Departamento de Ciencias y Técnicas Fisicoquímicas, Facultad de Ciencias, Universidad Nacional de Educación a Distancia, Paseo Senda del Rey 9, 28040 Madrid, Spain.
J Chem Phys. 2013 Jul 28;139(4):044502. doi: 10.1063/1.4813635.
A path integral study of the fcc, hcp, and bcc quantum hard-sphere solids is presented. Ranges of densities within the interval of reduced de Broglie wavelengths 0.2≤λB(*)≤0.8 have been analyzed using Monte Carlo simulations with Cao-Berne propagator. Energies, pressures, and structural quantities (pair radial correlation functions, centroid structure factors, and Steinhardt order parameters) have been computed. Also, applications of the Einstein crystal technique [L. M. Sesé, J. Chem. Phys. 126, 164508 (2007)] have been made to compute the free energies of the fcc and hcp solids. Some technical points related to the latter technique are discussed, and it is shown that these calculations produce consistent results with increasing sample sizes. The fluid-solid (fcc and hcp) equilibria have been studied, thus completing prior work by this author on the fluid-fcc equilibrium. Within the accuracy attained no significant differences between the relative stabilities of the fcc and hcp lattices have been detected. The bcc case stands apart from the other two lattices, as the simulations lead either to irregular lattices (two types) that keep some traces of bcc-memory, or to spontaneous transitions to hcp-like lattices. The latter transitions make manifestly clear the potential repercussions that the quantum hard-sphere behavior can have on solid-solid equilibria at low temperatures in real systems (e.g., helium).
本文对 fcc、hcp 和 bcc 量子硬球固体进行了路径积分研究。利用 Cao-Berne 传播子的蒙特卡罗模拟分析了约化德布罗意波长 0.2≤λB(*)≤0.8 范围内的密度范围。计算了能量、压力和结构量(对径向关联函数、质心结构因子和 Steinhardt 序参量)。此外,还应用了爱因斯坦晶体技术[L. M. Sesé, J. Chem. Phys. 126, 164508 (2007)]来计算 fcc 和 hcp 固体的自由能。讨论了与后者技术相关的一些技术要点,并表明这些计算随着样本大小的增加会产生一致的结果。研究了流体-固体(fcc 和 hcp)平衡,从而完成了作者之前关于流体-fcc 平衡的工作。在达到的精度内,没有检测到 fcc 和 hcp 晶格相对稳定性之间的显著差异。bcc 情况与其他两个晶格不同,因为模拟导致不规则晶格(两种类型)保留了一些 bcc 记忆,或者自发转变为 hcp 样晶格。后一种转变清楚地表明了量子硬球行为在真实系统(例如氦)低温下对固-固平衡可能产生的潜在影响。