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Study of atom diffusion in a lattice gas model with the non-additive lateral interactions

机译:具有非加性横向相互作用的晶格气体模型中原子扩散的研究

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The behavior of a system of atoms adsorbed on a square lattice is investigated by the Monte Carlo simulations using a lattice gas model with the non-additive lateral interactions between the atoms. Here I consider an approach to the problem of the non-addivity principally different from the approach supposed by Milchev and Binder [1,2]. In the new approach the system of adsorbed atoms is described by a set of electric dipoles. The interaction between the atoms is the dipole-dipole electrostatic repulsion. The non-additivity arises due to the dependence of the dipole moments on the number of atoms which are actually present in the close vicinity of these dipoles. I have derived the analytical expressions for the diffusion coefficients and obtained the coverage dependencies for the tracer, center-of-mass and Fickian diffusion coefficients using the Monte Carlo method. The non-addivity of the lateral interaction results in the instability of the atom distribution over the lattice, which substantially changes the thermodynamics of the atom system. Also, it strongly affects the diffusion of the adsorbed atoms.
机译:通过蒙特卡罗模拟,使用具有原子间非加性侧向相互作用的晶格气体模型,通过蒙特卡洛模拟研究了吸附在正方形晶格上的原子系统的行为。在这里,我考虑一种解决非可加性问题的方法,该方法主要不同于米尔切夫和宾德[1,2]提出的方法。在新方法中,吸附原子的系统由一组电偶极子描述。原子之间的相互作用是偶极-偶极静电排斥。非可加性的产生是由于偶极矩对这些偶极附近实际存在的原子数的依赖性。我已经得出了扩散系数的解析表达式,并使用蒙特卡洛方法获得了示踪剂,质心和菲克扩散系数的覆盖率依赖性。横向相互作用的非可加性导致原子在晶格上分布的不稳定性,这实质上改变了原子系统的热力学。而且,它强烈影响吸附原子的扩散。

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