The Qz5 Survey. I. How the H <scp>i</scp> Mass Density of the Universe Evolves with Cosmic Time

Abstract We report that the neutral hydrogen (H i ) mass density of the Universe ( ρ H i ) increases with cosmic time since z ∼ 5, peaks at z ∼ 3, and then decreases toward z ∼ 0. This is the first result of Qz5, our spectroscopic survey of 63 quasars at z ≳ 5 with VLT/X-SHOOTER and Keck/ESI aimed at characterizing intervening H i gas absorbers at z ∼ 5. The main feature of Qz5 is the high resolution ( R ∼ 7000–9000) of the spectra, which allows us to (1) accurately detect high column density H i gas absorbers in an increasingly neutral intergalactic medium at z ∼ 5 and (2) determine the reliability of previous ρ H i measurements derived with lower resolution spectroscopy. We find five intervening damped Ly α absorbers (DLAs) at z &gt; 4.5, which corresponds to the lowest DLA incidence rate ( <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mn>0.03</mml:mn> <mml:msubsup> <mml:mrow> <mml:mn>4</mml:mn> </mml:mrow> <mml:mrow> <mml:mn>0.02</mml:mn> </mml:mrow> <mml:mrow> <mml:mn>0.05</mml:mn> </mml:mrow> </mml:msubsup> </mml:math> ) at z ≳ 2. We also measure the lowest ρ H i at z ≳ 2 from our sample of DLAs and subDLAs, corresponding to ρ H i <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mo>=</mml:mo> <mml:mn>0.5</mml:mn> <mml:msubsup> <mml:mrow> <mml:mn>6</mml:mn> </mml:mrow> <mml:mrow> <mml:mn>0.31</mml:mn> </mml:mrow> <mml:mrow> <mml:mn>0.82</mml:mn> </mml:mrow> </mml:msubsup> <mml:mo>×</mml:mo> <mml:mn>1</mml:mn> <mml:msup> <mml:mrow> <mml:mn>0</mml:mn> </mml:mrow> <mml:mrow> <mml:mn>8</mml:mn> </mml:mrow> </mml:msup> <mml:mspace width="0.25em"/> <mml:msub> <mml:mrow> <mml:mi>M</mml:mi> </mml:mrow> <mml:mrow> <mml:mo>⊙</mml:mo> </mml:mrow> </mml:msub> </mml:math> Mpc −3 at z ∼ 5. Taking into account our measurements at z ∼ 5 and systematic biases in the DLA detection rate at lower spectral resolutions, we conclude that ρ H i doubles from z ∼ 5 to z ∼ 3. From these results emerges a qualitative agreement between how the cosmic densities of H i gas mass, molecular gas mass, and star formation rate build up with cosmic time.

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Publication Details

Journal
The Astrophysical Journal
Published
2025-04-01
DOI
https://doi.org/10.3847/1538-4357/adb430
Citations
1
Primary Topic
Galaxies: Formation, Evolution, Phenomena
Type
article
Field-Weighted Citation Impact
1.15

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article

The Qz5 Survey. I. How the H i Mass Density of the Universe Evolves with Cosmic Time

Michele Fumagalli, L. Christensen, Marc Rafelski, Regina A. Jorgenson et al.
1 citations
The Astrophysical Journal
Galaxies: Formation, Evolution, Phenomena
1.15
article

The Qz5 Survey. I. How the H i Mass Density of the Universe Evolves with Cosmic Time

Michele Fumagalli, L. Christensen, Marc Rafelski, Regina A. Jorgenson, Jason Xavier Prochaska, Grecco A. Oyarzún, Sebastián López, G. Worseck, Fiona Ozyurt, George D. Becker, Marcel Neeleman, M. E. Wisz
article en
1 citations

Abstract

Abstract We report that the neutral hydrogen (H i ) mass density of the Universe ( ρ H i ) increases with cosmic time since z ∼ 5, peaks at z ∼ 3, and then decreases toward z ∼ 0. This is the first result of Qz5, our spectroscopic survey of 63 quasars at z ≳ 5 with VLT/X-SHOOTER and Keck/ESI aimed at characterizing intervening H i gas absorbers at z ∼ 5. The main feature of Qz5 is the high resolution ( R ∼ 7000–9000) of the spectra, which allows us to (1) accurately detect high column density H i gas absorbers in an increasingly neutral intergalactic medium at z ∼ 5 and (2) determine the reliability of previous ρ H i measurements derived with lower resolution spectroscopy. We find five intervening damped Ly α absorbers (DLAs) at z &gt; 4.5, which corresponds to the lowest DLA incidence rate ( <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mn>0.03</mml:mn> <mml:msubsup> <mml:mrow> <mml:mn>4</mml:mn> </mml:mrow> <mml:mrow> <mml:mn>0.02</mml:mn> </mml:mrow> <mml:mrow> <mml:mn>0.05</mml:mn> </mml:mrow> </mml:msubsup> </mml:math> ) at z ≳ 2. We also measure the lowest ρ H i at z ≳ 2 from our sample of DLAs and subDLAs, corresponding to ρ H i <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mo>=</mml:mo> <mml:mn>0.5</mml:mn> <mml:msubsup> <mml:mrow> <mml:mn>6</mml:mn> </mml:mrow> <mml:mrow> <mml:mn>0.31</mml:mn> </mml:mrow> <mml:mrow> <mml:mn>0.82</mml:mn> </mml:mrow> </mml:msubsup> <mml:mo>×</mml:mo> <mml:mn>1</mml:mn> <mml:msup> <mml:mrow> <mml:mn>0</mml:mn> </mml:mrow> <mml:mrow> <mml:mn>8</mml:mn> </mml:mrow> </mml:msup> <mml:mspace width="0.25em"/> <mml:msub> <mml:mrow> <mml:mi>M</mml:mi> </mml:mrow> <mml:mrow> <mml:mo>⊙</mml:mo> </mml:mrow> </mml:msub> </mml:math> Mpc −3 at z ∼ 5. Taking into account our measurements at z ∼ 5 and systematic biases in the DLA detection rate at lower spectral resolutions, we conclude that ρ H i doubles from z ∼ 5 to z ∼ 3. From these results emerges a qualitative agreement between how the cosmic densities of H i gas mass, molecular gas mass, and star formation rate build up with cosmic time.

The Astrophysical JournalVol. 983(1)
National Science Foundation, Space Telescope Science Institute
Openalex Percentile: Top 20%
Galaxies: Formation, Evolution, Phenomena
1.15
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