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In order to give the steady state
theory the rank back it deserves in cosmology, I will try to create a
symbiosis
between the big bang and the steady state theories, on the basis of the
CTH.
Therefore, in short, a repetition
of those statements of the CTH important for this task:
- The universe has no beginning
in time. We see the big bang in a finite past only when we look back
through
the glasses of the “now time ”.
- We measure the velocities of light
and expansion as constant values at any time and from any
reference
system. Related to the present time scale t however, c ~ t
-1/3 .
- In the universe, matter is created
continuously, at any time and in all space areas.
Obviously, these statements coincide
with the steady state theory to a large degree when we look at the
universe
in a cosmic time scale. But the CTH also supports the big
bang
theory in an impressive way when we apply the “now time” scale.
From the now time view, there is
a perfection in the accordance between the big bang theory and the CTH,
which valid theories of physics were far off to achieve until now.
The CTH not only solves all
problems of the big bang theory in an elegant and convincing manner(
see
section 4.1), but also relieves it from unnecessary ballast ( the
inflationary
model becomes superfluous).
6. Support of the CTH by observation
The universe we observe should,
theoretically,
not exist in reality! At least, its existence would be very
unlikely
if it were based on the theories in physics accepted nowadays. As
mentioned before, any smallest deviation from exact planarity would,
according
to these theories, increase in proportion to time. If, e. g., such a
deviation
had amounted to wee 10 -17 only
at
the moment 1 s after big bang, the universe would , as already
mentioned
before, either have collapsed long ago or would have dissolved into a
homogenous
continuum in which neither stars nor galaxies nor live beings to watch
it could exist.
Only if the planarity had been
adjusted
with the incredible accuracy of <10 -50
by an inflationary period in the early era of the universe and if this
highly instable balance had persisted for over 10 billion years,
the evolution of the observable universe would have been possible on
the
basis of the physics valid today.
In section 4.1 was already pointed
out, the CTH demands the planarity of the universe as a stable state.
The fact the cosmos has, until now,
developed in such a way as we observe, i. e. as Euclidean (plane)
within
large space, convincingly supports the correctness of the CTH.
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