Abstract

We analyze the cold dark matter density profiles of 54 galaxy halos simulated with FIRE-2 galaxy formation physics, each resolved within 0.5%0.5\% of the halo virial radius. These halos contain galaxies with masses that range from ultra-faint dwarfs (M⋆≃104.5M⊙M_\star \simeq 10^{4.5} M_{\odot}) to the largest spirals (M⋆≃1011M⊙M_\star \simeq 10^{11} M_{\odot}) and have density profiles that are both cored and cuspy. We characterize our results using a new analytic density profile that extends the standard Einasto form to allow for a pronounced constant-density core in the resolved innermost radius. With one additional core-radius parameter, rcr_{c}, this "core-Einasto" profile is able to characterize the shape and normalization of our feedback-impacted dark matter halos. In order to enable comparisons with observations, we provide fitting functions for rcr_{c} and other profile parameters as a function of both M⋆M_\star and M⋆/MhaloM_{\star}/M_{\rm halo}. In agreement with similar studies done in the literature, we find that dark matter core formation is most efficient at the characteristic stellar-mass to halo-mass ratio M⋆/Mhalo≃5×10−3M_\star/M_{\rm halo} \simeq 5 \times 10^{-3}, or M⋆∼109 M⊙M_{\star} \sim 10^9 \, M_{\odot}, with cores that are roughly the size of the galaxy half-light radius, rc≃1−5r_{c} \simeq 1-5 kpc. Furthermore, we find no evidence for core formation at radii ≳100 pc\gtrsim 100\ \rm pc in galaxies with M⋆/Mhalo<5×10−4M_{\star}/M_{\rm halo} < 5\times 10^{-4} or M⋆≲106 M⊙M_\star \lesssim 10^6 \, M_{\odot}. For Milky Way-size galaxies, baryonic contraction often makes halos significantly more concentrated and dense at the stellar half-light radius than dark matter only runs. However, even at the Milky Way scale, FIRE-2 galaxy formation still produces small dark matter cores of ≃0.5−2\simeq 0.5-2 kpc in size. Recent evidence for a ∼2{\sim} 2 kpc core in the Milky Way's dark matter halo is consistent with this expectation.

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