2011A&A...536A..44E


Query : 2011A&A...536A..44E

2011A&A...536A..44E - Astronomy and Astrophysics, volume 536A, 44-44 (2011/12-1)

Time delays for eleven gravitationally lensed quasars revisited.

EULAERS E. and MAGAIN P.

Abstract (from CDS):

We test the robustness of published time delays for 11 lensed quasars by using two techniques to measure time shifts in their light curves. We chose to use two fundamentally different techniques to determine time delays in gravitationally lensed quasars: a method based on fitting a numerical model and another one derived from the minimum dispersion method introduced by Pelt and collaborators. To analyse our sample in a homogeneous way and avoid bias caused by the choice of the method used, we apply both methods to 11 different lensed systems for which delays have been published: JVAS B0218+357, SBS 0909+523, RX J0911+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 Time delays for three double lenses, JVAS B0218+357, HE 1104-1805, and CLASS B1600+434, as well as the quadruply lensed quasar CLASS B1608+656 are confirmed within the error bars. We correct the delay for SBS 1520+530. For PG 1115+080 and RX J0911+0551, the existence of a second solution on top of the published delay is revealed. The time delays in four systems, SBS 0909+523, FBQS J0951+2635, JVAS B1422+231, and HE 2149-2745 prove to be less reliable than previously claimed. If we wish to derive an estimate of H0 based on time delays in gravitationally lensed quasars, we need to obtain more robust light curves for most of these systems in order to achieve a higher accuracy and robustness on the time delays.

Abstract Copyright:

Journal keyword(s): methods: numerical - cosmological parameters - quasars: general - gravitational lensing: strong

Simbad objects: 22

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Number of rows : 22
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2023
#notes
1 7C 021804.09+354230.00 QSO 02 21 05.4920852208 +35 56 13.848581904   20.0 20.0 19.60   ~ 542 3
2 [BCL98] RX J0911.4+0551 A1 LeI 09 11 27.55 +05 50 52.8           ~ 32 0
3 [BCL98] RX J0911.4+0551 A3 LeI 09 11 27.55 +05 50 53.7           ~ 25 0
4 JCMTSE J091127.6+055050 LeI 09 11 27.57 +05 50 53.2           ~ 21 0
5 QSO B0908+0603 QSO 09 11 27.6052 +05 50 54.281   18.44 18.16     ~ 228 2
6 QSO B0909+5312 QSO 09 13 01.031 +52 59 28.90   17.29 16.71     ~ 146 1
7 [VV98] J095122.6+263513 QSO 09 51 22.5840 +26 35 13.786   17.66 17.31     ~ 109 1
8 QSO B1104-181 QSO 11 06 33.3845199936 -18 21 23.829049296   15.8 15.9 15.7   ~ 323 1
9 QSO B1115+080A QSO 11 18 16.951 +07 45 58.23   16.61 16.44     ~ 676 2
10 [YDG81] QSO 1115+080 A1 LeI 11 18 17.09 +07 45 55.7           ~ 47 0
11 [YDG81] QSO 1115+080 A2 LeI 11 18 17.10 +07 45 56.1           ~ 45 0
12 [PBW92] 1422+231 C LeI 14 24 38.07 +22 55 59.9           ~ 46 0
13 [PBW92] 1422+231 B LeI 14 24 38.09 +22 56 00.6           ~ 48 0
14 QSO B1422+2309 BLL 14 24 38.0938 +22 56 00.587   16.77 15.84 14.79   ~ 444 1
15 [PBW92] 1422+231 gLS 14 24 38.09400 +22 56 00.5900   16.77 15.84 14.79   ~ 356 0
16 [PBW92] 1422+231 A AGN 14 24 38.1184835294 +22 56 00.871789934           ~ 47 0
17 QSO B1520+530 QSO 15 21 44.8 +52 54 49   18.2       ~ 122 2
18 [CVS97] A LeI 15 21 44.91 +52 54 48.7   18.61 18.17     ~ 21 0
19 [CVS97] B LeI 15 21 45.11 +52 54 48.6   18.89 18.70     ~ 21 0
20 QSO B1600+4344 QSO 16 01 40.4818 +43 16 47.394   22.12 21.92     ~ 181 1
21 NVSS J160914+653229 rG 16 09 13.96 +65 32 28.8     19.4     ~ 205 1
22 QSO B2149-2745 QSO 21 52 07.4534 -27 31 49.718   18.70 18.39     ~ 102 2

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2023.09.29-17:06:06

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