Myers-Pospelov Model as an Ensemble of Pais-Uhlenbeck Oscillators: Unitarity and Lorentz Invariance Violation
arXiv:1304.4966 · doi:10.1140/epjc/s10052-013-2391-0
Abstract
We study a generalization of a Pais-Uhlenbeck oscillator for fermionic variables. Next, we consider an ensemble of these oscillators and we identify a particular case of the Myers-Pospelov model which is relevant for effective theories of quantum gravity. Finally, by taking the advantage of this connection, we analyze, for this model, the unitarity at one loop order in the low energy regime where no ghost states can be created on-shell. This energy regime is the relevant one when we consider the Myers-Pospelov model as a true effective theory coming from new space-time structure.
8 pages, 5 figures, to appear in Eur.Phys.Jour. C
References in corpus (9)
- Avoiding Dark Energy with 1/R Modifications of Gravity
- Electrodynamics with Lorentz-violating operators of arbitrary dimension
- No-ghost theorem for the fourth-order derivative Pais-Uhlenbeck oscillator model
- Lorentz symmetry breaking as a quantum field theory regulator
- Classification of Dimension 5 Lorentz Violating Interactions in the Standard Model
- Radiatively induced Lorentz-violating operator of mass dimension five in QED
- Neutrino Masses in the Lee-Wick Standard Model
- Living with Ghosts and their Radiative Corrections
- Lee-Wick Theories at High Temperature
Cited by in corpus (8)
- Hamiltonian formulation of an effective modified gravity with nondynamical background fields
- Unitarity in Maxwell-Carroll-Field-Jackiw electrodynamics
- Unitarity and Lee-Wick prescription at one loop level in the effective Myers-Pospelov electrodynamics: the annihilation
- N=2 supersymmetric Pais-Uhlenbeck oscillator
- Unitarity and non-relativistic potential energy in a higher-order Lorentz symmetry breaking electromagnetic model
- Tree-level unitarity, causality and higher-order Lorentz and CPT violation
- Optical theorem and indefinite metric in delta-theory
- N=2 supersymmetric odd-order Pais-Uhlenbeck oscillator