2005MNRAS.364.1459C


Query : 2005MNRAS.364.1459C

2005MNRAS.364.1459C - Mon. Not. R. Astron. Soc., 364, 1459-1466 (2005/December-3)

Multipole models of four-image gravitational lenses with anomalous flux ratios.

CONGDON A.B. and KEETON C.R.

Abstract (from CDS):

It has been known for over a decade that many four-image gravitational lenses exhibit anomalous radio flux ratios. These anomalies can be explained by adding a clumpy cold dark matter (CDM) component to the background galactic potential of the lens. As an alternative, (Evans & Witt (2003)) recently suggested that smooth multipole perturbations provide a reasonable alternative to CDM substructure in some but not all cases. We generalize their method in two ways so as to determine whether multipole models can explain highly anomalous systems. We carry the multipole expansion to higher order, and also include external tidal shear as a free parameter. Fitting for the shear proves crucial to finding a physical (positive-definite density) model. For B1422+231, working to order kmax= 5 (and including shear) yields a model that is physical but implausible. Going to higher order (kmax≳ 9) reduces global departures from ellipticity, but at the cost of introducing small-scale wiggles in proximity to the bright images. These localized undulations are more pronounced in B2045+265, where kmax∼ 17 multipoles are required to smooth out large-scale deviations from elliptical symmetry. Such modes surely cannot be taken at face value; they must indicate that the models are trying to reproduce some other sort of structure. Our formalism naturally finds models that fit the data exactly, but we use B0712+472 to show that measurement uncertainties have little effect on our results. Finally, we consider the system B1933+503, where two sources are lensed by the same foreground galaxy. The additional constraints provided by the images of the second source render the multipole model unphysical. We conclude that external shear must be taken into account to obtain plausible models, and that a purely smooth angular structure for the lens galaxy does not provide a viable alternative to the prevailing CDM clump hypothesis.

Abstract Copyright: 2005 The Authors. Journal compilation © 2005 RAS

Journal keyword(s): gravitational lensing - galaxies: haloes - galaxies: structure - dark matter

Simbad objects: 25

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Number of rows : 25
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 [JNB98] B0712+472 A LeI 07 16 03.633 +47 08 50.12           ~ 14 0
2 [JNB98] B0712+472 B LeI 07 16 03.638 +47 08 49.96           ~ 14 0
3 QSO B0712+472 QSO 07 16 03.64335360 +47 08 50.2272600     23.0     ~ 116 2
4 [JNB98] B0712+472 C LeI 07 16 03.712 +47 08 49.45           ~ 12 0
5 [JNB98] B0712+472 D LeI 07 16 03.747 +47 08 50.58           ~ 12 0
6 [PBW92] 1422+231 C LeI 14 24 38.07 +22 55 59.9           ~ 49 0
7 [PBW92] 1422+231 B LeI 14 24 38.09 +22 56 00.6           ~ 51 0
8 QSO B1422+2309 BLL 14 24 38.0938 +22 56 00.587   16.77 15.84 14.79   ~ 464 1
9 [PBW92] 1422+231 gLS 14 24 38.09400 +22 56 00.5900   16.77 15.84 14.79   ~ 359 0
10 [PBW92] 1422+231 A AGN 14 24 38.1184835294 +22 56 00.871789934           ~ 50 0
11 [PBW92] 1422+231 D LeI 14 24 38.16 +22 55 59.8           ~ 39 0
12 CLASS B1555+375 LeQ 15 57 11.884 +37 21 35.80           ~ 45 0
13 [SBJ98] 4 Rad 19 34 30.899 +50 25 23.22           ~ 8 0
14 CLASS B1933+503 Rad 19 34 31.02 +50 25 23.5           ~ 85 1
15 [MKF2007] C LeI 20 47 20.26445 +26 44 01.9007           ~ 10 0
16 [MKF2007] B LeI 20 47 20.27594 +26 44 02.4428           ~ 10 0
17 [FBC99] 2045+265 A LeI 20 47 20.28593 +26 44 02.6911           ~ 8 0
18 [VV2000] J204719.3+264340 QSO 20 47 20.3 +26 44 03     20.60     ~ 112 2
19 [FBC99] 2045+265 D LeI 20 47 20.40736 +26 44 01.6847           ~ 8 0
20 QSO J2240+0321 QSO 22 40 30.234 +03 21 30.63           ~ 705 1
21 Z 378-15 AGN 22 40 30.23447 +03 21 30.6290           ~ 636 0
22 QSO B2237+0305D LeI 22 40 30.28 +03 21 29.3   18.98       ~ 78 0
23 QSO B2237+0305B LeI 22 40 30.30 +03 21 30.5   17.82       ~ 78 0
24 QSO B2237+0305A LeI 22 40 30.34 +03 21 28.8   17.96       ~ 90 0
25 QSO B2237+0305C LeI 22 40 30.38 +03 21 30.0   18.66       ~ 81 0

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