Stable Higher-Order Topological Dirac Semimetals with Monopole Charge in Alternating-twisted Multilayer Graphenes and beyond
arXiv:2312.15131 · doi:10.1103/PhysRevB.108.L241406
Abstract
We demonstrate that a class of stable monopole charge Dirac point (DP) phases can robustly exist in real materials, which surmounts the understanding: that is, a DP is unstable and generally considered to be only the critical point of a nodal line (NL) characterized by a monopole charge (the second Stiefel-Whitney number ) with space-time inversion symmetry but no spin-orbital coupling. For the first time, we explicitly reveal the higher-order bulk-boundary correspondence in the stable DP phase. We propose the alternating-twisted multilayer graphene, which can be regarded as 3D twisted bilayer graphene (TBG), as the first example to realize such stable DP phase and show that the Dirac points in the 3D TBG are essential degenerate at high symmetric points protected by crystal symmetries and carry a nontrivial monopole charge (), which results in higher-order hinge states along the entire Brillouin zone of the direction. By breaking some crystal symmetries or tailoring interlayer coupling we are able to access NL phases or other DP phases with hinge states of adjustable length. In addition, we present other 3D materials which host DPs in the electronic band structures and phonon spectra. We construct a minimal eight-band tight-binding lattice model that captures these nontrivial topological characters and furthermore tabulate all possible space groups to allow the existence of the stable DP phases, which will provide direct and strong guidance for the realization of the monopole semimetal phases in electronic materials, metamaterials and electrical circuits, etc.
arXiv commentPRB Letter, in press
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