TY - JOUR
T1 - Simulation of diffusion instability of a mercury atomic distribution in the cadmium-mercury-tellurium alloy
AU - Vasin, A. S.
AU - Vasilevsky, M. I.
PY - 2006/1
Y1 - 2006/1
N2 - The formation of inhomogeneities in CdxHg1-x Te alloys upon post-growth cooling or upon low-temperature annealing is simulated numerically. The mechanism of the formation of inhomogeneities is based on the diffusion instability in a system involving mercury atoms located at lattice sites, interstitial mercury atoms, and cation vacancies. It is revealed that, upon prolonged annealing of the CdxHg1-x Te alloys with a cadmium content x = 0.2 at a temperature of ∼200°C, the concentrations of mercury atoms at lattice sites, interstitial mercury atoms, and vacancies are characterized by an inhomogeneous nearly periodical distribution arising from a small fluctuation when the initial equilibrium concentration of interstitial mercury atoms exceeds a threshold value (∼3 × 1017 cm -3). The spatial and time scales of the concentration distribution are determined primarily by the equilibrium concentration of vacancies and do not depend on the type of fluctuation involved. The spatial period of the concentration distribution increases linearly from 0.01 to 3.00 μm as the equilibrium concentration of vacancies changes from 1019 to 10 14 cm-3. At lower concentrations of vacancies, the periodic structure is formed for a considerably longer time. © Pleiades Publishing, Inc., 2006.
AB - The formation of inhomogeneities in CdxHg1-x Te alloys upon post-growth cooling or upon low-temperature annealing is simulated numerically. The mechanism of the formation of inhomogeneities is based on the diffusion instability in a system involving mercury atoms located at lattice sites, interstitial mercury atoms, and cation vacancies. It is revealed that, upon prolonged annealing of the CdxHg1-x Te alloys with a cadmium content x = 0.2 at a temperature of ∼200°C, the concentrations of mercury atoms at lattice sites, interstitial mercury atoms, and vacancies are characterized by an inhomogeneous nearly periodical distribution arising from a small fluctuation when the initial equilibrium concentration of interstitial mercury atoms exceeds a threshold value (∼3 × 1017 cm -3). The spatial and time scales of the concentration distribution are determined primarily by the equilibrium concentration of vacancies and do not depend on the type of fluctuation involved. The spatial period of the concentration distribution increases linearly from 0.01 to 3.00 μm as the equilibrium concentration of vacancies changes from 1019 to 10 14 cm-3. At lower concentrations of vacancies, the periodic structure is formed for a considerably longer time. © Pleiades Publishing, Inc., 2006.
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U2 - 10.1134/S1063783406010082
DO - 10.1134/S1063783406010082
M3 - RGC 21 - Publication in refereed journal
SN - 1063-7834
VL - 48
SP - 37
EP - 41
JO - Physics of the Solid State
JF - Physics of the Solid State
IS - 1
ER -