Duncan Peter D, Dennison Matthew, Masters Andrew J, Wilson Mark R
Department of Chemistry, University of Durham, South Road, Durham DH1 3LE, United Kingdom.
Phys Rev E Stat Nonlin Soft Matter Phys. 2009 Mar;79(3 Pt 1):031702. doi: 10.1103/PhysRevE.79.031702. Epub 2009 Mar 4.
The phase behavior of a system of hard-cut spheres has been studied using a high-order virial theory and by Monte Carlo simulation. The cut-sphere particles are disks of thickness L formed by symmetrically truncating the end caps of a sphere of diameter D . The virial theory predicts a stable nematic phase for aspect ratio LD=0.1 and a stable cubatic phase for LD=0.15-0.3 . The virial series converges rapidly on the equation of state of the isotropic and nematic phases, while for the cubatic phase the convergence is slower, but still gives good agreement with the simulation at high order. It is found that a high-order expansion (up to B8 ) is required to predict a stable cubatic phase for LD> or =0.15 , indicating the importance of many-body interactions in stabilizing this phase. Previous simulation work on this system has focused on aspect ratios LD=0.1 , 0.2, and 0.3. We expand this to include also LD=0.15 and 0.25, and we introduce a fourth-rank tensor to measure cubatic ordering. We have applied a multiparticle move which dramatically speeds the attainment of equilibrium in the nematic phase and therefore is of great benefit in the study of the isotropic-nematic phase transition. In agreement with the theory, our simulations confirm the stability of the nematic phase for LD=0.1 and the stability of the cubatic phase over the nematic for LD=0.15-0.3 . There is, however, some doubt about the stability of the cubatic phase with respect to the columnar. We have shown that the cubatic phase found on compression at LD=0.1 is definitely metastable, but the results for LD=0.2 were less conclusive.
已使用高阶维里理论并通过蒙特卡罗模拟研究了硬切割球体系统的相行为。切割球体粒子是厚度为L的圆盘,由对称截断直径为D的球体的端盖形成。维里理论预测,对于长径比L/D = 0.1,会出现稳定的向列相;对于L/D = 0.15 - 0.3,会出现稳定的立方相。维里级数在各向同性相和向列相的状态方程上收敛迅速,而对于立方相,收敛较慢,但在高阶时仍与模拟结果吻合良好。研究发现,对于L/D≥0.15,需要进行高阶展开(高达B8)才能预测出稳定的立方相,这表明多体相互作用在稳定该相方面的重要性。此前关于该系统的模拟工作主要集中在长径比L/D = 0.1、0.2和0.3上。我们将其扩展到包括L/D = 0.15和0.25,并引入了一个四阶张量来测量立方有序性。我们应用了一种多粒子移动方法,该方法极大地加快了向列相达到平衡的速度,因此对研究各向同性 - 向列相转变非常有益。与理论一致,我们的模拟证实了L/D = 0.1时向列相的稳定性以及L/D = 0.15 - 0.3时立方相相对于向列相的稳定性。然而,关于立方相相对于柱状相的稳定性存在一些疑问。我们已经表明,在L/D = 0.1时压缩得到的立方相肯定是亚稳的,但L/D = 0.2时的结果不太确定。