The Evolution of Optical Depth in the Lyα Forest: Evidence Against Reionization atz∼6

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Abstract

We examine the evolution of the IGM Ly optical depth distribution using the transmitted flux probability dis-tribution function (PDF) in a high-resolution sample of 55 QSOs spanning absorption redshifts 1:7 < z < 5:8. The data are compared to two theoretical distributions: a model distribution based on the density distribution of Miralda-Escude ́ et al. (2000; MHR00) and a lognormal distribution. Assuming a spatially uniform UV background and an isothermal IGM, as was done in previous works where transmitted flux statistics have been used to infer an end to cosmic reionization at z 6, the MHR00 model fails to reproduce the observed flux PDFs at redshifts where the optical depth distribution is well sampled unless large continuum corrections are applied. A lognormal distribution, in contrast, fits the data well at all redshifts with onlyminor continuum adjustments. Extrapolating the evolution of the lognormal distribution at z < 5:4 predicts the observed upturn in the Ly and Ly effective optical depths at z> 5:7, while simultaneously reproducing the mean transmitted flux down to z 1:6. In this empirical sense, the evolution of the Ly forest at z 6 is consistent with observed trends at lower redshift. If the evolution of the forest at z P 5 reflects a slowly evolving density field, temperature, and UV background, then no sudden change in the IGM, such as one due to late reionization, appears necessary to explain the disappearance of transmitted flux at z 6. If the MHR00 density distribution is correct, then a nonuniformUV background and/or IGM temperature may be required to produce the correct distribution of optical depths. We find that an inverse temperature-density relation for the MHR00 model significantly improves the PDF fits, but with a large scatter in the equation-of-state index. Subject headinggs: cosmology: observations — early universe — intergalactic medium — quasars: absorption lines Online material: color figures 1.

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