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首页> 外文期刊>Physica status solidi, B. Basic research >Thermodynamic and mechanical stability of many-body systems interacting with coarse-grained bounded potentials
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Thermodynamic and mechanical stability of many-body systems interacting with coarse-grained bounded potentials

机译:多体系统与粗粒界电势相互作用的热力学和机械稳定性

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We discuss the stability criteria of Fisher and Ruelle [J. Math. Phys. 7, 260 (1966)] which can be used to establish if a given pair potential satisfies the requirements for thermodynamic stability. The mechanical and thermodynamic stability are considered for systems composed of particles interacting with a bounded potential, which could be used to model a mesostructured material at a coarse-grained level. The elastic moduli of fee and bee solids at zero temperature are calculated as a function of density for an assembly of particles interacting via the following (at r = 0) bounded potentials: (a) a Gaussian Core Model, GCM, potential, phi(r) = exp (-r(2)), and (b) the separation-shifted Lennard-Jones, SSLJ, bounded potential, phi(r)=4[1(alpha(2)+r(2))(6) - 1/(alpha(2) + r(2))3], with alpha > 0, where in both cases the characteristic energy and lengthscale are set to unity, and r is the separation between the particles. For both potential forms, at low densities, the static fee structure is the thermodynamically stable structural form but from above a certain density the bee lattice becomes the stable structure. It is shown that for the SSLJ potential this transition density varies roughly as similar to alpha(-3). In the T -> 0 limit, auxetic behaviour is demonstrated to occur for both fee and bee structures, but at high pressure and for the bee structural form its response to external strain can be entirely nonauxetic. A significant role of the attractive part of the interparticle interaction in enhancing auxetic behaviour is observed. The ranges of the mechanical stability are determined for both systems. At zero temperature, the lattice becomes mechanically unstable for alpha > alpha(c), which appears to coincide with the value alpha(c) = (7/32)(1/6) = 0.7762 proved previously to lead to thermodynamically unstable fluid states for this potential. (C) 2008 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim
机译:我们讨论了Fisher和Ruelle的稳定性标准[J.数学。物理[J.Am.Chem.Soc。,第7卷,第260页(1966)]可用于确定给定的对电位是否满足热力学稳定性的要求。对于由与有限电势相互作用的粒子组成的系统,应考虑其机械和热力学稳定性,该系统可用于在粗粒度水平上对介孔结构材料进行建模。计算通过以下(在r = 0)有界电势相互作用的粒子集合时,电荷和蜂固体在零温度下的弹性模量与密度的关系:(a)高斯核模型GCM,电势phi( r)= exp(-r(2)),并且(b)分离移位的Lennard-Jones,SSLJ,有界电势,phi(r)= 4 [1(alpha(2)+ r(2))(6 )-1 /(alpha(2)+ r(2))3],且alpha> 0,在这两种情况下,特征能量和长度尺度都设置为1,r是粒子之间的间隔。对于两种可能的形式,在低密度下,静电荷结构都是热力学稳定的结构形式,但是从一定密度以上,蜂巢变成稳定的结构。结果表明,对于SSLJ电位,该跃迁密度大致变化,类似于alpha(-3)。在T-> 0极限中,已证明蜂和蜂结构都发生了促生长行为,但是在高压和蜂结构形式下,其对外部应变的响应可能完全是非促生长的。观察到粒子间相互作用的吸引部分在增强促生长行为中的重要作用。确定了两个系统的机械稳定性范围。在零温度下,对于alpha> alpha(c),晶格会变得机械不稳定,这似乎与先前证明导致热力学不稳定流体状态的值alpha(c)=(7/32)(1/6)= 0.7762一致为这个潜力。 (C)2008 WILEY-VCH Verlag GmbH&Co.KGaA,Weinheim

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