English

Quintessence and Supergravity

Astrophysics 2009-10-31 v2 General Relativity and Quantum Cosmology High Energy Physics - Phenomenology High Energy Physics - Theory

Abstract

In the context of quintessence, the concept of tracking solutions allows to address the fine-tuning and coincidence problems. When the field is on tracks today, one has QmPlQ\approx m_{\rm Pl} demonstrating that, generically, any realistic model of quintessence must be based on supergravity. We construct the most simple model for which the scalar potential is positive. The scalar potential deduced from the supergravity model has the form V(Q)=Λ4+αQαeκ2Q2V(Q)=\frac{\Lambda^{4+\alpha}}{Q^{\alpha}}e^{\frac{\kappa}{2}Q^2}. We show that despite the appearence of positive powers of the field, the coincidence problem is still solved. If α11\alpha \ge 11, the fine-tuning problem can be overcome. Moreover, due to the presence of the exponential term, the value of the equation of state, ωQ\omega_Q, is pushed towards the value -1 in contrast to the usual case for which it is difficult to go beyond ωQ0.7\omega_Q\approx -0.7. For Ωm0.3\Omega_{\rm m}\approx 0.3, the model presented here predicts ωQ0.82\omega_Q\approx -0.82. Finally, we establish the ΩmωQ\Omega_{\rm m}-\omega_Q relation for this model.

Keywords

Cite

@article{arxiv.astro-ph/9905040,
  title  = {Quintessence and Supergravity},
  author = {Philippe Brax and Jerome Martin},
  journal= {arXiv preprint arXiv:astro-ph/9905040},
  year   = {2009}
}

Comments

9 pages, 4 figures. Accepted for publication in Physics Letters B. Numerical value of \omega_Q changed: correct value is -0.82. New references and one figure added