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Ultraviolet Luminosity Functions from 132 z ∼ 7 and z ∼ 8 Lyman-break Galaxies in the Ultra-deep HUDF09 and Wide-area Early Release Science WFC3/IR Observations

  • Authors: R. J. Bouwens, G. D. Illingworth, P. A. Oesch, I. Labbé, M. Trenti, P. van Dokkum, M. Franx, M. Stiavelli, C. M. Carollo, D. Magee, and V. Gonzalez

Bouwens et al. 2011 The Astrophysical Journal 737 90.

  • Provider: AAS Journals

Caption: Figure 17.

Comparison of the SFR density determinations at z gsim 4 with that implied by recent determinations of the stellar mass density (Section 7.4). The red hatched region gives the SFR densities implied by current compilations of the stellar mass density at z gsim 4 (Labbé et al. 2010a, 2010b; Stark et al. 2009; González et al. 2010) where the width of this region indicates a roughly ±1σ uncertainty. The change in density of the cross-hatching at z > 7 is intended to indicate that the mass-density-derived SFR may be more subject to systematic uncertainty from limited measurements and the extrapolation required from the measurements at z ≲ 7. At z gsim 8, the stellar mass density in galaxies brightward of −18 AB mag is assumed to scale with redshift as (1 + z) −4.4 (as found in Labbé et al. 2010b). Interestingly, at z < 7 the mass-density-derived SFR is only about 40% larger than the SFR density estimated from the LFs; such a small difference is quite encouraging. This suggests that (1) the IMF at high redshift ( z ~ 4–7) may not be that different from what it is at later times and (2) that stellar mass density estimates at z > 4 are reasonably accurate.

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