JADES: Rest-frame UV-to-NIR Size Evolution of Massive Quiescent Galaxies from Redshift z = 5 to z = 0.5
JADES: Rest-frame UV-to-NIR Size Evolution of Massive Quiescent Galaxies from Redshift z = 5 to z = 0.5
Jan 1, 2024·,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,
Zhiyuan Ji
Christina C. Williams
Katherine A. Suess
Sandro Tacchella
Benjamin D. Johnson
Brant Robertson
Stacey Alberts
William M. Baker
Stefi Baum
Rachana Bhatawdekar
Nina Bonaventura
Kristan Boyett
Andrew J. Bunker
Stefano Carniani
Stephane Charlot
Zuyi Chen
Jacopo Chevallard
Emma Curtis-Lake
Francesco D'Eugenio
Anna De Graaff
Christa DeCoursey
Eiichi Egami
Daniel J. Eisenstein
Kevin Hainline
Ryan Hausen
Jakob M. Helton
Tobias J. Looser
Jianwei Lyu
Roberto Maiolino
Michael v. Maseda
Erica Nelson
George Rieke
Marcia Rieke
Hans-Walter Rix
Lester Sandles
Fengwu Sun
Hannah Übler
Christopher N. A. Willmer
Chris Willott
Joris Witstok
Abstract
We present the UV-to-NIR size evolution of a sample of $161$
quiescent galaxies (QGs) with $M_{\ast} > 10^{10}\ M_{\odot}$
over $0.5 < z < 5$
. With deep multi-band NIRCam images in GOODS-South from JADES, we measure the effective radii ($R_{e}$
) of the galaxies at rest-frame $0.3$
, $0.5$
and $1\ \mu\mathrm{m}$
. On average, QGs are $45\%$
($15\%$
) more compact at rest-frame $1\ \mu\mathrm{m}$
than they are at $0.3\ \mu\mathrm{m}$
($0.5\ \mu\mathrm{m}$
). Regardless of wavelengths, the $R_{e}$
of QGs strongly evolves with redshift, and this evolution depends on stellar mass. For lower-mass QGs with $M_{\ast} = 10^{10.0}-10^{10.6}\ M_{\odot}$
, the evolution follows $R_{e} \sim (1 + z)^{-1.1}$
, whereas it becomes steeper, following $R_{e} \sim (1 + z)^{-1.7}$
, for higher-mass QGs with $M_{\ast} > 10^{10.6}\ M_{\odot}$
. To constrain the physical mechanisms driving the apparent size evolution, we study the relationship between $R_{e}$
and the formation redshift ($z_{\mathrm{form}}$
) of QGs. For lower-mass QGs, this relationship is broadly consistent with $R_{e} \sim (1 + z_{\mathrm{form}})^{-1}$
, in line with the expectation of the progenitor effect. For higher-mass QGs, the relationship between $R_{e}$
and $z_{\mathrm{form}}$
depends on stellar age. Older QGs have a steeper relationship between $R_{e}$
and $z_{\mathrm{form}}$
than that expected from the progenitor effect alone, suggesting that mergers and/or post-quenching continuous gas accretion drive additional size growth in very massive systems. We find that the $z > 3$
and $z_{\mathrm{form}}$
QGs in our sample are very compact, with mass surface densities $\Sigma_{e} \geq 10^{10}\ M_{\odot}/\mathrm{kpc}^{2}$
and $z_{\mathrm{form}}$
, and their $R_{e}$
are possibly even smaller than anticipated from the size evolution measured for lower-redshift QGs. Finally, we take a close look at the structure of GS-9209, one of the earliest confirmed massive QGs at $z_{\mathrm{spec}} \sim 4.7$
. From UV to NIR, GS-9209 becomes increasingly compact, and its light profile becomes more spheroidal, showing that the color gradient is already present in this earliest massive QG.
Type
Publication
eprint arXiv:2401.00934
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