English

Tachyonic (phantom) power-law cosmology

Cosmology and Nongalactic Astrophysics 2014-03-11 v3 General Relativity and Quantum Cosmology

Abstract

Tachyonic scalar field-driven late universe with dust matter content is considered. The cosmic expansion is modeled with power-law and phantom power-law expansion at late time, i.e. z0.45z \lesssim 0.45. WMAP7 and its combined data are used to constraint the model. The forms of potential and the field solution are different for quintessence and tachyonic cases. Power-law cosmology model (driven by either quintessence or tachyonic field) predicts unmatched equation of state parameter to the observational value, hence the power-law model is excluded for both quintessence and tachyonic field. In the opposite, the phantom power-law model predicts agreeing valued of equation of state parameter with the observational data for both quintessence and tachyonic cases, i.e. wϕ,0=1.494.08+11.64w_{\phi, 0} = -1.49^{+11.64}_{-4.08} (WMAP7+BAO+H0H_0) and wϕ,0=1.516.72+3.89 w_{\phi, 0} = -1.51^{+3.89}_{-6.72} (WMAP7). The phantom-power law exponent β\beta must be less than about -6, so that the 2<wϕ,0<1-2 < w_{\phi, 0} < -1. The phantom power-law tachyonic potential is reconstructed. We found that dimensionless potential slope variable Γ\Gamma at present is about 1.5. The tachyonic potential reduced to V=V0ϕ2V= V_0\phi^{-2} in the limit Ωm,00\Omega_{{\rm m}, 0} \rightarrow 0.

Keywords

Cite

@article{arxiv.1210.5550,
  title  = {Tachyonic (phantom) power-law cosmology},
  author = {Rachan Rangdee and Burin Gumjudpai},
  journal= {arXiv preprint arXiv:1210.5550},
  year   = {2014}
}

Comments

11 pages, 5 figures

R2 v1 2026-06-21T22:25:00.644Z