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Phase coexistence in confined Ising systems: a density matrix renormalization approach

机译:受限Ising系统中的相位共存:密度矩阵重归一化方法

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Using a density matrix renormalization approach we have calculated the phase diagram of a two-dimensional Ising model confined between two infinite walls, with opposing surface fields and a bulk field which grows linearly as a function of the distance from the walls and models the effect of gravity on a confined fluid. In the absence of gravity, two-phase coexistence is restricted to temperatures below the wetting temperature as pointed out by Parry acid Evans [A.O. Parry, R. Evans, Phys. Rev. Lett. 64, (1990) 439]. We find that the competing effects of gravity and surface fields restore the 'ordinary' finite size scaling to the bulk critical point, in agreement with previous mean-field results. We have calculated the exponents related to the shift toward the critical point in the limit L --> infinity, where L is the distance between the walls and we have found good agreement with previous scaling assumptions. Magnetization profiles calculated from a solid-on-solid Hamiltonian agree well with density matrix renormalization results for temperatures not too close to the bulk critical temperature. (C) 1998 Elsevier Science B.V. All rights reserved. [References: 15]
机译:使用密度矩阵重归一化方法,我们计算了二维伊辛模型的相位图,该模型限制在两个无限的壁之间,具有相对的表面场和体场,该场随与壁的距离而线性增长,并模拟了在封闭流体上的重力。在没有重力的情况下,两相共存仅限于低于润湿温度的温度,如Parry acid Evans所指出的。 Parry,R. Evans,物理学。莱特牧师64,(1990)439]。我们发现,重力和表面场的竞争效应将“普通”有限尺寸缩放恢复到了本体临界点,与之前的平均场结果一致。我们已经计算出了与极限L->无穷大内的临界点移动相关的指数,其中L是壁之间的距离,并且我们发现与先前的缩放假设非常吻合。对于不太接近整体临界温度的温度,从固体对固体哈密顿量计算出的磁化曲线与密度矩阵重新归一化结果非常吻合。 (C)1998 Elsevier Science B.V.保留所有权利。 [参考:15]

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