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Implications of the $S_8$ tension for decaying dark matter with warm decay products

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arxiv 2008.09615 v2 pith:7AMGFYWW submitted 2020-08-21 astro-ph.CO hep-ph

classification astro-ph.COhep-ph
keywords sigmamassivemattermodeldarkdatadecayingfactor
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abstract

Recent weak lensing surveys have revealed that the direct measurement of the parameter combination $S_8\equiv\sigma_8(\Omega_m/0.3)^{0.5}$ -- where $\sigma_8$ is a measure of the amplitude of matter fluctuations on 8 $h^{-1}$Mpc scales -- is $\sim3\sigma$ discrepant with the value reconstructed from cosmic microwave background (CMB) data assuming the $\Lambda$CDM model. In this article, we show that it is possible to resolve the tension if dark matter (DM) decays with a lifetime of $\Gamma^{-1} \simeq 55 \ \text{Gyrs}$ into one massless and one massive product, and transfers a fraction $\varepsilon\simeq 0.7 \ \%$ of its rest mass energy to the massless component. The velocity-kick received by the massive daughter leads to a suppression of gravitational clustering below its free-streaming length, thereby reducing the $\sigma_8$ value as compared to that inferred from the standard $\Lambda$CDM model, in a similar fashion to massive neutrino and standard warm DM. Contrarily to the latter scenarios, the time-dependence of the power suppression and the free-streaming scale allows the 2-body decaying DM scenario to accommodate CMB, baryon acoustic oscillation, growth factor and un-calibrated supernova Ia data. We briefly discuss implications for DM model building, galactic small-scale structure problems and the recent Xenon-1T excess. Future experiments measuring the growth factor to high accuracy at $0\lesssim z\lesssim1$ can further test this scenario.

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Cited by 7 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. Cosmological evolution with decaying dark matter: an integral-equation approach

    astro-ph.CO 2026-07 accept novelty 6.0 of 10

    CLASSIER-DDM evaluates generic two-body decaying dark matter perturbations via iterative integral equations at O(0.1%) accuracy and O(1 min) cost without a Boltzmann hierarchy or fluid approximation.

  2. Decaying Dark Matter Halo Abundance from a Revised Spherical Collapse Model

    astro-ph.CO 2026-07 conditional novelty 6.0 of 10

    A mass-dependent collapse threshold from a revised spherical collapse model predicts the decaying-dark-matter halo mass function, matching N-body simulations at z≈1 and for mild kicks at z=0.

  3. Neutrino mass limits and decaying dark matter: background evolution versus perturbations

    astro-ph.CO 2026-03 accept novelty 6.0 of 10

    Decaying dark matter can hide neutrino mass from expansion-history data, but CMB lensing unmasks it and restores ∑mν ≲ 0.079 eV.

  4. Interpreting the Hubble tension with a cascade decaying dark matter sector

    astro-ph.CO 2025-07 conditional novelty 6.0 of 10

    A cascade decaying dark matter model combining early and late effects still cannot reduce the Hubble tension below about 3 sigma, and is statistically disfavored relative to Lambda CDM.

  5. Rapid and accurate numerical evolution of linear cosmological perturbations with non-cold relics

    astro-ph.CO 2025-06 conditional novelty 6.0 of 10

    CLASSIER computes cosmological perturbation spectra with non-cold relics using iterated integral equations and non-uniform fast Fourier transforms, matching a converged Boltzmann hierarchy to <0.01% in the matter powe...

  6. A frequentist view on the two-body decaying dark matter model

    astro-ph.CO 2025-05 conditional novelty 6.0 of 10

    A frequentist reanalysis of Planck and KiDS-1000 data shows that a two-body decaying dark matter model can produce S8 values consistent with weak lensing surveys, and that prior choices dominated earlier Bayesian exclusions.

  7. Sign Switching in Dark Sector Coupling Interactions as a Candidate for Resolving Cosmological Tensions

    astro-ph.CO 2025-01 conditional novelty 5.0 of 10

    A sign-switching dark-sector coupling, fitted to CMB, DESI BAO, and supernova data, can simultaneously raise H0 and lower S8, but the preference over LambdaCDM depends on using SH0ES-calibrated supernovae.

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