TY - JOUR
T1 - Evidence for a Shallow Evolution in the Volume Densities of Massive Galaxies at z = 4-8 from CEERS
AU - Chworowsky, Katherine
AU - Finkelstein, Steven L.
AU - Boylan-Kolchin, Michael
AU - McGrath, Elizabeth J.
AU - Iyer, Kartheik G.
AU - Papovich, Casey
AU - Dickinson, Mark
AU - Taylor, Anthony J.
AU - Yung, L. Y.Aaron
AU - Arrabal Haro, Pablo
AU - Bagley, Micaela B.
AU - Backhaus, Bren E.
AU - Bhatawdekar, Rachana
AU - Cheng, Yingjie
AU - Cleri, Nikko J.
AU - Cole, Justin W.
AU - Cooper, M. C.
AU - Costantin, Luca
AU - Dekel, Avishai
AU - Franco, Maximilien
AU - Fujimoto, Seiji
AU - Hayward, Christopher C.
AU - Holwerda, Benne W.
AU - Huertas-Company, Marc
AU - Hirschmann, Michaela
AU - Hutchison, Taylor A.
AU - Koekemoer, Anton M.
AU - Larson, Rebecca L.
AU - Li, Zhaozhou
AU - Long, Arianna S.
AU - Lucas, Ray A.
AU - Pirzkal, Nor
AU - Rodighiero, Giulia
AU - Somerville, Rachel S.
AU - Vanderhoof, Brittany N.
AU - de la Vega, Alexander
AU - Wilkins, Stephen M.
AU - Yang, Guang
AU - Zavala, Jorge A.
N1 - Publisher Copyright:
© 2024. The Author(s). Published by the American Astronomical Society.
PY - 2024/9/1
Y1 - 2024/9/1
N2 - We analyze the evolution of massive (log10[M ⋆/M ⊙] > 10) galaxies at z ∼ 4-8 selected from JWST Cosmic Evolution Early Release Survey (CEERS). We infer the physical properties of all galaxies in the CEERS NIRCam imaging through spectral energy distribution (SED) fitting with dense basis to select a sample of high-redshift massive galaxies. Where available we include constraints from additional CEERS observing modes, including 18 sources with MIRI photometric coverage, and 28 sources with spectroscopic confirmations from NIRSpec or NIRCam WFSS. We sample the recovered posteriors in stellar mass from SED fitting to infer the volume densities of massive galaxies across cosmic time, taking into consideration the potential for sample contamination by active galactic nuclei. We find that the evolving abundance of massive galaxies tracks expectations based on a constant baryon conversion efficiency in dark matter halos for z ∼ 4-8. At higher redshifts, we observe an excess abundance of massive galaxies relative to this simple model, resulting in a shallower decline of observed volume densities of massive galaxies. These higher abundances can be explained by modest changes to star formation physics and/or the efficiencies with which star formation occurs in massive dark matter halos, and are not in tension with modern cosmology.
AB - We analyze the evolution of massive (log10[M ⋆/M ⊙] > 10) galaxies at z ∼ 4-8 selected from JWST Cosmic Evolution Early Release Survey (CEERS). We infer the physical properties of all galaxies in the CEERS NIRCam imaging through spectral energy distribution (SED) fitting with dense basis to select a sample of high-redshift massive galaxies. Where available we include constraints from additional CEERS observing modes, including 18 sources with MIRI photometric coverage, and 28 sources with spectroscopic confirmations from NIRSpec or NIRCam WFSS. We sample the recovered posteriors in stellar mass from SED fitting to infer the volume densities of massive galaxies across cosmic time, taking into consideration the potential for sample contamination by active galactic nuclei. We find that the evolving abundance of massive galaxies tracks expectations based on a constant baryon conversion efficiency in dark matter halos for z ∼ 4-8. At higher redshifts, we observe an excess abundance of massive galaxies relative to this simple model, resulting in a shallower decline of observed volume densities of massive galaxies. These higher abundances can be explained by modest changes to star formation physics and/or the efficiencies with which star formation occurs in massive dark matter halos, and are not in tension with modern cosmology.
UR - http://www.scopus.com/inward/record.url?scp=85202684818&partnerID=8YFLogxK
U2 - 10.3847/1538-3881/ad57c1
DO - 10.3847/1538-3881/ad57c1
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AN - SCOPUS:85202684818
SN - 0004-6256
VL - 168
JO - Astronomical Journal
JF - Astronomical Journal
IS - 3
M1 - 113
ER -