Multiscale Modeling in Epitaxial Growth
DOI: 10.1007/3-7643-7343-1_1
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Lattice Gas Models and Kinetic Monte Carlo Simulations of Epitaxial Growth

Abstract: A brief introduction is given to Kinetic Monte Carlo (KMC) simulations of epitaxial crystal growth. Molecular Beam Epitaxy (MBE) serves as the prototype example for growth far from equilibrium. However, many of the aspects discussed here would carry over to other techniques as well. A variety of approaches to the modeling and simulation of epitaxial growth have been applied. They range from the detailed quantum mechanics treatment of microscopic processes to the coarse grained description in terms of stochasti… Show more

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Cited by 19 publications
(25 citation statements)
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“…In order to discuss detailed balance, we consider the behavior of our model in the absence of deposition and desorption 22 . Under such conditions, we assume the incorporation of an As atom from the surface of a droplet into the liquid bulk to be a rare event.…”
Section: B Detailed Balancementioning
confidence: 99%
“…In order to discuss detailed balance, we consider the behavior of our model in the absence of deposition and desorption 22 . Under such conditions, we assume the incorporation of an As atom from the surface of a droplet into the liquid bulk to be a rare event.…”
Section: B Detailed Balancementioning
confidence: 99%
“…The parameters of migration depend on the temperature. This surface migration can be modeled by many methods, for example Kinetic Monte-Carlo method [14,15]. In this paper, instead of this algorithm the dynamic viscosity of liquid gallium will be applied.…”
Section: The Mechanism Of the Atomic Displacementmentioning
confidence: 99%
“…This is achieved by forbidding any moves of atoms, which end up on top of a B atom. All atoms perform thermally activated hops to unoccupied nearest neighbor sites with Arrhenius rates k a = k 0a exp(−βE a (i → f )), (a = A, B), where β = 1/kT and E a (i → f ) denotes the barrier for a hop of an "a" particle from initial site i to final site f. This barrier consists of two contributions: a term, which counts the net number of bonds, which have to be broken by the move and an Ehrlich-Schwoebel (ES) barrier [10]. The former is given by…”
Section: Continuum Theory and Monte Carlo Modelmentioning
confidence: 99%