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A Local Order Parameter-Based Method for Simulation of Free Energy Barriers in Crystal Nucleation

机译:基于本地秩序参数的晶体成核自由能屏障的方法

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While global order parameters have been widely used as reaction coordinates in nucleation and crystallization studies, their use in nucleation studies is claimed to have a serious drawback. In this work, a local order parameter is introduced as a local reaction coordinate to drive the simulation from the liquid phase to the solid phase and vice versa. This local order parameter holds information regarding the order in the first- and second-shell neighbors of a particle and has different well-defined values for local crystallites and disordered neighborhoods but is insensitive to the type of the crystal structure. The order parameter is employed in metadynamics simulations to calculate the solid liquid phase equilibria and free energy barrier to nucleation. Our results for repulsive soft spheres and the LennardJones potential, LJ(12-6), reveal better-resolved solid and liquid basins compared with the case in which a global order parameter is used. It is also shown that the configuration space is sampled more efficiently in the present method, allowing a more accurate calculation of the free energy barrier and the solid liquid interfacial free energy. Another feature of the present local order parameter-based method is that it is possible to apply the bias potential to regions of interest in the order parameter space, for example, on the largest nucleus in the case of nucleation studies. In the present scheme for metadynamics simulation of the nucleation in supercooled LJ(12-6) particles, unlike the cases in which global order parameters are employed, there is no need to have an estimate of the size of the critical nucleus and to refine the results with the results of umbrella sampling simulations. The barrier heights and the nucleation pathway obtained from this method agree very well with the results of former umbrella sampling simulations.
机译:虽然全局有序参数已被广泛用作成核和结晶研究中的反应坐标,但它们在成核研究中的使用据称有一个严重的缺点。在这项工作中,我们引入了一个局部序参数作为局部反应坐标,以驱动模拟从液相到固相,反之亦然。该局部有序参数包含有关粒子第一和第二壳层邻域中的有序度的信息,对于局部微晶和无序邻域具有不同的定义值,但对晶体结构的类型不敏感。为了计算固液相平衡和成核自由能垒,在亚动力学模拟中采用了序参量。我们对排斥软球和LennardJones势LJ(12-6)的结果显示,与使用全局序参数的情况相比,固体和液体盆地的分辨率更好。研究还表明,本方法能更有效地对组态空间进行采样,从而更准确地计算自由能垒和固液界面自由能。目前基于局部序参量的方法的另一个特点是,可以将偏压势应用于序参量空间中的感兴趣区域,例如,在成核研究的情况下,在最大的核上。在目前的过冷LJ(12-6)粒子成核的亚动力学模拟方案中,与采用全局序参数的情况不同,不需要对临界核的大小进行估计,也不需要使用伞式采样模拟的结果来改进结果。该方法得到的势垒高度和成核路径与以往伞式取样模拟的结果非常吻合。

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