2025MNRAS.541..409H


Query : 2025MNRAS.541..409H

2025MNRAS.541..409H - Mon. Not. R. Astron. Soc., 541, 409-428 (2025/July-3)

Distinct origins of environmentally quenched galaxies in the core and outer virialized regions of massive clusters at 0.8 < z < 1.5.

HEWITT G., SARRON F., BALOGH M.L., RUDNICK G., BAHE Y., BAXTER D.C., CASTIGNANI G., CERULO P., COOPER M.C., DEMARCO R., EDWARD A.H., FINN R.A., FORREST B., MUZZIN A., NANTAIS J., VULCANI B., WILSON G. and ZARITSKY D.

Abstract (from CDS):

High-redshift ($z\sim 1$) galaxy clusters are the domain where environmental quenching mechanisms are expected to emerge as important factors in the evolution of the quiescent galaxy population. Uncovering these initially subtle effects requires exploring multiple dependencies of quenching across the cluster environment, and through time. We analyse the stellar mass functions (SMFs) of 17 galaxy clusters within the GOGREEN and GCLASS surveys in the range $0.8< z<1.5$, and with $\log {(M/{\rm {M_\odot }})}>9.5$. The data are fit simultaneously with a Bayesian model that allows the Schechter function parameters of the quiescent and star-forming populations to vary smoothly with cluster-centric radius and redshift. The model also fits the radial galaxy number density profile of each population, allowing the global quenched fraction to be parametrized as a function of redshift and cluster velocity dispersion. We find the star-forming SMF to not depend on radius or redshift. For the quiescent population however, there is $\sim 2\sigma$ evidence for a radial dependence. Outside the cluster core ($R>0.3\, R_{\rm 200}$), the quenched fraction above $\log {(M/{\rm {M_\odot }})}=9.5$ is $\sim 40{\rm\,\,per\, cent}$, and the quiescent SMF is similar in shape to the star-forming field. In contrast, the cluster core has an elevated quenched fraction ($\sim 70{\rm \,\,per\, cent}$), and a quiescent SMF similar in shape to the quiescent field population. We explore contributions of 'early mass-quenching' and mass-independent 'environmental-quenching' models in each of these radial regimes. The core is well described primarily by early mass-quenching, which we interpret as accelerated quenching of massive galaxies in protoclusters, possibly through merger-driven feedback mechanisms. The non-core is better described through mass-independent environmental-quenching of the infalling field population.

Abstract Copyright: © The Author(s) 2025. Published by Oxford University Press on behalf of Royal Astronomical Society.

Journal keyword(s): galaxies: clusters: general - galaxies: evolution - galaxies: general - galaxies: high-redshift

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 SpARCS J003442-430752 ClG 00 34 42.0860 -43 07 53.360           ~ 15 0
2 SpARCS J003550-431224 ClG 00 35 50.0 -43 12 24           ~ 35 0
3 ACT-CL J0036.7-4410 ClG 00 36 42.0407 -44 10 49.516           ~ 23 0
4 ACT-CL J0205.7-5829 ClG 02 05 46.5 -58 29 08           ~ 54 0
5 ACT-CL J0215.3-0343 ClG 02 15 23.99 -03 43 32.2           ~ 41 0
6 SpARCS J021943-053129 ClG 02 19 43.56 -05 31 29.6           ~ 11 0
7 SpARCS J033504-292855 ClG 03 35 03.58 -29 28 55.6           ~ 16 0
8 ACT-CL J0546.6-5345 ClG 05 46 37.6557 -53 45 33.242           ~ 98 0
9 SpARCS J103325+575324 ClG 10 33 25.0 +57 53 24           ~ 4 0
10 SpARCS J103449+581833 ClG 10 34 49.47 +58 18 33.1           ~ 9 0
11 SpARCS J104737+574137 ClG 10 47 37.4630 +57 41 37.960           ~ 15 0
12 SpARCS J105111+581803 ClG 10 51 11.2320 +58 18 03.128           ~ 22 0
13 SpARCS J161315+564930 ClG 16 13 14.60 +56 49 29.9           ~ 18 0
14 SpARCS J161641+554513 ClG 16 16 41.30 +55 45 12.5           ~ 26 0
15 SpARCS J163437+402149 ClG 16 34 35.0 +40 21 51           ~ 25 0
16 SpARCS J163852+403843 ClG 16 38 52.0 +40 38 43           ~ 27 0
17 ACT-CL J2106.0-5844 ClG 21 06 04.3 -58 44 32           ~ 103 0

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