4.7 Article

Hubble Space Telescope Space Telescope Imaging System observations of the HeII Gunn-Peterson effect toward HE 2347-4342

Journal

ASTROPHYSICAL JOURNAL
Volume 564, Issue 2, Pages 542-558

Publisher

UNIV CHICAGO PRESS
DOI: 10.1086/324397

Keywords

cosmology : observations; intergalactic medium; quasars : absorption lines; quasars : individual (HE 2347-4342)

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We present an HST Space Telescope Imaging System (STIS) spectrum of the He II Gunn-Peterson effect toward HE 2347-4342. Compared to the previous HST Goddard High Resolution Spectrograph data obtained by Reimers et al. the STIS spectrum has a much improved resolution. The two-dimensional detector also allows us to better characterize the sky and dark background. We confirm the presence of two spectral ranges of much reduced opacity, the opacity gaps, and provide improved lower limits on the He II Gunn-Peterson opacity tau(He II) in the high-opacity regions. We use the STIS spectrum together with a Keck-HIRES spectrum covering the corresponding H I Lyalpha forest to calculate a onedimensional map of the softness S of the ionization radiation along the line of sight toward HE 2347-4342, where S is the ratio of the H I to He II photoionization rates. We find that S is generally large but presents important variations, from similar to30 in the opacity gaps to a 1 sigma lower limit of 2300 at z similar or equal to 2.86, in a region that shows an extremely low H I opacity over a 6.5 Angstrom spectral range. We note that a large softness parameter naturally accounts for most of the large Si IV/C IV ratios seen in other quasar absorption line spectra. We present a simple model that reproduces the shape of the opacity gaps in absence of large individual absorption lines. We extend the model described in Heap et al. to account for the presence of sources close to the line of sight of the background quasar. As an alternative to the delayed reionization model suggested by Reimers et al., we propose that the large softness observed at z similar or equal to 2.86 is due to the presence of bright soft sources close to the line of sight, i.e., for which the ratio between the number of H I to He II ionizing photons reaching the intergalactic medium is large. We discuss these two models and suggest ways to discriminate between them.

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