PT-Invariant Periodic Potentials with a Finite Number of Band Gaps
arXiv:math-ph/0505027 · doi:10.1063/1.2000207
Abstract
We obtain the band edge eigenstates and the mid-band states for the complex, PT-invariant generalized associated Lamé potentials $V^{PT}(x)=-a(a+1)m \sn^2(y,m)-b(b+1)m {\sn^2 (y+K(m),m)} -f(f+1)m {\sn^2 (y+K(m)+iK'(m),m)}-g(g+1)m {\sn^2 (y+iK'(m),m)}$, where , and there are four parameters . This work is a substantial generalization of previous work with the associated Lamé potentials $V(x)=a(a+1)m\sn^2(x,m)+b(b+1)m{\sn^2 (x+K(m),m)}$ and their corresponding PT-invariant counterparts , both of which involving just two parameters . We show that for many integer values of , the PT-invariant potentials are periodic problems with a finite number of band gaps. Further, usingsupersymmetry, we construct several additional, new, complex, PT-invariant, periodic potentials with a finite number of band gaps. We also point out the intimate connection between the above generalized associated Lamé potential problem and Heun's differential equation.
30 pages, 0 figures
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Cited by in corpus (8)
- Making Sense of Non-Hermitian Hamiltonians
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- Spectral singularities in PT-symmetric periodic finite-gap systems
- Conditional observability
- Generalized Swanson models and their solutions
- Complex Periodic Potentials with a Finite Number of Band Gaps
- The Heun equation and the Calogero-Moser-Sutherland system V: generalized Darboux transformations
- Quasi-Periodic Solutions of Heun's Equation