Abstract:To describe the homogeneous nucleation process, an interfacial free energy adjustable phase-field crystal model (IPFC) was proposed by reconstructing the energy functional of the original phase field crystal (PFC) methodology. Compared with the original PFC model, the additional interface term in the IPFC model effectively can adjust the magnitude of the interfacial free energy, but does not affect the equilibrium phase diagram and the interfacial energy anisotropy. The IPFC model overcame the limitation that … Show more
“…Thus, the approach proposed in Ref. [36] cannot be directly considered within our framework. However, similar information is directly gathered from A 2 , which is a measure of the crystalline order, and from its variation in space.…”
Section: A Additional Energy Termmentioning
confidence: 99%
“…Within the range of β's used, a relative scaling factor of up to ∼ 1.6 can be achieved, and no restrictions are present for larger values. This can be used in order to match the solid-liquid interface energies from experiments or first-principles approaches, while they are typically underestimated in classical PFC methods [36]. Negative values of β, even small ones, lead to instabilities in the solid phase.…”
Section: Tuning the Solid-liquid Interfacial Energymentioning
confidence: 99%
“…An additional term in the free energy is considered, which is nonvanishing when the order of the solid phases changes. A similar approach has been recently proposed for the PFC model in order to include phase transition [35] and to introduce an adjustable interface energy [36]. Here we propose a suitable formulation to account for these effects in APFC models, exploiting an order parameter directly connected to the amplitude functions.…”
One of the major difficulties in employing phase field crystal (PFC) modeling and the associated amplitude (APFC) formulation is the ability to tune model parameters to match experimental quantities. In this work we address the problem of tuning the defect core and interface energies in the APFC formulation. We show that the addition of a single term to the free energy functional can be used to increase the solid-liquid interface and defect energies in a well-controlled fashion, without any major change to other features. The influence of the new term is explored in 2D triangular and honeycomb structures as well as bcc and fcc lattices in 3D. In addition, a Finite Element Method (FEM) is developed for the model that incorporates a mesh refinement scheme. The combination of FEM and mesh refinement to simulate amplitude expansion with a new energy term provides a method of controlling microscopic features such as defect and interface energies while simultaneously delivering a coarse-grained examination of the system.
“…Thus, the approach proposed in Ref. [36] cannot be directly considered within our framework. However, similar information is directly gathered from A 2 , which is a measure of the crystalline order, and from its variation in space.…”
Section: A Additional Energy Termmentioning
confidence: 99%
“…Within the range of β's used, a relative scaling factor of up to ∼ 1.6 can be achieved, and no restrictions are present for larger values. This can be used in order to match the solid-liquid interface energies from experiments or first-principles approaches, while they are typically underestimated in classical PFC methods [36]. Negative values of β, even small ones, lead to instabilities in the solid phase.…”
Section: Tuning the Solid-liquid Interfacial Energymentioning
confidence: 99%
“…An additional term in the free energy is considered, which is nonvanishing when the order of the solid phases changes. A similar approach has been recently proposed for the PFC model in order to include phase transition [35] and to introduce an adjustable interface energy [36]. Here we propose a suitable formulation to account for these effects in APFC models, exploiting an order parameter directly connected to the amplitude functions.…”
One of the major difficulties in employing phase field crystal (PFC) modeling and the associated amplitude (APFC) formulation is the ability to tune model parameters to match experimental quantities. In this work we address the problem of tuning the defect core and interface energies in the APFC formulation. We show that the addition of a single term to the free energy functional can be used to increase the solid-liquid interface and defect energies in a well-controlled fashion, without any major change to other features. The influence of the new term is explored in 2D triangular and honeycomb structures as well as bcc and fcc lattices in 3D. In addition, a Finite Element Method (FEM) is developed for the model that incorporates a mesh refinement scheme. The combination of FEM and mesh refinement to simulate amplitude expansion with a new energy term provides a method of controlling microscopic features such as defect and interface energies while simultaneously delivering a coarse-grained examination of the system.
“…MD calculations [33,35]. Alternatively, extra parameters [36] or even extra terms [37] can be added into the free energy of the model in order to exactly fit to the interface free energy; however, a careful attention must be devoted to not compromise the advantageous features of the model.…”
This work deals with the quantification and application of the modified two-mode phase-field crystal model (M2PFC; Asadi and Asle Zaeem, Comput. Mater. Sci. 105 (2015) 110-113) for face-centered cubic (FCC) metals at their melting point. The connection of M2PFC model to the classical density functional theory is explained in this article. M2PFC model in its dimensionless form contains three parameters (two independent and one dependent) which are determined using an iterative procedure based on the molecular dynamics and experimental data. The quantification process and computer simulations are performed for Ni and Al as two case studies. The quantitative M2PFC models are used in series of numerical simulations to determine the two-phase FCC-liquid coexisting and the bulk properties at the melting points of Ni and Al. The calculated and predicted properties are the expansion in melting, elastic constants, solidliquid interface free energy, and surface anisotropy, which are also compared with their available experimental or computational counterparts in the literature.
“…In this work we introduce spatially smoothed atomic density fields coupled to the atomic density fields n i that enables well-controlled phase separation and, therefore, facilitates modelling heterostructures and composite materials. Smoothed densities have been employed in PFC modelling recently for introducing a vapor phase 28 and arXiv:1908.05564v1 [cond-mat.mes-hall] 15 Aug 2019 for controlling liquid/solid interface energies 29 . Here we apply this modelling approach to 2D heterostructures composed of multiple elements.…”
Atomically thin 2-dimensional heterostructures are a promising, novel class of materials with groundbreaking properties. The possiblity of choosing the many constituent components and their proportions allows optimizing these materials to specific requirements. The wide adaptability comes with a cost of large parameter space making it hard to experimentally test all the possibilities. Instead, efficient computational modelling is needed. However, large range of relevant time and length scales related to physics of polycrystalline materials poses a challenge for computational studies. To this end, we present an efficient and flexible phase-field crystal model to describe the atomic configurations of multiple atomic species and phases coexisting in the same physical domain. We extensively benchmark the model for two-dimensional binary systems in terms of their elastic properties and phase boundary configurations and their energetics. As a concrete example, we demonstrate modelling lateral heterostructures of graphene and hexagonal boron nitride. We consider both idealized bicrystals and large-scale systems with random phase distributions. We find consistent relative elastic moduli and lattice constants, as well as realistic continuous interfaces and faceted crystal shapes. Zigzag-oriented interfaces are observed to display the lowest formation energy.
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