2017
DOI: 10.1103/physrevmaterials.1.060801
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Simulating complex crystal structures using the phase-field crystal model

Abstract: We introduce a phase-field crystal model that creates an array of complex three-and twodimensional crystal structures via a numerically tractable three-point correlation function. The three-point correlation function is designed in order to energetically favor the principal interplanar angles of a target crystal structure. This is achieved via an analysis performed by examining the crystal's structure factor. This approach successfully yields energetically stable simple cubic, diamond cubic, simple hexagonal, … Show more

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Cited by 19 publications
(13 citation statements)
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“…Finally, to model the hexagonal structures in three dimensions one should use the more complex form of the excessive energy term and also introduce higher modes to the pair-correlation functions of eight-order or 12-order approximations [16]. The general question here: is it enough to have a higher-order expansion pair-correlation function to describe hexagonal symmetries, or it is necessary to introduce three-point correlations even approximated as combinations of pair-correlation functions [47][48][49][50][51]?…”
Section: Results and Discussion (A) Dynamical Distributionmentioning
confidence: 99%
“…Finally, to model the hexagonal structures in three dimensions one should use the more complex form of the excessive energy term and also introduce higher modes to the pair-correlation functions of eight-order or 12-order approximations [16]. The general question here: is it enough to have a higher-order expansion pair-correlation function to describe hexagonal symmetries, or it is necessary to introduce three-point correlations even approximated as combinations of pair-correlation functions [47][48][49][50][51]?…”
Section: Results and Discussion (A) Dynamical Distributionmentioning
confidence: 99%
“…Formally, there is one peak representing the main Bragg reflection peak from a set of crystal planes; in practice, only the first few [smallest] kpeaks are retained (e.g., one for 2D HCP and 3D BCC, two for 2D squares and 3D FCC, three for 3D HPC 3D [37], etc). We can also expand to 3-point correlations following the recent work of Seymour et al [38][39][40] in order to extend the range of crystalline structures to non-metallic materials. It is noted that the use of higher order correlations typically requires that we go beyond 1-mode analysis of the free energy in order to retain the accuracy of simpler 1-mode approximations used for simpler structures.…”
Section: A a New Density Functional Approach: Expanding Around The Vmentioning
confidence: 99%
“…More importantly, the incorporation of multi-point correlations can enable the study of broader material systems and enrich the properties of the PFC modeling. Limited attempts have been made to explore the influence of multipoint correlations in PFC [35,[39][40][41][42]. For example, Seymour and Provatas [39] approximated the three-point direct correlation function as the product of two-point direct correlations to model structures with a specific bond angle, such as triangular, honeycomb, or square, and Kocher and Provatas [40] used both three-and four-point direct correlations to model vapor-liquid-solid transitions.…”
Section: Introductionmentioning
confidence: 99%
“…For example, Seymour and Provatas [39] approximated the three-point direct correlation function as the product of two-point direct correlations to model structures with a specific bond angle, such as triangular, honeycomb, or square, and Kocher and Provatas [40] used both three-and four-point direct correlations to model vapor-liquid-solid transitions. Alternatively, Alster et al [41] expanded the three-point correlation function in terms of Legen-dre polynomials in Fourier space and constructed various crystalline phases (including the ABX 3 perovskite structure) from their PFC model. Recently, we developed a general PFC formulation to incorporate any multipoint direct correlations satisfying the condition of rotational invariance [35], from which effects of bond-angle dependency and adjustment can be achieved through the four-point correlation, and a variety of 2D and 3D crystal structures, such as 3D diamond cubic phase and 2D rhombic or 3D simple monoclinic structure with tunable bond angles, can be stabilized.…”
Section: Introductionmentioning
confidence: 99%