2009ApJ...698.2093D


Query : 2009ApJ...698.2093D

2009ApJ...698.2093D - Astrophys. J., 698, 2093-2113 (2009/June-3)

The cusp/core problem and the secondary infall model.

DEL POPOLO A.

Abstract (from CDS):

We study the cusp/core problem using a secondary infall model that takes into account the effect of ordered and random angular momentum, dynamical friction, and baryons adiabatic contraction (AC). The model is applied to structures on galactic scales (normal and dwarfs spiral galaxies) and on clusters of galaxies scales. Our analysis suggest that angular momentum and dynamical friction are able, on galactic scales, to overcome the competing effect of AC eliminating the cusp. The slope of density profile of inner halos flattens with decreasing halo mass and the profile is well approximated by a Burkert's profile. In order to obtain the Navarro-Frenk-White (NFW) profile, starting from the profiles obtained from our model, the magnitude of angular momentum and dynamical friction must be reduced with respect to the values predicted by the model itself. The rotation curves of four lower sideband galaxies from Gentile et al. are compared to the rotation curves obtained by the model in the present paper obtaining a good fit to the observational data. The time evolution of the density profile of a galaxy of 108-109 M☉ shows that after a transient steepening, due to the AC, the density profile flattens to α ≃ 0. On cluster scales we observe a similar evolution of the dark matter (DM) density profile but in this case the density profile slope flattens to α ≃ 0.6 for a cluster of ≃1014 M☉. The total mass profile, differently from that of DM, shows a central cusp well fitted by an NFW model.

Abstract Copyright: ∼

Journal keyword(s): cosmology: theory - galaxies: formation - large-scale structure of universe

Simbad objects: 12

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Number of rows : 12
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 NGC 360 Sy2 01 02 51.4684833528 -65 36 35.652293964   13.42   11.99 12.5 ~ 103 0
2 NGC 1090 AG? 02 46 33.9359016984 -00 14 49.627749660   12.3   12.1 12.4 ~ 178 0
3 ESO 116-12 EmG 03 13 04.746 -57 21 26.09   12.96   12.07 12.2 ~ 103 0
4 ACO 426 ClG 03 19 47.6 +41 30 54           ~ 2508 1
5 NGC 2976 GiG 09 47 15.458 +67 54 58.97 11.77 11.03 10.16 9.51   ~ 712 1
6 NGC 4605 GiG 12 39 59.2837284936 +61 36 32.822365392   10.94   10.35   ~ 347 2
7 Z 318-18 G 15 09 08.0 +67 13 21   13.60 10.6     ~ 1459 0
8 NGC 5949 AG? 15 28 00.6695692032 +64 45 47.413223532   12.70       ~ 152 0
9 NGC 5963 EmG 15 33 27.7333715909 +56 33 33.938950529   13.34 13.65     ~ 113 0
10 NGC 6689 AG? 18 34 50.244 +70 31 26.00   12.60       ~ 128 0
11 ESO 287-13 AG? 21 23 13.9872161040 -45 46 23.292820920   12.94   11.84 12.4 ~ 83 0
12 ClG 2137-2353 ClG 21 40 12.8 -23 39 27     18.5     ~ 390 0

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