Interpreting Hubble tension with a cascade decaying dark matter sector
Quan Zhou, Zixuan Xu, Sibo Zheng
TL;DR
This work investigates a cascade decaying dark matter (CDDM) sector to address the Hubble tension by combining early-time relativistic DM production with late-time decay to neutrinos within a single $\Lambda$CDM extension. Using a minimal parameter set $\{\tau_M, M, m, \tau_m\}$, the authors derive the background and perturbation evolution, and perform MCMC fits to Planck 2018+BAO+Pantheon data with four model variants. They find that models incorporating both early and late-time effects (II and III) can reduce the tension to about $3.2σ$, with $M/m \approx 1.1\times10^4$, $\tau_M \approx 2.5\times10^3$ s, $\tau_m \approx 150$–$300$ Gyr, and $m \lesssim 5$ MeV, while remaining compatible with BBN, neutrino flux bounds, and matter-power/structure-formation constraints. The viable CDDM scenarios predict $S_8 \approx 0.84$ and $n_s \approx 0.95$, and a modestly enhanced matter power spectrum at intermediate scales, providing concrete observational targets for future tests and model realizations of the late- and early-time effects.
Abstract
Hubble tension can be alleviated by altering either early- or late-time $Λ$CDM. So far, extensive studies have shown that only early dark energy or ad hoc combinations of those two-fold effects can reduce the tension to $3σ$ level or lower. In this work, we improve the latter solution by considering a cascade decaying dark matter sector, where a parent particle produces relativistic dark matter in the early Universe and the dark matter subsequently decays to neutrinos in the late-time Universe. We parametrize this model with four model parameters, carry out a Markov Chain Monte Carlo fit to Planck 2018+BAO+Pantheon data sets, and compare it to Big Bang Nucleosynthesis limits, neutrino flux bounds, Planck data about matter power spectrum, and structure formation constraint. Within parameter regions reducing the Hubble tension to $3.2σ$ and compatible with the existing constraints, the main phenomenological features include a larger $S_{8}\sim 0.84$, smaller $n_{s}\sim 0.95$ and larger matter power spectrum relative to the $Λ$CDM, which are left for future tests.
