Abstract

We propose a novel explanation for the smallness of the observed cosmological constant (CC). Regions of space with a large CC are short lived and are dynamically driven to crunch soon after the end of inflation. Conversely, regions with a small CC are metastable and long lived and are the only ones to survive until late times. While the mechanism assumes many domains with different CC values, it does not result in eternal inflation nor does it require a long period of inflation to populate them. We present a concrete dynamical model, based on a super-cooled first order phase transition in a hidden conformal sector, that may successfully implement such a crunching mechanism. We find that the mechanism can only solve the CC problem up to the weak scale, above which new physics, such as supersymmetry, is needed to solve the CC problem all the way to the UV cutoff scale. The absence of experimental evidence for such new physics already implies a mild little hierarchy problem for the CC. Curiously, in this approach the weak scale arises as the geometric mean of the temperature in our universe today and the Planck scale, hinting at a new “CC miracle”, motivating new physics at the weak scale independent of electroweak physics. We further predict the presence of new relativistic degrees of freedom in the CFT that should be visible in the next round of CMB experiments. Our mechanism is therefore predictive and experimentally falsifiable.

Highlights

  • We find that the mechanism can only solve the cosmological constant (CC) problem up to the weak scale, above which new physics, such as supersymmetry, is needed to solve the CC problem all the way to the UV cutoff scale

  • In this paper we have proposed a new approach to addressing the CC problem

  • The paradigm discussed in this paper requires no eternal inflation and the mechanism for the selection of the CC is novel and introduces a new form of cosmological dynamics

Read more

Summary

Basic concept

This sector drives a primary phase of inflation for a finite time, before reheating our universe. The dynamics in this sector reacts to the presence of a large CC and acts to lower its value, thereby driving the relevant patch to crunch In this paper this sector is a CFT spontaneously broken at low temperatures and with a vacuum energy density of order −Λ4CFT. The patches’ energy densities are distributed (possibly non-symmetrically) around zero with the same range of order Λ4max Those with large negative cosmological constant will crunch independently of the crunching sector while those with positive (or small negative) crunch only once the CFT phase transition is completed, thereby reducing their energy density by Λ4CFT and driving it to negative values. We move on to explain these statements in detail

The crunching sector
RS at zero temperature
RS at finite temperature
The potential at small χ
Preliminaries
Dynamics of the phase transition
Maximal CC
Phenomenological implications
The scanning and inflationary sectors
Discussion and outlook
A Goldberger-Wise stabilization of the RS model
B Effects of an additional bulk gauge group
C Detailed derivation of the bubble nucleation rate
Numerical calculation of the bounce action
Evaluation of the cosmological constraints
Uncertainties and caveats of the calculation
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call