Evidence for Half-Quantized Chiral Edge Current in a C = 1/2 Parity Anomaly State
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A single massive Dirac surface band is predicted to exhibit a half-quantized Hall conductance, a hallmark of the C = 1/2 parity anomaly state in quantum field theory. Experimental signatures of the C = 1/2 parity anomaly state have been observed in semi-magnetic topological insulator (TI) bilayers, yet whether it supports a half-quantized chiral edge current remains elusive. Here, we observe a robust half-quantized Hall conductance plateau in a molecular beam epitaxy (MBE)-grown asymmetric magnetic TI trilayer under specific in-plane magnetic field regimes, corresponding to the C = 1/2 parity anomaly state. Within this state, both nonlocal and nonreciprocal transport signals are greatly enhanced, which we identify as direct evidence for a half-quantized chiral edge current localized at the boundary of the top gapped surface. Our numerical simulations demonstrate that this half-quantized chiral edge channel is the essential carrier of the observed half-quantized Hall conductance plateau, analogous to the quantized chiral edge channel in the C = 1 quantum anomalous Hall state. Our results provide experimental evidence for the half-quantized chiral edge transport in a C = 1/2 parity anomaly state. This work establishes asymmetric magnetic TI trilayers as a platform for probing single Dirac fermion physics and paves the way to explore a series of exciting phenomena in the C = 1/2 parity anomaly state, including the topological magnetoelectric effect and quantized magneto-optical response.
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Cited by 2 Pith papers
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Parity Anomalous Semimetal with Minimal Conductivity Induced by an In-Plane Magnetic Field
Realization of a parity anomalous semimetal with minimal conductivity of a single gapless Dirac cone in a magnetic topological sandwich induced by in-plane magnetic field, shown via two-stage conductivity tensor evolution.
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Absence of Parity Anomaly in Massive Dirac Fermions on a Lattice
Massive Dirac fermions on a lattice yield integer-quantized Hall conductivity; half-quantization appears only in the unphysical infinite-cutoff limit or for massless cones.
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