The evolution of the low-density H i intergalactic medium from z = 3.6 to 0: data, transmitted flux, and H i column density,,

Author:

Kim T-S12,Wakker B P1,Nasir F34ORCID,Carswell R F5ORCID,Savage B D1,Bolton J S3ORCID,Fox A J6,Viel M2789,Haehnelt M G5,Charlton J C10,Rosenwasser B E1

Affiliation:

1. Department of Astronomy, University of Wisconsin, 475 North Charter Street, Madison, WI 53706, USA

2. Osservatorio Astronomico di Trieste, Via G. B. Tiepolo, 11, I-34143 Trieste, Italy

3. School of Physics and Astronomy, University of Nottingham, University Park, Nottingham NG7 2RD, UK

4. Department of Physics and Astronomy, University of California, 900 University Avenue, Riverside, CA 92507, USA

5. Institute of Astronomy, University of Cambridge, Madingley Road, Cambridge CB3 0HA, UK

6. AURA for ESA, Space Telescope Science Institute, 3700 San Martin Drive, Baltimore, MD 21218, USA

7. SISSA, International School for Advanced Studies, Via Bonomea 265, I-34136 Trieste, Italy

8. INFN, Sezione di Trieste, Via Valerio 2, I-34127 Trieste, Italy

9. IFPU, Institute for Fundamental Physics of the Universe, Via Beirut 2, I-34014 Trieste, Italy

10. Department of Astronomy and Astrophysics, The Pennsylvania State University, 525 Davey Lab, University Park, PA 16802, USA

Abstract

ABSTRACT We present a new, uniform analysis of the H i transmitted flux (F) and H i column density ($N_{\mathrm{H\,{\small I}}}$) distribution in the low-density IGM as a function of redshift z for 0 < z < 3.6 using 55 HST/COS FUV (Δz = 7.2 at z < 0.5), five HST/STIS + COS NUV (Δz = 1.3 at z ∼ 1) and 24 VLT/UVES, and Keck/HIRES (Δz = 11.6 at 1.7 < z < 3.6) AGN spectra. We performed a consistent, uniform Voigt profile analysis to combine spectra taken with different instruments, to reduce systematics and to remove metal-line contamination. We confirm previously known conclusions on firmer quantitative grounds in particular by improving the measurements at z ∼ 1. Two flux statistics at 0 < F < 1, the mean H i flux and the flux probability distribution function (PDF), show that considerable evolution occurs from z = 3.6 to z = 1.5, after which it slows down to become effectively stable for z < 0.5. However, there are large sightline variations. For the H i column density distribution function (CDDF, f ∝ $N_{\rm H\,{\small I}}^{-\beta }$) at $\log (N_{\mathrm{H\,{\small I}}}/1\, {\mathrm{cm}^{-2}})$ ∈ [13.5, 16.0], β increases as z decreases from β = 1.60 at z ∼ 3.4 to β = 1.82 at z ∼ 0.1. The CDDF shape at lower redshifts can be reproduced by a small amount of clockwise rotation of a higher-z CDDF with a slightly larger CDDF normalization. The absorption line number per z (dn/dz) shows a similar evolutionary break at z ∼ 1.5 as seen in the flux statistics. High-$N_{\mathrm{H\,{\small I}}}$ absorbers evolve more rapidly than low-$N_{\mathrm{H\,{\small I}}}$ absorbers to decrease in number or cross-section with time. The individual dn/dz shows a large scatter at a given z. The scatter increases towards lower z, possibly caused by a stronger clustering at lower z.

Funder

National Aeronautics and Space Administration

Space Telescope Science Institute

H2020 European Research Council

Publisher

Oxford University Press (OUP)

Subject

Space and Planetary Science,Astronomy and Astrophysics

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