2019
DOI: 10.3390/condmat4020039
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Quantized Alternate Current on Curved Graphene

Abstract: Based on the numerical solution of the quantum lattice Boltzmann method in curved space, we predict the onset of a quantized alternating current on curved graphene sheets. Such numerical prediction is verified analytically via a set of semi-classical equations relating the Berry curvature to real space curvature. The proposed quantised oscillating current on curved graphene could form the basis for the implementation of quantum information processing algorithms.

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Cited by 4 publications
(3 citation statements)
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“…It is also obvious that the undeformed Dirac equation is obtained in the limit a → 0. However, we underscore the fact that, experimentally, the deformation parameter a is greatly limited by an upper bound of the order of a < 10 −29 m [31]. Several effects can be investigated using this new Hamiltonian.…”
Section: The κ-Deformed Dirac Equationmentioning
confidence: 83%
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“…It is also obvious that the undeformed Dirac equation is obtained in the limit a → 0. However, we underscore the fact that, experimentally, the deformation parameter a is greatly limited by an upper bound of the order of a < 10 −29 m [31]. Several effects can be investigated using this new Hamiltonian.…”
Section: The κ-Deformed Dirac Equationmentioning
confidence: 83%
“…The calculation of x(t) for the more general case α = 0 is, however, straightforward and we shall proceed in this direction. In the Heisenberg picture, we have [31]: where H = −ασ z + ξσ x p x . To see the dependence on the deformation parameter more clearly, we focus now on the width of wave packets (∆x) 2 = x 2 − x 2 .…”
Section: Evolution Of Position In κ-Deformed Dirac Theorymentioning
confidence: 99%
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