2014MNRAS.441..127G


Query : 2014MNRAS.441..127G

2014MNRAS.441..127G - Mon. Not. R. Astron. Soc., 441, 127-135 (2014/June-2)

Measuring gravitational lens time delays using low-resolution radio monitoring observations.

GURKAN G., JACKSON N., KOOPMANS L.V.E., FASSNACHT C.D. and BERCIANO ALBA A.

Abstract (from CDS):

Obtaining lensing time-delay measurements requires long-term monitoring campaigns with a high enough resolution (<1 arcsec) to separate the multiple images. In the radio, a limited number of high-resolution interferometer arrays make these observations difficult to schedule. To overcome this problem, we propose a technique for measuring gravitational time delays which relies on monitoring the total flux density with low-resolution but high-sensitivity radio telescopes to follow the variation of the brighter image. This is then used to trigger high-resolution observations in optimal numbers which then reveal the variation in the fainter image. We present simulations to assess the efficiency of this method together with a pilot project observing radio lens systems with the Westerbork Synthesis Radio Telescope to trigger Very Large Array observations. This new method is promising for measuring time delays because it uses relatively small amounts of time on high-resolution telescopes. This will be important because instruments that have high sensitivity but limited resolution, together with an optimum usage of follow-up high-resolution observations from appropriate radio telescopes may in the future be useful for gravitational lensing time-delay measurements by means of this new method.

Abstract Copyright: © 2014 The Authors Published by Oxford University Press on behalf of the Royal Astronomical Society (2014)

Journal keyword(s): gravitational lensing: strong - techniques: interferometric

Simbad objects: 18

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Number of rows : 18
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 CLASS B0445+123 rG 04 48 +12.4           ~ 24 0
2 ICRF J052109.8+163822 Sy1 05 21 09.88596258 +16 38 22.0515459   19.37 18.84 18.480   ~ 910 1
3 ICRF J054236.1+495107 Sy1 05 42 36.13789710 +49 51 07.2337139   18.45 17.80 17.210   ~ 1573 1
4 CLASS B0631+519 rG 06 35 +51.9           ~ 22 0
5 4C 33.21 QSO 07 35 55.5731 +33 07 09.728   21.0       ~ 41 1
6 CLASS B0739+366 LeQ 07 42 51 +36 34.7           ~ 18 0
7 CLASS B0850+054 rG 08 53 +05.2           ~ 25 0
8 QSO B1030+074 Bla 10 33 34.02429368 +07 11 26.1475933     20.34 20.22   ~ 111 2
9 GB6 B1140+1851 rG 11 43 26.06966082 +18 34 38.3598598           ~ 25 1
10 [VV2000] J115518.3+193942 QSO 11 55 18.2955044232 +19 39 42.228456840   17.15 16.89     ~ 100 2
11 3C 286 Sy1 13 31 08.2883506368 +30 30 32.960091564   17.51 17.25     ~ 4558 2
12 QSO B1422+2309 BLL 14 24 38.0938 +22 56 00.587   16.77 15.84 14.79   ~ 464 1
13 [PBW92] 1422+231 gLS 14 24 38.09400 +22 56 00.5900   16.77 15.84 14.79   ~ 359 0
14 4C 22.41 Rad 14 29 24.779 +21 48 01.77           ~ 11 1
15 NVSS J160914+653229 rG 16 09 13.93704 +65 32 27.9024     19.4     ~ 215 0
16 [MFD95] 1608+656 A LeG 16 09 13.9559 +65 32 28.999           ~ 22 0
17 FIRST J232140.7+052737 Rad 23 21 40.801 +05 27 37.23           ~ 29 1
18 4C 03.59 BLL 23 38 07.6549667136 +03 26 48.845665752   18.29 17.76     ~ 74 1

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