Equivalence of a Complex $\cP\cT$-Symmetric Quartic Hamiltonian and a Hermitian Quartic Hamiltonian with an Anomaly

dc.creatorBender, Carl M.
dc.creatorBrody, Dorje C.
dc.creatorChen, Jun-Hua
dc.creatorJones, Hugh F.
dc.creatorMilton, Kimball A.
dc.creatorOgilvie, Michael C.
dc.date2006-05-05
dc.date2006-05-08
dc.date.accessioned2026-07-07T10:46:35Z
dc.date.available2026-07-07T10:46:35Z
dc.descriptionIn a recent paper Jones and Mateo used operator techniques to show that the non-Hermitian $\cP\cT$-symmetric wrong-sign quartic Hamiltonian $H=\half p^2-gx^4$ has the same spectrum as the conventional Hermitian Hamiltonian $\tilde H=\half p^2+4g x^4-\sqrt{2g} x$. Here, this equivalence is demonstrated very simply by means of differential-equation techniques and, more importantly, by means of functional-integration techniques. It is shown that the linear term in the Hermitian Hamiltonian is anomalous; that is, this linear term has no classical analog. The anomaly arises because of the broken parity symmetry of the original non-Hermitian $\cP\cT$-symmetric Hamiltonian. This anomaly in the Hermitian form of a $\cP\cT$-symmetric quartic Hamiltonian is unchanged if a harmonic term is introduced into $H$. When there is a harmonic term, an immediate physical consequence of the anomaly is the appearance of bound states; if there were no anomaly term, there would be no bound states. Possible extensions of this work to $-ϕ^4$ quantum field theory in higher-dimensional space-time are discussed.
dc.description19 pages, 7 figures, corrected references
dc.identifierhttps://arxiv.org/abs/hep-th/0605066
dc.identifierhttp://arxiv.org/abs/hep-th/0605066
dc.identifierPhys.Rev.D74:025016,2006
dc.identifierdoi:10.1103/PhysRevD.74.025016
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/183283
dc.subjectHigh Energy Physics - Theory
dc.subjectMathematical Physics
dc.subjectQuantum Physics
dc.titleEquivalence of a Complex $\cP\cT$-Symmetric Quartic Hamiltonian and a Hermitian Quartic Hamiltonian with an Anomaly
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