Second Chern Number Protected Gapless Vortex Modes in Superconducting Weyl Semimetals

arXiv:2610.24401 · cond-mat.supr-con, cond-mat.mes-hall · Submitted 2026-10-17 · Read on arXiv

cond-mat.supr-con, cond-mat.mes-hall

Submitted: 2026-10-17

Updated: 2026-10-17

Comments: main text: 6 pages, 4 figuers; supplemental materials: 6 pages, 2 figures

License: http://creativecommons.org/licenses/by/4.0/

The gist: We have studied the vortex bound states of superconducting linear and quadratic Weyl semimetals with time reversal symmetry.

Terminology

Abstract

We have studied the vortex bound states of superconducting linear and quadratic Weyl semimetals with time reversal symmetry. For vortex with vorticity n (vortex line along z direction) and Weyl semimetals with Weyl point chirality χ, there are nχ gapless vortex modes around the location of each Weyl point in superconducting Weyl semimetals. We show that the appearance of nχ gapless vortex modes originates from the imbalanced pumping of flux bound states between Chern insulators obtained at k z and-k z in Weyl semimetals. Such a physical picture is verified by numerical calculations on lattice models. Moreover, the gapless modes around each Weyl point can be characterized by the second Chern number defined in a synthetic four-dimensional space based on the effective BdG Hamiltonian. Finally, these gapless vortex modes are found to be robust against rotational symmetry-breaking terms.

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