Predescu Cristian, Frantsuzov Pavel A, Mandelshtam Vladimir A
Chemistry Department, University of California at Berkeley, Berkeley, California 94720, USA.
J Chem Phys. 2005 Apr 15;122(15):154305. doi: 10.1063/1.1860331.
The equilibrium properties of classical Lennard-Jones (LJ38) versus quantum Ne38 Lennard-Jones clusters are investigated. The quantum simulations use both the path-integral Monte Carlo (PIMC) and the recently developed variational-Gaussian wave packet Monte Carlo (VGW-MC) methods. The PIMC and the classical MC simulations are implemented in the parallel tempering framework. The classical heat capacity Cv(T) curve agrees well with that of Neirotti et al. [J. Chem. Phys. 112, 10340 (2000)], although a much larger confining sphere is used in the present work. The classical Cv(T) shows a peak at about 6 K, interpreted as a solid-liquid transition, and a shoulder at approximately 4 K, attributed to a solid-solid transition involving structures from the global octahedral (Oh) minimum and the main icosahedral (C5v) minimum. The VGW method is used to locate and characterize the low energy states of Ne38, which are then further refined by PIMC calculations. Unlike the classical case, the ground state of Ne38 is a liquidlike structure. Among the several liquidlike states with energies below the two symmetric states (Oh and C5v), the lowest two exhibit strong delocalization over basins associated with at least two classical local minima. Because the symmetric structures do not play an essential role in the thermodynamics of Ne38, the quantum heat capacity is a featureless curve indicative of the absence of any structural transformations. Good agreement between the two methods, VGW and PIMC, is obtained. The present results are also consistent with the predictions by Calvo et al. [J. Chem. Phys. 114, 7312 (2001)] based on the quantum superposition method within the harmonic approximation. However, because of its approximate nature, the latter method leads to an incorrect assignment of the Ne38 ground state as well as to a significant underestimation of the heat capacity.
研究了经典的 Lennard-Jones(LJ38)与量子 Ne38 Lennard-Jones 团簇的平衡性质。量子模拟使用路径积分蒙特卡罗(PIMC)方法和最近开发的变分高斯波包蒙特卡罗(VGW-MC)方法。PIMC 和经典蒙特卡罗模拟在并行回火框架中实现。经典的热容 Cv(T)曲线与 Neirotti 等人[《化学物理杂志》112, 10340 (2000)]的曲线吻合良好,尽管在本工作中使用了大得多的限制球。经典的 Cv(T)在约 6 K 处出现一个峰值,被解释为固-液转变,在约 4 K 处出现一个肩部,归因于涉及来自全局八面体(Oh)最小值和主要二十面体(C5v)最小值结构的固-固转变。VGW 方法用于定位和表征 Ne38 的低能态,然后通过 PIMC 计算进一步优化。与经典情况不同,Ne38 的基态是类似液体的结构。在能量低于两个对称态(Oh 和 C5v)的几个类似液体的态中,最低的两个态在与至少两个经典局部最小值相关的盆地中表现出强烈的离域。由于对称结构在 Ne38 的热力学中不发挥重要作用,量子热容是一条无特征的曲线,表明没有任何结构转变。VGW 和 PIMC 这两种方法之间取得了良好的一致性。目前的结果也与 Calvo 等人[《化学物理杂志》114, 7312 (2001)]基于谐波近似内的量子叠加方法的预测一致。然而,由于其近似性质,后一种方法导致对 Ne38 基态的错误归属以及对热容的显著低估。