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The GOGREEN survey: constraining the satellite quenching time-scale in massive clusters at z ≳ 1
Author
Baxter, D.C.Cooper, M.C.
Balogh, M.L.
Carleton, T.
Cerulo, P.
De Lucia, G.
Demarco, R.
Mcgee, S.
Muzzin, A.
Nantais, J.
Pintos-Castro, I.
Reeves, A.M.M.
Rudnick, G.H.
Sarron, F.
Van Der Burg, R.F.J.
Vulcani, B.
Wilson, G.
Zaritsky, D.
Affiliation
Steward Observatory and Department of Astronomy, University of ArizonaIssue Date
2022
Metadata
Show full item recordPublisher
Oxford University PressCitation
Baxter, D. C., Cooper, M. C., Balogh, M. L., Carleton, T., Cerulo, P., De Lucia, G., Demarco, R., Mcgee, S., Muzzin, A., Nantais, J., Pintos-Castro, I., Reeves, A. M. M., Rudnick, G. H., Sarron, F., Van Der Burg, R. F. J., Vulcani, B., Wilson, G., & Zaritsky, D. (2022). The GOGREEN survey: Constraining the satellite quenching time-scale in massive clusters at z ≳ 1. Monthly Notices of the Royal Astronomical Society, 515(4), 5479–5494.Rights
Copyright © 2022 The Author(s). Published by Oxford University Press on behalf of Royal Astronomical Society.Collection Information
This item from the UA Faculty Publications collection is made available by the University of Arizona with support from the University of Arizona Libraries. If you have questions, please contact us at repository@u.library.arizona.edu.Abstract
We model satellite quenching at z ∼1 by combining 14 massive (1013.8 < Mhalo/M⊙ < 1015) 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 (τquench), 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 τquench 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⋆ > 1010 M⊙), we find that the satellite quenching time-scale decreases with increasing satellite stellar mass from ∼1.6 Gyr at 1010 M⊙ to ∼0.6-1 Gyr at 1011 M⊙ and is roughly consistent with the total cold gas (HI + H2) 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⋆ > 1011 M⊙) are quenched prior to infall. © 2022 The Author(s) Published by Oxford University Press on behalf of Royal Astronomical Society.Note
Immediate accessISSN
0035-8711Version
Final published versionae974a485f413a2113503eed53cd6c53
10.1093/mnras/stac2149