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UV Continuum Slope and Dust Obscuration from z ∼ 6 to z ∼ 2: The Star Formation Rate Density at High Redshift

  • Authors: R. J. Bouwens, G. D. Illingworth, M. Franx, R.-R. Chary, G. R. Meurer, C. J. Conselice, H. Ford, M. Giavalisco, and P. van Dokkum

BOUWENS et al. 2009 The Astrophysical Journal 705 936.

  • Provider: AAS Journals

Caption: Figure 9.

Fraction of the total UV luminosity density that arises from galaxies brighter than a given luminosity (solid line). This calculation assumes the faint-end slope α of −1.73 preferred in recent determinations of the LF at z ~ 2–6 (e.g., Yoshida et al. 2006; Bouwens et al. 2007; Oesch et al. 2007; Reddy & Steidel 2009). The dashed lines show the fraction of the luminosity density brighter than specific luminosities for faint-end slopes α of −1.68 and −1.78 (which differ at the 1σ level from the α = −1.73 value preferred at z ~ 4; Bouwens et al. 2007). Note that >50% and >80% of the luminosity density occurs in galaxies fainter than 10 −1.3 L* ~ 0.05 L* and 10 −0.4 L* ~ 0.4 L*, respectively, demonstrating how important it is to understand the dust correction down to very low luminosities.

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