Precision predictions of Starobinsky inflation with self-consistent Weyl-squared corrections

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Precision predictions of Starobinsky inflation with self-consistent Weyl-squared corrections

Authors

Eugenio Bianchi, Mauricio Gamonal

Abstract

Starobinsky's R+αR2R+\alpha R^2 inflation provides a compelling one-parameter inflationary model that is supported by current cosmological observations. However, at the same order in spacetime derivatives as the R2R^2 term, an effective theory of spacetime geometry must also include the Weyl-squared curvature invariant W2W^2. In this paper, we study the inflationary predictions of the gravitational theory with action of the form R+αR2βW2R+\alpha R^2 - \beta W^2, where the coupling constant α\alpha sets the scale of inflation, and corrections due to the W2W^2 term are treated self-consistently via reduction of order in an expansion in the coupling constant β\beta, at the linear order in β/α\beta/\alpha. Cosmological perturbations are found to be described by an effective action with a non-trivial speed of sound csc_{\textrm{s}} for scalar and ctc_{\textrm{t}} for tensor modes, satisfying the relation ct/cs1+β6αc_{\textrm{t}}/c_{\textrm{s}} \simeq 1+ \frac{\beta}{6\, \alpha} during the inflationary phase. Within this self-consistent framework, we compute several primordial observables up to the next-to-next-to-next-to leading order (N3LO). We find the tensor-to-scalar ratio r3(1β6α)(ns1)2r \simeq 3(1-\frac{\beta}{6\alpha})(n_\textrm{s}-1)^2, the tensor tilt ntr8n_{\textrm{t}}\simeq-\frac{r}{8} and the running of the scalar tilt as12(ns1)2\mathfrak{a}_{\textrm{s}}\simeq-\frac{1}{2} (n_{\textrm{s}} - 1)^2, all expressed in terms of the observed scalar tilt nsn_{\textrm{s}}. We also provide the corresponding corrections up to N3LO, O((ns1)3)\mathcal{O}((n_{\textrm{s}} - 1)^3).

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