Abstract

Following the discovery of the first significant samples of galaxies at z > 6.5 with Wide Field Camera 3/Infra-Red (WFC3/IR) on board Hubble Space Telescope (HST), it has been claimed that the faintest high-redshift galaxies display extremely blue ultraviolet (UV) continuum slopes, with a UV power-law index β≃−3 (where fλ∝λβ). Such slopes are bluer than previously reported for any other galaxy population, and are most readily explained theoretically by extinction-free, young and very low metallicity stellar populations with a high ionizing photon escape fraction. Here we undertake a critical study of the evidence for such extreme values of β, combining three new WFC3/IR-selected samples of galaxies spanning nearly two decades in UV luminosity over the redshift range z≃ 4.5–8. We explore the impact of inclusion/exclusion of less robust high-redshift candidates and use the varying depths of the samples to explore the effects of noise and selection bias at a given UV luminosity. Simple data-consistency arguments suggest that artificially blue average values of β can result when the analysis is extended into the deepest ≃0.5 mag bin of these WFC3/IR-selected galaxy samples, regardless of the actual luminosity or redshift range probed. By confining attention to robust high-redshift galaxy candidates, with at least one 8σ detection in the WFC3/IR imaging, we find that the average value of β is consistent with 〈β〉=−2.05 ± 0.10 over the redshift range z= 5–7 and the UV absolute magnitude range −22 < MUV,AB < − 18, and that 〈β〉 shows no significant trend with either redshift or MUV. We create and analyse a set of simple end-to-end simulations based on the WFC3/IR+ACS Hubble Ultra Deep Field (HUDF) and Early Release Science data sets which demonstrate that a bias towards artificially low/blue average values of β is indeed ‘expected’ when the UV slope analysis is extended towards the source detection threshold, and conclude that there is as yet no clear evidence for UV slopes significantly bluer than β≃−2, the typical value displayed by the bluest star-forming galaxies at more modest redshifts. A robust measurement of 〈β〉 for the faintest galaxies at z≃ 7 (and indeed z≃ 8) remains a key observational goal, as it provides a fundamental test for high escape fractions from a potentially abundant source of re-ionizing photons. This goal is achievable with HST, but requires still deeper WFC3/IR imaging in the HUDF.

Highlights

  • The first galaxies, by definition, are expected to contain very young stellar populations of very low metallicity

  • This reflects the fact that galaxies detected with relatively low signal-to-noise ratio in Wide Field Camera 3/Infra-Red (WFC3/IR), even if completely undetected at shorter wavelengths, do not display sufficiently strong breaks in their spectral energy distribution (SED) to rule out an alternative low-redshift solution

  • Our analysis is based on three new Wide Field Camera 3 (WFC3)/IR-selected samples of galaxies spanning nearly two decades in UV luminosity over the redshift range z 4.5–8 (McLure et al 2011)

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Summary

Introduction

The first galaxies, by definition, are expected to contain very young stellar populations of very low metallicity. Recent attention has focused on whether the broad-band near-IR photometry which has been successfully used to discover galaxies at z 6.5–8.5 (e.g. Bouwens et al 2010b; Bunker et al 2010; Finkelstein et al 2010; McLure et al 2010; Oesch et al 2010; Vanzella et al 2011) can be used to establish the rest-frame continuum slopes of the highest redshift galaxies. Very young, metal-poor stellar populations are arguably expected to result in substantially bluer continuum slopes around λrest 1500 Å than have been detected to date in galaxies discovered at any lower redshift z < 6.5 Very young, metal-poor stellar populations are arguably expected to result in substantially bluer continuum slopes around λrest 1500 Å than have been detected to date in galaxies discovered at any lower redshift z < 6.5 (e.g. Meurer et al 1999; Steidel et al 1999; Adelberger & Steidel 2000; Ouchi et al 2004; Stanway et al 2005; Bouwens et al 2006; Hathi et al 2008; Bouwens et al 2009; Erb et al 2010)

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