4.7 Article

SPIDER - II. The Fundamental Plane of early-type galaxies in grizYJHK

期刊

出版社

OXFORD UNIV PRESS
DOI: 10.1111/j.1365-2966.2010.17091.x

关键词

galaxies: evolution; galaxies: formation; galaxies: fundamental parameters

资金

  1. Alfred P. Sloan Foundation
  2. National Science Foundation
  3. US Department of Energy
  4. National Aeronautics and Space Administration
  5. Japanese Monbukagakusho
  6. Max Planck Society
  7. Higher Education Funding Council for England
  8. American Museum of Natural History
  9. Astrophysical Institute Potsdam
  10. University of Basel
  11. University of Cambridge
  12. Case Western Reserve University
  13. University of Chicago
  14. Drexel University
  15. Institute for Advanced Study
  16. Japan Participation Group
  17. Johns Hopkins University
  18. Joint Institute for Nuclear Astrophysics
  19. Kavli Institute for Particle Astrophysics and Cosmology
  20. Korean Scientist Group
  21. Chinese Academy of Sciences (LAMOST)
  22. Los Alamos National Laboratory
  23. Max-Planck-Institute for Astronomy (MPIA)
  24. Max-Planck-Institute for Astrophysics (MPA)
  25. New Mexico State University
  26. Ohio State University
  27. University of Pittsburgh
  28. University of Portsmouth
  29. Princeton University
  30. United States Naval Observatory
  31. University of Washington
  32. Fermilab

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We present a complete analysis of the Fundamental Plane (FP) of early-type galaxies (ETGs) in the nearby Universe (z < 0.1). The sample, as defined in Paper I, comprises 39 993 ETGs located in environments covering the entire domain in local density (from field to cluster). We derive the FP in the grizYJHK wavebands with a detailed discussion on fitting procedure, bias due to selection effects and bias due to correlated errors on the effective parameters, r(e) and <>(e), as key factors in obtaining meaningful FP coefficients. Studying the Kormendy relation (KR) we find that its slope varies from g (3.44 +/- 0.04) through K (3.80 +/- 0.02) implying that smaller size ETGs have a larger ratio of optical to near-infrared (NIR) radii than galaxies with larger r(e). We also examine the Faber-Jackson (FJ) relation and find that its slope is similar for all wavebands, within the uncertainties, with a mean value of 0.198 +/- 0.007. Writing the FP equation as log r(e) = a log Sigma(0) + b <>(e) + c, we find that the 'a' varies from 1.38 +/- 0.02 in g to 1.55 +/- 0.02 in K, implying a 12 per cent variation across the grizYJHK wavelength baseline. The corresponding variation of 'b' is negligible (b similar to 0.316), while 'c' varies by similar to 10 per cent. We show that the waveband dependence of the FJ and KR results from the complex variation of the distribution of galaxies in the face-on projection of the FP as well as by the change of FP coefficients with waveband. We find that 'a' and 'b' become smaller for higher Sersic index and larger axial ratios, independent of the waveband. This suggests that these variations are likely to be related to differences in structural and dynamical (rather than stellar population) properties of ETGs. It is noticeable that galaxies with bluer colours and disc-like isophotes have smaller 'b', with the effect decreasing smoothly from g through K. Considering a power-law relation between mass-to-light ratio and (dynamical) mass, M/L proportional to M gamma, we estimate gamma from the FP coefficients in grizYJHK. The gamma decreases from 0.224 +/- 0.008 in g to 0.186 +/- 0.009 in K band. Using the gamma values, we estimate the variation of age and metallicity of the stellar populations present in massive galaxies per decade in stellar mass. This analysis shows that in the NIR the tilt of the FP is not due to stellar population variation, and that ETGs have coeval stellar populations with an age variation of a few per cent per decade in mass, and a corresponding metallicity increase of similar to 23 per cent. We also show that current semi-analytical models of galaxy formation reproduce very well these amounts of variation of age and metallicity with respect to stellar mass.

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