Spin Weyl Topological Insulators

Abstract

The quantum nature of electron spin is crucial for establishing topological invariants in real materials. Since the spin does not in general commute with the Hamiltonian, some of the topological features of the material can be extracted from its study. In insulating materials, the spin operator induces a projected operator on valence states called the spin valence operator. Its spectrum contains information with regard to the different phases of the spin Chern class. If the spin valence spectrum is gapped, the spin Chern numbers are constant along parallel planes thus defining spin Chern insulating materials. If the spin valence spectrum is not gapped, the changes in the spin Chern numbers occur whenever this spectrum is zero. Materials whose spin valence spectrum is gapless will be denoted spin Weyl topological insulators and their definition together with some of their properties will be presented in this work. The classification of materials from the properties of the spin valence operator provides a characterization that complements the existing list of topological invariants.

12 pages, 6 figures

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Cited by in corpus (3)

• Spin Chern number in altermagnets
• Model Hamiltonian for Altermagnetic Topological Insulators
• Tuning the Topological Properties of the Antiferromagnetic V(Bi${}_{1-x}$Sb${}_x$)${}_2$Te${}_4$ via Sb concentration