3.2. (r)
on recent samples
Fig. 5 shows the two-point correlation function
in redshift space calculated on three different deep redshift
surveys: LCRS
[23],
d2F (Hawkins et al. - the 2dFGRS team -, in preparation), and SDSS
[24].
The agreement is quite remarkable, in fact the differences between
LCRS and SDSS are mainly due to the fact that comoving distances have
been calculated assuming different cosmological models. It is
clear that trying to fit reasonably well a power-law
(s) =
(s / s0)-
to the
data is hopeless. In
fact, the dotted lines show the real space correlation function
calculated from the Automatic Plate Machine (APM) angular data
[25]
after deprojecting the angular correlation
function with the Limber equation. Now, a reliable power-law
(r) =
(r/r0)-
, with
= 1.7 and
r0 = 4.1 h-1 Mpc, can be fitted to
the curves for scales r
4 h-1 Mpc. The slope is in agreement with the results
inferred by Zehavi et al.
[24]
for the SDSS early data:
=
1.75±0.03 and r0 = 6.1 ± 0.2
h-1 Mpc, within the range
0.1
r
16 h-1
Mpc. Although the APM amplitude was smaller, Baugh
[25]
reported an appreciable
shoulder in
(r) for
scales 4
r
25 h-1 Mpc
where the correlation function was rising above the fitted power
law. The diagram also illustrates the effects of the peculiar
velocities in redshift surveys suppressing the short-range
correlations and enhancing the amplitude at intermediate scales
due to coherent flows
[3,
4].
It is also interesting to note that the first zero crossing of the two-point
correlation function occurs at scales around 30-40 h-1
Mpc.
![]() |
Figure 5. The two-point redshift correlation function for the deepest available redshift surveys: The Las Campanas Redshift Survey [23], the 2dF (Hawkins et al. - the 2dFGRS team -, in preparation), and the early public release of the Sloan Digital Sky Survey [24]. The dotted lines, that fit well a power law, correspond to the real-space correlation function deprojected from the APM angular data using two different models of galactic evolution [25], (figure from Guzzo [4]). |