1999
DOI: 10.1063/1.479985
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On the applicability of the classical nucleation theory in an Ising system

Abstract: Large-scale dynamic Monte Carlo simulations of a lattice gas on a 2000×2000 square lattice with a Glauber-type spin flip dynamics were performed. The results are discussed in the light of classical nucleation theory (CNT) which can be fully specified for the problem due to the availability of exact values for the interfacial energy of a large nucleus, known from the Onsager solution. Several alternative (field-theoretic or nonclassical) descriptions were also considered. Special attention was paid to the pre-e… Show more

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Cited by 77 publications
(56 citation statements)
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“…Because a non-square droplet cannot be accommodated perfectly on a square lattice, it is also useful to consider the orientationally-averaged effective droplet surface tension σ eff (T ) derived by Shneidman et al [25]:…”
Section: Results: 2d Simulationsmentioning
confidence: 99%
“…Because a non-square droplet cannot be accommodated perfectly on a square lattice, it is also useful to consider the orientationally-averaged effective droplet surface tension σ eff (T ) derived by Shneidman et al [25]:…”
Section: Results: 2d Simulationsmentioning
confidence: 99%
“…Nucleation pathway of Ising model in three-dimensional lattice has also been studied using transition path sampling approach [27]. In addition, Ising model has been frequently used to test the validity of classical nucleation theory (CNT) [28][29][30][31][32]. However, all these studies are limited to regular lattices in Euclidean space.…”
Section: Introductionmentioning
confidence: 99%
“…The Arp 2/3 protein complex imitates the shape of an unfavorable intermediate of the spontaneous actin nucleation process [22]. In contrast, in two-and three-dimensional systems-condensation of a gas [31], crystallization [30], or in the Ising model [45]-classical nucleation theory [56,11] predicts that a barrier to nucleation exists because clusters have unfavorable energies proportional to the surface area of the cluster (possibly due to interfacial tension or pressure differences with respect to the surrounding solution), and favorable energies proportional to the volume of the cluster. Because volume grows more quickly than surface area as clusters grow larger, a supersaturated regime exists where small clusters tend to melt, but above a critical size, cluster growth rather than melting is favored.…”
Section: Stages Of An Assembly Reaction During An Anneal Are Separatementioning
confidence: 99%