Action with Acceleration II: Euclidean Hamiltonian and Jordan Blocks
arXiv:1211.7166 · doi:10.1142/S0217751X13501388
Abstract
The Euclidean action with acceleration has been analyzed in [1], hereafter cited as reference I, for its Hamiltonian and path integral. In this paper, the state space of the Hamiltonian is analyzed for the case when it is pseudo-Hermitian (equivalent to a Hermitian Hamiltonian), as well as the case when it is inequivalent. The propagator is computed using both creation/destruction operators as well as the path integral. A state space calculation of the propagator shows the crucial role played by the dual state vectors that yields a result impossible to obtain from a Hermitian Hamiltonian acting on a Hilbert space. When it is not pseudo-Hermitian, the Hamiltonian is shown to be a direct sum of Jordan blocks.
References in corpus (6)
- No-ghost theorem for the fourth-order derivative Pais-Uhlenbeck oscillator model
- Exactly solvable PT-symmetric Hamiltonian having no Hermitian counterpart
- Solution to the ghost problem in fourth order derivative theories
- PT Symmetry as a Generalization of Hermiticity
- PT symmetry in relativistic quantum mechanics
- Action with Acceleration I: Euclidean Hamiltonian and Path Integral