Bound States of Non-Hermitian Quantum Field Theories
arXiv:hep-th/0108057 · doi:10.1016/S0375-9601(01)00745-9
Abstract
The spectrum of the Hermitian Hamiltonian (), which describes the quantum anharmonic oscillator, is real and positive. The non-Hermitian quantum-mechanical Hamiltonian , where the coupling constant is real and positive, is -symmetric. As a consequence, the spectrum of is known to be real and positive as well. Here, it is shown that there is a significant difference between these two theories: When is sufficiently small, the latter Hamiltonian exhibits a two-particle bound state while the former does not. The bound state persists in the corresponding non-Hermitian -symmetric quantum field theory for all dimensions but is not present in the conventional Hermitian field theory.
14 pages, 3figures
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Cited by in corpus (18)
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