Doubling theorem under PT symmetry with nonlinear Kramers pairs
Establish whether a doubling theorem holds for n-fold exceptional points in the nonlinear eigenvalue equation F(ω,k)|ψ⟩=0 when the system has parity–time symmetry satisfying U_PT U_PT* = −1 (i.e., nonlinear Kramers pairs), specifically determining whether every n-fold exceptional point must be accompanied by another of opposite frequency–momentum winding number across the Brillouin zone.
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While we have focused on the cases of $U_{\mathrm{PT}U*_{\mathrm{PT}=1$ so far, the doubling theorem for cases of $U_{\mathrm{PT}U*_{\mathrm{PT}=-1$ remains an open question due to nonlinear Kramers pairs. If $|\psi_n\rangle$ is an eigenstate with eigenvalue $\omega_n$, then $U_{\mathrm{PT}\mathcal{K}|\psi_{n}\rangle$ is also an eigenstate with eigenvalue $\omega*_n$ where $\mathcal{K}$ denotes the complex conjugate operator.