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Evolution of infrared luminosity functions of galaxies in the AKARI NEP-deep field: Revealing the cosmic star formation history hidden by dust

  • T. Goto
  • , T. Takagi
  • , H. Matsuhara
  • , T. T. Takeuchi
  • , C. Pearson
  • , T. Wada
  • , T. Nakagawa
  • , O. Ilbert
  • , E. Le Floc'H
  • , S. Oyabu
  • , Y. Ohyama
  • , M. Malkan
  • , H. M. Lee
  • , M. G. Lee
  • , H. Inami
  • , N. Hwang
  • , H. Hanami
  • , M. Im
  • , K. Imai
  • , T. Ishigaki
  • S. Serjeant, H. Shim
  • University of Hawai'i at Mānoa
  • National Institutes of Natural Sciences - National Astronomical Observatory of Japan
  • JAXA Institute of Space and Astronautical Science
  • Nagoya University
  • Rutherford Appleton Laboratory
  • University of Lethbridge
  • Open University Milton Keynes
  • Aix Marseille Université
  • Service d'Astrophysique
  • Academia Sinica Taiwan HQ
  • University of California at Los Angeles
  • Seoul National University
  • California Institute of Technology
  • The Graduate University for Advanced Studies
  • Iwate University
  • TOME R and D Inc. Kawasaki
  • National Institute of Technology, Asahikawa College

Research output: Contribution to journalArticlepeer-review

72 Scopus citations

Abstract

Aims. Dust-obscured star-formation increases with increasing intensity and increasing redshift. We aim to reveal the cosmic star-formation history obscured by dust using deep infrared observation with AKARI. Methods. We constructed restframe 8 μm, 12 μm, and total infrared (TIR) luminosity functions (LFs) at 0.15 < z < 2.2 using 4128 infrared sources in the AKARI NEP-deep field. A continuous filter coverage in the mid-IR wavelength (2.4, 3.2, 4.1, 7, 9, 11, 15, 18, and 24 μm) by the AKARI satellite allowed us to estimate restframe 8 μm and 12 μm luminosities without using a large extrapolation based on an SED fit, which was the largest uncertainty in previous work. Results. We find that all 8 μm (0.38 < z < 2.2), 12 μm (0.15 < z < 1.16), and TIR LFs (0.2 < z <1.6) show continuous and strong evolution toward higher redshift. Our direct estimate of 8 μm LFs is useful since previous work often had to use a large extrapolation from the Spitzer 24 μm to 8 μm, where SED modeling is more difficult because of the PAH emissions. In terms of cosmic infrared luminosity density (ΩIR) , which was obtained by integrating analytic fits to the LFs, we find good agreement with previous work at z<1.2. We find the ΩIR evolves as ∞(1 + z)4.4±m 1.0. When we separate contributions to Ω IR by LIRGs and ULIRGs, we found more IR luminous sources are increasingly more important at higher redshift. We find that the ULIRG (LIRG) contribution increases by a factor of 10 (1.8) from z = 0.35 to z = 1.4.

Original languageEnglish
Article numberA6
JournalAstronomy and Astrophysics
Volume514
Issue number1
DOIs
StatePublished - 3 May 2010

Keywords

  • Galaxies: evolution
  • Galaxies: formation
  • Galaxies: high-redshift
  • Galaxies: luminosity function, mass function
  • Galaxies: starburst
  • Infrared: galaxies

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