2024MNRAS.527.9206U


Query : 2024MNRAS.527.9206U

2024MNRAS.527.9206U - Mon. Not. R. Astron. Soc., 527, 9206-9235 (2024/January-3)

Galaxy kinematics and mass estimates at z ∼ 1 from ionized gas and stars.

UBLER H., FORSTER SCHREIBER N.M., VAN DER WEL A., BEZANSON R., PRICE S.H., D'EUGENIO F., WISNIOSKI E., GENZEL R., TACCONI L.J., WUYTS S., NAAB T., LUTZ D., STRAATMAN C.M.S., SHIMIZU T.T., DAVIES R., LIU D. and MENDEL T.

Abstract (from CDS):

We compare ionized gas and stellar kinematics of 16 star-forming galaxies (log (M⋆/M⊙) = 9.7-11.2, SFR =6 - 86 M⊙ yr–1) at z ∼ 1 using near-infrared integral field spectroscopy (IFS) of Hα emission from the KMOS3D (the K-band Multi-Object Spectrograph 3D) survey and optical slit spectroscopy of stellar absorption and gas emission from the LEGA-C (Large Early Galaxy Astrophysics Census) survey. Hα is dynamically colder than stars, with higher disc rotation velocities (by ∼45 per cent) and lower disc velocity dispersions (by a factor ∼2). This is similar to trends observed in the local Universe. We find higher rotational support for Hα relative to [O II], potentially explaining systematic offsets in kinematic scaling relations found in the literature. Regarding dynamical mass measurements, for six galaxies with cumulative mass profiles from Jeans Anisotropic Multi-Gaussian Expansion (JAM) models the Hα dynamical mass models agree remarkably well out to ∼10 kpc for all but one galaxy (average $\Delta M_{\rm dyn}(R_{e,\rm F814W})\lt 0.1$ dex). Simpler dynamical mass estimates based on integrated stellar velocity dispersion are less accurate (standard deviation 0.24 dex). Differences in dynamical mass estimates are larger, for example, for galaxies with stronger misalignments of the Hα kinematic major axis and the photometric position angle, highlighting the added value of IFS observations for dynamics studies. The good agreement between the JAM and the dynamical models based on Hα kinematics at z ∼ 1 corroborates the validity of dynamical mass measurements from Hα IFS observations, which can be more easily obtained for higher redshift galaxies.

Abstract Copyright: © The Author(s) 2023. Published by Oxford University Press on behalf of Royal Astronomical Society.

Journal keyword(s): methods: observational - stars: kinematics and dynamics - ISM: kinematics and dynamics - galaxies: high-redshift - galaxies: kinematics and dynamics

Simbad objects: 17

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Number of rows : 17
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 ACS-GC 20092931 AGN 10 00 13.42 +02 14 00.5 23.33 22.915 22.585   20.828 ~ 38 0
2 CANDELS COSMOS F160W J100016.43+021555.7 G 10 00 16.435 +02 15 55.71 24.99 24.57 23.64 22.95 21.830 ~ 25 0
3 COSMOS 1981985 G 10 00 17.22 +02 21 39.8 23.839 23.61 22.78 22.55 21.600 ~ 21 0
4 ACS-GC 20120345 rG 10 00 17.688 +02 20 48.49 23.281 23.14 22.72 22.51 22.015 ~ 30 0
5 CANDELS COSMOS F160W J100020.01+021642.4 G 10 00 20.01 +02 16 42.4 26.40 25.90 24.82 24.23 23.09 ~ 17 0
6 COSMOS 1996230 G 10 00 21.04 +02 18 38.6 24.95 24.73 23.68 23.21 22.34 ~ 12 0
7 CANDELS COSMOS F160W J100021.71+021351.1 G 10 00 21.713 +02 13 51.18 23.605 23.37 22.65 22.26 21.362 ~ 22 0
8 COSMOS2015 655097 G 10 00 24.68 +02 17 34.0 24.87 24.70 23.97 23.71 22.76 ~ 16 0
9 CANDELS COSMOS F160W J100025.39+022248.8 rG 10 00 25.40 +02 22 49.0 22.819 22.71 22.17 22.002 21.302 ~ 17 0
10 NAME COSMOS Field reg 10 00 28.60 +02 12 21.0           ~ 3639 0
11 COSMOS 1610723 G 10 00 32.523 +02 14 44.54 24.60 24.28 23.32   21.873 ~ 22 0
12 CANDELS COSMOS F160W J100033.89+021622.7 AG? 10 00 33.89 +02 16 22.7 24.52 24.43 23.68 23.47 22.73 ~ 17 0
13 CANDELS COSMOS F160W J100036.83+022635.0 AGN 10 00 36.83 +02 26 35.1 23.498 23.34 22.70 22.44 21.589 ~ 20 0
14 COSMOS 1991080 G 10 00 39.84 +02 19 55.2   22.847 22.295   20.157 ~ 11 0
15 ACS-GC 20090022 G 10 00 40.968 +02 13 09.01 24.33 24.13 23.30 22.82 21.806 ~ 19 0
16 COSMOS2015 615964 EmG 10 00 41.396 +02 14 01.10 24.60 24.43 23.66 23.28 22.36 ~ 23 0
17 ZFOURGE COSMOS 3864 BiC 10 00 41.72 +02 12 57.1 24.47 24.00 23.13 22.52 21.652 ~ 20 0

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