2018
DOI: 10.1098/rspa.2017.0612
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Discrete-to-continuum modelling of weakly interacting incommensurate two-dimensional lattices

Abstract: In this paper, we derive a continuum variational model for a two-dimensional deformable lattice of atoms interacting with a two-dimensional rigid lattice. The starting point is a discrete atomistic model for the two lattices which are assumed to have slightly different lattice parameters and, possibly, a small relative rotation. This is a prototypical example of a three-dimensional system consisting of a graphene sheet suspended over a substrate. We use a discrete-to-continuum procedure to obtain the continuum… Show more

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Cited by 8 publications
(4 citation statements)
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“…This problem is also discussed in Ref. [74] using an analytic description of domain wall formation, but for rectangular domains.…”
Section: Classical Atomistic Simulationsmentioning
confidence: 99%
“…This problem is also discussed in Ref. [74] using an analytic description of domain wall formation, but for rectangular domains.…”
Section: Classical Atomistic Simulationsmentioning
confidence: 99%
“…The study of bilayer graphene has grown recently due to the discovery of superconductivity in low-temperature bilayer graphene with a small relative twist [3]. These twisted bilayer graphene systems form a large scale moiré pattern [12,13,23] that is incommensurate [11,14,18,21], or aperiodic, which has motivated the development of methods to overcome the theoretical and computational challenge posed by the lack of periodicity. Most current physics investigations overcome the lack of periodicity by utilizing the lowenergy approximation of Bistritzer and MacDonald [1,9] that restricts interlayer scattering to nearest neighbor reciprocal superlattice vectors.…”
Section: Introductionmentioning
confidence: 99%
“…Crystal relaxation in vdW heterostructures has been studied in the continuum limit by energy minimization [12][13][14][15][16][17][18] . In twisted bilayer graphene, for instance, relaxation enlarges the AB/BA stacking regions (the equilibrium stacking) and forms a thin domain line in between adjacent AB/BA stacking regions, while the AA stacking regions (high energy stacking order) shrink to localized spots.…”
Section: Introductionmentioning
confidence: 99%