Inflation, the Hubble tension, and early dark energy: An alternative overview

Author:

Giarè William1ORCID

Affiliation:

1. University of Sheffield

Abstract

I review and discuss the possible implications for inflation resulting from considering new physics in light of the Hubble tension. My study is motivated by a simple argument that the constraints on inflationary parameters, most typically the spectral index ns, depend to some extent on the cosmological framework. To avoid broadening the uncertainties resulting from marginalizing over additional parameters (typical in many alternative models), I first adopt the same alternative viewpoint of previous studies and analyze what happens if a physical theory can extra parameters to nonstandard values. Focusing on the dark energy equation of state w and the effective number of relativistic species Neff, I confirm that physical theories able to fix w1.2 or Neff3.9 produce values of H0 from Cosmic Microwave Background and Baryon Acoustic Oscillations in line with the local distance ladder estimate. While in the former case I do not find any relevant implications for inflation, in the latter scenarios, I observe a shift toward ns1. From a model-selection perspective, both cases are strongly disfavored compared to Λ cold dark matter. However, models with Neff3.33.4 could bring the H0 tension down to 3σ while being moderately disfavored. Yet, this is enough to change the constraints on inflation so that the most accredited models (e.g., Starobinsky inflation) would no longer be favored by data. I then focus on Early Dark Energy (EDE), arguing that an EDE fraction fEDE0.040.06 (only able to mildly reduce the H0 tension down to 3σ) could already require a similar change in perspective on inflation. In fact, performing a full joint analysis of EDE and Starobinsky inflation, I find that the two models can hardly coexist for fEDE0.06. Published by the American Physical Society 2024

Funder

European Cooperation in Science and Technology

Publisher

American Physical Society (APS)

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