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中间密度量子硬球系统中熔化-凝固转变的计算研究。I. 热力学结果。

Computational study of the melting-freezing transition in the quantum hard-sphere system for intermediate densities. I. Thermodynamic results.

作者信息

Sesé Luis M

机构信息

Departamento de Ciencias y Técnicas Fisicoquímicas, Facultad de Ciencias, Universidad Nacional de Educación a Distancia, Paseo Senda del Rey 9, 28040 Madrid, Spain.

出版信息

J Chem Phys. 2007 Apr 28;126(16):164508. doi: 10.1063/1.2718523.

Abstract

The points where the fluid-solid (face-centered-cubic) transition takes place in the quantum hard-sphere system, for reduced densities 0.85>rhoN*>0.5 (reduced de Broglie wavelengths lambdaB*<or=0.8), have been determined via calculations of Helmholtz free energies. A number of complementary methods have been utilized, namely, path-integral Monte Carlo simulations for fixing the basic thermodynamic and structural quantities, Ornstein-Zernike computations of the fluid isothermal compressibilities using the centroid correlations, and applications of the Einstein crystal technique. Attention is paid to the evaluation of the statistical uncertainties in the isothermal compressibilities and also to the quantum implementation of the Einstein crystal technique by including explicitly the constraint of fixed center of mass. The equation of state along the fluid lambdaB* branches studied has been determined with two methods, one based on the isothermal compressibilities and the other on the usual virial estimator. Along the solid lambdaB* branches the equation of state has been fixed with the virial estimator. The results indicate that the phase transition investigated is governed by entropic effects and that the fluid-solid coexistence densities are arranged along a straight line rhoFCC*=rho(rhoF*), a behavior which at least holds even for lambdaB*<2, as revealed by completing the present analysis with data available in the literature.

摘要

在量子硬球系统中,对于约化密度0.85>ρN*>0.5(约化德布罗意波长λB*≤0.8),通过亥姆霍兹自由能的计算确定了液 - 固(面心立方)转变发生的点。使用了多种互补方法,即路径积分蒙特卡罗模拟来确定基本的热力学和结构量,利用质心关联进行流体等温压缩率的奥恩斯坦 - 泽尔尼克计算,以及应用爱因斯坦晶体技术。关注了等温压缩率中统计不确定性的评估,并且通过明确包含质心固定的约束来实现爱因斯坦晶体技术的量子化。沿着所研究的流体λB分支的状态方程通过两种方法确定,一种基于等温压缩率,另一种基于通常的维里估计器。沿着固体λB分支,状态方程通过维里估计器确定。结果表明,所研究的相变受熵效应控制,并且液 - 固共存密度沿直线ρFCC* = ρ(ρF*)排列,正如通过用文献中的现有数据完成当前分析所揭示的,这种行为至少在λB*<2时仍然成立。

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