The Dilaton: A Natural Resolution to the Hubble Tension via Spontaneous Scale Symmetry Breaking
Arpit Kottur, Jui Mahajan, Raka Dabhade
TL;DR
The paper tackles the Hubble tension by proposing that late-time cosmic acceleration is driven by a Dilaton, the PNGB of spontaneously broken scale invariance in a non-minimally coupled gravity sector. A simple quadratic mass term in the Jordan frame maps to a thawing exponential potential in the Einstein frame, with the slope $λ$ determined by the coupling $ξ$; this relation is tested against Bayesian reconstructions of dark energy dynamics from Planck, Pantheon+, and SH0ES data. The analysis finds $λ_{obs} ≈ 0.056$ and infers $ξ ≈ 7.8 × 10^{-4}$, yielding a present equation of state $w_0 ≈ -0.85$ and a natural mass scale $m ∼ H_0$, protected by approximate shift symmetry. The mechanism links a fundamental symmetry to cosmological evolution, offering a physically motivated resolution to the Hubble tension and making testable predictions for future surveys and local gravity tests through screening behaviors and thawing dynamics.
Abstract
The statistical tension between early and late universe measurements of the Hubble constant ($H_0$) suggests that the dark sector is dynamical rather than static. We propose that this dynamics arises from a fundamental symmetry principle: the Spontaneous Breaking of Scale Invariance. We introduce the Dilaton ($χ$), a Pseudo-Nambu-Goldstone Boson (PNGB) associated with dilatation symmetry breaking. We demonstrate that a simple quadratic mass term in the fundamental theory transforms, via conformal coupling to gravity, into a ''thawing'' exponential potential $V(φ) \propto e^{-λφ}$ in the Einstein frame. Using recent Bayesian reconstructions of dark energy dynamics from Planck, Pantheon+, and SH0ES data, we constrain the potential slope to be $λ\approx 0.056$. We show that this observational value is not arbitrary but corresponds to a fundamental non-minimal coupling strength of $ξ\approx 7.8 \times 10^{-4}$. The Dilaton mechanism naturally generates the late-time equation of state evolution ($w_0 \approx -0.85$) required to alleviate the Hubble tension while protecting the field mass $m \sim H_0$ through approximate shift symmetry.
