2011ApJ...727...96R


Query : 2011ApJ...727...96R

2011ApJ...727...96R - Astrophys. J., 727, 96 (2011/February-1)

The SL2S galaxy-scale lens sample. II. Cosmic evolution of dark and luminous mass in early-type galaxies.

RUFF A.J., GAVAZZI R., MARSHALL P.J., TREU T., AUGER M.W. and BRAULT F.

Abstract (from CDS):

We present a joint gravitational lensing and stellar-dynamical analysis of 11 early-type galaxies (median deflector redshift zd= 0.5) from Strong Lenses in the Legacy Survey (SL2S). Using newly measured redshifts and stellar velocity dispersions from Keck spectroscopy with lens models from Paper I, we derive the total mass-density slope inside the Einstein radius for each of the 11 lenses. The average total density slope is found to be = 2.16+0.09–0.09(), with an intrinsic scatter of 0.25+0.10–0.07. We also determine the dark matter fraction for each lens within half the effective radius, Reff/2, and find the average-projected dark matter mass fraction to be 0.42+0.08–0.08 with a scatter of 0.20+0.09–0.07 for a Salpeter initial mass function. By combining the SL2S results with those from the Sloan Lens ACS Survey (median zd= 0.2) and the Lenses Structure and Dynamics Survey (median zd= 0.8), we investigate cosmic evolution of γ' and find a mild trend ∂/∂z d= -0.25+0.10–0.12. This suggests that the total density profile of massive galaxies has become slightly steeper over cosmic time. If this result is confirmed by larger samples, it would indicate that dissipative processes played some role in the growth of massive galaxies since z ∼ 1.

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Journal keyword(s): dark matter - galaxies: elliptical and lenticular, cD - galaxies: evolution - galaxies: fundamental parameters - galaxies: structure - gravitational lensing: strong

Nomenclature: Table 2: SL2S JHHMMSS+DDMMSS N=11 added, SL2S JHHMMSS+DDMMSS source N=5.

Simbad objects: 28

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Number of rows : 28
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 Einstein Ring LeI 00 49 41.86 -27 52 25.7           ~ 28 1
2 HSCS J021411-040502 gLe 02 14 11.240 -04 05 02.71         19.07 ~ 20 0
3 SL2S J021737-051329 source G 02 17 37.0 -05 13 29           ~ 15 0
4 SDSS J021737.16-051329.5 rG 02 17 37.14752 -05 13 29.5242   23.372 22.054 21.102 19.12 ~ 51 0
5 SL2S J021902-082934 gLe 02 19 02.0 -08 29 34           ~ 14 0
6 SL2S J022056-063934 gLe 02 20 56.0 -06 39 34           ~ 6 0
7 FIRST J022511.0-045433 rG 02 25 11.0432107507 -04 54 33.577072969           ~ 21 2
8 SL2S J022511-045433 source LeG 02 25 11.0432107512 -04 54 33.577072956           ~ 7 0
9 SL2S J022610-042011 source G 02 26 10.0 -04 20 11           ~ 5 0
10 SL2S J022610-042011 gLe 02 26 10.0 -04 20 11           ~ 17 0
11 SL2S J022648-040610 gLe 02 26 48.0 -04 06 10           ~ 9 0
12 SL2S J022648-090421 gLe 02 26 48.0 -09 04 21           ~ 6 0
13 GAMA J023251.57-040823.8 gLe 02 32 51.58 -04 08 23.9           ~ 17 0
14 SL2S J140123+555705 gLe 14 01 23.0 +55 57 05           ~ 6 0
15 SL2S J140614+520252 gLe 14 06 14.0 +52 02 52           ~ 6 0
16 SL2S J141137+565119 gLe 14 11 37.0 +56 51 19           ~ 15 0
17 SL2S J141137+565119 source G 14 11 37.0 +56 51 19           ~ 5 0
18 QSO J1417+5226 QSO 14 17 35.738 +52 26 46.34           ~ 21 0
19 [MMN2007] A1 gLS 14 17 35.9 +52 26 46     21.53   19.69 ~ 66 0
20 H 1543+535 G 15 43 20.9 +53 51 52           ~ 17 1
21 NAME HST 15433+5352 System gLS 15 43 20.9 +53 51 52           ~ 21 0
22 QSO B2016+112 QSO 20 19 18.2 +11 27 14     22.5     ~ 195 1
23 SL2S J220629+005728 gLe 22 06 29.0 +00 57 28           ~ 6 0
24 SL2S J221326-000946 gLe 22 13 26.0 -00 09 46           ~ 12 0
25 SL2S J221407-180712 gLe 22 14 07.0 -18 07 12           ~ 6 0
26 SL2S J221606-175131 gLe 22 16 06.0 -17 51 31           ~ 3 0
27 SL2S J221929-001743 source G 22 19 29.0 -00 17 43           ~ 3 0
28 SL2S J221929-001743 gLe 22 19 29.0 -00 17 43           ~ 9 0

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