Surface density of dark matter haloes on galactic and cluster scales
AD Popolo, VF Cardone… - Monthly Notices of the …, 2013 - academic.oup.com
AD Popolo, VF Cardone, G Belvedere
Monthly Notices of the Royal Astronomical Society, 2013•academic.oup.comIn this paper, we analysed the correlation between the central surface density and the halo
core radius of galaxies, and cluster of galaxies dark matter (DM) haloes, in the framework of
the secondary infall model. We used Del Popolo secondary infall model taking into account
ordered and random angular momentum, dynamical friction and DM adiabatic contraction to
calculate the density profile of haloes, and then these profiles are used to determine the
surface density of DM haloes. The main result is that r*(the halo characteristic radius) is not a …
core radius of galaxies, and cluster of galaxies dark matter (DM) haloes, in the framework of
the secondary infall model. We used Del Popolo secondary infall model taking into account
ordered and random angular momentum, dynamical friction and DM adiabatic contraction to
calculate the density profile of haloes, and then these profiles are used to determine the
surface density of DM haloes. The main result is that r*(the halo characteristic radius) is not a …
Abstract
In this paper, we analysed the correlation between the central surface density and the halo core radius of galaxies, and cluster of galaxies dark matter (DM) haloes, in the framework of the secondary infall model. We used Del Popolo secondary infall model taking into account ordered and random angular momentum, dynamical friction and DM adiabatic contraction to calculate the density profile of haloes, and then these profiles are used to determine the surface density of DM haloes. The main result is that r* (the halo characteristic radius) is not a universal quantity as claimed by Donato et al. and Gentile et al. On the contrary, we find a correlation with the halo mass M200 in agreement with Cardone & Tortora, Boyarsky et al. and Napolitano, Romanowsky & Tortora, but with a significantly smaller scatter, namely 0.16 ± 0.05. We also consider the baryon column density finding this latter being indeed a constant for low-mass systems, such as dwarfs, but correlating with mass with a slope of α = 0.18 ± 0.05. In the case of the surface density of DM for a system composed only of DM, as in dissipationless simulations, we get α = 0.20 ± 0.05. These results leave little room for the recently claimed universality of (dark and stellar) column density.
Oxford University Press
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