Introduction of the generalized Lorenz gauge condition into the vector-tensor theory
arXiv:1111.6342 · doi:10.1103/PhysRevD.85.023533
Abstract
We introduce the generalized Lorentz gauge condition in the theory of quantum electrodynamics into the general vector-tensor theories of gravity. Then we explore the cosmic evolution and the static, spherically symmetric solution of the four dimensional vector field with the generalized Lorenz gauge. We find that, if the vector field is minimally coupled to the gravitation, it behaves as the cosmological constant. On the other hand, if it is nonminimally coupled to the gravitation, the vector field could behave as vast matters in the background of spatially flat Friedmann-Robertson-Walker Universe. But it may be not the case. The weak, strong and dominant energy conditions, the stability analysis of classical and quantum aspects would put constraints on the parameters and so the equation of state of matters would be greatly constrained.
7 pages, 1 figure
References in corpus (12)
- Signals for Lorentz Violation in Post-Newtonian Gravity
- Inflationary Universe with Anisotropic Hair
- Vector Inflation
- Spontaneous Lorentz and Diffeomorphism Violation, Massive Modes, and Gravity
- Interacting Vector-like Dark Energy, the First and Second Cosmological Coincidence Problems
- A cosmic vector for dark energy
- Lorentz Violating Inflation
- Instabilities in the Aether
- Cheng-Weyl Vector Field and its Cosmological Application
- Cosmological models with Lagrange Multiplier Field
- Primordial Perturbations in Einstein-Aether and BPSH Theories
- Sigma-Model Aether