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http://dx.doi.org/10.5303/PKAS.2015.30.2.389

DISCOVERY OF A STRONG LENSING GALAXY EMBEDDED IN A CLUSTER AT z = 1.62  

WONG, KENNETH C. (Institute of Astronomy and Astrophysics, Academia Sinica (ASIAA))
TRAN, KIM-VY H. (George P. and Cynthia W. Mitchell Institute for Fundamental Physics and Astronomy, Department of Physics & Astronomy, Texas A&M University)
SUYU, SHERRY H. (Institute of Astronomy and Astrophysics, Academia Sinica (ASIAA))
MOMCHEVA, IVELINA G. (Astronomy Department, Yale University)
BRAMMER, GABRIEL B. (Space Telescope Science Institute)
BRODWIN, MARK (Department of Physics and Astronomy, University of Missouri)
GONZALEZ, ANTHONY H. (Department of Astronomy, University of Florida)
HALKOLA, ALEKSI (Institute of Astronomy and Astrophysics, Academia Sinica (ASIAA))
KACPRZAK, GLENN G. (Swinburne University of Technology)
KOEKEMOER, ANTON M. (Space Telescope Science Institute)
PAPOVICH, CASEY J. (George P. and Cynthia W. Mitchell Institute for Fundamental Physics and Astronomy, Department of Physics & Astronomy, Texas A&M University)
RUDNICK, GREGORY H. (Department of Physics and Astronomy, The University of Kansas)
Publication Information
Publications of The Korean Astronomical Society / v.30, no.2, 2015 , pp. 389-392 More about this Journal
Abstract
We identify a strong lensing galaxy in the cluster IRC 0218 that is spectroscopically confirmed to be at z = 1.62, making it the highest-redshift strong lens galaxy known. The lens is one of the two brightest cluster galaxies and lenses a background source galaxy into an arc and a counterimage. With Hubble Space Telescope (HST) grism and Keck/LRIS spectroscopy, we measure the source redshift to be $z_S=2.26$. Using HST imaging, we model the lens mass distribution with an elliptical power-law profile and account for the effects of the cluster halo and nearby galaxies. The Einstein radius is $^{\theta}E=0.38^{+0.02{\prime}{\prime}}_{-0.01}$ ($3.2^{+0.2}_{-0.1}kpc$) and the total enclosed mass is $M_{tot}(<^{\theta}_E)=1.8^{+0.2}_{-0.1}{\times}10^{11}M_{\odot}$. We estimate that the cluster environment contributes ~ 10% of this total mass. Assuming a Chabrier IMF, the dark matter fraction within $^{\theta}E$ is $f^{Chab}_{DM}=0.3^{+0.1}_{-0.3}$, while a Salpeter IMF is marginally inconsistent with the enclosed mass ($f^{Salp}_{DM}=-0.3^{+0.2}_{-0.5}$).
Keywords
galaxies: clusters: individual (XMM-LSS02182-05102); galaxies: elliptical and lenticular, cD; galaxies: structure; gravitational lensing: strong;
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