![]() | Annu. Rev. Astron. Astrophys. 1991. 29:
239-274 Copyright © 1991 by Annual Reviews. All rights reserved |
3.5.2
The velocity fields of emission-line gas disks have been used to determine
M / L-profiles in the central regions of elliptical galaxies (e.g.,
31,
55).
Combination with stellar
velocity dispersion profiles constrains the anisotropy in the velocity
distribution, but the intrinsic shape of the galaxy has a significant effect
on the modeling. This was demonstrated clearly for the E3 galaxy NGC 5077,
where spherical models with the gas on circular orbits give a central decline
in M / L, but triaxial models with constant M / L are able
to fit the data
equally well (31).
There is evidence, however, that
the central gas rotation curves are suspect: the emission-line gas in many
bulges often seems to rotate much slower than expected from the stellar
velocity dispersions
(117,
196,
311).
For NGC 4594, the gas velocities are smaller
than the mean stellar streaming velocities
(196). This may
indicate that the gas is flowing in towards the center.
Few ellipticals contain substantial amounts of HI out to large radii, e.g.,
NGC 1052
(352),
NGC 2974
(187),
NGC 4278
(208,
283),
NGC 5128
(353),
NGC 5666
(204),
and IC 2006
(311).
In NGC 1052 no radial change in M / L is
found, despite that fact that HI is observed as far out as
10re. A strong
outwards increase of M / L was found for
IC 2006, from
5h50 in the inner
parts to 16h50 at 6.5 re
(311). However,
interpretation of these observations is complex, as ellipticals as a class are
triaxial, so that even if the gas has settled, it generally is not on circular
orbits (244,
342).
This was
generally ignored in the past, but it influences the inferred M /
L behavior
(31,
208).
The velocities of individual planetary nebulae and globular clusters can be
measured to about 4re, but they do not give strong
constraints on M / L,
because of the relatively small number of measurements
(119,
158,
159,
256).
Hot X-ray gas may well
provide one of the best constraints on M / L at large
radii. However, few
temperature profiles are available, and as a result the mass determinations
are still uncertain [e.g.,
120,
300,
337,
and the review by Fabbiano
(111)].
The new data from ROSAT may help to improve this situation.
A completely different constraint on the dark halos comes from cluster
dynamics. Merritt has argued that no more than 15% of the mass in clusters can
be attached to individual galaxies
(241).
This implies that the total
M / L for a galaxy is 0.15 times the M / L of the total
cluster (typically
200h50), resulting in M / L 30h50. This would
imply that the
halos contain less than three times the mass of the luminous parts. This rather
low factor may result from stripping during the formation of the cluster; it
may very well be that the progenitors of ellipticals had heavier halos.
Furthermore, Merritt's result shows that in order to answer the question of
whether elliptical galaxies have dark halos one has to demonstrate that any
dark matter found is in fact related to the galaxy, and has a similar velocity
dispersion.