Table of Contents
Fetching ...

Constraining the EW Hierarchy from the Weak Gravity Conjecture

Luis E. Ibanez, Victor Martin-Lozano, Irene Valenzuela

Abstract

In this addendum we complement the remarks made in ref[1] constraining the value of the cosmological constant $Λ_4$ in terms of neutrino masses. Those were based on a sharpened version of the Weak Gravity Conjecture as applied to compactifications of the SM to lower dimensions. We argue that the same line of reasoning implies that for fixed values of $Λ_4$ and the Yukawa coupling of the lightest neutrino $Y_{ν_1}$, the EW scale is bounded above. This is a trivial consequence of neutrino masses depending on the Higgs vev. In the case of massive Majorana neutrinos with a see-saw mechanism associated to a large scale $M\simeq 10^{10-14}$ GeV and $Y_{ν_1}\simeq 10^{-3}$, one obtains that the EW scale cannot exceed $M_{EW}\lesssim 10^2-10^4$ GeV. From this point of view, the delicate fine-tuning required to get a small EW scale would be a mirage, since parameters yielding higher EW scales would be in the swampland and would not count as possible consistent theories. This would bring a new perspective into the issue of the EW hierarchy.

Constraining the EW Hierarchy from the Weak Gravity Conjecture

Abstract

In this addendum we complement the remarks made in ref[1] constraining the value of the cosmological constant in terms of neutrino masses. Those were based on a sharpened version of the Weak Gravity Conjecture as applied to compactifications of the SM to lower dimensions. We argue that the same line of reasoning implies that for fixed values of and the Yukawa coupling of the lightest neutrino , the EW scale is bounded above. This is a trivial consequence of neutrino masses depending on the Higgs vev. In the case of massive Majorana neutrinos with a see-saw mechanism associated to a large scale GeV and , one obtains that the EW scale cannot exceed GeV. From this point of view, the delicate fine-tuning required to get a small EW scale would be a mirage, since parameters yielding higher EW scales would be in the swampland and would not count as possible consistent theories. This would bring a new perspective into the issue of the EW hierarchy.

Paper Structure

This paper contains 1 equation, 2 figures.

Figures (2)

  • Figure 1: Constraints on the EW scale and the cosmological constant for the case of Majorana neutrinos and normal hierarchy, in the presence of an additional Weyl fermion of mass $m_\chi=10^{-3}$ eV. We have assumed $Y=10^{-3}$ and $M=10^{10}$ GeV.
  • Figure 2: Constraints on the EW scale and the cosmological constant for the case of Dirac neutrinos and normal hierarchy. We have assumed a Yukawa coupling $Y=10^{-14}$.