TY - JOUR
T1 - MUFASA
T2 - The assembly of the red sequence
AU - Davé, Romeel
AU - Rafieferantsoa, Mika H.
AU - Thompson, Robert J.
N1 - Funding Information:
The authors thank D. Anglés-Alcázar, F. Durier, K. Finlator, S. Huang, T. Naab and N. Katz for helpful conversations and comments. The authors thank P. Hopkins for allowing us access to the GIZMO code repository. We thank T. Mendel and L. Simard for providing us their SDSS catalogues, and to E. Taylor and M. Cluver for helping us with the GAMA catalogues. RD, MHR and RJT acknowledge support from the South African Research Chairs Initiative and the South African National Research Foundation. Support for MHR was also provided by the Square Kilometre Array post-graduate bursary program. RDacknowledges long-term visitor support provided by the Simons Foundation's Centre for Computational Astrophysics, as well as the Distinguished Visitor Program at Space Telescope Science Institute, where some of this work was conducted. The MUFASA simulations were run on the Pumbaa astrophysics computing cluster hosted at the University of the Western Cape, whichwas generously funded byUWC's Office of the Deputy Vice Chancellor. These simulations were run with revision e77f814 of GIZMO hosted at https://bitbucket.org/rthompson/gizmo.
Publisher Copyright:
© 2017 The Authors.
PY - 2017
Y1 - 2017
N2 - We examine the growth and evolution of quenched galaxies in the MUFASA cosmological hydrodynamic simulations that include an evolving halo mass-based quenching prescription, with galaxy colours computed accounting for line-of-sight extinction to individual star particles. MUFASA reproduces the observed present-day red sequence reasonably well, including its slope, amplitude and scatter. In MUFASA, the red sequence slope is driven entirely by the steep stellar mass-stellar metallicity relation, which independently agrees with observations. High-mass star-forming galaxies blend smoothly on to the red sequence, indicating the lack of a well-defined green valley at M* ≳ 1010.5M⊙. The most massive galaxies quench the earliest and then grow very little in mass via dry merging; they attain their high masses at earlier epochs when cold inflows more effectively penetrate hot haloes. To higher redshifts, the red sequence becomes increasingly contaminated with massive dusty star-forming (SF) galaxies; UVJ selection subtly but effectively separates these populations. We then examine the evolution of the mass functions of central and satellite galaxies split into passive and star-forming via UVJ. Massive quenched systems show good agreement with observations out to z ~ 2, despite not including a rapid early quenching mode associated with mergers. However, low-mass quenched galaxies are far too numerous at z ≲ 1 in MUFASA, indicating that MUFASA strongly overquenches satellites. A challenge for hydrodynamic simulations is to devise a quenching model that produces enough early massive quenched galaxies and keeps them quenched to z = 0, while not being so strong as to overquench satellites; MUFASA's current scheme fails at the latter.
AB - We examine the growth and evolution of quenched galaxies in the MUFASA cosmological hydrodynamic simulations that include an evolving halo mass-based quenching prescription, with galaxy colours computed accounting for line-of-sight extinction to individual star particles. MUFASA reproduces the observed present-day red sequence reasonably well, including its slope, amplitude and scatter. In MUFASA, the red sequence slope is driven entirely by the steep stellar mass-stellar metallicity relation, which independently agrees with observations. High-mass star-forming galaxies blend smoothly on to the red sequence, indicating the lack of a well-defined green valley at M* ≳ 1010.5M⊙. The most massive galaxies quench the earliest and then grow very little in mass via dry merging; they attain their high masses at earlier epochs when cold inflows more effectively penetrate hot haloes. To higher redshifts, the red sequence becomes increasingly contaminated with massive dusty star-forming (SF) galaxies; UVJ selection subtly but effectively separates these populations. We then examine the evolution of the mass functions of central and satellite galaxies split into passive and star-forming via UVJ. Massive quenched systems show good agreement with observations out to z ~ 2, despite not including a rapid early quenching mode associated with mergers. However, low-mass quenched galaxies are far too numerous at z ≲ 1 in MUFASA, indicating that MUFASA strongly overquenches satellites. A challenge for hydrodynamic simulations is to devise a quenching model that produces enough early massive quenched galaxies and keeps them quenched to z = 0, while not being so strong as to overquench satellites; MUFASA's current scheme fails at the latter.
KW - Galaxies: abundances
KW - Galaxies: evolution
KW - Galaxies: formation
KW - Galaxies: luminosity function
KW - Mass function
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U2 - 10.1093/MNRAS/STX1693
DO - 10.1093/MNRAS/STX1693
M3 - Article
AN - SCOPUS:85041279452
VL - 471
SP - 1671
EP - 1687
JO - Monthly Notices of the Royal Astronomical Society
JF - Monthly Notices of the Royal Astronomical Society
SN - 0035-8711
IS - 2
ER -