Landau diamagnetism (source code)

= Landau diamagnetism
{c}
{wiki}

<Landau diamagnetism> is the orbital response of mobile <Electrons> to an applied <magnetic field>, arising from quantization of their transverse motion. For a noninteracting three-dimensional isotropic <Electron> <gas> with quadratic dispersion, <electron spin> with $g=2$ and <magnetic fields> weak enough for the smooth-response limit, its susceptibility is $\chi_L=-\chi_P/3$, where $\chi_P$ is the <Pauli paramagnetism> susceptibility. Band effective masses, interactions, dimensionality and resolved magnetic quantum oscillations can change this simple relation.