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An Off-center Density Peak in the Milky Way's Dark Matter Halo?

  • Authors: Michael Kuhlen, Javiera Guedes, Annalisa Pillepich, Piero Madau, and Lucio Mayer

Kuhlen et al. 2013 The Astrophysical Journal 765 10.

  • Provider: AAS Journals

Caption: Figure 5.

Evolution of the inner DM density profiles. Top: density profiles at z = 3, 2, 1.5, 1, 0.5, and 0 for Eris (left) and ErisDark (right). All quantities are plotted in proper units. The black dotted lines indicate the best-fitting modified Burkert profile (see Equation (1)). The location of r 5000, the radius enclosing 5000 DM particles, is indicated with squares. r 5000 corresponds to the density profile convergence radius in ErisDark at z = 0. For Eris the density profile can be trusted to smaller radii due to its larger particle counts, and so we additionally mark r 1000 with a circle. The vertical bars indicate r = 3 epsilon soft. Bottom: the evolution of the logarithmic slope ( dln ρ/ dln  r) measured at different radii: the symbols and thick lines correspond to the slopes at r 5000, and for Eris we also show the slope at r 1000. All lines are boxcar averages over 10 outputs. This plot shows that baryonic physics in Eris leads to the flattening of the central density profile. This flattening appears to be correlated with the growth of the DM offset (see Figure  4). We emphasize that these slopes are not asymptotic slopes, and a value of less than −1 does not imply a strongly cusped profile all the way to the center, but merely indicates the local slope at r 5000, which may lie outside of the scale radius at early times.

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