2014ApJ...788..190W


Query : 2014ApJ...788..190W

2014ApJ...788..190W - Astrophys. J., 788, 190 (2014/June-3)

A comparison of cosmological models using time delay lenses.

WEI J.-J., WU X.-F. and MELIA F.

Abstract (from CDS):

The use of time-delay gravitational lenses to examine the cosmological expansion introduces a new standard ruler with which to test theoretical models. The sample suitable for this kind of work now includes 12 lens systems, which have thus far been used solely for optimizing the parameters of ΛCDM. In this paper, we broaden the base of support for this new, important cosmic probe by using these observations to carry out a one-on-one comparison between competing models. The currently available sample indicates a likelihood of ∼70%-80% that the Rh= ct universe is the correct cosmology versus ∼20%-30% for the standard model. This possibly interesting result reinforces the need to greatly expand the sample of time-delay lenses, e.g., with the successful implementation of the Dark Energy Survey, the VST ATLAS survey, and the Large Synoptic Survey Telescope. In anticipation of a greatly expanded catalog of time-delay lenses identified with these surveys, we have produced synthetic samples to estimate how large they would have to be in order to rule out either model at a ∼99.7% confidence level. We find that if the real cosmology is ΛCDM, a sample of ∼150 time-delay lenses would be sufficient to rule out Rh= ct at this level of accuracy, while ∼1000 time-delay lenses would be required to rule out ΛCDM if the real universe is instead Rh= ct. This difference in required sample size reflects the greater number of free parameters available to fit the data with ΛCDM.

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Journal keyword(s): cosmology: observations - cosmology: theory - galaxies: halos - galaxies: structure - gravitational lensing: strong - quasars: general

Simbad objects: 23

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Number of rows : 23
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 [SMS87] 0142-100 G G 01 44 -09.7           ~ 23 1
2 QSO B0142-100 QSO 01 45 16.5958283760 -09 45 17.265131352   17.23 16.95     ~ 247 1
3 [PBK93] B0218+357 G G 02 21 +35.9           ~ 27 1
4 6C 021803+354230 BLL 02 21 05.4920852208 +35 56 13.848581904   20.0 20.0 19.60   ~ 603 3
5 [KFS97] 0909+532 G G 09 13 +53.0           ~ 14 2
6 QSO B0909+5312 QSO 09 13 01.031 +52 59 28.90   17.29 16.71     ~ 157 1
7 [VV98] J095122.6+263513 QSO 09 51 22.5840 +26 35 13.786   17.66 17.31     ~ 120 1
8 [SGB98] J0951+2635 C G 09 51 22.59 +26 35 14.1   20.25 20.00     ~ 22 1
9 8C 0958+561 QSO 10 01 20.6918953728 +55 53 55.593949272   17.16 16.95     ~ 757 3
10 YGKOW G1 G 10 01 20.86 +55 53 50.7           ~ 51 1
11 [WKK93] G G 11 06 33.3 -18 21 23           ~ 35 1
12 QSO B1104-181 QSO 11 06 33.3845199936 -18 21 23.829049296   15.8 15.9 15.7   ~ 338 1
13 [VV2006] J120629.6+433217 QSO 12 06 29.6568052152 +43 32 17.587941108   17.93 17.74     ~ 48 0
14 [OIH2005] SDSS J1206+4332 G1 G 12 06 29.6965 +43 32 19.339           ~ 9 0
15 QSO B1520+530 QSO 15 21 44.8 +52 54 49   18.2       ~ 123 2
16 [CSB98] G G 15 21 45.03 +52 54 48.3           ~ 22 1
17 QSO B1600+4344 QSO 16 01 40.4818 +43 16 47.394   22.12 21.92     ~ 188 1
18 [JH97] B1600+434 Lens G 16 02 +43.3     22.5     ~ 23 1
19 QSO J1650+4251 QSO 16 50 43.4447423448 +42 51 49.367524032   17.78 17.58     ~ 67 1
20 [MSR2003] J1650+4251 G G 16 50 43.4448 +42 51 49.221           ~ 9 1
21 QSO B1830-211 Bla 18 33 39.9399138048 -21 03 39.368838780     18.70 21   ~ 724 1
22 QSO B2149-2745 QSO 21 52 07.4534 -27 31 49.718   18.70 18.39     ~ 108 2
23 [WKL96] HE 2149-2745 G G 21 52 07.48 -27 31 49.3           ~ 23 1

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