Volume 342, Issue 2 pp. 439-445

Lyman break galaxies and the star formation rate of the Universe at z≈ 6

Elizabeth R. Stanway

Corresponding Author

Elizabeth R. Stanway

E-mail: [email protected] (ERS); [email protected] (AJB); [email protected] (RGM)Search for more papers by this author
Andrew J. Bunker

Andrew J. Bunker

Institute of Astrophysics, University of Cambridge, Madingley Road, Cambridge, CB3 0HA

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Richard G. McMahon

Richard G. McMahon

Institute of Astrophysics, University of Cambridge, Madingley Road, Cambridge, CB3 0HA

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First published: 12 June 2003
Citations: 35

ABSTRACT

We determine the space density of UV-luminous starburst galaxies at z≈ 6 using deep HST ACS SDSS-i′ (F775W) and SDSS-z′ (F850LP) and VLT ISAAC J and Ks band imaging of the Chandra Deep Field South. We find eight galaxies and one star with (i′−z′) > 1.5 to a depth of zAB= 25.6 (an detection in each of the 3 available ACS epochs). This corresponds to an unobscured star formation rate of ≈15 h−270 M yr−1 at z= 5.9, equivalent to L* for the Lyman-break population at z= 3–4 (ΩΛ= 0.7, ΩM= 0.3). We are sensitive to star-forming galaxies at 5.6 ≲z≲ 7.0 with an effective comoving volume of ≈1.8 × 105h−370 Mpc3 after accounting for incompleteness at the higher redshifts due to luminosity bias. This volume should encompass the primeval subgalactic-scale fragments of the progenitors of about a thousand L* galaxies at the current epoch. We determine a volume-averaged global star formation rate of (6.7 ± 2.7) × 10−4h70 M yr−1 Mpc−3 at z∼ 6 from rest-frame UV selected starbursts at the bright end of the luminosity function: this is a lower limit because of dust obscuration and galaxies below our sensitivity limit. This measurement shows that at z∼ 6 the star formation density at the bright end is a factor of ∼6 times less than that determined by Steidel et al. for a comparable sample of UV-selected galaxies at z= 3–4, and so extends our knowledge of the star formation history of the Universe to earlier times than previous work and into the epoch where reionization may have occurred.

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