Abstract

The disparity between the density profiles of galactic dark matter haloes predicted by dark matter only cosmological simulations and those inferred from rotation curve decomposition, the so-called cusp–core problem, suggests that baryonic physics has an impact on dark matter density in the central regions of galaxies. Using a Markov Chain Monte Carlo analysis of galactic rotation curves we constrain density profiles and an estimated minimum radius for baryon influence, r1, which we couple with a feedback model to give an estimate of the fraction of matter within that radius that must be expelled to produce the observed halo profile. We examine the rotation curves of eight galaxies taken from the THINGS (The HI Nearby Galaxy Survey) data set and determine constraints on the radial density profiles of their dark matter haloes. For some of the galaxies, both cored haloes and cosmological ρ ∝ r−1 cusps are excluded which requires finely tuned baryonic feedback. For galaxies which exhibit extended cores in their haloes (e.g. NGC 925), the use of a split power-law halo profile yields models without the unphysical, sharp features seen in models based on the Einasto profile. We have found there is no universal halo profile which can describe all the galaxies studied here.

Highlights

  • Disc galaxies are presumed by CDM cosmology to be dominated by dark matter (e.g. Bosma 1978)

  • We will briefly summarize our data processing chain: first, the method used by de Blok et al (2008) to derive rotation curves from the The HI Nearby Galaxy Survey (THINGS) velocity fields; secondly, the halo density profile we fit to these data and the parameter space defined by it; and the Markov Chain Monte Carlo (MCMC) method that we use to constrain the density profiles of the dark matter haloes

  • Once we have generated distributions of density profiles for each galaxy, we investigate their systematic properties, with reference to previous claims regarding the nature of dark matter haloes

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Summary

Introduction

Disc galaxies are presumed by CDM cosmology to be dominated by dark matter (e.g. Bosma 1978). Dark matter-only cosmological simulations were found by Dubinski & Carlberg (1991) and Navarro, Frenk & White (1996) to produce haloes with an approximately universal density profile, with density proportional to r−1 towards r = 0 and r−3 towards r = ∞. These haloes follow a set of scaling relations with virial mass such that they behave as a single parameter family of models (Bullock et al 2001). The halo density profiles inferred from observing the rotation of disc galaxies appear to contradict this picture. This, coupled with an increase in resolution of kinematic data, has at this point resolved such concerns

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