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arXiv:2101.08799 · Annals of Physics

How spectrum-wide quantum criticality protects surface states of topological superconductors from Anderson localization: Quantum Hall plateau transitions (almost) all the way down

Jonas F. Karcher, Matthew S. Foster

Published Mar 20, 2021• 12 citations
arXivHTMLPDF
DOI
10.1016/j.aop.2021.168439

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Spectrum-Wide Quantum Criticality at the Surface of Class AIII Topological Phases: An “Energy Stack” of Integer Quantum Hall Plateau Transitions

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In the absence of spin-orbit coupling, the conventional dogma of Anderson localization asserts that all states localize in two dimensions, with a glaring exception: the quantum Hall plateau transition (QHPT).In that case, the localization length diverges and interference-induced quantum-critical spatial fluctuations appear at all length scales.Normally, QHPT states occur only at isolated energies; accessing them therefore requires fine-tuning of the electron density or magnetic field.In this paper we show that QHPT states can be realized throughout an energy continuum, i.e., as an "energy stack" of critical states wherein each state in the stack exhibits QHPT phenomenology.The stacking occurs without fine-tuning at the surface of a class AIII topological phase, where it is protected by U(1) and (anomalous) chiral or time-reversal symmetries.Spectrum-wide criticality is diagnosed by comparing numerics to universal results for the longitudinal Landauer conductance and wave function multifractality at the QHPT.Results are obtained from an effective 2D surface field theory and from a bulk 3D lattice model.We demonstrate that the stacking of quantum-critical QHPT states is a robust phenomenon that occurs for AIII topological phases with both odd and even winding numbers.The latter conclusion may have important implications for the still poorly understood logarithmic conformal field theory believed to describe the QHPT.

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We present numerical evidence that most two-dimensional surface states of a bulk topological superconductor (TSC) sit at an integer quantum Hall plateau transition. We study TSC surface states in class CI with quenched disorder. Low-energy (finite-energy) surface states were expected to be critically delocalized (Anderson localized). We confirm the low-energy picture, but find instead that finite-energy states are also delocalized, with universal statistics that are independent of the TSC winding number, and consistent with the spin quantum Hall plateau transition (percolation).

•Nov 10, 2017•0 citations
In the absence of spin-orbit coupling, the conventional dogma of Anderson localization asserts that all states localize in two dimensions, with a glaring exception: the quantum Hall plateau transition (QHPT).In that case, the localization length diverges and interference-induced quantum-critical spatial fluctuations appear at all length scales.Normally, QHPT states occur only at isolated energies; accessing them therefore requires fine-tuning of the electron density or magnetic field.In this paper we show that QHPT states can be realized throughout an energy continuum, i.e., as an "energy stack" of critical states wherein each state in the stack exhibits QHPT phenomenology.The stacking occurs without fine-tuning at the surface of a class AIII topological phase, where it is protected by U(1) and (anomalous) chiral or time-reversal symmetries.Spectrum-wide criticality is diagnosed by comparing numerics to universal results for the longitudinal Landauer conductance and wave function multifractality at the QHPT.Results are obtained from an effective 2D surface field theory and from a bulk 3D lattice model.We demonstrate that the stacking of quantum-critical QHPT states is a robust phenomenon that occurs for AIII topological phases with both odd and even winding numbers.The latter conclusion may have important implications for the still poorly understood logarithmic conformal field theory believed to describe the QHPT.
We present numerical evidence that most two-dimensional surface states of a bulk topological superconductor (TSC) sit at an integer quantum Hall plateau transition. We study TSC surface states in class CI with quenched disorder. Low-energy (finite-energy) surface states were expected to be critically delocalized (Anderson localized). We confirm the low-energy picture, but find instead that finite-energy states are also delocalized, with universal statistics that are independent of the TSC winding number, and consistent with the spin quantum Hall plateau transition (percolation).