| Solution of the horizon problem: The tremendous expansion means that regions that we see widely separated in the sky now at the horizon were much closer together before inflation and thus could have been in contact by light signals. |
| Solution of the flatness problem: The tremendous expansion greatly dilutes any initial curvature. Think, for example, of standing on a basketball. It would be obvious that you are standing on a two-dimensional curved surface. Now imagine expanding the basketball to the size of the Earth. As you stand on it now, it will appear to be flat, even though it is actually curved if you could see it from large enough distance. The same idea extended to four-dimensional spacetime accounts for the present flatness (lack of curvature) in the spacetime of the Universe. Out to the greatest distances that we can see the Universe looks flat on large scales, just as the Earth looks approximately flat out to our horizon. |
| Solution of the monopole problem: The rapid expansion of the Universe tremendously dilutes the concentration of any magnetic monopoles that are produced. Simple calculations indicate that they become so rare in any given volume of space that we would be very unlikely to ever encounter one in an experiment designed to search for them. Nor would they have sufficient density to alter the gravity and thereby the normal expansion of the Universe following inflation. |
Thus, at least schematically, the inflationary theory is capable of preserving the correct predictions of the big bang theory, while alleviating some of its difficulties. The following animation summarizes the problems of the big bang and their solution by the inflationary model.
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Thus, in curing the horizon, flatness, and monopole problems, inflation reintroduces
the baryon asymmetry problem. This means that if inflation is correct, we do not have a
very
satisfactory explanation for why there are baryons in the Universe (and since we are made
of baryons, of
why we exist). The most promising speculation on solving this problem, assuming that
inflation is
correct, invokes the possibility of new kinds of baryon nonconserving
reactions that can occur below the GUTs temperature scale.
There are ideas, but no very
compelling theory of how this
could happen currently exists.