Abstract

We study the effect of electron-phonon interactions on the electrical conductance of a helical edge state of a two-dimensional topological insulator. We show that the edge deformation caused by bulk acoustic phonons modifies the spin texture of the edge state, and that the resulting spin-phonon coupling leads to inelastic backscattering which makes the transport diffusive. Using a semiclassical Boltzmann equation we compute the electrical conductivity and show that it exhibits a metallic Bloch-Gr\"uneisen law. At temperatures on the order of the Debye temperature of the host material, spin-phonon scattering thus lowers the conductivity of the edge state drastically. Transport remains ballistic only for short enough edges, and in this case the correction to the quantized conductance vanishes as $\delta G \propto T^5$ at low temperatures. Relying only on parallel transport of the helical spin texture along the deformed edge, the coupling strength is determined by the host material's density and sound velocity. Our results impose fundamental limits for the finite-temperature conductivity of a helical edge channel.

Highlights

  • We study the effect of electron-phonon interactions on the electrical conductance of a helical edge state of a twodimensional topological insulator

  • Even at finite energies it remains true that the backscattering mechanisms which are most detrimental for the conductance of conventional 1D systems have a weaker effect in topological insulator edge channels

  • We will calculate the resistivity of the edge state as a function of temperature using the Boltzmann equation and find that its temperature dependence is given by a Bloch-Grüneisen law

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Summary

Introduction

We study the effect of electron-phonon interactions on the electrical conductance of a helical edge state of a twodimensional topological insulator. This has two reasons: First, we will show that the lattice deformations caused by phonons, in tandem with the helical spin texture of the electrons, give rise to “spin-phonon” coupling. We will move on to study the limit of long edges, where transport becomes diffusive due to spin-phonon coupling.

Results
Conclusion

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