Chiral Phonons in a Cubic Lattice

We have developed a theory for the energy dispersion of chiral phonons in a simplest cubic lattice. Among all the phonon modes, only the optical triplet modes exhibit the intrinsic characteristics of chiral phonons near k=0, and we examine their energy splitting in detail by analyzing the dynamical matrix. To first order in k, the splitting is described by a spin-1 Weyl Hamiltonian, and helicity becomes a good quantum number. It asymptotically coincides with the crystal angular momentum for k parallel <111> up to a global sign. The Hamiltonian incorporates a pseudoscalar coupling constant associated with electric toroidal monopoles, determined by the spatial configuration of the stiffness tensors.