Galaxy Luminosity Functions toz∼1 from DEEP2 and COMBO‐17: Implications for Red Galaxy Formation
Author(s) -
S. M. Faber,
Christopher N. A. Willmer,
Christian Wolf,
David C. Koo,
Benjamin J. Weiner,
Jeffrey A. Newman,
Myungshin Im,
Alison L. Coil,
Charlie Conroy,
Michael C. Cooper,
M. Davis,
Douglas P. Finkbeiner,
Brian F. Gerke,
Karl Gebhardt,
E. J. Groth,
Puragra Guhathakurta,
Justin Harker,
N. Kaiser,
Susan A. Kassin,
M. Kleinheinrich,
Nicholas P. Konidaris,
Richard G. Kron,
Lihwai Lin,
Gerard A. Luppino,
Darren S. Madgwick,
K. Meisenheimer,
K. G. Noeske,
A. C. Phillips,
Vicki L. Sarajedini,
Ricardo P. Schiavon,
L. Simard,
Alexander S. Szalay,
Nicole P. Vogt,
Renbin Yan
Publication year - 2007
Publication title -
the astrophysical journal
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 2.376
H-Index - 489
eISSN - 1538-4357
pISSN - 0004-637X
DOI - 10.1086/519294
Subject(s) - physics , astrophysics , elliptical galaxy , astronomy , galaxy , luminous infrared galaxy , stellar mass , lenticular galaxy , galaxy group , star formation
The DEEP2 and COMBO-17 surveys are used to study the evolution of theluminosity function of red and blue galaxies to $z \sim 1$. Schechter functionfits show that, since $z = 1$, $M^*_B$ dims by $\sim$ 1.3 mag per unit redshiftfor both color classes, $\phi^*$ of blue galaxies shows little change, while$\phi^*$ for red galaxies has formally nearly quadrupled. At face value, thenumber density of blue galaxies has remained roughly constant since $ z = 1$,whereas that of red galaxies has been rising. Luminosity densities support bothconclusions, but we note that most red-galaxy evolution occurs between our dataand local surveys and in our highest redshift bin, where the data are weakest.We discuss the implications of having most red galaxies emerge after $z = 1$from precursors among the blue population, taking into account the propertiesof local and distant E/S0s. We suggest a ``mixed'' scenario in which some bluegalaxies have their star-formation quenched in gas-rich mergers, migrate to thered sequence with a variety of masses, and merge further on the red sequence inone or more purely stellar mergers. E/S0s of a given mass today will haveformed via different routes, in a manner that may help to explain thefundamental plane and other local scaling laws.
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