{ "id": "1506.08432", "version": "v1", "published": "2015-06-28T18:14:45.000Z", "updated": "2015-06-28T18:14:45.000Z", "title": "Advancing the case for $PT$ Symmetry -- the Hamiltonian is always $PT$ Symmetric", "authors": [ "Philip D. Mannheim" ], "comment": "11 pages, revtex4", "categories": [ "quant-ph", "hep-ph" ], "abstract": "While a Hamiltonian can be both Hermitian and $PT$ symmetric, it is $PT$ symmetry that is the more general, as it can lead to real energy eigenvalues even if the Hamiltonian is not Hermitian. We discuss some specific ways in which $PT$ symmetry goes beyond Hermiticity and is more far reaching than it. We show that simply by virtue of being the generator of time translations, the Hamiltonian must always be $PT$ symmetric, regardless of whether or not it might be Hermitian. We show that the reality of the Euclidean time path integral is a necessary and sufficient condition for $PT$ symmetry of a quantum field theory, with Hermiticity only being a sufficient condition. We show that in order to construct the correct classical action needed for a path integral quantization one must impose $PT$ symmetry on each classical path, a requirement that has no counterpart in any Hermiticity condition since Hermiticity of a Hamiltonian is only definable after the quantization has been performed and the quantum Hilbert space has been constructed. With the spacetime metric being $PT$ even we show that a covariant action must always be $PT$ symmetric. Unlike Hermiticity, $PT$ symmetry does not need to be postulated as it is derivable from Poincare invariance. Hermiticity is just a particular realization of $PT$ symmetry, one in which the eigenspectrum is real and complete.", "revisions": [ { "version": "v1", "updated": "2015-06-28T18:14:45.000Z" } ], "analyses": { "keywords": [ "hamiltonian", "hermiticity", "euclidean time path integral", "sufficient condition", "real energy eigenvalues" ], "note": { "typesetting": "RevTeX", "pages": 11, "language": "en", "license": "arXiv", "status": "editable", "adsabs": "2015arXiv150608432M", "inspire": 1380207 } } }