Spin-1 Weyl Point and Surface Arc State in a Chiral Phononic Crystal
arXiv:2004.02412 · doi:10.1103/PhysRevB.101.214309
Abstract
Spin-1 Weyl point is formed by three bands touching at a single point in the three dimensional (3D) momentum space, with two of which show cone-like dispersion while the third band is flat. Such a triply degenerate point carries higher topological charge 2 and can be described by a three-band Hamiltonian. We first propose a tight-binding model of a 3D Lieb lattice with chiral interlayer coupling to form the Spin-1 Weyl point. Then we design a chiral phononic crystal that carries these spin-1 Weyl points and special straight-type acoustic Fermi arcs. We also computationally demonstrate the robust propagation of the topologically protected surface states that can travel around a corner or defect without reflection. Our results pave a new way to manipulate acoustic waves in 3D structures and provide a platform for exploring energy transport properties in 3D spin-1 Weyl systems.
References in corpus (9)
- Bulk Topological Invariants in Noninteracting Point Group Symmetric Insulators
- Multiple types of topological fermions in transition metal silicides
- Large Fermi Arcs in Unconventional Weyl Semimetal RhSi
- Discovery of topological chiral crystals with helicoid arc states
- New classes of chiral topological nodes with non-contractible surface Fermi arcs in CoSi
- Double-Weyl phonons in transition-metal monosilicides
- Do Linear Dispersions of Classical Waves Mean Dirac Cones?
- Emergent pseudospin-1 Maxwell fermions with a threefold degeneracy in optical lattices
- Double-zero-index structural waveguides