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arXiv 1903.08306cond-mat.stat-mech
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二维缔合格子气的有序-无序转变

Order-disorder transition in a two-dimensional associating lattice gas

A. P. Furlan, Tiago J. Oliveira, Jürgen F. Stilck, Ronald Dickman

摘要:

利用蒙特卡罗模拟和Husimi晶格上的解研究了缔合格子气(ALG)。在该模型中,分子具有取向自由度,相互作用依赖于最近邻分子的相对取向。我们专注于高密度液体(HDL)相和各向同性的气相之间的过渡,在充分占用的限制($μ\to \infty$)。模拟结果表明,连续相变在$τ_c=k_BT_c/γ=0.4763(1)$(其中$-γ$是键能)之间的低温HDL相,与非零的平均取向的分子,和高温各向同性相。临界指数和Binder累积量的结果表明,过渡属于三态Potts模型普适类,即使ALG哈密顿量不具有完全的排列对称性的Potts模型。与模拟结果相比,Husimi晶格结果提供了一个不连续的相变,其特征在于由一个不连续的的有序参数。转变温度(分别为用三角形和六边形构建的树的$τ_c=0.51403$和$0.51207$)略高于通过模拟发现的转变温度。由于Husimi晶格研究表明,ALG相图的特点是不连续的气体HDL线有限$μ$,三种可能的情况出现。第一个是在极限$μ\to \infty$中,一阶线终止于临界点;第二个是在某个有限化学势处,相变的性质发生了变化;第三个是整条线都是连续的相变。从其他ALG模型的结果和事实,即平均场近似显示一个不连续的相变的三态波茨模型(已知具有连续的过渡)借给一些重量的第三种选择。

英文摘要:

We study an associating lattice gas (ALG) using Monte Carlo simulation and solutions on Husimi lattices. In this model, the molecules have an orientational degree of freedom and the interactions depend on the relative orientations of nearest-neighbor molecules. We focus on the transition between the high-density liquid (HDL) phase and the isotropic gas phase in the limit of full occupancy ($μ\to \infty$). Simulation results show a continuous phase transition at $τ_c=k_BT_c/γ=0.4763(1)$ (where $-γ$ is the bond energy) between the low-temperature HDL phase, with a non-vanishing mean orientation of the molecules, and the high-temperature isotropic phase. Results for critical exponents and the Binder cumulant indicate that the transition belongs to the three-state Potts model universality class, even though the ALG Hamiltonian does not have the full permutation symmetry of the Potts model. In contrast with simulation, the Husimi lattice results furnish a discontinuous phase transition, characterized by a discontinuity of the nematic order parameter. The transition temperatures ($τ_c=0.51403$ and $0.51207$ for trees built with triangles and hexagons, respectively) are slightly higher than the one found via simulation. Since the Husimi lattice studies show that the ALG phase diagram features a discontinuous gas-HDL line for finite $μ$, three possible scenarios arise. The first is that in the limit $μ\to \infty$ the first-order line ends in a critical point; the second is a change in the nature of the transition at some finite chemical potential; the third is that the entire line is one of continuous phase transitions. Results from other ALG models and the fact that mean-field approximations show a discontinuous phase transition for the three-state Potts model (known to possess a continuous transition) lends some weight to the third alternative.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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