
1.65‐μm ( H ‐band) surface photometry of galaxies – VIII. The near‐IR κ space at z =0
Author(s) -
Pierini D.,
Gavazzi G.,
Franzetti P.,
Scodeggio M.,
Boselli A.
Publication year - 2002
Publication title -
monthly notices of the royal astronomical society
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 2.058
H-Index - 383
eISSN - 1365-2966
pISSN - 0035-8711
DOI - 10.1046/j.1365-8711.2002.05323.x
Subject(s) - physics , astrophysics , galaxy , fundamental plane (elliptical galaxies) , spiral galaxy , bulge , photometry (optics) , elliptical galaxy , lenticular galaxy , stars
We present the distribution of a statistical sample of nearby galaxies in the κ ‐space ( κ 1 ∝log M , κ 2 ∝log I e 3 M / L , κ 3 ∝log M / L ) . Our study is based on near‐IR ( H ‐band: λ =1.65 μm) observations, for the first time comprising early‐ and late‐type systems. Our data confirm that the mean effective dynamical mass‐to‐light ratio M / L of the E+S0+S0a galaxies increases with increasing effective dynamical mass M , as expected from the existence of the Fundamental Plane relation. Conversely, spiral and Im/BCD galaxies show a broad distribution in M / L with no detected trend of M / L with M , the former galaxies having M / L values about twice larger than the latter, on average. For all the late‐type galaxies, the M / L increases with decreasing effective surface intensity I e , consistent with the existence of the Tully–Fisher relation. These results are discussed on the basis of the assumptions behind the construction of the κ ‐space and their limitations. Our study is complementary to a previous investigation in the optical ( B ‐band: λ =0.44 μm) and allows us to study wavelength dependences of the galaxy distribution in the κ ‐space. As a first result, we find that the galaxy distribution in the κ 1 – κ 2 plane reproduces the transition from bulgeless to bulge‐dominated systems in galaxies of increasing dynamical mass. Conversely, it appears that the M / L of late‐types is higher (lower) than that of early‐types with the same M in the near‐IR (optical). The origins of this behaviour are discussed in terms of dust attenuation and star formation history.