2016MNRAS.456..870B


Query : 2016MNRAS.456..870B

2016MNRAS.456..870B - Mon. Not. R. Astron. Soc., 456, 870-884 (2016/February-2)

Light versus dark in strong-lens galaxies: dark matter haloes that are rounder than their stars.

BRUDERER C., READ J.I., COLES J.P., LEIER D., FALCO E.E., FERRERAS I. and SAHA P.

Abstract (from CDS):

We measure the projected density profile, shape and alignment of the stellar and dark matter mass distribution in 11 strong-lens galaxies. We find that the projected dark matter density profile - under the assumption of a Chabrier stellar initial mass function - shows significant variation from galaxy to galaxy. Those with an outermost image beyond ∼ 10 kpc are very well fit by a projected Navarro-Frenk-White (NFW) profile; those with images within 10 kpc appear to be more concentrated than NFW, as expected if their dark haloes contract due to baryonic cooling. We find that over several half-light radii, the dark matter haloes of these lenses are rounder than their stellar mass distributions. While the haloes are never more elliptical than edm = 0.2, their stars can extend to e* > 0.2. Galaxies with high dark matter ellipticity and weak external shear show strong alignment between light and dark; those with strong shear (γ ≳ 0.1) can be highly misaligned. This is reassuring since isolated misaligned galaxies are expected to be unstable. Our results provide a new constraint on galaxy formation models. For a given cosmology, these must explain the origin of both very round dark matter haloes and misaligned strong-lens systems.

Abstract Copyright: © 2015 The Authors Published by Oxford University Press on behalf of the Royal Astronomical Society (2015)

Journal keyword(s): gravitational lensing: strong - galaxies: elliptical and lenticular, cD - galaxies: formation - galaxies: haloes - galaxies: structure

Simbad objects: 26

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Number of rows : 26
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 [WHL96] 0047-2808 lensed G LeG 00 49 41.88 -27 52 25.7           ~ 19 1
2 QSO B0047-2808 G 00 49 41.896 -27 52 25.35   21.2   20.1   ~ 40 1
3 [HTL92] MG J0414+0534 system gLS 04 14 37.7 +05 34 42           ~ 23 0
4 [HTL92] G G 04 14 37.70 +05 34 43.0     24.4     ~ 37 1
5 4C 05.19 QSO 04 14 37.76734974 +05 34 42.3295956   24.100 23.800 21.270   ~ 371 2
6 QSO B0712+472 QSO 07 16 03.64335360 +47 08 50.2272600     23.0     ~ 116 2
7 [FC98] B0712+472 G G 07 16 03.65 +47 08 50.6           ~ 19 1
8 [KCH2000] L2 GiC 09 11 27.50 +05 50 53.3           ~ 23 1
9 QSO B0908+0603 QSO 09 11 27.6052 +05 50 54.281   18.44 18.16     ~ 248 2
10 8C 0958+561 QSO 10 01 20.6918953728 +55 53 55.593949272   17.16 16.95     ~ 757 3
11 YGKOW G1 G 10 01 20.86 +55 53 50.7           ~ 51 1
12 [WZA2016] pg1115 6 169.57063+07.76630 G 11 18 16.95 +07 45 58.7           ~ 47 1
14 QSO B1115+080A QSO 11 18 16.951 +07 45 58.23   16.61 16.44     ~ 703 2
15 [PBW92] 1422+231 E G 14 24 38.09 +22 56 00.7           ~ 41 1
16 QSO B1422+2309 BLL 14 24 38.0938 +22 56 00.587   16.77 15.84 14.79   ~ 464 1
17 [PBW92] 1422+231 gLS 14 24 38.09400 +22 56 00.5900   16.77 15.84 14.79   ~ 359 0
18 NAME 3C 330G2 Sy2 16 09 34.92456720 +65 56 37.8351240   20.33       ~ 280 1
19 [LSS84] 2016+112 D G 20 19 18.07 +11 27 13.2           ~ 34 1
20 NAME MG 2016+112 System gLS 20 19 18.1 +11 27 11           ~ 17 0
21 QSO B2016+112 QSO 20 19 18.2 +11 27 14     22.5     ~ 195 1
22 [VV2000] J204719.3+264340 QSO 20 47 20.3 +26 44 03     20.60     ~ 112 2
23 [FBC99] 2045+265 E rG 20 47 20.36859 +26 44 01.8840           ~ 21 1
25 QSO J2240+0321 QSO 22 40 30.234 +03 21 30.63           ~ 705 1
26 Z 378-15 AGN 22 40 30.23447 +03 21 30.6290           ~ 636 0

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