4.6 Article

Herschel PEP/HerMES: the redshift evolution (0 ≤ z ≤ 4) of dust attenuation and of the total (UV plus IR) star formation rate density

Journal

ASTRONOMY & ASTROPHYSICS
Volume 554, Issue -, Pages -

Publisher

EDP SCIENCES S A
DOI: 10.1051/0004-6361/201321651

Keywords

early Universe; cosmology: observations; galaxies: star formation; infrared: galaxies; galaxies: starburst; ultraviolet: galaxies

Funding

  1. BMVIT (Austria)
  2. ESA-PRODEX (Belgium)
  3. CEA/CNES (France)
  4. DLR (Germany)
  5. ASI/INAF (Italy)
  6. CICYT/MCYT (Spain)
  7. CSA (Canada)
  8. NAOC (China)
  9. CEA (France)
  10. CNES (France)
  11. CNRS (France)
  12. ASI (Italy)
  13. MCINN (Spain)
  14. SNSB (Sweden)
  15. STFC (UK)
  16. UKSA (UK)
  17. NASA (USA)
  18. PRIN-INAF [1.06.09.05]
  19. ASI-INAF [I00507/1, I005110]
  20. Stockholm Observatory (Sweden)
  21. STFC [ST/K000977/1, ST/J001422/1, ST/I000976/1] Funding Source: UKRI
  22. Science and Technology Facilities Council [ST/K000977/1, ST/J001422/1, ST/I000976/1] Funding Source: researchfish

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Using new homogeneous luminosity functions (LFs) in the far-ultraviolet (FUV) from VVDS and in the far-infrared (FIR) from Herschel/PEP and Herschel/HerMES, we studied the evolution of the dust attenuation with redshift. With this information, we were able to estimate the redshift evolution of the total (FUV + FIR) star formation rate density (SFRDTOT). By integrating SFRDTOT, we followed the mass building and analyzed the redshift evolution of the stellar mass density (SMD). This article aims at providing a complete view of star formation from the local Universe to z similar to 4 and, using assumptions on earlier star formation history, compares this evolution with previously published data in an attempt to draw a homogeneous picture of the global evolution of star formation in galaxies. Our main conclusions are that: 1) the dust attenuation A(FUV) is found to increase from z = 0 to z similar to 1.2 and then starts to decrease until our last data point at z = 3 : 6; 2) the estimated SFRD confirms published results to z similar to 2. At z > 2, we observe either a plateau or a small increase up to z similar to 3 and then a likely decrease up to z = 3.6; 3) the peak of AFUV is delayed with respect to the plateau of SFRDTOT and a probable origin might be found in the evolution of the bright ends of the FUV and FIR LFs; 4) using assumptions (exponential rise and linear rise with time) for the evolution of the star formation density from z = 3 : 6 to z(form) = 10, we integrated SFRDTOT and obtained a good agreement with the published SMDs.

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