Explicit exceptional-point parameters are computed for PT-symmetric imaginary potentials in discrete Schrodinger models with up to six grid points, with a unitarity-preserving corridor leading to each extreme.
On the Role of the Normalization Factors $\kappa_n$ and of the Pseudo-Metric ${\cal P} \neq {\cal P}^\dagger$ in Crypto-Hermitian Quantum Models
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abstract
Among ${\cal P}$-pseudo-Hermitian Hamiltonians $H ={\cal P}^{-1} H^\dagger \cal P}$ with real spectra, the ''weakly pseudo-Hermitian" ones (i.e., those employing non-self-adjoint ${\cal P} \neq {\cal P}^\dagger$) form a remarkable subfamily. We list some reasons why it deserves a special attention. In particular we show that whenever ${\cal P} \neq {\cal P}^\dagger$, the current involutive operator of charge ${\cal C}$ gets complemented by a nonequivalent alternative involutive quasiparity operator ${\cal Q}$. We show how, in this language, the standard quantum mechanics is restored via the two alternative inner products in the physical Hilbert space of states, with $<\psi_1|{\cal PQ}|\psi_2>=< \psi_1|{\cal CP}|\psi_2>$.
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Construction of maximally non-Hermitian potentials under unbroken PT-symmetry constraint
Explicit exceptional-point parameters are computed for PT-symmetric imaginary potentials in discrete Schrodinger models with up to six grid points, with a unitarity-preserving corridor leading to each extreme.