Related Experiment Video
Updated: Sep 29, 2026

Advanced Experimental Methods for Low-temperature Magnetotransport Measurement of Novel Materials
Published on: January 21, 2016
Non-Hermitian topology from edge transport in Hermitian quantum anomalous Hall systems
Humian Zhou1, Ming Lu2, Chui-Zhen Chen3,4
1International Center for Quantum Materials, School of Physics, Peking University, Beijing, China.
Abstract:
Non-Hermitian physics, known for phenomena like exceptional points and the skin effect, has been most prominently realized in engineered systems relying on controlled gain and loss. Here we show that it can also arise naturally as an intrinsic transport response of a globally Hermitian quantum anomalous Hall system, without the need for external non-Hermitian engineering. We show that the interplay between unidirectional chiral edge modes and diffusive normal edge modes induces intrinsic non-reciprocal transport described by a continuum Hatano-Nelson model. Consequently, the non-Hermitian skin effect is encoded directly in experimentally accessible Hall-bar observables: the electrochemical potential and local heat dissipation acquire chirality-dependent exponential spatial profiles, while the longitudinal conductance decays exponentially with system size and the Hall conductance remains quantized. Using Landauer-Büttiker simulations, we confirm these transport signatures and identify magnetic topological insulators as a realistic platform for an intrinsic non-Hermitian transport response. Our results bridge non-Hermitian topology with mesoscopic transport, opening a pathway toward non-Hermitian topological devices in solid-state systems.
Related Concept Videos
The Hall Effect
Debye–Huckel–Onsager Conductance Equation
Reynolds Transport Theorem
The Pauli Exclusion Principle
Equipotential Surfaces and Conductors
Second Uniqueness Theorem
In contrast, consider that the electric field is non-unique and apply Gauss's law in divergence form in the region between the conductors and the integral form to the surface...
