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JADES: Rest-frame UV-to-NIR Size Evolution of Massive Quiescent Galaxies from Redshift z=5 to z=0.5

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

TL;DR

This study leverages JWST/JADES deep multi-band imaging to map rest-frame UV-to-NIR sizes of 161 massive quiescent galaxies ($M_*>10^{10}M_⊙$) from $z\sim5$ to $z\sim0.5$, measuring $R_e$ at $\sim0.3$, $0.5$, and $1\,\mu$m. It finds a strong, mass-dependent size evolution with $R_e \propto (1+z)^\beta$ and $\beta \approx -1.25\pm0.20$ across wavelengths, while the rest-frame 1 μm sizes best trace stellar-mass distributions. The UV/optical sizes reveal color gradients, with $R_e^{0.3μm}$ larger by about 45% and $R_e^{0.5μm}$ larger by about 15% relative to $R_e^{1μm}$. The analysis indicates that low-mass quiescent galaxies largely follow the progenitor effect ($R_e \propto (1+z_{form})^{-1}$), whereas high-mass systems show additional growth likely from mergers and ongoing gas accretion, especially at $z>3$ where galaxies are exceptionally compact with $Σ_e \gtrsim 10^{10} M_⊙\,\mathrm{kpc}^{-2}$. The GS-9209 case exemplifies early color gradients and increasing spheroidality, underscoring the rapid establishment of dense central regions in the earliest massive quiescent galaxies. Overall, the work demonstrates JWST’s power to resolve high-redshift galaxy structure and refines our understanding of quenching and structural evolution in the early Universe.

Abstract

We present the UV-to-NIR size evolution of a sample of 161 quiescent galaxies (QGs) with $M_*>10^{10}M_\odot$ 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$μm$. On average, QGs are 45% (15%) more compact at rest-frame 1$μm$ than they are at 0.3$μm$ (0.5$μm$). Regardless of wavelengths, the $R_e$ of QGs strongly evolves with redshift, and this evolution depends on stellar mass. For lower-mass QGs with $M_*=10^{10}-10^{10.6}M_\odot$, 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 $M_*>10^{10.6}M_\odot$. To constrain the physical mechanisms driving the apparent size evolution, we study the relationship between $R_e$ and the formation redshift ($z_{form}$) of QGs. For lower-mass QGs, this relationship is broadly consistent with $R_e\sim(1+z_{form})^{-1}$, in line with the expectation of the progenitor effect. For higher-mass QGs, the relationship between $R_e$ and $z_{form}$ depends on stellar age. Older QGs have a steeper relationship between $R_e$ and $z_{form}$ 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 $z>3$ QGs in our sample are very compact, with mass surface densities $Σ_e\gtrsim10^{10} M_\odot/\rm{kpc}^2$, 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 $z_{spec}\sim4.7$. 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.

JADES: Rest-frame UV-to-NIR Size Evolution of Massive Quiescent Galaxies from Redshift z=5 to z=0.5

TL;DR

This study leverages JWST/JADES deep multi-band imaging to map rest-frame UV-to-NIR sizes of 161 massive quiescent galaxies () from to , measuring at , , and m. It finds a strong, mass-dependent size evolution with and across wavelengths, while the rest-frame 1 μm sizes best trace stellar-mass distributions. The UV/optical sizes reveal color gradients, with larger by about 45% and larger by about 15% relative to . The analysis indicates that low-mass quiescent galaxies largely follow the progenitor effect (), whereas high-mass systems show additional growth likely from mergers and ongoing gas accretion, especially at where galaxies are exceptionally compact with . The GS-9209 case exemplifies early color gradients and increasing spheroidality, underscoring the rapid establishment of dense central regions in the earliest massive quiescent galaxies. Overall, the work demonstrates JWST’s power to resolve high-redshift galaxy structure and refines our understanding of quenching and structural evolution in the early Universe.

Abstract

We present the UV-to-NIR size evolution of a sample of 161 quiescent galaxies (QGs) with over . With deep multi-band NIRCam images in GOODS-South from JADES, we measure the effective radii () of the galaxies at rest-frame 0.3, 0.5 and 1. On average, QGs are 45% (15%) more compact at rest-frame 1 than they are at 0.3 (0.5). Regardless of wavelengths, the of QGs strongly evolves with redshift, and this evolution depends on stellar mass. For lower-mass QGs with , the evolution follows , whereas it becomes steeper, following , for higher-mass QGs with . To constrain the physical mechanisms driving the apparent size evolution, we study the relationship between and the formation redshift () of QGs. For lower-mass QGs, this relationship is broadly consistent with , in line with the expectation of the progenitor effect. For higher-mass QGs, the relationship between and depends on stellar age. Older QGs have a steeper relationship between and 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 QGs in our sample are very compact, with mass surface densities , and their 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 . 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.
Paper Structure (26 sections, 4 equations, 19 figures, 3 tables)

This paper contains 26 sections, 4 equations, 19 figures, 3 tables.

Figures (19)

  • Figure 1: The final sample of 161 massive quiescent galaxies presented in this work (Section \ref{['sec:sample']}). Quiescent galaxies at $z>2$ are shown as stars, while those at $0.5<z<2$ are shown as circles. The orange square marks the quiescent galaxy GS-9209 at $z_{\rm{spec}}=4.658$Carnall2023. Each one of the galaxies is color-coded according to its star formation intensity, quantified using $(\frac{1}{\rm{sSFR}})/t_{\rm{H}}$ (Section \ref{['sec:final_sample']}). Left: Rest-frame UVJ color diagram. Background grey contours show the distribution of all galaxies with stellar mass $\log M_*>10$ and redshift $0.5<z<5$ from 3D-HST. Black dashed lines show the criteria from Schreiber2015, which we use for the selection of quiescent galaxies at $z<2$. Following recent studies, we relax the criterion of the horizontal cut on $(U-V)$ to select quiescent galaxies at $z\ge2$ (Section \ref{['sec:sample']}). Right: The distribution of the quiescent galaxy sample in the stellar mass-redshift space.
  • Figure 2: Comparisons of the redshift (top) and stellar-mass (bottom) measures. Galaxies with spectroscopically confirmed redshifts are color coded in pink. GS-9209 is marked with the orange square. The grey, dashed line marks the one-to-one relationship. The uncertainty of photometric redshifts from our Prospector fitting is smaller than the point, hence hard to see in the plot. Our stellar-mass measures with Prospector are systematically higher by 0.16 dex relative to the measures from 3D-HST.
  • Figure 3: Wide-band filters used for the rest-frame 0.3$\hbox{$\mu$m}$ (blue), 0.5$\hbox{$\mu$m}$ (green) and 1$\hbox{$\mu$m}$ (red) size measures. Expect the HST/ACS F606W, all other filters are from JWST/NIRCam.
  • Figure 4: Size from our measurements using the NIRCam/F150W images ($y$-axis, Section \ref{['sec:galfit']}) as a function of size from vanderWel2012 who performed the measurements using the HST/WFC3 F160W images ($x$-axis). The agreement between the two measurements is great, with a median difference ($y-x$) of 0.03 dex and a standard deviation of 0.07 dex.
  • Figure 5: Rest-frame 1$\hbox{$\mu$m}$ sizes of the $z>3$ quiescent galaxies from different methods. The $x$-axis shows the fiducial measurements in this work (Section \ref{['sec:galfit']}). The $y$-axis shows the measurements from alternative methods detailed in Section \ref{['sec:test_re_zgt3']}, including using (1) a different morphological fitting tool Lenstronomy (black circles), (2) Galfit but fixing Sérsic index $n=1$ (blue squares) or $n=4$ (red squares) during the fit and (3) a nonparametric method with the Richardson–Lucy deconvolution (orange triangles). The main purpose here is to compare the sizes from different methodologies, we thus do not estimate uncertainties for the $y$-axis. The dashed line marks the one-to-one relation, and the dotted lines mark the 2 times above/below the one-to-one relation. For the vast majority of the $z>3$ quiescent galaxies, the relative difference in sizes from different methods is $<50\%$.
  • ...and 14 more figures