Spectrum of the Dirac Hamiltonian with the mass-hedgehog in arbitrary dimension
arXiv:1010.0728 · doi:10.1103/PhysRevB.83.125412
Abstract
It is shown that the square of the Dirac Hamiltonian with the isotropic mass-hedgehog potential in d dimensions is the number operator of fictitious bosons and fermions over d quantum states. This result allows one to obtain the complete spectrum and degeneracies of the Dirac Hamiltonian with the hedgehog mass configuration in any dimension. The result pertains to low-energy states in the core of a general superconducting or insulating vortex in graphene in two dimensions, and in the superconducting vortex at the topological - trivial insulator interface in three dimensions, for example. The spectrum in d=2 is also understood in terms of the underlying accidental SU(2) symmetry and the supersymmetry of the Hamiltonian.
6 pages: typos corrected, new section on accidental supersymmetry, added references, many comments, and a figure. Published version
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- Supersymmetric Runge-Lenz-Pauli vector for Dirac vortex in topological insulators and graphene
- Zero modes of the generalized fermion-vortex system in magnetic field
- Dynamic zero modes of Dirac fermions and competing singlet phases of antiferromagnetic order
- Majorana bound state of a Bogoliubov-de Gennes-Dirac Hamiltonian in arbitrary dimensions
- Quantum Mechanical Hamiltonians with Large Ground-State Degeneracy
- Spectrum of the Vortex Bound States of the Dirac and Schrodinger Hamiltonian in the presence of Superconducting Gaps