Weak lensing analysis of C1 1358+62 using Hubble Space Telescope observations

被引:265
作者
Hoekstra, H
Franx, M
Kuijken, K
Squires, G
机构
[1] Univ Groningen, Kapteyn Astron Inst, NL-9700 AV Groningen, Netherlands
[2] Univ Calif Berkeley, Ctr Particle Astrophys, Berkeley, CA 94720 USA
关键词
galaxies : clusters : individual (Cl 1358+62); galaxies : fundamental parameters; gravitational lensing;
D O I
10.1086/306102
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
We report on the detection of weak gravitational lensing of faint, distant background objects by Cl 1358+62, a rich cluster of galaxies at a redshift of z = 0.33. The observations consist of a large, multicolor mosaic of Hubble Space Telescope WFPC2 images. The number density of approximately 50 background objects arcmin(-2) allows us to do a detailed weak lensing analysis of this cluster. We detect a weak lensing signal out to similar to 1.5 Mpc from the cluster center. The observed distortion is consistent with a singular isothermal sphere model with a velocity dispersion of 780 +/- 50 km s(-1). The total projected mass within a radius of 1 Mpc corresponding to this model is (4.4 +/- 0.6) x 10(14) M.. The errors given here represent the random error due to the ellipticities of the background galaxies. The uncertainty in the redshift distribution introduces an additional systematic error of similar to 10% in the weak lensing mass. The weak lensing mass is slightly lower than dynamical estimates and agrees well with X-ray mass estimates. The mass distribution is elongated in a similar way as the light. The axis ratio of 0.30 +/- 0.15 and position angle of -21 degrees +/- 7 degrees were measured directly from the observations and agree very well with a previous strong lensing determination. A two-dimensional reconstruction of the cluster mass surface density shows that the peak of the mass distribution coincides with the peak of the light distribution. We find a value of (90 +/- 13)h(50) M. L-V.(-1) for the mass-to-light ratio, consistent with being constant with radius. The point-spread function of HST is highly anisotropic at the edges of the individual chips. This systematically perturbs the shapes of objects, and we present a method for applying the appropriate correction.
引用
收藏
页码:636 / 660
页数:25
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