2022
DOI: 10.1016/j.actamat.2021.117583
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Grain rotation and coupled grain boundary motion in two-dimensional binary hexagonal materials

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Cited by 13 publications
(8 citation statements)
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“…Among them the binary honeycomb phase, with each of its triangular sublattices occupied by A or B component separately, corresponds to the lattice structure of monolayer h-BN or the in-plane projection of trigonal prismatic 2H phase of MX 2 TMDs, while the phase with triangular A(B) and honeycomb B(A) sublattices is the in-plane version of octahedral 1T phase of TMDs. This PFC model has been used to identify and predict the defect structure, energy, and dynamics of h-BN grain boundaries [30,36], with results consistent with experiments and atomistic calculations (DFT or MD), and to examine graphene/h-BN and h-BN/h-BN heterostructures and bilayers [33,34] as well as thermal transport of h-BN monolayers [35]. It is important to note that the model can also be applied to a wider range of 2D compound materials with binary honeycomb lattice, including the atomically thin MX 2 TMDs of 2H phase (e.g., M = Mo, W, Nb, X = S, Se; MoTe 2 , TaS 2 ) and transition metal chalcogenides of 1H phase (e.g., FeSe) [37].…”
Section: Modelmentioning
confidence: 99%
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“…Among them the binary honeycomb phase, with each of its triangular sublattices occupied by A or B component separately, corresponds to the lattice structure of monolayer h-BN or the in-plane projection of trigonal prismatic 2H phase of MX 2 TMDs, while the phase with triangular A(B) and honeycomb B(A) sublattices is the in-plane version of octahedral 1T phase of TMDs. This PFC model has been used to identify and predict the defect structure, energy, and dynamics of h-BN grain boundaries [30,36], with results consistent with experiments and atomistic calculations (DFT or MD), and to examine graphene/h-BN and h-BN/h-BN heterostructures and bilayers [33,34] as well as thermal transport of h-BN monolayers [35]. It is important to note that the model can also be applied to a wider range of 2D compound materials with binary honeycomb lattice, including the atomically thin MX 2 TMDs of 2H phase (e.g., M = Mo, W, Nb, X = S, Se; MoTe 2 , TaS 2 ) and transition metal chalcogenides of 1H phase (e.g., FeSe) [37].…”
Section: Modelmentioning
confidence: 99%
“…A starting point of our modeling of 2D heterostructural growth is the understanding of individual grain growth dynamics, based on some basic mechanisms and outcomes revealed in the study of binary AB grains [30,36]. As shown in Fig.…”
Section: Heterostructures and Multijunctions Via Lateral Edge-epitaxymentioning
confidence: 99%
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“…[15,17] a binary PFC model with sublattice ordering was developed, and was used to examine various types of grain boundaries and defect core structures in hBN monolayers, with results shown to be in good agreement with experiments and other theoretical studies. These PFC models have been applied and extended to study various other structural and dynamical properties of 2D materials, such as grain rotation and coupled motion in graphene and hBN [18], g/hBN lateral heterostructures [19], and ternary 2D hexagonal materials and in-plane TMD/TMD heterostructures and multijunctions [20]. However, these models were strictly 2D and did not allow for out-of-plane variations.…”
Section: Introductionmentioning
confidence: 99%
“…[ 7 ] Grain rotation and grain boundary migration caused by plastic deformation are the main factors involved in grain growth in both 2D and 3D materials. [ 8 ] The nanotwin also plays a key role in changing local grain orientation and dissociating boundaries of nanograins, which helps the grain growth. [ 9 ] Apart from plastic deformation, grain coarsening assisted by thermal effects will be involved when rising to a certain temperature.…”
Section: Introductionmentioning
confidence: 99%