2.3 Cluster Baryon Fraction
This issue was discussed in detail by
White et al. (1993)
for the Coma cluster, and has been addressed now in many
contexts by a number of authors (e.g.,
White & Frenk 1991;
White & Fabian 1995;
Steigman & Felten
1995).
The calculation goes as follows:
First, the number density of baryons (b) can be
determined based on the observed densities of light elements from
big-bang nucleosynthesis. Hence, the fraction of baryons (fb)
measured in clusters of galaxies can be used to estimate of the
overall matter density assuming
There are four explicit assumptions made:
1) The gas is in hydrostatic equilibrium.
2) There is a smooth potential.
3) Most of the baryons in the clusters are in the X-ray gas.
4) The cluster baryon fraction is representative of the Universe.
If the gas is clumped or there is another source of pressure (magnetic fields or turbulence) in addition to the thermal pressure, the baryon fraction would be decreased and the matter density would be increased (Steigman & Felten 1995).
Recent measurements of X-ray clusters (e.g., Loewenstein & Mushotsky 1996; White & Fabian 1995) indicate that the baryon fraction has a range of values from about 10 -> 20%. The values for fb tend to be smaller for small groups and in the inner regions of larger clusters. These results underscore the importance of ensuring that such measurements are made on large enough scales to be truly representative of the large-scale Universe as a whole.
Taken at face value, the cluster-baryon method estimates again favor
low values of m. For
b h2 =
0.024 ± 12%
(Tytler, this conference) relatively low values of
m <
0.5 are favored for the range of baryon fractions observed. The
Tytler et al. 1997
baryon determination is at the high end of
recent measures of this quantity (low end of the deuterium abundance
measurements); lower baryon densities only serve to decrease the
m
estimates. (However, see the discussion by
Bothun, Impey and
McGaugh 1997;
these authors suggest that perhaps
low-surface-brightness galaxies could be source of most of the baryons
in the Universe and that rich clusters are not representative of the
overall baryon density.)