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Use of polydispersity index as control parameter to study melting/freezing of Lennard-Jones system: Comparison among predictions of bifurcation theory with Lindemann criterion, inherent structure analysis and Hansen-Verlet rule

机译:使用多分散指数作为控制参数,以研究Lennard-Jones系统的熔化/冻结:利用Lindemann标准,固有结构分析和Hansen-Verlet规则的分叉理论预测比较

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摘要

Using polydispersity index as an additional order parameter we investigate freezing/melting transition of Lennard-Jones polydisperse systems (with Gaussian polydispersity in size), especially to gain insight into the origin of the terminal polydispersity. The average inherent structure (IS) energy and root mean square displacement (RMSD) of the solid before melting both exhibit quite similar polydispersity dependence including a discontinuity at solid-liquid transition point. Lindemann ratio, obtained from RMSD, is found to be dependent on temperature. At a given number density, there exists a value of polydispersity index (delta (P)) above which no crystalline solid is stable. This transition value of polydispersity(termed as transition polydispersity, delta (P) ) is found to depend strongly on temperature, a feature missed in hard sphere model systems. Additionally, for a particular temperature when number density is increased, delta (P) shifts to higher values. This temperature and number density dependent value of delta (P) saturates surprisingly to a value which is found to be nearly the same for all temperatures, known as terminal polydispersity (delta (TP)). This value (delta (TP) similar to 0.11) is in excellent agreement with the experimental value of 0.12, but differs from hard sphere transition where this limiting value is only 0.048. Terminal polydispersity (delta (TP)) thus has a quasiuniversal character. Interestingly, the bifurcation diagram obtained from non-linear integral equation theories of freezing seems to provide an explanation of the existence of unique terminal polydispersity in polydisperse systems. Global bond orientational order parameter is calculated to obtain further insights into mechanism for melting.
机译:使用多分散指数作为附加订单参数,我们调查Lennard-Jones PolyDisperse Systems的冷冻/熔化过渡(具有高斯多分散性的大小),特别是进入终端多分散性的起源。在熔化之前,固体的平均固有结构(IS)能量和均方根平均位移(RMSD)表现出非常相似的多分散性依赖性,包括固体液体过渡点处的不连续性。发现从RMSD获得的Lindemann比率依赖于温度。在给定数量的密度下,存在上述多分散性指数(Delta(P))的值,没有结晶固体是稳定的。发现多分散性的这种过渡值(称为转变多分散性,Delta(P))在强烈地依赖于温度,在硬球模型系统中错过了一个特征。另外,对于数量浓度增加时,对于特定温度,Delta(P)转移到更高的值。 δ(p)的该温度和数量密度依赖性值令人惊讶地饱和至发现与所有温度几乎相同的值,称为末端多分散物(Delta(TP))。该值(Delta(TP)类似于0.11),与实验值为0.12,但与硬球转换的不同之处在于该限制值仅为0.048。因此,终端多分散性(Delta(TP))具有Quasiununiversal特征。有趣的是,从冻结的非线性积分方程理论获得的分叉图似乎提供了对多分散系统中独特终端多分散性的存在的说明。计算全球债券取向顺序参数,以进一步了解熔化机制。

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