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Hubble Space Telescope Combined Strong and Weak Lensing Analysis of the CLASH Sample: Mass and Magnification Models and Systematic Uncertainties

Authors :
Zitrin, Adi
Fabris, Agnese
Merten, Julian
Melchior, Peter
Meneghetti, Massimo
Koekemoer, Anton
Coe, Dan
Maturi, Matteo
Bartelmann, Matthias
Postman, Marc
Umetsu, Keiichi
Seidel, Gregor
Sendra, Irene
Broadhurst, Tom
Balestra, Italo
Biviano, Andrea
Grillo, Claudio
Mercurio, Amata
Nonino, Mario
Rosati, Piero
Bradley, Larry
Carrasco, Mauricio
Donahue, Megan
Ford, Holland
Frye, Brenda L.
Moustakas, John
Publication Year :
2014

Abstract

We present results from a comprehensive lensing analysis in HST data, of the complete CLASH cluster sample. We identify new multiple-images previously undiscovered allowing improved or first constraints on the cluster inner mass distributions and profiles. We combine these strong-lensing constraints with weak-lensing shape measurements within the HST FOV to jointly constrain the mass distributions. The analysis is performed in two different common parameterizations (one adopts light-traces-mass for both galaxies and dark matter while the other adopts an analytical, elliptical NFW form for the dark matter), to provide a better assessment of the underlying systematics - which is most important for deep, cluster-lensing surveys, especially when studying magnified high-redshift objects. We find that the typical (median), relative systematic differences throughout the central FOV are $\sim40\%$ in the (dimensionless) mass density, $\kappa$, and $\sim20\%$ in the magnification, $\mu$. We show maps of these differences for each cluster, as well as the mass distributions, critical curves, and 2D integrated mass profiles. For the Einstein radii ($z_{s}=2$) we find that all typically agree within $10\%$ between the two models, and Einstein masses agree, typically, within $\sim15\%$. At larger radii, the total projected, 2D integrated mass profiles of the two models, within $r\sim2\arcmin$, differ by $\sim30\%$. Stacking the surface-density profiles of the sample from the two methods together, we obtain an average slope of $d\log (\Sigma)/d\log(r)\sim-0.64\pm0.1$, in the radial range [5,350] kpc. Lastly, we also characterize the behavior of the average magnification, surface density, and shear differences between the two models, as a function of both the radius from the center, and the best-fit values of these quantities.<br />Comment: 35 pages (20 main text pages, plus 15 pages for additional figures and tables); 2 Tables, 17 Figures. V3: accepted version; some minor corrections and additions made. V4: corrected several entries in Table 2. All mass models and magnification maps are made publicly available for the community

Details

Database :
arXiv
Publication Type :
Report
Accession number :
edsarx.1411.1414
Document Type :
Working Paper
Full Text :
https://doi.org/10.1088/0004-637X/801/1/44