Quantum Hall Effect without Chern Bands

Fuente: arXiv
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Autores principales: Michen, Benjamin, Budich, Jan Carl
Formato: Preprint
Publicado: 2025
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author Michen, Benjamin
Budich, Jan Carl
author_facet Michen, Benjamin
Budich, Jan Carl
contents The quantum Hall effect was originally observed in a two-dimensional electron gas forming Landau levels when exposed to a strong perpendicular magnetic field and was later generalized to Chern insulators without net magnetization. Here, further extending the realm of the quantum Hall effect, we report on the robust occurrence of an integer quantized transverse conductance at the onset of disorder in a microscopic lattice model, all bands of which are topologically trivial (zero Chern number). We attribute this phenomenon to the energetic separation of nonquantized Berry fluxes within those bands. Adding disorder then nudges the system into a quantum Hall phase from an extended critical regime obtained by placing the Fermi energy within a broad window inside a trivial band. This natural integer-rounding mechanism manifests as the mobility-gap-induced quantization of a nonuniversal Hall conductance. Our results are corroborated by numerical transport simulations and the analysis of two complementary topological markers.
format Preprint
id arxiv_https___arxiv_org_abs_2505_09677
institution arXiv
publishDate 2025
record_format arxiv
spellingShingle Quantum Hall Effect without Chern Bands
Michen, Benjamin
Budich, Jan Carl
Mesoscale and Nanoscale Physics
Disordered Systems and Neural Networks
Quantum Physics
The quantum Hall effect was originally observed in a two-dimensional electron gas forming Landau levels when exposed to a strong perpendicular magnetic field and was later generalized to Chern insulators without net magnetization. Here, further extending the realm of the quantum Hall effect, we report on the robust occurrence of an integer quantized transverse conductance at the onset of disorder in a microscopic lattice model, all bands of which are topologically trivial (zero Chern number). We attribute this phenomenon to the energetic separation of nonquantized Berry fluxes within those bands. Adding disorder then nudges the system into a quantum Hall phase from an extended critical regime obtained by placing the Fermi energy within a broad window inside a trivial band. This natural integer-rounding mechanism manifests as the mobility-gap-induced quantization of a nonuniversal Hall conductance. Our results are corroborated by numerical transport simulations and the analysis of two complementary topological markers.
title Quantum Hall Effect without Chern Bands
topic Mesoscale and Nanoscale Physics
Disordered Systems and Neural Networks
Quantum Physics
url https://arxiv.org/abs/2505.09677