Power-counting and Renormalizability in Lifshitz Scalar Theory
arXiv:1502.01820 · doi:10.1103/PhysRevD.91.125007
Abstract
We study the renormalizability in theories of a self-interacting Lifshitz scalar field. We show that although the statement of power-counting is true at one-loop order, in generic cases where the scalar field is dimensionless, an infinite number of counter terms are involved in the renormalization procedure. This problem can be avoided by imposing symmetries, the shift symmetry in the present paper, which allow only a finite number of counter terms to appear. The symmetry requirements might have important implications for the construction of matter field sectors in the Horava-Lifshitz gravity.
16 pages, 3 figures
References in corpus (10)
- Quantum Gravity at a Lifshitz Point
- Membranes at Quantum Criticality
- Horava-Lifshitz Cosmology: A Review
- Lorentz symmetry breaking as a quantum field theory regulator
- Renormalization of Lorentz violating theories
- Renormalization group in Lifshitz-type theories
- Weighted power counting and Lorentz violating gauge theories. I: General properties
- Weighted power counting and Lorentz violating gauge theories. II: Classification
- Non-Gaussianity from Lifshitz Scalar
- On the effective potential for Horava-Lifshitz-like theories with the arbitrary critical exponent
Cited by in corpus (5)
- Stable Singularity-free Cosmological Solutions in non-projectable Horava-Lifshitz Gravity
- High-energy properties of the graviton scattering in quadratic gravity
- Auxiliary fields approach to shift-symmetric theories: the derivative theory and the crumpled-to-flat transition of membranes at two-loop order
- Aspects of Black Holes in Gravitational Theories with Broken Lorentz and Diffeomorphism Symmetries
- New dynamical realizations of the Lifshitz group