Single particle flat bands
The single-electron Hamiltonian on spherical surface with a magnetic monopole of strength Q at the center of the sphere is15
$${\hat{H}}_{k}=\frac{{{\bf{L}}}^{2}-{\hslash }^{2}{Q}^{2}}{2{m}_{{\rm{e}}}{R}^{2}},$$
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The single-electron Hamiltonian on spherical surface with a magnetic monopole of strength Q at the center of the sphere is15
$${\hat{H}}_{k}=\frac{{{\bf{L}}}^{2}-{\hslash }^{2}{Q}^{2}}{2{m}_{{\rm{e}}}{R}^{2}},$$
…