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de Sitter Swampland, $H_0$ tension & observation

Eoin Ó Colgáin, Maurice H. P. M. van Putten, Hossein Yavartanoo

Abstract

Realising de Sitter vacua in string theory is challenging. For this reason it has been conjectured that de Sitter vacua inhabit the Swampland of inconsistent low-energy effective theories coupled to gravity. Since de Sitter is an attractor for $Λ$CDM, the conjecture calls $Λ$CDM into question. Reality appears sympathetic to this idea as local measurements of the Hubble constant $H_0$ are also at odds with $Λ$CDM analysis of Planck data. This tension suggests that the de Sitter state is unstable, thereby implying a turning point in the Hubble parameter. We present a model relieving this tension, which predicts a turning at small positive redshift $z_*$ that is dictated by present-day matter density $ω_m$. This feature is easily identified by homogeneous surveys covering redshifts $z \leq 0.1$. We comment on the implications for the Swampland program.

de Sitter Swampland, $H_0$ tension & observation

Abstract

Realising de Sitter vacua in string theory is challenging. For this reason it has been conjectured that de Sitter vacua inhabit the Swampland of inconsistent low-energy effective theories coupled to gravity. Since de Sitter is an attractor for CDM, the conjecture calls CDM into question. Reality appears sympathetic to this idea as local measurements of the Hubble constant are also at odds with CDM analysis of Planck data. This tension suggests that the de Sitter state is unstable, thereby implying a turning point in the Hubble parameter. We present a model relieving this tension, which predicts a turning at small positive redshift that is dictated by present-day matter density . This feature is easily identified by homogeneous surveys covering redshifts . We comment on the implications for the Swampland program.

Paper Structure

This paper contains 1 section, 13 equations, 2 figures.

Table of Contents

  1. Acknowledgements

Figures (2)

  • Figure 1: Normalised cosmological evolution according to (\ref{['ODE']}) and $\Lambda$CDM (\ref{['EQN_LCDM']}). While evolution are relatively similar in the past ($z>0$), they are vastly distinct in the future ($z<0$).
  • Figure 2: Cosmological evolution outside the Swampland is expected to violate NEC ($w<-1)$, inevitably giving rise to a turn $z_*$ point in $H(z)$. Holography predicts $0<z_*<0.1$ as a new observable accessible by homogeneous supernova surveys covering extremely low redshifts of the Local Universe. Shown is the predicted location (\ref{['EQN_zs']}) for various canonical values of $\omega_m$, where $z_*$ for $\omega_m=0.27$ is illustrative for the anticipated location suggested by current cosmological data $H(z)$.