Abstract

One possible and natural derivation from the collisionless cold dark matter (CDM) standard cosmological framework is the assumption of the existence of interactions between dark matter (DM) and photons or neutrinos. Such a possible interacting dark matter (IDM) model would imply a suppression of small-scale structures due to a large collisional damping effect, even though the weakly-interacting massive particle (WIMP) can still be the DM candidate. Because of this, IDM models can help alleviate alleged tensions between standard CDM predictions and observations at small mass scales. In this work, we investigate the properties of the DM halo substructure or subhalos formed in a high-resolution cosmological N-body simulation specifically run within these alternative models. We also run its CDM counterpart, which allowed us to compare subhalo properties in both cosmologies. We show that, in the lower mass range covered by our simulation runs, both subhalo concentrations and abundances are systematically lower in IDM compared to the CDM scenario. Yet, as in CDM, we find that median IDM subhalo concentration values increase towards the innermost regions of their hosts for the same mass subhalos. Similarly to CDM, we find IDM subhalos to be more concentrated than field halos of the same mass. Our work has a direct application to studies aimed at the indirect detection of DM where subhalos are expected to boost the DM signal of their host halos significantly. From our results, we conclude that the role of the halo substructure in DM searches will be less important in interacting scenarios than in CDM, but is nevertheless far from being negligible.

Highlights

  • The current standard model of cosmology, ΛCDM, is based on a cosmological constant to explain the late-time accelerated expansion of the Universe and a cold dark matter (CDM) component to Galaxies 2019, 7, 80; doi:10.3390/galaxies7040080 www.mdpi.com/journal/galaxiesGalaxies 2019, 7, 80 account for the required additional gravitational attraction to form and support the galaxies and larger structures we observe today [1]

  • We study the properties of the halo substructure in the same interacting dark matter (IDM) scenario of [50], for which we use a set of N-body, DM-only cosmological simulations with higher particle resolution

  • The IDM matter power spectrum features a cut-off around a smooth scale of ∼100 kpc for the cross-section that we are considering in this work (σ/σTh = 2 × 10−9)

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Summary

Introduction

The current standard model of cosmology, ΛCDM, is based on a cosmological constant to explain the late-time accelerated expansion of the Universe and a cold dark matter (CDM) component to Galaxies 2019, 7, 80; doi:10.3390/galaxies7040080 www.mdpi.com/journal/galaxies. One natural deviation from the collisionless CDM in the standard model is the assumption of the existence of interactions between DM and the standard model (SM) particles we know about, in particular, photons or neutrinos [27,28,29] This does affect, as we show in this article, the formation of DM structures on small scales, and provides an explanation for the exact relic abundance of DM, Ωcdm h2 = 0.12011, found in the Universe today [1]. The considered cosmological model is crucial for such DM searches as different predictions for structure formation on small scales imply different gamma-ray or neutrino signal estimations This may translate into different constraints on the DM annihilation cross-section when compared to those obtained assuming the standard ΛCDM scenario.

Interacting Dark Matter
Simulations
Results
Halo Concentrations
Subhalo Concentrations
Subhalo Abundances
Summary and Discussion

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