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In topological mechanics, the identification of a mechanical system's rigidity matrix with an electronic tight-binding model allows to infer topological properties of the mechanical system, such as the occurrence of `floppy' boundary modes, from the associated electronic band structure.
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Cited in the paper.
More precisely, such a one-to-one identification is possible only for non-zero energy eigenstates
Cited in the paper.
For the common case of a uniform sign structure of the Majorana hopping terms, the intersite springs have negative
Cited in the paper.
Our model can also be considered to be a particularly simple balls and springs incarnation of “mechanical graphene”, which has been first put forward in Ref. \rev@citealpnum
Cited in the paper.
Note that for the system at hand, there are no gapless acoustic phonons, i.e. Goldstone modes arising from the spontaneous breaking of translational symmetry, since our system explicitly breaks this symmetry
Cited in the paper.
Note that any change to the intersite spring constant also requires a compensating change to the onsite spring constants
Cited in the paper.
2018
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V. Dwivedi, C. Hickey, T. Eschmann, and S. Trebst, “Majorana corner modes in a second-order Kitaev spin liquid,” Phys. Rev. B 98
2018
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