2024A&A...689A..87W


Query : 2024A&A...689A..87W

2024A&A...689A..87W - Astronomy and Astrophysics, volume 689A87 (2024/9-1)

TDCOSMO XV. Population analysis of lines of sight of 25 strong galaxy-galaxy lenses with extreme value statistics.

WELLS P.R., FASSNACHT C.D., BIRRER S. and WILLIAMS D.

Abstract (from CDS):

Context. Time-delay cosmography is a technique for measuring H0 with strong gravitational lensing. It requires a correction for line-of-sight perturbations, and thus it is necessary to build tools to assess populations of these lines of sight efficiently.
Aims. We demonstrate the techniques necessary to analyze line-of-sight effects at a population level, and investigate whether strong lenses fall in preferably overdense environments.
Methods. We analyzed a set of 25 galaxy-galaxy lens lines of sight in the Strong Lensing Legacy Survey sample using standard techniques, then performed a hierarchical analysis to constrain the population-level parameters. We introduce a new statistical model for these posteriors that may provide insight into the underlying physics of the system.
Reults. We find the median value of κext in the population model to be 0.033 ± 0.010. The median value of κext for the individual lens posteriors is 0.008 ± 0.015. Both approaches demostrate that our systems are drawn from an overdense sample. The different results from these two approaches show the importance of population models that do not multiply the effect of our priors.

Abstract Copyright: © The Authors 2024

Journal keyword(s): methods: data analysis - methods: statistical - surveys - cosmological parameters - cosmology: observations

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 SL2S J021247-055552 source G 02 12 47.8 -05 55 52           ~ 3 0
2 SL2S J021411-040502 source G 02 14 11.2 -04 05 03           ~ 3 0
3 SL2S J021737-051329 source G 02 17 37.0 -05 13 29           ~ 15 0
4 SL2S J021801-080247 source G 02 18 01.3 -08 02 47           ~ 2 0
5 SL2S J021902-082934 source G 02 19 02.1 -08 29 35           ~ 3 0
6 SL2S J022046-094927 source G 02 20 46.1 -09 49 28           ~ 2 0
7 SL2S J022511-045433 source LeG 02 25 11.0432107512 -04 54 33.577072956           ~ 7 0
8 SL2S J022610-042011 source G 02 26 10.0 -04 20 11           ~ 5 0
9 SL2S J023251-040823 source G 02 32 51.6 -04 08 24           ~ 3 0
10 SL2S J023307-043838 source G 02 33 07.1 -04 38 38           ~ 2 0
11 SL2S J084847-035103 source G 08 48 47.2 -03 51 04           ~ 3 0
12 SL2S J084909-041226 source G 08 49 09.5 -04 12 27           ~ 3 0
13 SL2S J085540-014730 source G 08 55 40.1 -01 47 30           ~ 3 0
14 SL2S J090106-025906 source G 09 01 06.0 -02 59 07           ~ 2 0
15 SL2S J090407-005952 source G 09 04 07.9 -00 59 53           ~ 3 0
16 SL2S J135949+553550 source G 13 59 49.6 +55 35 50           ~ 3 0
17 SL2S J140454+520024 source G 14 04 54.5 +52 00 24           ~ 3 0
18 SL2S J140546+524311 source G 14 05 46.2 +52 43 11           ~ 3 0
19 SL2S J140650+522619 source G 14 06 50.3 +52 26 19           ~ 3 0
20 SL2S J141137+565119 source G 14 11 37.0 +56 51 19           ~ 5 0
21 SL2S J142059+563007 source G 14 20 59.9 +56 30 08           ~ 3 0
22 SL2S J142731+551645 source G 14 27 31.3 +55 16 45           ~ 2 0
23 SL2S J220329+020518 source G 22 03 29.0 +02 05 19           ~ 4 0
24 SL2S J220506+014703 source G 22 05 06.9 +01 47 04           ~ 3 0
25 SL2S J222148+011542 source G 22 21 48.8 +01 15 43           ~ 3 0

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