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High-Redshift Galaxies in Cluster Fields Wei Zheng, Larry Bradley, and the CLASH high-z search group.

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Presentation on theme: "High-Redshift Galaxies in Cluster Fields Wei Zheng, Larry Bradley, and the CLASH high-z search group."— Presentation transcript:

1 High-Redshift Galaxies in Cluster Fields Wei Zheng, Larry Bradley, and the CLASH high-z search group

2 High-Redshift Galaxies Key Science Questions: How do the first generations of galaxies build up and evolve at the earliest times? Number densities, sizes/morphologies, UV slopes, brightness distribution (UVLF), star-formation rates, masses, ages, metallicities How do these quantities change with cosmic time (e.g. N(z), L(z), SFR(z), M(z))? What are their stellar populations and how do they evolve: unique conditions in the early universe (e.g. low metallicities, no dust, top-heavy IMF)? What is the contribution of star-forming galaxies to reionization?

3 Galaxy Clusters as Cosmic Telescopes Strong Lensing Basics: Galaxy cluster mass density deforms local space-time Pure geometrical effect with no dependence on photon energy Provides large areas of high magnification (μ ~ 10) Amplifies both galaxy flux and size while conserving surface brightness Can have multiply-imaged background galaxies Predicted by Einstein in 1915 (GR) Observationally confirmed by Eddington during the 1919 solar eclipse

4 Lyman Break “Dropout” Technique VizJH Attenuated Spectrum Unattenuated Spectrum No detection Blue continuum Star-forming galaxies are relatively bright in the rest-frame UV (O & B stars) Redshift: Their spectra are shifted to the red (longer wavelengths) due to cosmological expansion: Intervening Hydrogen attenuates the UV spectrum creating a sharp featured called the Lyman break λ obs = λ em (z + 1)

5 Lyman Break Color Selection Rest-frame UV Continuum Color Lyman Break Color Low-mass stars (M, L, T- dwarfs): exclude point sources in z 850 z~7 (z- dropouts) Bouwens et al. 2008

6 LBG at z ~ 7.6 ± 0.4 H AB = 24.7 (observed) H AB = 27.1 (intrinsic)

7 NASA, Bradley et al. STScI PRC08-08a

8 3.4 x 3.4 arcmin WFC3/IR vs. NICMOS/NIC3 ACS/WFC 2.2 x 2.2 arcmin WFC3/IR NIC3 WFC3/IR is ~6x larger in area than NICMOS and has much higher sensitivity WFC3/IR has a discovery efficiency ~30-40x NICMOS NICMOS required ~100 orbits to find one z ~ 7 galaxy, but it takes WFC3/IR only a few orbits! z ~ 7 galaxy comparisons WFC3/IR NICMOS/NIC3 2.2” x 2.2” cutouts Bouwens et al. 2010

9 WFC3/IR Bright Lensed z-dropouts ■Abell 1703: 1 orbit each in WFC3/IR F125W (J) and F160W (H) 8 z-dropout candidates! (some may be multiply- imaged) μ ~ 3 - 40 Bradley et al. 2011 (arXiv1104.2035B)

10 WFC3/IR Bright Lensed z-dropouts Brightest candidate: z ~ 6.7, H 160 ~ 24.0 AB! (brightest z 850 - dropout candidate known) A1703-zD6 spectroscopically confirmed at z = 7.045 (z phot = 7.0) (Schenker et al. 2011, arXiv1107.1251S) Bradley et al. 2011 (arXiv1104.2035B)

11 Abell 2261 AB~25.5

12 Another Dropout Candidate in Abell 2261 that Shows Multiple Components

13 Dropout Candidate in MS2137

14 MACS0744 F125W F160W F814W F775W

15 More Candidates in Cluster Fields? OrbitsZ~7 Candidates CLASH50~10 HIPPIES1303 UDF9616

16 Summary We have found ~10 candidates at z~7 One or two of them are marginally bright (AB~25) Work in progress towards fainter candidates Many of the candidates display multiple components Finding opportunity high inhomogeneous among clusters Many more red objects. Spitzer data important


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