2014
DOI: 10.1063/1.4886806
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Computer simulation study of surface wave dynamics at the crystal-melt interface

Abstract: We study, by means of computer simulations, the crystal-melt interface of three different systems: hard-spheres, Lennard Jones and the TIP4P/2005 water model. In particular, we focus on the dynamics of surface waves. We observe that the processes involved in the relaxation of surface waves are characterized by distinct time scales: a slow one related to the continuous recrystallization and melting, that is governed by capillary forces; and a fast one which we suggest to be due to a combination of processes tha… Show more

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Cited by 26 publications
(38 citation statements)
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“…From Fig. 5 we also see that the long-wavelength modes (small k n ) are insensitive to the choice of coarse-graining algorithm, as observed before in this type of analysis [42,43]. At intermediate values of k n the cluster algorithm is observed to follow the CFM prediction, Eq.…”
Section: Step Profile Determinationsupporting
confidence: 71%
“…From Fig. 5 we also see that the long-wavelength modes (small k n ) are insensitive to the choice of coarse-graining algorithm, as observed before in this type of analysis [42,43]. At intermediate values of k n the cluster algorithm is observed to follow the CFM prediction, Eq.…”
Section: Step Profile Determinationsupporting
confidence: 71%
“…When analyzing ice/water systems we follow the same procedure as in Ref. [75]. In this procedure we get rid of fluid-like molecules by making use of the order parameter and the biggest solid cluster is found.…”
Section: Methodsmentioning
confidence: 99%
“…1, where particles in the ice phase are shown in orange and particles in the liquid phase are shown in blue. Particles are labelled as ice or liquid-like based on local bond order parameters [17,18]. By knowing which particles belong to each phase, one can establish a discretized interface profile along the x direction, h(x n ) (in Ref.…”
Section: Methodsmentioning
confidence: 99%
“…By knowing which particles belong to each phase, one can establish a discretized interface profile along the x direction, h(x n ) (in Ref. [18] a detailed explanation of the way we establish h(x n ) is given). Then, h(x n ) is Fourier-transformed,…”
Section: Methodsmentioning
confidence: 99%