A Massive H <scp>i</scp>-absorption-selected Galaxy at <i>z</i> ≈ 2.356

Abstract We use the Karl G. Jansky Very Large Array (VLA) and the Atacama Large Millimeter/submillimeter Array to detect CO(1–0), CO(3–2), and rest-frame 349 GHz continuum emission from an H i -selected galaxy, DLA1020+2733g, at z ≈ 2.3568 in the field of the z = 2.3553 damped Ly α absorber (DLA) toward QSO J1020+2733. The VLA CO(1–0) detection yields a molecular gas mass of (2.84 ± 0.42) × 10 11 × ( α CO /4.36) M ⊙ , the largest ever measured in an H i -selected galaxy. The DLA metallicity is +0.28 ± 0.16, from the Zn ii λ 2026 absorption line detected in a Keck Echellette Spectrograph and Imager spectrum. This continues the trend of high-metallicity DLAs being frequently associated with massive galaxies. We obtain a star formation rate (SFR) of ≲400 M ⊙ yr −1 from the rest-frame 349 GHz continuum emission and a relatively long molecular gas depletion timescale of ≳0.6 Gyr. The excitation of the J = 3 rotational level is subthermal, with <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:msub> <mml:mrow> <mml:mi>r</mml:mi> </mml:mrow> <mml:mrow> <mml:mn>31</mml:mn> </mml:mrow> </mml:msub> <mml:mo>≡</mml:mo> <mml:mrow> <mml:mi>L</mml:mi> </mml:mrow> <mml:msub> <mml:mrow> <mml:mi>′</mml:mi> </mml:mrow> <mml:mrow> <mml:mi mathvariant="normal">CO</mml:mi> <mml:mo stretchy="false">(</mml:mo> <mml:mn>3</mml:mn> <mml:mo>−</mml:mo> <mml:mn>2</mml:mn> <mml:mo stretchy="false">)</mml:mo> </mml:mrow> </mml:msub> <mml:mo>/</mml:mo> <mml:mrow> <mml:mi>L</mml:mi> </mml:mrow> <mml:msub> <mml:mrow> <mml:mi>′</mml:mi> </mml:mrow> <mml:mrow> <mml:mi mathvariant="normal">CO</mml:mi> <mml:mo stretchy="false">(</mml:mo> <mml:mn>1</mml:mn> <mml:mo>−</mml:mo> <mml:mn>0</mml:mn> <mml:mo stretchy="false">)</mml:mo> </mml:mrow> </mml:msub> <mml:mo>=</mml:mo> <mml:mn>0.513</mml:mn> <mml:mo>±</mml:mo> <mml:mn>0.081</mml:mn> </mml:math> , suggesting that DLA1020+2733g has a low SFR surface density. The large velocity spread of the CO lines, ≈500 km s −1 , and the long molecular gas depletion timescale suggest that DLA1020+2733g is likely to be a cold rotating-disk galaxy.

Authors

Publication Details

Journal
The Astrophysical Journal Letters
Published
2025-03-19
DOI
https://doi.org/10.3847/2041-8213/adb83d
Citations
2
Primary Topic
Galaxies: Formation, Evolution, Phenomena
Type
article
Field-Weighted Citation Impact
2.31

Funders

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article

A Massive H i-absorption-selected Galaxy at z ≈ 2.356

Marc Rafelski, Jason Xavier Prochaska, B. Kaur, Yongda Zhu et al.
2 citations
The Astrophysical Journal Letters
Galaxies: Formation, Evolution, Phenomena
2.31
article

A Massive H i-absorption-selected Galaxy at z ≈ 2.356

Marc Rafelski, Jason Xavier Prochaska, B. Kaur, Yongda Zhu, George D. Becker, Nissim Kanekar, Marcel Neeleman
article en
2 citations

Abstract

Abstract We use the Karl G. Jansky Very Large Array (VLA) and the Atacama Large Millimeter/submillimeter Array to detect CO(1–0), CO(3–2), and rest-frame 349 GHz continuum emission from an H i -selected galaxy, DLA1020+2733g, at z ≈ 2.3568 in the field of the z = 2.3553 damped Ly α absorber (DLA) toward QSO J1020+2733. The VLA CO(1–0) detection yields a molecular gas mass of (2.84 ± 0.42) × 10 11 × ( α CO /4.36) M ⊙ , the largest ever measured in an H i -selected galaxy. The DLA metallicity is +0.28 ± 0.16, from the Zn ii λ 2026 absorption line detected in a Keck Echellette Spectrograph and Imager spectrum. This continues the trend of high-metallicity DLAs being frequently associated with massive galaxies. We obtain a star formation rate (SFR) of ≲400 M ⊙ yr −1 from the rest-frame 349 GHz continuum emission and a relatively long molecular gas depletion timescale of ≳0.6 Gyr. The excitation of the J = 3 rotational level is subthermal, with <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:msub> <mml:mrow> <mml:mi>r</mml:mi> </mml:mrow> <mml:mrow> <mml:mn>31</mml:mn> </mml:mrow> </mml:msub> <mml:mo>≡</mml:mo> <mml:mrow> <mml:mi>L</mml:mi> </mml:mrow> <mml:msub> <mml:mrow> <mml:mi>′</mml:mi> </mml:mrow> <mml:mrow> <mml:mi mathvariant="normal">CO</mml:mi> <mml:mo stretchy="false">(</mml:mo> <mml:mn>3</mml:mn> <mml:mo>−</mml:mo> <mml:mn>2</mml:mn> <mml:mo stretchy="false">)</mml:mo> </mml:mrow> </mml:msub> <mml:mo>/</mml:mo> <mml:mrow> <mml:mi>L</mml:mi> </mml:mrow> <mml:msub> <mml:mrow> <mml:mi>′</mml:mi> </mml:mrow> <mml:mrow> <mml:mi mathvariant="normal">CO</mml:mi> <mml:mo stretchy="false">(</mml:mo> <mml:mn>1</mml:mn> <mml:mo>−</mml:mo> <mml:mn>0</mml:mn> <mml:mo stretchy="false">)</mml:mo> </mml:mrow> </mml:msub> <mml:mo>=</mml:mo> <mml:mn>0.513</mml:mn> <mml:mo>±</mml:mo> <mml:mn>0.081</mml:mn> </mml:math> , suggesting that DLA1020+2733g has a low SFR surface density. The large velocity spread of the CO lines, ≈500 km s −1 , and the long molecular gas depletion timescale suggest that DLA1020+2733g is likely to be a cold rotating-disk galaxy.

The Astrophysical Journal LettersVol. 982(1)
Department of Science and Technology, Ministry of Science and Technology, India, Department of Atomic Energy, Government of India
Openalex Percentile: Top 13%
Galaxies: Formation, Evolution, Phenomena
2.31
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