English

Scalar Field Dark Energy Parametrization

Cosmology and Nongalactic Astrophysics 2011-12-09 v2 General Relativity and Quantum Cosmology High Energy Physics - Phenomenology High Energy Physics - Theory

Abstract

We propose a new Dark Energy parametrization based on the dynamics of a scalar field. We use an equation of state w=(x1)/(x+1)w=(x-1)/(x+1), with x=Ek/Vx=E_k/V, the ratio of kinetic energy Ek=ϕ˙2/2E_k=\dot\phi^2/2 and potential VV. The eq. of motion gives x=(L/6)(V/3H2)x=(L/6)(V/3H^2) and with a solution x=([1+2L/3(1+y)]1/21)(1+y)/2x=([1+2 L/3(1+y)]^{1/2}-1)(1+y)/2 where y/Vy\equiv \rm/V and L(V/V)2(1+q)2,q\p¨/VL\equiv (V'/V)^2 (1+q)^2,\, q\equiv\ddot\p/V'. Since the universe is accelerating at present time we use the slow roll approximation in which case we have q1|q|\ll 1 and L(V/V)2L\simeq (V'/V)^2. However, the derivation of LL is exact and has no approximation. By choosing an appropriate ansatz for LL we obtain a wide class of behavior for the evolution of Dark Energy without the need to specify the potential VV. In fact ww can either grow and later decrease, or other way around, as a function of redshift and it is constraint between 1w1-1\leq w\leq 1 as for any canonical scalar field with only gravitational interaction. Furthermore, we also calculate the perturbations of DE and since the evolution of DE is motivated by the dynamics of a scalar field the homogenous and its perturbations can be used to determine the form of the potential and the nature of Dark Energy. Since our parametrization is on LL we can easily connect it with the scalar potential V(ϕ)V(\phi).

Keywords

Cite

@article{arxiv.1108.0876,
  title  = {Scalar Field Dark Energy Parametrization},
  author = {Axel de la Macorra},
  journal= {arXiv preprint arXiv:1108.0876},
  year   = {2011}
}

Comments

10 Pages, 9 figures

R2 v1 2026-06-21T18:46:03.133Z