3.2.1. Shape Parameter of the Transfer Function
The initial perturbations of the density fluctuation
P(k) =
|k|2 ~
kn receive a modification as P(k) =
|
k|2 ~
kn T(k) as they grow,
where T(k) is called the transfer function.
Fluctuations of a small scale that enter the horizon in the radiation dominant
epoch do not grow for a while, till the universe becomes matter dominated.
The transfer function T(k) thus damps for small scales as ~
k-4,
whereas it stays close to unity for long-wave lengths.
The transition region is controlled by a parameter
k ~ 2
/
cteq, cteq being the horizon size at the
time of matter-radiation equality, i.e., a characteristic length of
6.5(
h)-1
h-1 Mpc. The parameter
=
h determines the
behaviour of the transfer function and
is called the shape parameter. To give a sufficient power to several
tens of Mpc,
must be as small as 0.2
(Efstathiou et
al. 1990).
This small value (
= 0.15-0.25) is
supported by later analyses (e.g.,
Peacock & Dodds
1994;
Eke et al. 1998).