Abstract

New ideas for low-mass dark matter direct detection suggest that narrow band gap materials, such as Dirac semiconductors, are sensitive to the absorption of meV dark matter or the scattering of keV dark matter. Here we propose spin-orbit semiconductors - materials whose band gap arises due to spin-orbit coupling - as low-mass dark matter targets owing to their ~10 meV band gaps. We present three material families that are predicted to be spin-orbit semiconductors using Density Functional Theory (DFT), assess their electronic and topological features, and evaluate their use as low-mass dark matter targets. In particular, we find that that the tin pnictide compounds are especially suitable having a tunable range of meV-scale band gaps with anisotropic Fermi velocities allowing directional detection. Finally, we address the pitfalls in the DFT methods that must be considered in the ab initio prediction of narrow-gapped materials, including those close to the topological critical point.

Highlights

  • New models of dark matter (DM) offer the tantalizing possibility that direct detection is within the realms of short and modestly scaled experiments [1]

  • We report the trends in electronic structure with these substitutions and their effectiveness in tuning the band gap and sensitivity to various DM masses

  • CuInTe2, SrSn2As2, and Li6Bi2O7, predicted by density functional theory (DFT) to have band gaps induced by spin-orbit coupling interactions, were investigated for their electronic and topological properties

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Summary

Introduction

New models of dark matter (DM) offer the tantalizing possibility that direct detection is within the realms of short and modestly scaled experiments [1]. Recent models assigning DM mass to the sub-GeV range have incentivized the design of detection experiments that push the bounds of mass sensitivity. Semiconductors with meV-scale band gaps are suitable for the absorption of DM with meV mass and scattering of DM with keV mass due to the meV-magnitude kinetic energy. Semiconductors with ultranarrow band gaps are sought to maximize the reach of direct-detection experiments. Narrow band gap semiconductors are desired for infrared radiation detection, especially for sensitivity to long wavelengths [12].

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