1105.0090 (A. Del Popolo)
A. Del Popolo
In the present paper, we study how the dark matter density profiles of dwarfs
galaxies in the mass range $10^8-10^{10} M_{\odot}$ are modified by the
interaction of the dwarf in study with the neighboring structures, and by
changing baryon fraction in dwarfs. As already shown in Del Popolo (2009), the
slope of density profile of inner halos flattens with decreasing halo mass and
the profile is well approximated by a Burkert's profile. The analysis shows
that dwarfs who suffered a smaller tidal torquing (consequently having smaller
angular momentum) are characterized by steeper profiles with respect to dwarfs
subject to higher torque, and similarly dwarfs having a smaller baryons
fraction have also steeper profiles than those having a larger baryon fraction.
In the case tidal torquing is shut down and baryons are not present, the
density profile is very well approximated by an Einasto profile, similarly to
dwarfs obtained in dissipationless N-body simulations. We then apply the result
of the previous analysis to the dark matter halo rotation curves of three
different dwarfs, namely NGC 2976, known to have a flat inner core, NGC 5949
having a profile intermediate between a cored and a cuspy one, and NGC 5963
having a cuspy profile. After calculating baryon fraction, which is $\simeq
0.1$ for the three galaxies, we fitted the rotation curves changing the value
of angular momentum. NGC 2976, has an higher value of ordered angular momentum
($\lambda \simeq 0.04$) with respect to NGC 5949 ($\lambda \simeq 0.025$) and
in the case of NGC 5963 the very steep profile can be obtained with a low value
of $\lambda$ ($\lambda \simeq 0.02$) and also decreasing the value of the
random angular momentum. In the case of NGC 2976 tidal interaction with M81
could have also influenced the inner part of the density profile.
View original:
http://arxiv.org/abs/1105.0090
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