2006ApJ...642...22Y


Query : 2006ApJ...642...22Y

2006ApJ...642...22Y - Astrophys. J., 642, 22-29 (2006/May-1)

Halo structures of gravitational lens galaxies.

YOO J., KOCHANEK C.S., FALCO E.E. and McLEOD B.A.

Abstract (from CDS):

We explore the halo structure of four gravitational lenses with well-observed, thin Einstein rings. We find that the gravitational potentials are well described by ellipsoidal density distributions in the sense that the best-fit nonellipsoidal models have parameters consistent with their ellipsoidal counterparts. We find upper limits on the standard parameters for the deviation from an ellipse of|aB3/a0|<0.023, 0.019, 0.037, and 0.035 and|aB4/a0|<0.034, 0.041, 0.051, and 0.064 for SDSS J0924+0219, HE 0435-1223, B1938+666, and PG 1115+080, respectively. We find that the lens galaxies are at the centers of their dark matter halos and obtain upper limits for the offset of each center of mass from the center of light of|Δx|<0".004, 0".005, 0".009, and 0".005, corresponding to 22, 29, 70, and 23 pc, respectively. These limits also exclude the possibility of any significant lopsidedness of the dark matter halos and set an upper limit of fsat≲sqrt(N)% on the mass fraction of massive substructures inside the Einstein ring if they are divided over N satellites. We also explore the properties of galaxies as substructures in groups for the lens PG 1115+080, finding evidence for dark matter halos associated with the galaxies but no evidence for a clear distinction between satellite and central galaxies.

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Journal keyword(s): Cosmology: Observations - Cosmology: Dark Matter - Cosmology: Gravitational Lensing - quasars: individual (B1938+666) - quasars: individual (HE 0435-1223) - Galaxies: Quasars: Individual: Alphanumeric: PG 1115+080 - quasars: individual (SDSS J0924+0219)

Simbad objects: 30

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Number of rows : 30
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 [MKP2005] G22 G 04 38 14.724 -12 17 18.20     22.253   21.260 ~ 16 1
2 [WSB2002] 0435-1223 C LeQ 04 38 14.73 -12 17 15.0     19.149   19.631 ~ 39 0
3 [WSB2002] 0435-1223 B LeQ 04 38 14.80 -12 17 13.8     19.082   19.623 ~ 43 0
4 [WSB2002] 0435-1223 D LeQ 04 38 14.84 -12 17 16.0     19.196   19.824 ~ 42 0
5 [VV2006] J043814.8-122314 QSO 04 38 14.88 -12 17 14.6     17.15     ~ 245 2
6 [WSB2002] 0435-1223 G G 04 38 14.88 -12 17 14.6     20.80   19.83 ~ 25 0
7 [WSB2002] 0435-1223 A LeQ 04 38 14.90 -12 17 14.4     18.545   19.106 ~ 41 0
8 [IBB2003] SDSS J0924+0219 C LeI 09 24 55.7659 +02 19 24.691           ~ 17 0
9 [IBB2003] SDSS J0924+0219 gLS 09 24 55.80 +02 19 24.8           ~ 26 0
10 QSO J0924+0219 QSO 09 24 55.8048 +02 19 24.850   18.58 18.36     ~ 142 1
11 [IBB2003] SDSS J0924+0219 G G 09 24 55.8185 +02 19 24.509           ~ 12 1
12 [IBB2003] SDSS J0924+0219 A LeI 09 24 55.8293 +02 19 25.356           ~ 24 0
13 [IBB2003] SDSS J0924+0219 B LeI 09 24 55.8327 +02 19 23.565           ~ 23 0
14 [IBB2003] SDSS J0924+0219 D LeI 09 24 55.8653 +02 19 24.897           ~ 14 0
15 QSO J1004+4112 LeQ 10 04 34.9243842216 +41 12 42.771018060   19.14 19.03     ~ 206 1
16 SDSS J111815.50+074547.6 G 11 18 15.50551 +07 45 47.6543     20.40   17.9 ~ 15 0
17 SDSS J111815.97+074546.3 G 11 18 15.96857 +07 45 46.3513     21.69   19.6 ~ 11 0
18 [IFK98] G9 G 11 18 15.97 +07 45 54.6         22.05 ~ 6 0
19 SDSS J111816.09+074557.7 G 11 18 16.08318 +07 45 57.9183     21.05   19.0 ~ 13 0
20 [IFK98] G11 G 11 18 16.2 +07 45 56     22.98     ~ 3 0
21 [WZA2016] pg1115 6 169.57063+07.76630 G 11 18 16.95 +07 45 58.7           ~ 47 1
22 QSO B1115+080A QSO 11 18 16.951 +07 45 58.23   16.61 16.44     ~ 703 2
23 QSO B1115+080B QSO 11 18 16.98 +07 45 55.7   18.74 18.1     ~ 53 0
24 QSO B1115+080C QSO 11 18 17.00 +07 45 57.7   18.26 17.6     ~ 57 0
25 [IFK98] G15 G 11 18 17.1 +07 45 47           ~ 3 0
26 [IFK98] G14 G 11 18 17.2 +07 45 52           ~ 3 0
27 [IFK98] G13 G 11 18 17.5 +07 45 56           ~ 3 0
28 NVSS J193825+664853 Rad 19 38 25.28898 +66 48 52.9152           ~ 117 2
30 [TK2000] B1938 GL G ~ ~           ~ 9 1

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