2019
DOI: 10.1103/physrevb.100.140201
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Random network models with variable disorder of geometry

Abstract: Recently it was shown (I. A. Gruzberg, A. Klümper, W. Nuding and A. Sedrakyan, Phys. Rev. B 95, 125414 (2017)) that taking into account random positions of scattering nodes in the network model with U (1) phase disorder yields a localization length exponent 2.37 ± 0.011 for plateau transitions in the integer quantum Hall effect. This is in striking agreement with the experimental value of 2.38 ± 0.06. Randomness of the network was modeled by replacing standard scattering nodes of a regular network by pure tun… Show more

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Cited by 35 publications
(43 citation statements)
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References 54 publications
(89 reference statements)
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“…In the 1D limit a 2D magnet splits into a set of independent 1D magnets that are completely isolated from each other. For each 1D magnet the 1D Heisenberg model for spin-1/2 can be diagonalised exactly using Bethe ansatz [28] and the heat capacity can also be evaluated using this diagonalisation procedure without any approximation [29,30]. The exact result reproduces quite well the J /J = 0 curve in Fig.…”
Section: Thermodynamicsmentioning
confidence: 78%
See 1 more Smart Citation
“…In the 1D limit a 2D magnet splits into a set of independent 1D magnets that are completely isolated from each other. For each 1D magnet the 1D Heisenberg model for spin-1/2 can be diagonalised exactly using Bethe ansatz [28] and the heat capacity can also be evaluated using this diagonalisation procedure without any approximation [29,30]. The exact result reproduces quite well the J /J = 0 curve in Fig.…”
Section: Thermodynamicsmentioning
confidence: 78%
“…(26). The dash-dotted line is the result of Bethe ansatz from [30]. where u 1 ≡ u x and u 2 ≡ u y are now the variables in the orthogonal directions of the primitive vectors of the square lattice and V = (2π) 2 is the volume of the primitive cell in the reciprocal space of the square lattice.…”
Section: Square Latticementioning
confidence: 99%
“…The authors acknowledge helpful discussions with E Agliari, E Barkai, S Redner and A Gorsky, and also wish to thank the latter for pointing us on [38].…”
Section: Acknowledgmentsmentioning
confidence: 98%
“…[37]). A generalisation of a random Manhattan lattice was invoked as an example of a plausible geometric disorder in a recent analysis of the localisation length exponent for plateau transition in quantum Hall effect [38]. This latter setting, however, is clearly more complicated than the MdM model with the layered flows and the theoretical progress here is rather limited; the behaviour beyond the temporal evolution of a DA MSD is still largely unknown.…”
Section: Introductionmentioning
confidence: 99%
“…with Ω = J and the contribution c H of the isotropic Heisenberg model 16 . As can be clearly seen the Einstein phonons are dominant at high temperatures, in particular the constancy of the specific heat, as expected according to the Dulong-Petit rule, is visible.…”
Section: B Specific Heat Phonon Occupation Numbermentioning
confidence: 99%