Issues in Palatini ${\cal{R}}^2$ inflation: Bounds on the Reheating Temperature

We consider ${\cal{R}}^2$-inflation in Palatini gravity, in the presence of scalar fields coupled to gravity. These theories, in the Einstein frame, and for one scalar field $h$, share common features with $K$ - inflation models. We apply this formalism for the study of single-field inflationary models, whose potentials are monomials, $V \sim h^{n}$, with $n$ a positive even integer. We also study the Higgs model non-minimally coupled to gravity. With ${\cal{R}}^2$-terms coupled to gravity as $\sim α{\cal{R}}^2$, with $α$ constant, the instantaneous reheating temperature $T_{ins}$, is bounded by $T_{ins} \leq { 0.290 \, m_{Planck}} / {\, α^{1/4}}$, with the upper bound being saturated for large $α$. For such large $α$ need go beyond slow-roll to calculate reliably the cosmological parameters, among these the end of inflation through which $T_{ins}$ is determined. In fact, as inflaton rolls towards the end of inflation point, the quartic in the velocity terms, unavoidable in Palatini gravity, play a significant role and can not be ignored. The values of $α$, and other parameters, are constrained by cosmological data, setting bounds on the inflationary scale $M_{s} \sim 1/\sqrtα$ and the reheating temperature of the Universe.

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