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5.7. Solving the Problems of the Standard Cosmology

Let's stick with the simple model of the last section. It is rather easy to see that the Einstein equations are solved by

Equation 213 (213)

as we might expect in inflation. The period of time during which (208) is valid ends at t ~ Deltat, at which

Equation 214 (214)

Now, taking a typical value for m, for which epsilon < 10-4, we obtain

Equation 215 (215)

This has a remarkable consequence. A proper distance LP at t = 0 will inflate to a size 10108cm after a time Deltat ~ 5 × 10-36 seconds. It is important at this point to know that the size of the observable universe today is H0-1 ~ and has not had enough 1028 cm! Therefore, only a small fraction of the original Planck length comprises today's entire visible universe. Thus, homogeneity over a patch less than or of order the Planck length at the onset of inflation is all that is required to solve the horizon problem. Of course, if we wait sufficiently long we will start to see those inhomogeneities (originally sub-Planckian) that were inflated away. However, if inflation lasts long enough (typically about sixty e-folds or so) then this would not be apparent today. Similarly, any unwanted relics are diluted by the tremendous expansion; so long as the GUT phase transition happens before inflation, monopoles will have an extremely low density.

Inflation also solves the flatness problem. There are a couple of ways to see this. The first is to note that, assuming inflation begins, the curvature term in the Friedmann equation very quickly becomes irrelevant, since it scales as a(t)-2. Of course, after inflation, when the universe is full of radiation (and later dust) the curvature term redshifts more slowly than both these components and will eventually become more important than both of them. However, if inflation lasts sufficiently long then even today the total energy density will be so close to unity that we will notice no curvature.

A second way to see this is that, following a similar analysis to that leading to (173) leads to the conclusion that Omega = 1 is an attractor rather than a repeller, when the universe is dominated by energy with w < - 1/3. Therefore, Omega is forced to be very close to one by inflation; if the inflationary period lasts sufficiently long, the density parameter will not have had time since to stray appreciably away from unity.

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