Photoninduced Weyl half-metal phase and spin filter effect from topological Dirac semimetals

TL;DR

This paper explores how circularly polarized light induces a novel Weyl half-metal phase in topological Dirac semimetals, enabling a highly tunable and robust spin filter effect with potential spintronics applications.

Contribution

It introduces the Weyl half-metal phase in Dirac semimetals under light irradiation and demonstrates a tunable, robust spin filter effect based on bulk properties.

Findings

Discovery of Weyl half-metal phase in DSMs under light

Spin-dependent Weyl node behavior constrained by topological charges

Robust, tunable spin filter effect demonstrated in junctions

Abstract

Recently discovered Dirac semimetals (DSMs) with two Dirac nodes, such as Na$_{3}$Bi and Cd$_{2}$As$_{3}$, are regarded to carry the $\mathbb{Z}_{2}$ topological charge in addition to the chiral charge. Here, we study the Floquet phase transition of $\mathbb{Z}_{2}$ topological DSMs subjected to a beam of circularly polarized light. Due to the resulting interplay of the chiral and $\mathbb{Z}_{2}$ charges, the Weyl nodes are not only chirality-dependent but also spin-dependent, which constrains the behaviors in creation and annihilation of the Weyl nodes in pair. Interestingly, we find a novel phase: One spinband is in Weyl semimetal phase while the other spinband is in insulator phase, and we dub it Weyl half-metal (WHM) phase. We further study the spin-dependent transport in a Dirac-Weyl semimetal junction and find a spin filter effect as a fingerprint of existence of the WHM phase. The proposed spin filter effect, based on the WHM bulk band, is highly tunable in a broad parameter regime and robust against magnetic disorder, which is expected to overcome the shortcomings of the previously proposed spin filter based on the topological edge/surface states. Our results offer a unique opportunity to explore the potential applications of topological DSMs in spintronics.