Proceedings of the Workshop
"The Magellanic Clouds and Other Dwarf Galaxies"
of the Bonn/Bochum-Graduiertenkolleg

The Near-IR Tully-Fisher Relation

for Giant and Dwarf Late-type Galaxies

Daniele Pierini and Richard Tuffs

Max-Planck-Institut für Kernphysik, Saupfercheckweg 1, D-69117, Heidelberg, Germany

Received 11th March 1998
Abstract. We present the Near-IR (K'-band, i.e.: λeq = 2.1 µm) Tully-Fisher (TF) relation for 50 giant and dwarf late-type galaxies of the Virgo cluster. We find that L ∝ VMax4 for dwarf, faint, slow rotators as well as for giant, bright, fast rotators. The present slope is in agreement with the recent results on the Near-IR Fundamental Plane for disk systems and with the scenario of self-regulation of star formation in disks.

1. Introduction

The origin of the relation between the maximum rotational velocity and the luminosity of giant high surface brightness late-type galaxies (Tully & Fisher 1977) is still debated. Aaronson et al. (1979) gave an ``a posteriori'' justification of the Near-IR TF law (L ∝ VMax4), based on the virial theorem and the three following assumptions:
  1. ``all galaxies have the same mass profiles and rotation curves as a function of some dimensionless scale-length'';
  2. ``all galaxies have the same central mass surface density'';
  3. ``all galaxies have the same mean M/L''.
Some of the previous seminal ideas have been restated by Burstein et al. (1997), who claimed that the Tully-Fisher relation is a projection of the so-called κ-space three-dimensional parameter system of the late-type galaxies. However, Silk (1997) has proposed a scenario of self-regulated star formation for disk systems explaining the (B-band) TF relation, without any dynamical assumption. In the present work we extend previous determinations of the Near-IR (NIR) TF relation to dwarf galaxies and discuss the two hypotheses of its origin.

2. Results and Conclusions

K'-band imaging of a complete sample of 84 VCC (Binggeli et al. 1985) member (Binggeli et al. 1993) dwarf and giant galaxies later than S0a, with BT≤16 mag, was obtained by Boselli et al. (1997). From the latter sample we selected 50 objects (24 with 1≤T≤8 and 26 with 9≤T≤11) according to the following criteria:
  1. 35°<i<80°;
  2. no interacting system;
  3. H I linewidths (W, i.e.: full width at 20% level of I/Imax) with σW/W < 1/3 (see Pierini & Tuffs 1998 for H I references).
Near-IR magnitudes (at the isophotal diameter D25) are taken from Boselli et al. (1997) and corrected for Galactic and internal extinction. The equation of the Tully-Fisher relation, obtained through a bivariate least-squares fit algorithm, is: K' = -9.82 (±0.13)·log(V)+30.06 (±0.25), when turbulent and z-motion corrections are not applied (Fig. 1).

We want to emphasize the following results:

  1. the linearity of the NIR TF relation seems to prevail over a range of 8 magnitudes, for galaxies with different phenomenologies, structures, and, perhaps, age and metallicities (see Fig. 1);
  2. the present slope of -9.81±0.13 is fully consistent with the derivations of the Near-IR TF relation for giant spiral galaxies in the literature, e.g: Aaronson et al. (1979) (-9.67±0.24), Kraan-Korteweg et al. (1988) (-9.81), Pierce & Tully (1988) (-9.25±0.43), Peletier & Willner (1993) (-10.2±0.6).

[Click here to see Fig. 1!]

The existence of the L ∝ VMax4 law in the Near-IR is confirmed by the distribution of galaxies within the NIR (H-band, i.e.: λ = 1 µm) κ2 - κ3 plane (where κ2 ∝ log(M/L·Ieff3) and κ3 ∝ log(M/L)), shown in Fig. 2 (see Pierini & Tuffs for its derivation). However, the present slope is also consistent with the scenario of Silk (1997). In fact, assuming that LK'∝VMax4 and LB ∝ VMax2.1 (Silk 1997), it follows that ΣB∼0.5 ΣK' (where Σ is for the mean surface brightness within D25), as shown in Fig. 3 for our sample.

[Click here to see Figs. 2 and 3!]

On the basis of the present data, we cannot exclude the possibility that the two building blocks for the physical basis of the Tully-Fisher relation (dynamical equilibrium and self-regulated star formation) are independent.

References


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First version: 02ndAugust,1998
Last update: 30thSeptember,1998

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 (E-Mail: jbraun|richtler@astro.uni-bonn.de)