“…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].…”