A note on the PT-invariant periodic potential V(x)=4 cos^2 x + 4 i V_0 sin 2x
arXiv:1004.3218 · doi:10.1016/j.physleta.2010.04.046
Abstract
It is shown that the PT symmetric Hamiltonian with the periodic potential V(x) = 4 cos^2 x + 4 i V_0 sin 2x can be mapped into a Hermitian Hamiltonian for , by a similarity transformation. It is also shown that there exist a second critical point of the potential V(x), apart from the known critical point , for after which no part of the eigenvalues and the band structure remains real. Relevant physical consequence of this finding has been pointed out.
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- Infinite families of (non)-Hermitian Hamiltonians associated with exceptional Jacobi polynomials
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- PT-symmetric optical superlattices
- Use of Equivalent Hermitian Hamiltonian for -Symmetric Sinusoidal Optical Lattices
- Peregrine rogue waves in the nonlocal nonlinear Schrödinger equation with parity-time symmetric self-induced potential
- Spectral Singularity in confined PT symmetric optical potential
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- A unidirectional invisible PT-symmetric complex crystal with arbitrary thickness
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- Spontaneous PT-symmetry breaking for systems of noncommutative Euclidean Lie algebraic type
- Spectral Analysis of the Schrodinger Operator with an Optical Potential
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- A new non-Hermitian E2-quasi-exactly solvable model
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- Singular Mapping for a -Symmetric Sinusoidal Optical Lattice at the Symmetry-Breaking Threshold
- Refractive index profiles for a -symmetric optical structure
- A unifying E2-quasi-exactly solvable model