2012
DOI: 10.1063/1.4748312
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Integer quantum Hall effect in a lattice model revisited: Kubo formalism

Abstract: We investigate numerically the integer quantum Hall effect (IQHE) in a two-dimensional square lattice with non-interacting electrons in presence of disorder and subjected to uniform magnetic field in a direction perpendicular to the lattice plane. We employ nearest-neighbor tight-binding Hamiltonian to describe the system, and obtain the longitudinal and transverse conductivities using Kubo formalism. The interplay between the magnetic field and disorder is also discussed. Our analysis may be helpful in studyi… Show more

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Cited by 27 publications
(13 citation statements)
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“…In this case the system becomes periodic in the remaining spatial direction and one can use the Bloch decomposition with respect to that direction. Hence, the 2-dimensional Schrödinger equation can be reduced to a 1-dimensional Harper's like equation, which has been studied computationally by various techniques [15,16,36,63,51,62,56,57,32,35,17]. As such, the rigorous error bounds reported in this section (see Theorem 6.3) can still be of interest to numerical analysts.…”
Section: Approximating Algebras: First Roundmentioning
confidence: 98%
“…In this case the system becomes periodic in the remaining spatial direction and one can use the Bloch decomposition with respect to that direction. Hence, the 2-dimensional Schrödinger equation can be reduced to a 1-dimensional Harper's like equation, which has been studied computationally by various techniques [15,16,36,63,51,62,56,57,32,35,17]. As such, the rigorous error bounds reported in this section (see Theorem 6.3) can still be of interest to numerical analysts.…”
Section: Approximating Algebras: First Roundmentioning
confidence: 98%
“…The magnetic field is introduced as an phase factor 2π Bzya φo felt by an electron when moving along the x−direction, where φ o = h/e is the magnetic flux quantum. To keep the periodicity along the y-direction, the magnetic flux is chosen to be a rational number and commensurate with the width N y [28,29].…”
Section: Model Hamiltonianmentioning
confidence: 99%
“…It should be noted that, like a conventional disordered material, the localization of energy levels always starts from the band edges, keeping the extended states towards the band centre. This phenomenon has been revisited in our recent work in the context of studying integer quantum Hall effect 56 within a tight-binding framework. It reveals that, for large enough electric field almost all the energy levels get localized, and therefore, no such crossover between a conducting zone and an insulating phase is observed.…”
Section: Numerical Results and Discussionmentioning
confidence: 99%