A shallow slope for the stellar mass–angular momentum relation of star-forming galaxies at 1.5 &amp;lt; <i>z</i> &amp;lt; 2.5

ABSTRACT We present measurements of the specific angular momentum $j_\star$ of 41 star-forming galaxies at $1.5\lt z\lt 2.5$. These measurements are based on radial profiles inferred from near-infrared Hubble Space Telescope photometry, along with multiresolution emission-line kinematic modelling using integral field spectroscopy (IFS) data from K-band multi-object spectrograph, Spectrograph for Integral Field Observations in the Near Infrared, and OH-Suppressing Infra-Red Imaging Spectrograph. We identified 24 discs (disc fraction of $58.6\pm 7.7~{{\ \rm per\ cent}}$) and used them to parametrize the $j_\star$ versus stellar mass $M_\star$ relation (Fall relation) as $j_\star \propto M_\star ^{\beta }$. We measure a power-law slope $\beta =0.25\pm 0.15$, which deviates by approximately $3\sigma$ from the commonly adopted local value $\beta = 0.67$, indicating a statistically significant difference. We find that two key systematic effects could drive the steep slopes in previous high-redshift studies: first, including irregular (non-disc) systems due to limitations in spatial resolution and second, using the commonly used approximation $\tilde{j}_\star \approx k_n v_s r_\mathrm{eff}$, which depends on global unresolved quantities. In our sample, both effects lead to steeper slopes of $\beta =0.48\pm 0.21$ and $0.61\pm 0.21$, respectively. To understand the shallow slope, we discuss observational effects and systematic uncertainties and analyse the retention of $j_\star$ relative to the angular momentum of the halo $j_h$ (angular momentum retention factor $f_j =j_\star /j_h$). For the $M_\star$ range covered by the sample $9.5 \lt \log _{10} (M_\star /\mathrm{ M}_\odot) \lt 11.5$ (halo mass $11.5 \lt \log _{10} (M_h/\mathrm{ M}_\odot) \lt 14$), we find large $f_j$ values ($\gt 1$ in some cases) in low-mass haloes that decrease with increasing mass, suggesting a significant role of efficient angular momentum transport in these gas-rich systems, aided by the removal of low-$j_\star$ gas via feedback-driven outflows in low-mass galaxies.

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Journal
Monthly Notices of the Royal Astronomical Society
Published
2024-11-29
DOI
https://doi.org/10.1093/mnras/stae2647
Citations
3
Primary Topic
Galaxies: Formation, Evolution, Phenomena
Type
article
Field-Weighted Citation Impact
0.99

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article

A shallow slope for the stellar mass–angular momentum relation of star-forming galaxies at 1.5 &lt; z &lt; 2.5

Juan M. Espejo Salcedo, Karl Glazebrook, David B. Fisher, Sarah M. Sweet et al.
3 citations
Monthly Notices of the Royal Astronomical Society
Galaxies: Formation, Evolution, Phenomena
0.99
article

A shallow slope for the stellar mass–angular momentum relation of star-forming galaxies at 1.5 &lt; z &lt; 2.5

Juan M. Espejo Salcedo, Karl Glazebrook, David B. Fisher, Sarah M. Sweet, Danail Obreschkow, N. M. Förster Schreiber
article en
3 citations

Abstract

ABSTRACT We present measurements of the specific angular momentum $j_\star$ of 41 star-forming galaxies at $1.5\lt z\lt 2.5$. These measurements are based on radial profiles inferred from near-infrared Hubble Space Telescope photometry, along with multiresolution emission-line kinematic modelling using integral field spectroscopy (IFS) data from K-band multi-object spectrograph, Spectrograph for Integral Field Observations in the Near Infrared, and OH-Suppressing Infra-Red Imaging Spectrograph. We identified 24 discs (disc fraction of $58.6\pm 7.7~{{\ \rm per\ cent}}$) and used them to parametrize the $j_\star$ versus stellar mass $M_\star$ relation (Fall relation) as $j_\star \propto M_\star ^{\beta }$. We measure a power-law slope $\beta =0.25\pm 0.15$, which deviates by approximately $3\sigma$ from the commonly adopted local value $\beta = 0.67$, indicating a statistically significant difference. We find that two key systematic effects could drive the steep slopes in previous high-redshift studies: first, including irregular (non-disc) systems due to limitations in spatial resolution and second, using the commonly used approximation $\tilde{j}_\star \approx k_n v_s r_\mathrm{eff}$, which depends on global unresolved quantities. In our sample, both effects lead to steeper slopes of $\beta =0.48\pm 0.21$ and $0.61\pm 0.21$, respectively. To understand the shallow slope, we discuss observational effects and systematic uncertainties and analyse the retention of $j_\star$ relative to the angular momentum of the halo $j_h$ (angular momentum retention factor $f_j =j_\star /j_h$). For the $M_\star$ range covered by the sample $9.5 \lt \log _{10} (M_\star /\mathrm{ M}_\odot) \lt 11.5$ (halo mass $11.5 \lt \log _{10} (M_h/\mathrm{ M}_\odot) \lt 14$), we find large $f_j$ values ($\gt 1$ in some cases) in low-mass haloes that decrease with increasing mass, suggesting a significant role of efficient angular momentum transport in these gas-rich systems, aided by the removal of low-$j_\star$ gas via feedback-driven outflows in low-mass galaxies.

Monthly Notices of the Royal Astronomical SocietyVol. 536(2)
The University of Queensland (AU), The University of Western Australia (AU), Max Planck Institute for Extraterrestrial Physics (DE), ARC Centre of Excellence for All-sky Astrophysics (AU), International Centre for Radio Astronomy Research (AU), Swinburne University of Technology (AU)
National Aeronautics and Space Administration, University of California, California Institute of Technology, Australian Government, Australian Research Council, Division of Arctic Sciences
Openalex Percentile: Top 22%
Galaxies: Formation, Evolution, Phenomena
0.99
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