2025MNRAS.536.1188E


Query : 2025MNRAS.536.1188E

2025MNRAS.536.1188E - Mon. Not. R. Astron. Soc., 536, 1188-1216 (2025/January-2)

A shallow slope for the stellar mass-angular momentum relation of star-forming galaxies at 1.5 < z < 2.5.

ESPEJO SALCEDO J.M., GLAZEBROOK K., FISHER D.B., SWEET S.M., OBRESCHKOW D. and FOERSTER SCHREIBER N.M.

Abstract (from CDS):

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.

Abstract Copyright: © 2024 The Author(s). Published by Oxford University Press on behalf of Royal Astronomical Society.

Journal keyword(s): galaxies: disc - galaxies: evolution - galaxies: high-redshift - galaxies: kinematics and dynamics

Simbad objects: 42

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Number of rows : 42
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 KGES 276 EmG 02 17 34.1931 -05 10 16.604           ~ 5 0
2 KGES 293 EmG 02 18 51.0497 -04 57 23.441           ~ 2 0
3 EIS-DEEP CDFS-2 J 1 793 EmG 03 32 29.0657 -27 46 28.607 23.93 23.57 23.40 23.33 23.8130 ~ 44 0
4 [AZW2014] 19 EmG 03 32 29.07929 -27 45 21.4837 25.86 24.85 24.64 24.36 24.06 ~ 20 0
5 NAME Extended Chandra Deep Field South reg 03 32 30.0 -27 48 20           ~ 862 0
6 GMASS 2540 G 03 32 30.343 -27 42 40.38   23.3125 23.22 23.234 23.0087 ~ 25 0
7 GMASS 2303 EmG 03 32 38.870 -27 43 21.58   24.387 24.14 24.221   ~ 21 0
8 GMASS 2363 G 03 32 39.401 -27 42 35.65   25.6786     24.5204 ~ 24 0
9 COSMOS 1323716 G 09 58 59.10 +02 05 04.5   22.58 22.15     ~ 34 0
10 COSMOS2015 633567 G 09 59 14.17 +02 15 46.9   23.860 23.734     ~ 8 0
11 COSMOS2015 692333 EmG 09 59 33.995 +02 20 54.54           ~ 6 0
12 COSMOS2015 769008 G 09 59 36.41 +02 27 59.3   24.758 24.362     ~ 10 0
13 COSMOS2015 659829 G 09 59 37.94 +02 18 02.1 23.643 23.48 23.24 23.17 22.89 ~ 8 0
14 COSMOS2015 298447 rG 09 59 47.5992 +01 44 18.949   23.71 23.34     ~ 20 0
15 COSMOS2015 513443 EmG 09 59 50.78 +02 04 49.9 24.89 24.48 24.11 23.79 23.30 ~ 8 0
16 [MFR2011b] ZC405501 G 09 59 53.7 +02 01 09   23.97 23.61     ~ 13 0
17 COSMOS2015 533904 G 09 59 55.94 +02 06 51.3 24.12 23.62 23.05 23.09 22.88 ~ 17 0
18 COSMOS2015 680053 EmG 10 00 00.74 +02 19 47.9 23.659 23.53 23.21 23.10 22.74 ~ 6 0
19 COSMOS2015 667991 G 10 00 07.62 +02 18 44.4 23.813 23.66 23.40 23.34 23.11 ~ 5 0
20 COSMOS2015 867530 G 10 00 09.39 +02 36 58.6 25.20 24.60 23.91 23.86 23.69 ~ 11 0
21 COSMOS2015 411551 G 10 00 18.3768 +01 55 08.101   24.06 23.77     ~ 11 0
22 CANDELS COSMOS F160W J100024.21+022741.2 EmG 10 00 24.21 +02 27 41.3 25.82 24.72 24.15 24.14 24.04 ~ 17 0
23 CANDELS COSMOS F160W J100032.35+022120.9 EmG 10 00 32.35 +02 21 21.2 24.80 24.32 23.94 23.88 23.74 ~ 18 0
24 CANDELS COSMOS F160W J100044.27+021558.5 EmG 10 00 44.27 +02 15 58.5 24.72 24.25 23.89 23.91 23.82 ~ 23 0
25 COSMOS2015 536983 G 10 00 45.13 +02 07 05.2 25.39 24.90 24.28 24.30 24.00 ~ 9 0
26 COSMOS2015 342863 G 10 01 01.67 +01 48 38.3 24.35 24.10 23.70 23.64 23.64 ~ 11 0
27 COSMOS2015 300906 G 10 01 08.6976 +01 44 28.194   24.27 23.79     ~ 18 0
28 ACS-GC 20031147 AGN 10 01 41.3112 +01 56 42.805   23.86 23.49     ~ 9 0
29 COSMOS2015 716499 G 10 01 46.94 +02 23 24.7   24.01 23.699     ~ 11 0
30 COSMOS2015 639939 G 10 02 06.51 +02 16 15.5 24.59 24.21 23.78 23.81 23.68 ~ 12 0
31 COSMOS2015 465880 G 10 02 19.5120 +02 00 18.035   24.21 23.58     ~ 12 0
32 [KDA2006] D3a 15504 G 11 24 16.0 -21 39 31           ~ 16 0
33 [KDA2006] D3a 6004 G 11 25 03.80 -21 45 32.7   25.88   24.69 24.31 ~ 17 0
34 [KDA2006] D3a 6397 G 11 25 10.50 -21 45 06.1   24.14   23.32 22.78 ~ 13 0
35 GDDS SA12-6339 G 12 05 32.70 -07 23 37.7   25.46 24.08 23.71   ~ 10 0
36 [ESS2003] Q1623-BX455 G 16 25 51.66 +26 46 54.9           ~ 15 0
37 [ESS2003] Q1623-BX543 G 16 25 57.70 +26 50 08.6           ~ 11 0
38 [ESS2003] Q1623-BX599 G 16 26 02.54 +26 45 31.9           ~ 26 0
39 [ESS2003] Q2343-BX610 G 23 46 09.43 +12 49 19.2           ~ 57 0
40 [ESS2003] Q2343-BX513 G 23 46 11.13 +12 48 32.1           ~ 11 0
41 [ESS2003] Q2343-BX389 G 23 46 28.90 +12 47 33.6           ~ 38 0
42 [ESS2003] Q2346-BX482 G 23 48 12.97 +00 25 46.3           ~ 40 0

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