Half-Quantized Hall Metal and Marginal Metal in Disordered Magnetic Topological Insulators
Shi-Hao Bi, Bo Fu, Shun-Qing Shen

TL;DR
This paper demonstrates the robustness of the half-quantized Hall effect in disordered magnetic topological insulators and uncovers a novel marginal metallic phase with scale-invariant conductance properties, challenging traditional localization theories.
Contribution
It reveals the stability of the half-quantized Hall effect under disorder and identifies a new marginal metallic phase with unique scale-invariant properties in magnetic topological insulators.
Findings
Robustness of half-quantized Hall effect in weakly disordered systems.
Discovery of a marginal metallic phase with scale-invariant conductance.
Challenging of conventional localization theories by observed phenomena.
Abstract
A semimagnetic topological insulator -- a heterostructure combining a topological insulator with a ferromagnet -- exhibits a half-quantized Hall effect, characterized by a quantized Hall conductance of (where is the elementary charge and is the Planck constant), which reinforces the established understanding of topological phenomena in condensed matter physics. However, its stability in realistic, disordered systems remains poorly understood. Here, we demonstrate the robustness of the half-quantized Hall effect in weakly disordered systems, stemming from a single gapless Dirac cone of fermions and coexisting with weak antilocalization due to the Berry phase that suppresses backscattering. Furthermore, we uncover a marginal metallic phase emerging between weak antilocalization and Anderson insulation -- a transition that defies conventional…
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