Is space-time symmetry a suitable generalization of parity-time symmetry?
arXiv:1405.5234 · doi:10.1016/j.aop.2014.07.026
Abstract
We discuss space-time symmetric Hamiltonian operators of the form , where is Hermitian and real. is invariant under the unitary operations of a point group while is invariant under transformation by elements of a subgroup of . If exhibits irreducible representations of dimension greater than unity, then it is possible that has complex eigenvalues for sufficiently small nonzero values of . In the particular case that is parity-time symmetric then it appears to exhibit real eigenvalues for all , where is the exceptional point closest to the origin. Point-group symmetry and perturbation theory enable one to predict whether may exhibit real or complex eigenvalues for . We illustrate the main theoretical results and conclusions of this paper by means of two- and three-dimensional Hamiltonians exhibiting a variety of different point-group symmetries.
References in corpus (12)
- Repulsion of Resonance States and Exceptional Points
- The Chirality of Exceptional Points
- Quantum Complex Henon-Heiles Potentials
- Non-hermitean hamiltonians with unitary and antiunitary symmetry
- PT-symmetry broken by point-group symmetry
- Exactly Solvable Non-Separable and Non-Diagonalizable 2-Dim Model with Quadratic Complex Interaction
- PT phase transition in multidimensional quantum systems
- Variational collocation for systems of coupled anharmonic oscillators
- On the symmetry of the quantum-mechanical particle in a cubic box
- Level Crossings in Complex Two-Dimensional Potentials
- Critical parameters for non-hermitian Hamiltonians
- On the real matrix representation of PT-symmetric operators
Cited by in corpus (5)
- Spectrum and normal modes of non-hermitian quadratic boson operators
- Non-Hermitian oscillators with symmetry
- Non-Hermitian Hamiltonians and similarity transformations
- Group theoretical analysis of a quantum-mechanical three-dimensional quartic anharmonic oscillator
- On the symmetry of three identical interacting particles in a one-dimensional box