Lauri Antti, Zapadinsky Evgeni, Vehkamäki Hanna, Kulmala Markku
Department of Physical Sciences, University of Helsinki, Finland.
J Chem Phys. 2006 Oct 28;125(16):164712. doi: 10.1063/1.2358343.
We have performed Monte Carlo simulations of homogeneous and heterogeneous nucleations of Lennard-Jones argon clusters. The simulation results were interpreted using the major concept posing a difference between the homogeneous and heterogeneous classical nucleation theories-the contact parameter. Our results show that the multiplication concept of the classical heterogeneous nucleation theory describes the cluster-substrate interaction surprisingly well even for small molecular clusters. However, in the case of argon nucleating on a rigid monolayer of fcc(111) substrate at T=60 K, the argon-substrate atom interaction being approximately one-third as strong as the argon-argon interaction, the use of the classical theory concept results in an underestimation of the heterogeneous nucleation rate by two to three orders of magnitude even for large clusters. The main contribution to this discrepancy is induced by the failure of the classical theory of homogeneous nucleation to predict the energy involved in bringing one molecule from the vapor to the cluster for clusters containing less than approximately 15 molecules.
我们对 Lennard-Jones 氩团簇的均匀成核和非均匀成核进行了蒙特卡罗模拟。利用提出均匀成核理论和非均匀成核理论之间差异的主要概念——接触参数,对模拟结果进行了解释。我们的结果表明,经典非均匀成核理论的倍增概念即使对于小分子团簇,也能很好地描述团簇与衬底的相互作用。然而,在 T = 60 K 时氩在 fcc(111) 衬底的刚性单层上成核的情况下,氩与衬底原子的相互作用强度约为氩 - 氩相互作用的三分之一,即使对于大团簇,使用经典理论概念也会导致非均匀成核速率被低估两到三个数量级。这种差异的主要原因是,对于包含少于约 15 个分子的团簇,经典均匀成核理论未能预测将一个分子从气相带到团簇中所涉及的能量。