4.5 Article

Evolution of the specific star formation rate function at z < 1.4 Dissecting the mass-SFR plane in COSMOS and GOODS

Journal

ASTRONOMY & ASTROPHYSICS
Volume 579, Issue -, Pages -

Publisher

EDP SCIENCES S A
DOI: 10.1051/0004-6361/201425176

Keywords

galaxies: evolution; galaxies: luminosity function, mass function; galaxies: stellar content; galaxies: star formation; galaxies: statistics; galaxies: formation

Funding

  1. NASA [HST-GO-09822]
  2. ESO programme [179.A-2005]
  3. Lyon Institute of Origins [ANR-10-LABX-66]
  4. Collaborative Research Council 956 - Deutsche Forschungsgemeinschaft (DFG)
  5. Grants-in-Aid for Scientific Research [23244031] Funding Source: KAKEN

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The relation between the stellar mass (M-star) and the star formation rate (SFR) characterizes how the instantaneous star formation is determined by the galaxy past star formation history and by the growth of the dark matter structures. We deconstruct the M-star-SFR plane by measuring the specific SFR functions in several stellar mass bins from z = 0.2 out to z = 1.4 (specific SFR = SFR/M-star, noted sSFR). Our analysis is primary based on a 24 mu m selected catalogue combining the COSMOS and GOODS surveys. We estimate the SFR by combining mid-and far-infrared data for 20500 galaxies. The sSFR functions are derived in four stellar mass bins within the range 9.5 < log(M-star/M-circle dot) < 11.5. First, we demonstrate the importance of taking into account selection effects when studying the M-star-SFR relation. Secondly, we find a mass-dependent evolution of the median sSFR with redshift varying as sSFR proportional to (1 + z)(b), with b increasing from b = 2.88(+/- 0.12) to b = 3.78(+/- 0.60) between M-star = 10(9.75) M-circle dot and M-star = 10(11.1) M-circle dot, respectively. At low masses, this evolution is consistent with the cosmological accretion rate and predictions from semi-analytical models (SAM). This agreement breaks down for more massive galaxies showing the need for a more comprehensive description of the star formation history in massive galaxies. Third, we obtain that the shape of the sSFR function is invariant with time at z < 1.4 but depends on the mass. We observe a broadening of the sSFR function ranging from 0.28 dex at M-star = 10(9.75) M-circle dot to 0.46 dex at M-star = 10(11.1) M-circle dot. Such increase in the intrinsic scatter of the M-star-SFR relation suggests an increasing diversity of star formation histories (SFHs) as the stellar mass increases. Finally, we find a gradual decline of the sSFR with stellar mass as log(10)(sSFR) proportional to-0.17M(star). We discuss the numerous physical processes, as gas exhaustion in hot gas halos or secular evolution, which can gradually reduce the sSFR and increase the SFH diversity.

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