scholarly journals Oxygen self-diffusion in ThO2under pressure: connecting point defect parameters with bulk properties

2016 ◽  
Vol 3 (6) ◽  
pp. 065501 ◽  
Author(s):  
M W D Cooper ◽  
M E Fitzpatrick ◽  
L H Tsoukalas ◽  
A Chroneos
RSC Advances ◽  
2016 ◽  
Vol 6 (58) ◽  
pp. 53324-53330 ◽  
Author(s):  
V. Saltas ◽  
A. Chroneos ◽  
F. Vallianatos

GaAs diffusion is investigated with respect to temperature and pressure using a model that interconnects point defect with bulk properties.


2002 ◽  
Vol 717 ◽  
Author(s):  
Heidi Meyer ◽  
Scott T. Dunham

AbstractThe work investigates simple transient enhanced diffusion (TED) behavior, which is a reflection of the interstitial behavior in the system. The analysis shows that TED depends mainly on two factors: the intial demage profiles and the DICI product. We find that, based on these two inputs, the extent of TED can be accurately diffusion capacity (DICI) which is compared to values previously extracted from diffcusion and silicon self-diffusion experiments.


1993 ◽  
Vol 300 ◽  
Author(s):  
Teh Y. Tan ◽  
Homg-Ming You ◽  
Ulrich M. Gösele

ABSTRACTWe have calculated the thermal equilibrium concentrations of the various Ga vacancy species in GaAs. That of the triply-negatively-charged Ga vacancy, V3Ga has been emphasized, since it dominates Ga self-diffusion and Ga-Al interdiffusion under intrinsic and ndoping conditions, as well as the diffusion of Si donor atoms occupying Ga sites. Under strong n-doping conditions, the thermal equilibrium V3Ga concentration, CeqvGa.3−(n), has been found to exhibit a temperature independence or a negative temperature dependence, in the sense that the CeqvGa.3−(n) value is either unchanged or increases as the temperature is lowered. This is contrary to the normal positive temperature dependence of point defect theerqmal equilibrium concentrations, which decreases as the temperature is lowered. This CeqvGa.3−(n) property provides explanations to a number of outstanding experimental results, either requiring the interpretation thatV3−Ga has attained its thermal equilibrium concentration at the onset of each experiment, or requiring mechanisms involving point defect non-equilibrium phenomena. Furthermore, there exist also a few quantitative data which are in agreement with the presently calculated results.


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