2018MNRAS.475.2403L


Query : 2018MNRAS.475.2403L

2018MNRAS.475.2403L - Mon. Not. R. Astron. Soc., 475, 2403-2414 (2018/April-1)

Mass density slope of elliptical galaxies from strong lensing and resolved stellar kinematics.

LYSKOVA N., CHURAZOV E. and NAAB T.

Abstract (from CDS):

We discuss constraints on the mass density distribution (parametrized as ρ ∝ r–γ) in early-type galaxies provided by strong lensing and stellar kinematics data. The constraints come from mass measurements at two 'pinch' radii. One 'pinch' radius r1 = 2.2REinst is defined such that the Einstein (i.e. aperture) mass can be converted into the spherical mass almost independently of the mass-model. Another 'pinch' radius r2 = Ropt is chosen so that the dynamical mass, derived from the line-of-sight velocity dispersion, is least sensitive to the anisotropy of stellar orbits. We verified the performance of this approach on a sample of simulated elliptical galaxies and on a sample of 15 SLACS lens galaxies at 0.01 <= z <= 0.35, which have already been analysed in Barnabe et al. by the self-consistent joint lensing and kinematic code. For massive simulated galaxies, the density slope γ is recovered with an accuracy of ∼13 per cent, unless r1 and r2 happen to be close to each other. For SLACS galaxies, we found good overall agreement with the results of Barnabe et al. with a sample-averaged slope γ = 2.1 ± 0.05. Although the two-pinch-radii approach has larger statistical uncertainties, it is much simpler and uses only few arithmetic operations with directly observable quantities.

Abstract Copyright: © 2018 The Author(s) Published by Oxford University Press on behalf of the Royal Astronomical Society

Journal keyword(s): gravitational lensing: strong - galaxies: elliptical and lenticular, cD - galaxies: kinematics and dynamics

Simbad objects: 15

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Number of rows : 15
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 SLACS SDSS J0037-0942 gLS 00 37 53.2145165976 -09 42 20.158898652           ~ 37 0
2 SLACS SDSS J0216-0813 gLS 02 16 52.5460001904 -08 13 45.314813820           ~ 34 0
3 SLACS SDSS J0912+0029 gLS 09 12 05.3091659568 +00 29 01.201406532           ~ 38 0
4 SLACS SDSS J0935-0003 gLS 09 35 43.933 -00 03 34.78           ~ 24 0
5 SLACS SDSS J0959+0410 gLS 09 59 44.0693722248 +04 10 17.036993460           ~ 34 0
6 SLACS SDSS J1204+0358 gLS 12 04 44.070 +03 58 06.40           ~ 30 0
7 SLACS SDSS J1250+0523 gLS 12 50 28.2624714720 +05 23 49.075233504           ~ 35 0
8 SLACS SDSS J1330-0148 gLS 13 30 45.5278367400 -01 48 41.586194484           ~ 13 0
9 SLACS SDSS J1443+0304 gLS 14 43 19.6212254016 +03 04 08.320747908           ~ 18 0
10 SLACS SDSS J1451-0239 gLS 14 51 28.1924331144 -02 39 36.467229672           ~ 25 0
11 SLACS SDSS J1627-0053 gLS 16 27 46.4442031920 -00 53 57.542699832           ~ 40 0
12 SLACS SDSS J2238-0754 gLS 22 38 40.2024029760 -07 54 56.006014176           ~ 31 0
13 SLACS SDSS J2300+0022 gLS 23 00 53.1509681304 +00 22 37.970088744           ~ 36 0
14 SLACS SDSS J2303+1422 gLS 23 03 21.7279540536 +14 22 17.928240960           ~ 36 0
15 SLACS SDSS J2321-0939 gLS 23 21 20.9352730488 -09 39 10.318081968           ~ 22 0

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