4.7 Article

Cosmological simulations with self-interacting dark matter - I. Constant-density cores and substructure

Journal

MONTHLY NOTICES OF THE ROYAL ASTRONOMICAL SOCIETY
Volume 430, Issue 1, Pages 81-104

Publisher

OXFORD UNIV PRESS
DOI: 10.1093/mnras/sts514

Keywords

methods: numerical; galaxies: haloes; dark matter

Funding

  1. CONACyT
  2. NASA [NNX09AG01G, NNX09AD09G]
  3. Gary McCue Fellowship through the Center for Cosmology at UC Irvine
  4. NASA at UCI [NNX09AD09G]
  5. National Science Foundation (NSF) at UCI [0855462]
  6. NSF [0855462, NSF PHY11-25915]
  7. Miller Institute for Basic Research in Science
  8. Fullbright-MICINN
  9. Perimeter Institute of Theoretical Physics
  10. Government of Canada through Industry Canada
  11. Province of Ontario through the Ministry of Economic Development and Innovation
  12. NASA ATFP
  13. NASA [118606, NNX09AG01G, 120339, NNX09AD09G] Funding Source: Federal RePORTER
  14. Direct For Mathematical & Physical Scien
  15. Division Of Astronomical Sciences [1009973] Funding Source: National Science Foundation
  16. Division Of Physics
  17. Direct For Mathematical & Physical Scien [1214648, 0855462] Funding Source: National Science Foundation

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We use cosmological simulations to study the effects of self-interacting dark matter (SIDM) on the density profiles and substructure counts of dark-matter haloes from the scales of spiral galaxies to galaxy clusters, focusing explicitly on models with cross-sections over dark-matter particle mass sigma/m = 1 and 0.1 cm(2) g(-1). Our simulations rely on a new SIDM N-body algorithm that is derived self-consistently from the Boltzmann equation and that reproduces analytic expectations in controlled numerical experiments. We find that well-resolved SIDM haloes have constant-density cores, with significantly lower central densities than their cold dark matter (CDM) counterparts. In contrast, the subhalo content of SIDM haloes is only modestly reduced compared to CDM, with the suppression greatest for large hosts and small halo-centric distances. Moreover, the large-scale clustering and halo circular velocity functions in SIDM are effectively identical to CDM, meaning that all of the large-scale successes of CDM are equally well matched by SIDM. From our largest cross-section runs, we are able to extract scaling relations for core sizes and central densities over a range of halo sizes and find a strong correlation between the core radius of an SIDM halo and the NFW scale radius of its CDM counterpart. We construct a simple analytic model, based on CDM scaling relations, that captures all aspects of the scaling relations for SIDM haloes. Our results show that halo core densities in sigma/m = 1 cm(2) g(-1) models are too low to match observations of galaxy clusters, low surface brightness spirals (LSBs) and dwarf spheroidal galaxies. However, SIDM with sigma/m similar or equal to 0.1 cm(2) g(-1) appears capable of reproducing reported core sizes and central densities of dwarfs, LSBs and galaxy clusters without the need for velocity dependence. Higher resolution simulations over a wider range of masses will be required to confirm this expectation. We discuss constraints arising from the Bullet cluster observations, measurements of dark-matter density on small scales and subhalo survival requirements, and show that SIDM models with sigma/m similar or equal to 0.1 cm(2) g(-1) similar or equal to 0.2 barn GeV-1 are consistent with all observational constraints.

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