Multi-wavelength lens construction of a Planck and Herschel-detected star-bursting galaxy

We present a source-plane reconstruction of a Herschel and Planck-detected gravitationally lensed dusty star-forming galaxy (DSFG) at z = 1.68 using Hubble, Submillimeter Array (SMA), and Keck observations. The background submillimeter galaxy (SMG) is strongly lensed by a foreground galaxy cluster a...

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Bibliographic Details
Main Authors: Timmons, Nicholas, Cooray, A., Riechers, D.A., Nayyeri, H., Fu, Hai, Jullo, Eric, Gladders, Michael D., Baes, Maarten, Bussmann, R.S., Calanog, Jae, Clements, D.L., da Cunha, E., Dye, S., Eales, S.A., Furlanetto, C., Gonzalez-Nuevo, J., Greenslade, J., Gurwell, M., Messias, Hugo, Michalowski, M.J., Oteo, I., Pérez-Fournón, I., Scott, Douglas, Valiante, E.
Format: Article
Published: American Astronomical Society 2016
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Online Access:https://eprints.nottingham.ac.uk/42360/
Description
Summary:We present a source-plane reconstruction of a Herschel and Planck-detected gravitationally lensed dusty star-forming galaxy (DSFG) at z = 1.68 using Hubble, Submillimeter Array (SMA), and Keck observations. The background submillimeter galaxy (SMG) is strongly lensed by a foreground galaxy cluster at z = 0.997 and appears as an arc with a length of ∼15″ in the optical images. The continuum dust emission, as seen by SMA, is limited to a single knot within this arc. We present a lens model with source-plane reconstructions at several wavelengths to show the difference in magnification between the stars and dust, and highlight the importance of multi-wavelength lens models for studies involving lensed DSFGs. We estimate the physical properties of the galaxy by fitting the flux densities to model spectral energy distributions leading to a magnification-corrected starformation rate (SFR) of 390 ± 60 M yr−1 and a stellar mass of 1.1 ± 0.4 10 x 11 M. These values are consistent with high-redshift massive galaxies that have formed most of their stars already. The estimated gas-to-baryon fraction, molecular gas surface density, and SFR surface density have values of 0.43 ± 0.13, 350 ± 200 M pc−2, and ~ 12 7 M yr−1 kpc−2, respectively. The ratio of SFR surface density to molecular gas surface density puts this among the most star-forming systems, similar to other measured SMGs and local ULIRGs.