Abstract
We demonstrate the extension to parity-time ()-symmetric field theories of the Goldstone theorem, confirming that the spontaneous appearance of a field vacuum expectation value via minimization of the effective potential in a non-Hermitian model is accompanied by a massless scalar boson. Laying a basis for our analysis, we first show how the conventional quantization of the path-integral formulation of quantum field theory can be extended consistently to a non-Hermitian model by considering conjugation instead of Hermitian conjugation. The extension of the Goldstone theorem to a -symmetric field theory is made possible by the existence of a conserved current that does not, however, correspond to a symmetry of the non-Hermitian Lagrangian. In addition to extending the proof of the Goldstone theorem to a -symmetric theory, we exhibit a specific example in which we verify the existence of a massless boson at the tree and one-loop levels.
- Received 29 May 2018
DOI:https://doi.org/10.1103/PhysRevD.98.045001
Published by the American Physical Society under the terms of the Creative Commons Attribution 4.0 International license. Further distribution of this work must maintain attribution to the author(s) and the published article’s title, journal citation, and DOI. Funded by SCOAP3.
Published by the American Physical Society