Abstract

We consider Higgs inflation with an αR2αR^2 term. It adds a new scalar degree of freedom, which leads to a two-field model of inflation. We do a complete slow-roll analysis of the three-dimensional parameter space of the R2R^2 coefficient αα, the non-minimal coupling ξξ and the Higgs self-coupling λλ. We find three classes of inflationary solutions, but only pure R2R^2 and attractor solutions fit observations. We find that pure Higgs inflation is impossible when the R2R^2 term is present regardless of how small αα is. However, we can have Higgs-like inflation, where the amplitude of the perturbations does not depend on αα and the predictions as a function of e-folds are the same as in Higgs inflation, although the inflationary trajectory is curved in field space. The spectral index is 0.939<nR<0.9670.939 < n_R < 0.967, and constraining it to the observed range, the tensor-to-scalar ratio varies from 3.8×10−33.8\times10^{-3} to the maximum allowed by observations, 0.0790.079. Observational constraints on isocurvature perturbations contribute to these limits, whereas non-Gaussianity is automatically in the range allowed by observations.

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