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1.4.2 Large-scale Measurements
0 has been measured
with some precision on a scale of about
~ 50 h-1 Mpc, using the data on peculiar velocities of
galaxies,
and on a somewhat larger scale using redshift surveys based on the
IRAS galaxy catalog. Since the results of all such measurements to
date have been reviewed in detail (see Ch. 7; also see
Dekel 1994,
Strauss & Willick
1995),
only brief comments are provided
here. The ``POTENT''
analysis tries to recover the scalar velocity potential from the
galaxy peculiar velocities. It looks reliable, since it reproduces
the observed large scale distribution of galaxies - that is, many
galaxies are found where the converging velocities indicate that there
is a lot of matter, and there are voids in the galaxy distribution
where the diverging velocities indicate that the density is lower than
average. The comparison of the IRAS redshift surveys with POTENT and
related analyses typically give fairly large values for the parameter
I
00.6 /
bI (where bI is the biasing
parameter for IRAS galaxies), corresponding to 0.3
0
3 (for an assumed
bI = 1.15). It is not clear
whether it will be possible to reduce the spread in these
values significantly in the near future - probably both
additional data and a better understanding of systematic and
statistical effects will be required.
A particularly simple way to deduce a lower limit on 0 from
the POTENT peculiar velocity data was proposed by
Dekel & Rees (1994),
based on the fact that high-velocity outflows from voids are
not expected in low-
models.
Data on just one void indicates
that
0
0.3 at the 97% C.L.
This argument is independent
of assumptions about
or
galaxy formation, but of course it
does depend on the success of POTENT in recovering the peculiar
velocities of galaxies.
However, for the particular cosmological models that are at the focus of
this review - CHDM and CDM -
stronger constraints are
available. This is because these models, in common with almost all CDM
variants, assume that the probability distribution function (PDF) of
the primordial fluctuations was Gaussian (the assumption of Gaussianity
is also supported by observations, cf.
Section 7.4.5).
The PDF deduced by POTENT from observed velocities (i.e., the PDF of
the mass, if the POTENT reconstruction is reliable) is far from
Gaussian today, with a long positive-fluctuation tail and a sharp drop
for negative
/
(e.g., respecting the
requirement that
0). It agrees with
a Gaussian initial PDF if and only if
is about unity:
0
0.3 is ruled
out at a high sigma level
(Section 7.5.2; i.e.,
Nusser & Dekel 1993;
Bernardeau et
al. 1995).