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The onset of gravothermal core collapse in velocity-dependent self-interacting dark matter subhaloes

2020/10/31 by Hannah C. Turner, Mark R. Lovell, Jesús Zavala +1 · 1 citation
Physics and Astronomy · #Astrophysics #Black hole (networking) #Cold dark matter #Cosmology and Gravitation Theories #Dark Matter and Cosmic Phenomena #Dark matter #Dark matter halo #Galaxies: Formation, Evolution, Phenomena #Galaxy #Halo #Instability #Mechanics #Milky Way #Physics #astro-ph.CO #astro-ph.GA

paper · pdf · doi:10.1093/mnras/stab1725

13 pages, 14 figures. Version accepted by MNRAS. Contact: [email protected]; doi: 10.1093/mnras/stab1725

openalex publication_date 2021/06/17 · arxiv created 2021/08/04 · arxiv updated 2021/08/05 · openalex created_date 2025/10/10 · openalex updated_date 2026/08/06

Abstract

ABSTRACT It has been proposed that gravothermal collapse due to dark matter self-interactions (i.e. self-interacting dark matter, SIDM) can explain the observed diversity of the Milky Way (MW) satellites’ central dynamical masses. We investigate the process behind this hypothesis using an N-body simulation of a MW-analogue halo with velocity-dependent SIDM (vdSIDM) in which the low-velocity self-scattering cross-section, σ \rm T/m\rm x, reaches 100 cm2 g−1; we dub this model the vd100 model. We compare the results of this simulation to simulations of the same halo that employ different dark models, including cold dark matter (CDM) and other, less extreme SIDM models. The masses of the vd100 haloes are very similar to their CDM counterparts, but the values of their maximum circular velocities, Vmax, are significantly higher. We determine that these high Vmax subhaloes were objects in the mass range [5 × 106, 1 × 108] M⊙ at z = 1 that undergo gravothermal core collapse. These collapsed haloes have density profiles that are described by single power laws down to the resolution limit of the simulation, and the inner slope of this density profile is approximately −3. Resolving the ever decreasing collapsed region is challenging, and tailored simulations will be required to model the runaway instability accurately at scales <1 kpc.

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