![]() | Annu. Rev. Astron. Astrophys. 1994. 32:
115-52 Copyright © 1994 by Annual Reviews. All rights reserved |
Neutral Hydrogen Mass and Content
Because of the sensitivity available at centimeter wavelengths, the 21 cm line has been a valuable tool in measuring the redshifts of galaxies and serves as a general indicator of HI content. Since HI line fluxes, or upper limits, are available for some 15000 galaxies skywide, the HI content surpasses nearly all other quantitative indicators of the potential for star formation. The HI content of galaxies has been the subject of recent reviews by Haynes et al. (1984) and Giovanelli & Haynes (1990). Here we focus only on the morphological dependence among normal objects.
Several quantities are generally used in analyzing the total HI
content of galaxies: the total HI mass MHI, the hydrogen
mass to luminosity ratio MHI/LB, and
the HI surface
density, HI. While both
MHI/LB and
HI have
been used as the comparative measure of HI content, a residual
dependence of the former ratio on LB exists, in the
sense that
higher luminosity galaxies have systematically lower values of
MHI/LB. Numerous authors
(e.g.,
Bottinelli et
al. 1974)
have shown that caution is necessary in
using MHI/LB if the Malmquist bias
might play a role.
Furthermore, since LB includes contributions from
both disk and bulge, and the HI is a disk property, the morphological
dependence on MHI/LB is complicated.
Finally, the fraction of the total mass in the form of
HI can be examined via the ratio MHI/MT.
Figures 4a-c show
the results of our analysis of HI properties.
The total HI mass MHI is a scale parameter that is
seen to vary over at
least 4 orders of magnitude. It is well know that early-type systems
- E and S0 galaxies - contain proportionately lower HI masses, and
in fact show a much larger range in all measures of HI content, both
MHI and HI relative to the later spirals.
While some E's and S0's have HI contents similar to those of Sb-Sc
spirals, others contain several orders of magnitude less HI. For this
reason and because the HI within S0's is often located in an annulus
exterior to the optical disk,
van Driel and van
Woerden (1991)
and others have suggested that the HI gas has an external origin, the
result of a tidal interaction or the infall of a dwarf companion.
Bregman et al. (1992)
propose that almost no true E's have detectable HI gas except
for those few instances where, through the HI kinematics and
distribution, infall is indicated. As evident in
Figure 4c,
the fractional HI mass increases systematically from E/S0 to Im.
Among the later-type spirals, HI is useful as an indirect
probe of the effect of local environment on star formation potential.
In the study of the HI deficiency of cluster galaxies relative to
their counterparts in low density regions,
Haynes et al. (1984)
have defined the measure of HI content as the
difference between the observed HI mass (in logarithmic units) and
that expected for a galaxy of the same linear diameter and
morphological type in a comparison sample of isolated objects.
Specifically, the HI deficiency parameter is defined as
The use of the HI deficiency parameter has led numerous authors to conclude that spiral galaxies that pass through a hot X-ray intracluster medium are stripped of their HI gas. Warmels (1988a, b) and Cayatte et al. (1990) find that the HI disks of Virgo core galaxies are indeed shrunken with respect to their field counterparts or objects outside the core. Haynes & Giovanelli (1986) found a one-to-one correspondence between high HI deficiency and shrunken HI size. Although ram pressure stripping is the favored explanation for the HI deficiency, analysis of the the current data do not discriminate among the alternatives of ram pressure, conductive heat transport, turbulent viscosity or tidal effects (Magri et al. 1988). In other instances, slow but close, prograde tidal encounters can similarly remove the majority of a galaxy's interstellar HI. The effect of environment is discussed further in Section 4.