Dust in the Average Galaxy: Attenuation, Emission, and Opacity from 0<z<7

We present constraints on the dust emission and attenuation properties of galaxies across 0&lt;z&lt;7 using JWST imaging from the COSMOS-Web Survey combined with deep FIR/(sub)millimeter data from Spitzer, Herschel, SCUBA-2, NIKA-2 and ALMA. We analyze over 500,000 galaxies to independently constrain attenuation in the rest-frame ultraviolet (UV) and optical as well as dust emission from stacked FIR spectral energy distributions (SEDs), enabling a direct comparison between the two. We find UV/optical attenuation systematically underpredicts IR luminosity by a factor of ~3x at 0.5&lt;z&lt;7 and up to an order of magnitude for <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"> <mml:mrow> <mml:msub> <mml:mi>M</mml:mi> <mml:mo>⋆</mml:mo> </mml:msub> <mml:mo>&gt;</mml:mo> <mml:msup> <mml:mn>10</mml:mn> <mml:mn>10.5</mml:mn> </mml:msup> <mml:msub> <mml:mi>M</mml:mi> <mml:mo>⊙</mml:mo> </mml:msub> </mml:mrow> </mml:math> . We derive empirical relationships for the effective attenuation, dust temperature, fraction of star formation that is unobscured, and dust-to-stellar mass ratio as functions of redshift and stellar mass. We separate the first order effect of star/dust geometry from dust grain properties by combining constraints on the IR SED, UV SED, and dust mass surface density. Importantly, we measure over an order of magnitude decrease in <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"> <mml:mrow> <mml:msub> <mml:mi>κ</mml:mi> <mml:mrow> <mml:mi>U</mml:mi> <mml:mi>V</mml:mi> </mml:mrow> </mml:msub> <mml:mi>/</mml:mi> <mml:msub> <mml:mi>κ</mml:mi> <mml:mrow> <mml:mi>F</mml:mi> <mml:mi>I</mml:mi> <mml:mi>R</mml:mi> </mml:mrow> </mml:msub> </mml:mrow> </mml:math> –the ratio of dust mass absorption coefficients in the UV at 1600Å and FIR at 500 <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"> <mml:mi>μ</mml:mi> </mml:math> m–from z~0 to z~7. A depressed <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"> <mml:mrow> <mml:msub> <mml:mi>κ</mml:mi> <mml:mrow> <mml:mi>U</mml:mi> <mml:mi>V</mml:mi> </mml:mrow> </mml:msub> <mml:mi>/</mml:mi> <mml:msub> <mml:mi>κ</mml:mi> <mml:mrow> <mml:mi>F</mml:mi> <mml:mi>I</mml:mi> <mml:mi>R</mml:mi> </mml:mrow> </mml:msub> </mml:mrow> </mml:math> is consistent with a deficit of small dust grains, possibly attributable to the intense radiation fields of high- <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"> <mml:mi>z</mml:mi> </mml:math> star formation; indeed, we find a redshift-invariant inverse relationship between <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"> <mml:mrow> <mml:msub> <mml:mi>κ</mml:mi> <mml:mrow> <mml:mi>U</mml:mi> <mml:mi>V</mml:mi> </mml:mrow> </mml:msub> <mml:mi>/</mml:mi> <mml:msub> <mml:mi>κ</mml:mi> <mml:mrow> <mml:mi>F</mml:mi> <mml:mi>I</mml:mi> <mml:mi>R</mml:mi> </mml:mrow> </mml:msub> </mml:mrow> </mml:math> and <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"> <mml:msub> <mml:mi>Σ</mml:mi> <mml:mrow> <mml:mi>S</mml:mi> <mml:mi>F</mml:mi> <mml:mi>R</mml:mi> </mml:mrow> </mml:msub> </mml:math> . Most evolution in the dust-to-stellar ratio is at <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"> <mml:mrow> <mml:mi>z</mml:mi> <mml:mo>&lt;</mml:mo> <mml:mn>1</mml:mn> </mml:mrow> </mml:math> , the product of mild downward evolution in the dust-to-gas ratio combined with steep evolution in the gas-to-stellar ratio. The significant evolution and dynamic range of <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"> <mml:mrow> <mml:msub> <mml:mi>κ</mml:mi> <mml:mrow> <mml:mi>U</mml:mi> <mml:mi>V</mml:mi> </mml:mrow> </mml:msub> <mml:mi>/</mml:mi> <mml:msub> <mml:mi>κ</mml:mi> <mml:mrow> <mml:mi>F</mml:mi> <mml:mi>I</mml:mi> <mml:mi>R</mml:mi> </mml:mrow> </mml:msub> </mml:mrow> </mml:math> and prevailing disconnect between the UV/optical and FIR regimes emphasize that direct dust constraints are irreplaceable for the majority of star-forming galaxies at <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"> <mml:mrow> <mml:mi>z</mml:mi> <mml:mo>&lt;</mml:mo> <mml:mn>7</mml:mn> </mml:mrow> </mml:math> , not just the most extreme star-formers.

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Publication Details

Journal
The Open Journal of Astrophysics
Published
2026-08-18
DOI
https://doi.org/10.33232/001c.167549
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Galaxies: Formation, Evolution, Phenomena
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article

Dust in the Average Galaxy: Attenuation, Emission, and Opacity from 0<z<7

Seiji Fujimoto, Marko Shuntov, G. Gozaliasl, L. Moscardini et al.
The Open Journal of Astrophysics
Galaxies: Formation, Evolution, Phenomena
article

Dust in the Average Galaxy: Attenuation, Emission, and Opacity from 0<z<7

Seiji Fujimoto, Marko Shuntov, G. Gozaliasl, L. Moscardini, Nicole E. Drakos, Anton M. Koekemoer, Caitlin M. Casey, Desika Narayanan, Brant E. Robertson, Manuel Aravena, Laura Sommovigo, Sinclaire M. Manning, Andreas L. Faisst, Aswin P. Vijayan, Ali Hadi, Michaela Hirschmann, Dhruv Zimmerman, Maximilien Franco, Louise Paquereau, Richard Massey, Georgios E. Magdis, Andrew J. Battisti, Can Xu, Wuji Wang, Santosh Harish, Jason Rhodes, Jacqueline E. McCleary, Felix Martinez, Claudia Scarlata, Claudia del P. Lagos, Daizhong Liu, Yingjie Cheng, Ronaldo Laishram, Henry Joy McCracken, Jeyhan S. Kartaltepe, Olivier Ilbert, Hollis B. Akins, Arianna S. Long, Crystal L. Martin, Kohei Inayoshi, Erini Lambrides, Jorge A. Zavala, Jed McKinney, Hiddo Algera, Rasha M. Samir, Ezequiel Treister
article en

Abstract

We present constraints on the dust emission and attenuation properties of galaxies across 0&lt;z&lt;7 using JWST imaging from the COSMOS-Web Survey combined with deep FIR/(sub)millimeter data from Spitzer, Herschel, SCUBA-2, NIKA-2 and ALMA. We analyze over 500,000 galaxies to independently constrain attenuation in the rest-frame ultraviolet (UV) and optical as well as dust emission from stacked FIR spectral energy distributions (SEDs), enabling a direct comparison between the two. We find UV/optical attenuation systematically underpredicts IR luminosity by a factor of ~3x at 0.5&lt;z&lt;7 and up to an order of magnitude for <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"> <mml:mrow> <mml:msub> <mml:mi>M</mml:mi> <mml:mo>⋆</mml:mo> </mml:msub> <mml:mo>&gt;</mml:mo> <mml:msup> <mml:mn>10</mml:mn> <mml:mn>10.5</mml:mn> </mml:msup> <mml:msub> <mml:mi>M</mml:mi> <mml:mo>⊙</mml:mo> </mml:msub> </mml:mrow> </mml:math> . We derive empirical relationships for the effective attenuation, dust temperature, fraction of star formation that is unobscured, and dust-to-stellar mass ratio as functions of redshift and stellar mass. We separate the first order effect of star/dust geometry from dust grain properties by combining constraints on the IR SED, UV SED, and dust mass surface density. Importantly, we measure over an order of magnitude decrease in <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"> <mml:mrow> <mml:msub> <mml:mi>κ</mml:mi> <mml:mrow> <mml:mi>U</mml:mi> <mml:mi>V</mml:mi> </mml:mrow> </mml:msub> <mml:mi>/</mml:mi> <mml:msub> <mml:mi>κ</mml:mi> <mml:mrow> <mml:mi>F</mml:mi> <mml:mi>I</mml:mi> <mml:mi>R</mml:mi> </mml:mrow> </mml:msub> </mml:mrow> </mml:math> –the ratio of dust mass absorption coefficients in the UV at 1600Å and FIR at 500 <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"> <mml:mi>μ</mml:mi> </mml:math> m–from z~0 to z~7. A depressed <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"> <mml:mrow> <mml:msub> <mml:mi>κ</mml:mi> <mml:mrow> <mml:mi>U</mml:mi> <mml:mi>V</mml:mi> </mml:mrow> </mml:msub> <mml:mi>/</mml:mi> <mml:msub> <mml:mi>κ</mml:mi> <mml:mrow> <mml:mi>F</mml:mi> <mml:mi>I</mml:mi> <mml:mi>R</mml:mi> </mml:mrow> </mml:msub> </mml:mrow> </mml:math> is consistent with a deficit of small dust grains, possibly attributable to the intense radiation fields of high- <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"> <mml:mi>z</mml:mi> </mml:math> star formation; indeed, we find a redshift-invariant inverse relationship between <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"> <mml:mrow> <mml:msub> <mml:mi>κ</mml:mi> <mml:mrow> <mml:mi>U</mml:mi> <mml:mi>V</mml:mi> </mml:mrow> </mml:msub> <mml:mi>/</mml:mi> <mml:msub> <mml:mi>κ</mml:mi> <mml:mrow> <mml:mi>F</mml:mi> <mml:mi>I</mml:mi> <mml:mi>R</mml:mi> </mml:mrow> </mml:msub> </mml:mrow> </mml:math> and <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"> <mml:msub> <mml:mi>Σ</mml:mi> <mml:mrow> <mml:mi>S</mml:mi> <mml:mi>F</mml:mi> <mml:mi>R</mml:mi> </mml:mrow> </mml:msub> </mml:math> . Most evolution in the dust-to-stellar ratio is at <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"> <mml:mrow> <mml:mi>z</mml:mi> <mml:mo>&lt;</mml:mo> <mml:mn>1</mml:mn> </mml:mrow> </mml:math> , the product of mild downward evolution in the dust-to-gas ratio combined with steep evolution in the gas-to-stellar ratio. The significant evolution and dynamic range of <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"> <mml:mrow> <mml:msub> <mml:mi>κ</mml:mi> <mml:mrow> <mml:mi>U</mml:mi> <mml:mi>V</mml:mi> </mml:mrow> </mml:msub> <mml:mi>/</mml:mi> <mml:msub> <mml:mi>κ</mml:mi> <mml:mrow> <mml:mi>F</mml:mi> <mml:mi>I</mml:mi> <mml:mi>R</mml:mi> </mml:mrow> </mml:msub> </mml:mrow> </mml:math> and prevailing disconnect between the UV/optical and FIR regimes emphasize that direct dust constraints are irreplaceable for the majority of star-forming galaxies at <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"> <mml:mrow> <mml:mi>z</mml:mi> <mml:mo>&lt;</mml:mo> <mml:mn>7</mml:mn> </mml:mrow> </mml:math> , not just the most extreme star-formers.

The Open Journal of AstrophysicsVol. 9
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Galaxies: Formation, Evolution, Phenomena
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