Ordinary versus PT-symmetric quantum field theory
arXiv:1201.1244 · doi:10.1103/PhysRevD.85.085001
Abstract
A quantum-mechanical theory is PT-symmetric if it is described by a Hamiltonian that commutes with PT, where the operator P performs space reflection and the operator T performs time reversal. A PT-symmetric Hamiltonian often has a parametric region of unbroken PT symmetry in which the energy eigenvalues are all real. There may also be a region of broken PT symmetry in which some of the eigenvalues are complex. These regions are separated by a phase transition that has been repeatedly observed in laboratory experiments. This paper focuses on the properties of a PT-symmetric quantum field theory. This quantum field theory is the analog of the PT-symmetric quantum-mechanical theory described by the Hamiltonian , whose eigenvalues have been rigorously shown to be all real. This paper compares the renormalization-group properties of a conventional Hermitian quantum field theory with those of the PT-symmetric quantum field theory. It is shown that while the conventional theory in dimensions is asymptotically free, the theory is like a theory in dimensions; it is energetically stable, perturbatively renormalizable, and trivial.
13 pages, 2 figures
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