus, a simple three phase model (vacuum/thin film/substrate) can be used to obtain thin film data without uncertainties arising from a surface oxide layer of unknown composition and temperature dependence.In this study, we obtain the pseudodielectric functions of MBE-grown AlAs from growth temperature (650°C) to room temperature (30°C). The profile of the wavelength-dependent function from the ellipsometry data indicated a rough surface after growth of 0.5 μm of AlAs at a substrate temperature of 600°C, which is typical for MBE-growth of GaAs.


Author(s):  
C. Vannuffel ◽  
C. Schiller ◽  
J. P. Chevalier

Recently, interest has focused on the epitaxy of GaAs on Si as a promising material for electronic applications, potentially for integration of optoelectronic devices on silicon wafers. The essential problem concerns the 4% misfit between the two materials, and this must be accommodated by a network of interfacial dislocations with the lowest number of threading dislocations. It is thus important to understand the detailed mechanism of the formation of this network, in order to eventually reduce the dislocation density at the top of the layers.MOVPE growth is carried out on slightly misoriented, (3.5°) from (001) towards , Si substrates. Here we report on the effect of this misorientation on the interfacial defects, at a very early stage of growth. Only the first stage, of the well-known two step growth process, is thus considered. Previously, we showed that full substrate coverage occured for GaAs thicknesses of 5 nm in contrast to MBE growth, where substantially greater thicknesses are required.


1998 ◽  
Vol 184-185 (1-2) ◽  
pp. 66-69 ◽  
Author(s):  
K Takahashi
Keyword(s):  

1971 ◽  
Vol 32 (C1) ◽  
pp. C1-179-C1-185 ◽  
Author(s):  
S. CHIKAZUMI ◽  
K. TAJIMA ◽  
K. TOYAMA
Keyword(s):  

1979 ◽  
Vol 40 (C5) ◽  
pp. C5-17-C5-18
Author(s):  
M. de Jong ◽  
P. Touborg ◽  
J. Bijvoet

1988 ◽  
Vol 49 (C8) ◽  
pp. C8-511-C2-512 ◽  
Author(s):  
E. Gratz ◽  
E. Bauer ◽  
S. Pöllinger ◽  
H. Nowotny ◽  
A. T. Burkov ◽  
...  

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