2020
DOI: 10.1103/physrevb.102.054304
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Dynamics of interacting particle systems: Modeling implications of the repulsive interactions and experiments on magnetic prototypes

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Cited by 6 publications
(2 citation statements)
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“…To mimic the weak inter-layer interactions, we can resort to pairs of magnets placed at corresponding lattice sites on adjacent layers. While magnets have been used in phononics applications, either as particles of discrete lattices [22], or as a tool to endow structural lattices with programmable nodal mass [23] or to promote multistability [24], their use as a source of inter-layer interaction is less charted. In principle, an arrangement of two structural layers featuring nodal interaction should fully capture the morphology and kinetics of a graphene bilayer.…”
mentioning
confidence: 99%
“…To mimic the weak inter-layer interactions, we can resort to pairs of magnets placed at corresponding lattice sites on adjacent layers. While magnets have been used in phononics applications, either as particles of discrete lattices [22], or as a tool to endow structural lattices with programmable nodal mass [23] or to promote multistability [24], their use as a source of inter-layer interaction is less charted. In principle, an arrangement of two structural layers featuring nodal interaction should fully capture the morphology and kinetics of a graphene bilayer.…”
mentioning
confidence: 99%
“…Each disk has two degrees of freedom in the x and y directions. The dispersion relation of the system can be calculated using Bloch's theorem [29] as: [−ω 2 M + K(κ)]φ = 0, where ω is the frequency, κ is the wavenumber, φ = [u v] T is the Bloch displacement vector in the x and y directions, M is the mass matrix, and K(κ) is the stiffness matrix [30], taking into consideration the static repulsive forces between the disks in the equilibrium configuration [31] (See Supp. Mat.).…”
mentioning
confidence: 99%