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Czechoslovak Journal of Physics

Weakly non-Hermitian square well

Hynek Bíla, Vít Jakubský, Miloslav Znojil, Bijan Kumar Bagchi, Sadek Hossain Mallik, C. Quesne

Published Sep 1, 2005• 5 citations
Publisher
DOI
10.1007/s10582-005-0108-9

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A family of non-Hermitian real and tridiagonal-matrix candidates H(N)(λ)=H0(N)+λW(N)(λ) for a hiddenly Hermitian (a.k.a. quasi-Hermitian) quantum Hamiltonian is proposed and studied. Fairly weak assumptions are imposed upon the unperturbed matrix [the square-well-simulating spectrum of H0(N) is not assumed equidistant)] and upon its maximally non-Hermitian N-parametric antisymmetric-matrix perturbations [matrix W(N)(λ) is not even required to be PT-symmetric]. Despite that, the “physical” parametric domain D[N] is (constructively) shown to exist, guaranteeing that in its interior, the spectrum remains real and non-degenerate, rendering the quantum evolution unitary. Among the non-Hermitian degeneracies occurring at the boundary ∂D[N] of the domain of stability, our main attention is paid to their extreme version corresponding to Kato’s exceptional point of order N (EPN). The localization of the EPNs and, in their vicinity, of the quantum-phase-transition boundaries ∂D[N] is found feasible, at the not too large N, using computer-assisted symbolic manipulations, including, in particular, the Gröbner-basis elimination and the high-precision arithmetics.
PT\mathcal{PT}PT-Supersymmetric Square Well and Barrier
The Parity-Time (PT\mathcal{PT}PT) symmetric potentials are derived by non-Hermitian supersymmetric quantum mechanics for square well and barrier. These PT\mathcal{PT}PT-supersymmetric square well and barrier. The partners have complex partners. The partners are isospectral with real energies. PT\mathcal{PT}PT-symmetry is only unbroken for the bound states.