# Spin-valley locking, bulk quantum Hall effect and chiral surface state in a noncentrosymmetric Dirac semimetal BaMnSb$_2$

## TL;DR

This paper reports the discovery of spin-valley locking, quantum Hall effect, and chiral surface states in the bulk Dirac semimetal BaMnSb$_2$, revealing novel topological and spin-valley coupled phenomena in a noncentrosymmetric material.

## Contribution

It demonstrates for the first time spin-valley locking and stacked quantum Hall effect in a bulk Dirac semimetal BaMnSb$_2$, combining experimental and theoretical analyses.

## Key findings

- Spin-valley locking observed in bulk BaMnSb$_2$
- Stacked quantum Hall effect with near-degenerate valley and spin states
- Two-dimensional chiral surface state indicating topological quantum liquid

## Abstract

Spin-valley locking in the band structure of monolayers of MoS$_2$ and other group-VI dichalcogenides has attracted enormous interest, since it offers potential for valleytronic and optoelectronic applications. Such an exotic electronic state has sparsely been seen in bulk materials. Here, we report spin-valley locking in a bulk Dirac semimetal BaMnSb$_2$. We find valley and spin are inherently coupled for both valence and conduction bands in this material. This is revealed by comprehensive studies using first principle calculations, tight-binding and effective model analyses, angle-resolved photoemission spectroscopy and quantum transport measurements. Moreover, this material also exhibits a stacked quantum Hall effect. The spin-valley degeneracy extracted from the plateau height of quantized Hall resistivity is close to 2. This result, together with the observed Landau level spin splitting, further confirms the spin-valley locking picture. In the extreme quantum limit, we have also observed a two-dimensional chiral metal at the side surface, which represents a novel topological quantum liquid. These findings establish BaMnSb$_2$ as a rare platform for exploring coupled spin and valley physics in bulk single crystals and accessing 3D interacting topological states.

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Source: https://tomesphere.com/paper/1907.06318