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GOGREEN survey: constraining the satellite quenching time-scale in massive clusters at z ≳ 1.

Authors :
Baxter, Devontae C
Cooper, M C
Balogh, Michael L
Carleton, Timothy
Cerulo, Pierluigi
De Lucia, Gabriella
Demarco, Ricardo
McGee, Sean
Muzzin, Adam
Nantais, Julie
Pintos-Castro, Irene
Reeves, Andrew M M
Rudnick, Gregory H
Sarron, Florian
van der Burg, Remco F J
Vulcani, Benedetta
Wilson, Gillian
Zaritsky, Dennis
Source :
Monthly Notices of the Royal Astronomical Society; Oct2022, Vol. 515 Issue 4, p5479-5494, 16p
Publication Year :
2022

Abstract

We model satellite quenching at z ∼ 1 by combining 14 massive (10<superscript>13.8</superscript> < M <subscript>halo</subscript>/M<subscript>⊙</subscript> < 10<superscript>15</superscript>) clusters at 0.8 < z < 1.3 from the GOGREEN and GCLASS surveys with accretion histories of 56 redshift-matched analogues from the IllustrisTNG simulation. Our fiducial model, which is parametrized by the satellite quenching time-scale (τ<subscript>quench</subscript>), accounts for quenching in our simulated satellite population both at the time of infall by using the observed coeval field quenched fraction and after infall by tuning τ<subscript>quench</subscript> to reproduce the observed satellite quenched fraction versus stellar mass trend. This model successfully reproduces the observed satellite quenched fraction as a function of stellar mass (by construction), projected cluster-centric radius, and redshift and is consistent with the observed field and cluster stellar mass functions at z ∼ 1. We find that the satellite quenching time-scale is mass dependent, in conflict with some previous studies at low and intermediate redshift. Over the stellar mass range probed (M <subscript>⋆</subscript> > 10<superscript>10</superscript> M<subscript>⊙</subscript>), we find that the satellite quenching time-scale decreases with increasing satellite stellar mass from ∼1.6 Gyr at 10<superscript>10</superscript> M<subscript>⊙</subscript> to ∼0.6−1 Gyr at 10<superscript>11</superscript> M<subscript>⊙</subscript> and is roughly consistent with the total cold gas (HI + H<subscript>2</subscript>) depletion time-scales at intermediate z , suggesting that starvation may be the dominant driver of environmental quenching at z < 2. Finally, while environmental mechanisms are relatively efficient at quenching massive satellites, we find that the majority (⁠|$\sim 65{\!-\!}80{{\ \rm per\ cent}}$|⁠) of ultra-massive satellites (M <subscript>⋆</subscript> > 10<superscript>11</superscript> M<subscript>⊙</subscript>) are quenched prior to infall. [ABSTRACT FROM AUTHOR]

Details

Language :
English
ISSN :
00358711
Volume :
515
Issue :
4
Database :
Complementary Index
Journal :
Monthly Notices of the Royal Astronomical Society
Publication Type :
Academic Journal
Accession number :
158941896
Full Text :
https://doi.org/10.1093/mnras/stac2149