Fab Four Effective Field Theory Treatment
arXiv:1812.01881 · doi:10.1140/epjc/s10052-018-6470-0
Abstract
The article addresses the John interaction from Fab Four class of Horndeski models from the effective field theory point of view. Models with this interaction are heavily constrained by gravitational wave speed observations, so it is important to understand, if these constraints hold in the effective field theory framework. We show that John interaction induces new terms quadratic in curvature at the level of the effective (classical) action. These new terms generate additional low energy scalar and spin-2 gravitational degrees of freedom. Some of them have a non-vanishing decay width and some are ghosts. Discussion of these features is given
11 pages
References in corpus (10)
- GW170817: Observation of Gravitational Waves from a Binary Neutron Star Inspiral
- Multi-messenger Observations of a Binary Neutron Star Merger
- GW170814: A Three-Detector Observation of Gravitational Waves from a Binary Black Hole Coalescence
- GW170608: Observation of a 19-solar-mass Binary Black Hole Coalescence
- Dark Energy after GW170817: dead ends and the road ahead
- Non-local quantum effects in cosmology 1: Quantum memory, non-local FLRW equations and singularity avoidance
- What is modified gravity and how to differentiate it from particle dark matter?
- Self Tuning Scalar Fields in Spherically Symmetric Spacetimes
- Three Waves for Quantum Gravity
- Gravity Induced Non-Local Effects in the Standard Model
Cited by in corpus (10)
- FeynGrav 2.0
- One-loop effective scalar-tensor gravity
- Effective Potential of Scalar-Tensor Gravity
- Basic issues of conservative approaches to quantum theory of gravity
- Beyond Horndeski interactions induced by quantum effects
- Fab-Four cosmography to tackle the Hubble tension
- Extended Gravity Constraints at Different Scales
- FeynGrav and Recent Progress in Computational Perturbative Quantum Gravity
- On anomalies in effective models with nonlinear symmetry realization
- Non-minimal Effective Scalar-Tensor Gravity in the Early Universe