Abstract

Imposing that the excursion distance of inflaton in field space during inflation be less than the Planck scale, we derive an upper bound on the tensor-to-scalar ratio at the CMB scales, i.e. r∗,maxr_{*,max}, in the general canonical single-field slow-roll inflation model, in particular the model with non-negligible running of the spectral index αsα_s and/or the running of running βsβ_s. We find that r∗,max≃7×10−4r_{*,max}\simeq 7\times 10^{-4} for ns=0.9645n_s=0.9645 without running and running of running, and r∗,maxr_{*,max} is significantly relaxed to the order of O(10−2∼10−1){\cal O}(10^{-2}\sim 10^{-1}) in the inflation model with αsα_s and/or βs∼+O(10−2)β_s\sim +{\cal O}(10^{-2}) which are marginally preferred by the Planck 2015 data.

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