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Orbital susceptibility for Bloch electrons is calculated for the first timeup to the first order with respect to overlap integrals between the neighboringatomic orbitals, assuming single-band models. A general and rigorous theory oforbital susceptibility developed in the preceding paper is applied tosingle-band models in two-dimensional square and triangular lattices. Inaddition to the Landau-Peierls orbital susceptibility, it is found that thereare comparable contributions from the Fermi surface and from the occupiedstates in the partially filled band called intraband atomic diamagnetism. Thisresult means that the Peierls phase used in tight-binding models isinsufficient as the effect of magnetic field.

Orbital Magnetism of Bloch Electrons II. Application to Single-Band Models and Corrections to Landau-Peierls susceptibility