2012A&A...538A..99S


Query : 2012A&A...538A..99S

2012A&A...538A..99S - Astronomy and Astrophysics, volume 538A, 99-99 (2012/2-1)

COSMOGRAIL: the COSmological MOnitoring of GRAvItational lenses. X. Modeling based on high-precision astrometry of a sample of 25 lensed quasars: consequences for ellipticity, shear, and astrometric anomalies.

SLUSE D., CHANTRY V., MAGAIN P., COURBIN F. and MEYLAN G.

Abstract (from CDS):

Gravitationally lensed quasars can be used as powerful cosmological and astrophysical probes. We can (i) infer the Hubble constant H0 based on the so-called time-delay technique, (ii) unveil substructures along the line-of-sight toward distant galaxies, and (iii) compare the shape and the slope of baryons and dark matter distributions in the inner regions of galaxies. To reach these goals, we need high-accuracy astrometry of the quasar images relative to the lensing galaxy and morphology measurements of the lens. In this work, we first present new astrometry for 11 lenses with measured time delays, namely, JVAS B0218+357, SBS 0909+532, RX J0911.4+0551, FBQS J0951+2635, HE 1104-1805, PG 1115+080, JVAS B1422+231, SBS 1520+530, CLASS B1600+434, CLASS B1608+656, and HE 2149-2745. These measurements proceed from the use of the Magain-Courbin-Sohy (MCS) deconvolution algorithm applied in an iterative way (ISMCS) to near-IR HST images. We obtain a typical astrometric accuracy of about 1-2.5 mas and an accurate shape measurement of the lens galaxy. Second, we combined these measurements with those of 14 other lensing systems, mostly from the COSMOGRAIL set of targets, to present new mass models of these lenses. The modeling of these 25 gravitational lenses led to the following results: 1) in four double-image quasars (HE0047-1746, J1226-006, SBS 1520+530, and HE 2149-2745), we show that the influence of the lens environment on the time delay can easily be quantified and modeled, hence putting these lenses with high priority for time-delay determination; 2) for quadruple-image quasars, the difficulty often encountered in reproducing the image positions to milli-arcsec accuracy (astrometric anomaly problem) is overcome by explicitly including the nearest visible galaxy/satellite in the lens model. However, one anomalous system (RXS J1131-1231) does not show any luminous perturber in its vicinity, and three others (WFI 2026-4536, WFI 2033-4723, and B2045+265) have problematic modeling. These four systems are the best candidates for a pertubation by a dark matter substructure along the line-of-sight; 3) we revisit the correlation between the position angle (PA) and ellipticity of the light and of the mass distribution in lensing galaxies. As in previous studies, we find a significant correlation between the PA of the light and of the mass distributions. However, in contrast with these same studies, we find that the ellipticity of the light and of the mass also correlate well, suggesting that the overall spatial distribution of matter is not very different from the baryon distribution in the inner ∼5kpc of lensing galaxies. This offers a new test for high-resolution hydrodynamical simulations.

Abstract Copyright:

Journal keyword(s): gravitational lensing: strong - quasars: general - techniques: image processing

CDS comments: HE 0047-1746 is a misprint for HE 0047-1756

Simbad objects: 72

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Number of rows : 72
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 [VV2006] J005027.8-174009 QSO 00 50 27.8233690104 -17 40 09.170215068           ~ 49 1
2 CLASS B0128+437 Rad 01 31 +44.0           ~ 59 0
3 [PBK93] B0218+357 G G 02 21 +35.9           ~ 27 1
4 RORF 0218+35A LeI 02 21 05.4667 +35 56 13.730           ~ 34 0
5 6C 021803+354230 BLL 02 21 05.4920852208 +35 56 13.848581904   20.0 20.0 19.60   ~ 559 3
6 RORF 0218+35B LeI 02 21 05.5 +35 56 14           ~ 31 0
7 4C 05.19 QSO 04 14 37.76734974 +05 34 42.3295956   24.100 23.800 21.270   ~ 360 2
8 [VV2006] J043814.8-122314 QSO 04 38 14.88 -12 17 14.6     17.15     ~ 222 2
9 [BCL98] RX J0911.4+0551 B LeI 09 11 27.35 +05 50 53.6           ~ 21 0
10 [KCH2000] L2 GiC 09 11 27.50 +05 50 53.3           ~ 23 1
11 [BCL98] RX J0911.4+0551 A1 LeI 09 11 27.55 +05 50 52.8           ~ 32 0
12 [BCL98] RX J0911.4+0551 A3 LeI 09 11 27.55 +05 50 53.7           ~ 25 0
13 JCMTSE J091127.6+055050 LeI 09 11 27.57 +05 50 53.2           ~ 21 0
14 QSO B0908+0603 QSO 09 11 27.6052 +05 50 54.281   18.44 18.16     ~ 232 2
15 [KFS97] 0909+532 G G 09 13 +53.0           ~ 14 2
16 QSO B0909+532B LeI 09 12.7 +53 00           ~ 23 1
17 QSO B0909+5312 QSO 09 13 01.031 +52 59 28.90   17.29 16.71     ~ 150 1
18 QSO J0924+0219 QSO 09 24 55.8048 +02 19 24.850   18.58 18.36     ~ 138 1
19 [VV98] J095122.6+263513 QSO 09 51 22.5840 +26 35 13.786   17.66 17.31     ~ 114 1
20 [SGB98] J0951+2635 C G 09 51 22.59 +26 35 14.1   20.25 20.00     ~ 22 1
21 [SGB98] J0951+2635 A LeQ 09 51 22.629 +26 35 13.98   17.66 17.31     ~ 19 1
22 [SGB98] J0951+2635 B LeQ 09 51 22.695 +26 35 13.32   18.55 18.25     ~ 19 1
23 8C 0958+561 QSO 10 01 20.6918953728 +55 53 55.593949272   17.16 16.95     ~ 735 3
24 QSO J1004+4112 QSO 10 04 34.9243842216 +41 12 42.771018060   19.14 19.03     ~ 191 1
25 [WKK93] G G 11 06 33.3 -18 21 23           ~ 35 1
26 QSO B1104-181 QSO 11 06 33.3845199936 -18 21 23.829049296   15.8 15.9 15.7   ~ 326 1
27 [BDW2002] q1104-1805a LeQ 11 06 33.50 -18 21 24.0     16.8     ~ 50 0
28 [BDW2002] q1104-1805b LeQ 11 06 33.60 -18 21 26.0     18.8     ~ 45 0
29 [WZA2016] pg1115 6 169.57063+07.76630 G 11 18 16.95 +07 45 58.7           ~ 47 1
30 QSO B1115+080A QSO 11 18 16.951 +07 45 58.23   16.61 16.44     ~ 684 2
31 [YDG81] QSO 1115+080 A1 LeI 11 18 17.09 +07 45 55.7           ~ 47 0
32 [YDG81] QSO 1115+080 A2 LeI 11 18 17.10 +07 45 56.1           ~ 45 0
33 2MASS J11315154-1231588 Sy1 11 31 51.5387 -12 31 58.716           ~ 270 1
34 QSO J1138+0314 QSO 11 38 03.7483141008 +03 14 57.657960780   19.42 19.17     ~ 62 1
35 [PEI2004] SDSS J1155+6346 gLS 11 55 17.3 +63 46 22           ~ 12 0
36 QSO J1226-0006 QSO 12 26 08.0332 -00 06 02.284   19.03 18.54     ~ 51 1
37 QSO J1415+1129 QSO 14 15 46.25 +11 29 43.4   17.63 17.23     ~ 650 0
38 [PBW92] 1422+231 C LeI 14 24 38.07 +22 55 59.9           ~ 47 0
39 [PBW92] 1422+231 B LeI 14 24 38.09 +22 56 00.6           ~ 49 0
40 [PBW92] 1422+231 E G 14 24 38.09 +22 56 00.7           ~ 41 1
41 QSO B1422+2309 BLL 14 24 38.0938 +22 56 00.587   16.77 15.84 14.79   ~ 450 1
42 [PBW92] 1422+231 gLS 14 24 38.09400 +22 56 00.5900   16.77 15.84 14.79   ~ 356 0
43 [PBW92] 1422+231 A AGN 14 24 38.1184835294 +22 56 00.871789934           ~ 48 0
44 [PBW92] 1422+231 D LeI 14 24 38.16 +22 55 59.8           ~ 39 0
45 [CVS97] NW * 15 21 44.63 +52 54 49.5   20.17 19.49     ~ 7 0
46 QSO B1520+530 QSO 15 21 44.8 +52 54 49   18.2       ~ 122 2
47 [CVS97] A LeI 15 21 44.91 +52 54 48.7   18.61 18.17     ~ 21 0
48 [CSB98] G G 15 21 45.03 +52 54 48.3           ~ 22 1
49 [CVS97] B LeI 15 21 45.11 +52 54 48.6   18.89 18.70     ~ 21 0
50 [FCK2002] M G 15 21 45.18 +52 54 49.4           ~ 3 0
51 [CVS97] SE * 15 21 45.29 +52 54 46.0     21.5     ~ 7 0
52 QSO B1600+4344 QSO 16 01 40.4818 +43 16 47.394   22.12 21.92     ~ 183 1
53 [JH97] B1600+434 A LeQ 16 01 40.5 +43 16 47           ~ 11 0
54 [JH97] B1600+434 B LeQ 16 01 41.2 +43 16 48           ~ 11 0
55 [JH97] B1600+434 Lens G 16 02 +43.3     22.5     ~ 23 1
56 [MFD95] 1608+656 D LeG 16 09 13.7741 +65 32 27.742           ~ 21 0
57 [MFD95] 1608+656 A LeG 16 09 13.9559 +65 32 28.999           ~ 22 0
58 NVSS J160914+653229 rG 16 09 13.96 +65 32 28.8     19.4     ~ 206 1
59 [KF99] 1608+656 G2 G 16 09 14.00 +65 32 29.3           ~ 11 0
60 [KF99] 1608+656 G1 G 16 09 14.00 +65 32 29.3           ~ 13 0
61 [MFD95] 1608+656 B LeG 16 09 14.0749 +65 32 27.037           ~ 21 0
62 [MFD95] 1608+656 C LeG 16 09 14.0759 +65 32 28.546           ~ 21 0
63 NAME 3C 330G2 Sy2 16 09 36.6 +65 56 43   20.33       ~ 275 1
64 QSO B1830-211 Bla 18 33 39.9399138048 -21 03 39.368838780     18.70 21   ~ 671 1
65 [VV2006] J202610.4-453627 QSO 20 26 10.45 -45 36 27.1           ~ 49 1
66 [VV2006] J203342.1-472343 QSO 20 33 42.12 -47 23 43.9           ~ 124 1
67 [VV2000] J204719.3+264340 QSO 20 47 20.3 +26 44 03     20.60     ~ 110 2
68 QSO B2149-2745 QSO 21 52 07.4534 -27 31 49.718   18.70 18.39     ~ 105 2
69 [WKL96] HE 2149-2745 G G 21 52 07.48 -27 31 49.3           ~ 23 1
70 QSO B2149-2745A LeQ 21 52 07.53 -21 31 49.9   17.13 16.82     ~ 15 1
71 QSO B2149-2745B LeQ 21 55 -27.4   18.70 18.39     ~ 12 1
72 HS 2209+1914 QSO 22 11 30.32568 +19 29 13.1496   15.4   15.55   ~ 21 0

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