Non-Hermitian linear perturbation to a Hamiltonian with a constant electromagnetic field and Hall conductivity

The stationary Schrödinger equation for an electron in a constant electromagnetic field with a non-Hermitian linear perturbation is studied. The wave function and the spectrum of the system are derived analytically, with the spectrum consisting of Landau levels modified by an additional term associated with the linear Stark effect, proportional to a complex constant $\lambda$. It is shown that this constant arises from an operator $\widehat{\mathrm{\Pi }}$ that commutes with the Hamiltonian, i.e., $\widehat{\mathrm{\Pi }}$ is a symmetry of the system. Finally, the Hall conductivity for the lowest Landau level is calculated, showing that it remains exactly equal to the inverse of Klitzing’s constant despite the perturbation.