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硬方晶格气体的 Husimi 晶格解与相干反常方法分析

Husimi-lattice solutions and the coherent-anomaly-method analysis for hard-square lattice gases.

作者信息

Rodrigues Nathann T, Oliveira Tiago J

机构信息

Departamento de Física, Universidade Federal de Viçosa, 36570-900 Viçosa, MG, Brazil.

Instituto de Física and National Institute of Science and Technology for Complex Systems, Universidade Federal Fluminense, 24210-346 Niterói, Rio de Janeiro, Brazil.

出版信息

Phys Rev E. 2021 Mar;103(3-1):032153. doi: 10.1103/PhysRevE.103.032153.

DOI:10.1103/PhysRevE.103.032153
PMID:33862763
Abstract

Although lattice gases composed of particles preventing up to their kth nearest neighbors from being occupied (the kNN models) have been widely investigated in the literature, the location and the universality class of the fluid-columnar transition in the 2NN model on the square lattice are still a topic of debate. Here, we present grand-canonical solutions of this model on Husimi lattices built with diagonal square lattices, with 2L(L+1) sites, for L⩽7. The systematic sequence of mean-field solutions confirms the existence of a continuous transition in this system, and extrapolations of the critical chemical potential μ_{2,c}(L) and particle density ρ_{2,c}(L) to L→∞ yield estimates of these quantities in close agreement with previous results for the 2NN model on the square lattice. To confirm the reliability of this approach, we employ it also for the 1NN model, where very accurate estimates for the critical parameters μ_{1,c} and ρ_{1,c}-for the fluid-solid transition in this model on the square lattice-are found from extrapolations of data for L⩽6. The nonclassical critical exponents for these transitions are investigated through the coherent anomaly method (CAM), which in the 1NN case yields β and ν differing by at most 6% from the expected Ising exponents. For the 2NN model, the CAM analysis is somewhat inconclusive, because the exponents sensibly depend on the value of μ_{2,c} used to calculate them. Notwithstanding, our results suggest that β and ν are considerably larger than the Ashkin-Teller exponents reported in numerical studies of the 2NN system.

摘要

尽管文献中已对由阻止其第(k)个最近邻格点被占据的粒子组成的晶格气体((k)近邻模型)进行了广泛研究,但正方形晶格上二维近邻模型中流体 - 柱状转变的位置和普适类仍是一个有争议的话题。在此,我们给出该模型在由对角正方形晶格构建的胡西米晶格上的巨正则解,该晶格有(2L(L + 1))个格点,其中(L\leqslant7)。平均场解的系统序列证实了该系统中存在连续转变,并且将临界化学势(\mu_{2,c}(L))和粒子密度(\rho_{2,c}(L))外推到(L\rightarrow\infty)得到的这些量的估计值与正方形晶格上二维近邻模型的先前结果非常吻合。为了确认这种方法的可靠性,我们也将其用于一维近邻模型,通过对(L\leqslant6)的数据进行外推,得到了该模型在正方形晶格上流体 - 固体转变的临界参数(\mu_{1,c})和(\rho_{1,c})的非常精确的估计值。通过相干反常方法(CAM)研究了这些转变的非经典临界指数,在一维近邻模型的情况下,得到的(\beta)和(\nu)与预期的伊辛指数最多相差(6%)。对于二维近邻模型,CAM分析有些不确定,因为这些指数明显依赖于用于计算它们的(\mu_{2,c})值。尽管如此,我们的结果表明(\beta)和(\nu)比二维近邻系统数值研究中报道的阿什金 - 泰勒指数大得多。

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