Dark Energy as Double N-Flation--Observational Predictions

preprint2011arXivOpen access

Abstract

We propose a simple model for dark energy useful for comparison with observations. It is based on the idea that dark energy and inflation should be caused by the same physical process. As motivation, we note that Linde's simple chaotic inflation V=(1/2)m2ϕ2V=(1/2)m^{2}ϕ^{2} produces values of ns=0.967n_{s}=0.967 and r=0.13r=0.13, which are consistent with the WMAP 1-sigma error bars. We therefore propose V=(1/2)m22ϕ22+(1/2)m12ϕ12V=(1/2)m_{2}^{2}ϕ_{2}^{2}+(1/2)m_{1}^{2}ϕ_{1}^{2} with m1∼10−5m_{1}\sim10^{-5} and m2≤10−60m_{2}\leq10^{-60}, where c=1=ℏc=1=\hbar and the reduced Planck mass is set to unity. The field ϕ1ϕ_{1} drives inflation and has damped by now (ϕ1,0=0ϕ_{1,0}=0), while ϕ2ϕ_{2} is currently rolling down its potential to produce dark energy. Using this model, we derive the formula δw(z)≡w(z)+1=δw0(H0/H(z))2δw(z)\equiv w(z)+1=δw_{0}(H_0/H(z))^2 via the slow-roll approximation. Our numerical results from exact and self-consistent solution of the equations of motion for ϕ2ϕ_2 and the Friedmann equations support this formula, and it should hold for any slow-roll dark energy. Our potential can be easily realized in N-flation models with many fields, and is easily falsifiable by upcoming experiments -- for example, if Linde's chaotic inflation is ruled out. But if rr values consistent with Linde's chaotic inflation are detected then one should take this model seriously indeed.

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