Orbital Magnetism of Bloch Electrons II. Application to Single-Band Models and Corrections to Landau-Peierls susceptibility
arXiv:1606.01632 · doi:10.7566/JPSJ.85.064709
Abstract
Orbital susceptibility for Bloch electrons is calculated for the first time up to the first order with respect to overlap integrals between the neighboring atomic orbitals, assuming single-band models. A general and rigorous theory of orbital susceptibility developed in the preceding paper is applied to single-band models in two-dimensional square and triangular lattices. In addition to the Landau-Peierls orbital susceptibility, it is found that there are comparable contributions from the Fermi surface and from the occupied states in the partially filled band called intraband atomic diamagnetism. This result means that the Peierls phase used in tight-binding models is insufficient as the effect of magnetic field.
28 pages, 4 figures
References in corpus (2)
Cited by in corpus (10)
- sparse-ir: optimal compression and sparse sampling of many-body propagators
- Orbital diamagnetic susceptibility in excitonic condensation phase
- Orbital Magnetism of Bloch Electrons III. Application to Graphene
- Orbital magnetization and anomalous Hall effect in interacting Weyl semimetals
- Theory of Orbital Susceptibility in the Tight-Binding Model: Corrections to the Peierls Phase
- Theory of Orbital Susceptibility on Excitonic Insulator
- Topological contribution to magnetism in the Kane-Mele model: An explicit wave function approach
- Lorentz Covariance of Dirac Electrons in Solids: Dielectric and Diamagnetic Properties
- Disentangling Orbital Magnetic Susceptibility with Wannier Functions
- Microscopic Theory of the Magnetic Susceptibility of Insulators