A TURNOVER IN THE GALAXY MAIN SEQUENCE OF STAR FORMATION AT M* ∼ 1010 M☉ FOR REDSHIFTS z < 1.3

By N. Lee, D. Sanders, Caitlin M. Casey, S. Toft, N. Scoville, C. Hung, É. Le Floc'h, O. Ilbert, H. Zahid, H. Aussel and 7 more. 2015

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The relationship between galaxy star formation rates (SFRs) and stellar masses (M*) is reexamined using a mass-selected sample of ∼62,000 star-forming galaxies at z ⩽ 1.3 in the COSMOS 2 deg2 field. Using new far-infrared photometry from Herschel-PACS and SPIRE and Spitzer-MIPS 24 μm, along with derived infrared luminosities from the NRK method based on galaxies' locations in the restframe color–color diagram (NUV − r) versus (r − K), we are able to more accurately determine total SFRs for our complete sample. At all redshifts, the relationship between median SFR and M* follows a power law at low stellar masses, and flattens to nearly constant SFR at high stellar masses. We describe a new parameterization that provides the best fit to the main sequence and characterizes the low mass power-law slope, turnover mass, and overall scaling. The turnover in the main sequence occurs at a characteristic mass of about M0 ∼ 1010 M☉ at all redshifts. The low mass power-law slope ranges from 0.9–1.3 and the overall scaling rises in SFR as a function of (1 + z)4.12 ± 0.10. A broken power-law fit below and above the turnover mass gives relationships of below the turnover mass and above the turnover mass. Galaxies more massive than M* ≳ 1010 M☉ have a much lower average specific star formation rate (sSFR) than would be expected by simply extrapolating the traditional linear fit to the main sequence found for less massive galaxies.

Subfields: Astronomy and Astrophysics, Instrumentation

View Paper: https://www.semanticscholar.org/paper/680edbe1f35ef3a5404079d547b010767d8e066d

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In Astronomy and Astrophysics

  1. L. Hernquist
  2. P. Hopkins
  3. D. M. Alexander
  4. R. Dav'e
  5. Volker Springel
  6. R. Somerville
  7. P. V. van Dokkum
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In Instrumentation

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  2. P. Hopkins
  3. P. Capak
  4. R. Dav'e
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  6. P. V. van Dokkum
  7. Volker Springel
  8. J. Dunlop

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