We present a detailed numerical study of the evolutions of cosmological
linear perturbations through a simple bouncing world model based on two scalar
fields. We properly identify the relatively growing and decaying solutions in
expanding and collapsing phases. Using a decomposition based on the large-scale
limit exact solution of curvature (adiabatic) perturbations with two
independent modes, we assign the relatively growing/decaying one in an
expanding phase as the C/d-mode. In the collapsing phase, the roles are
reversed, and the C/d-mode is relatively decaying/growing. The analytic
solution shows that, as long as the large scale and the adiabatic conditions
are met, the C- and d-modes preserve their nature throughout the bounce. Here,
by using a concrete nonsingular bouncing world model based on two scalar
fields, we numerically follow the evolutions of the correctly identified C- and
d-modes which preserve their nature through the bounce, thus confirming our
previous anticipation based on the analytic solution. Thus, while the
large-scale condition is satisfied and the adiabatic condition is met during
the bounce, we conclude that it is not possible to obtain the near
Harrison-Zel'dovich scale-invariant density spectrum through a bouncing world
model as long as the seed fluctuations were generated from quantum fluctuations
of the curvature perturbation in the collapsing phase.Comment: 37pages, 23 figures, version 2 with a correction in tex forma