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Flatness ProblemThe Universe has total Ω ~ 1 or perhaps exactly 1 Is this a problem? Yes. To understand this point, note that Ω = 1 is special in that the radiation, matter, and dark energy of the Universe conspire to make the Universe precisely flat. If there was a slight imbalance in the begining, we would have problems. To understand this, consider the following. Analogy: Try and balance a pencil on its pointed end. If you are far from vertical, the pencil falls to the ground very quickly. The closer you can place the pencil to vertical the longer it stands-up before it falls over. If you could place it at precisely vertical then (classically) it could stand-up forever. It is hard to place the pencil at its critcal position. Universe: If the Universe started off far from critical, then it would have either quickly collapsed (not lasted for 13.7 billion years) or it would have expanded so quickly that it would have passed through the nucleosynthesis and galaxy formation epochs so fast that we would not be here. The only way for the Universe to have lasted this long and to have passed through the nucleosynthesis era at leisurely enough rates requires that the Universe started off very close to critical. How close? Amazingly,
to make Ω(t) ~ 1 today. This is Flatness Problem. |
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The above mysteries may be explained by what is known as the Inflation Theory . Recently results from the Wilkinson Microwave Anisotropy Probe (WMAP) offered strong support for the Inflation theory. To get a handle on inflation recall that the nature of the four forces of nature changes as the Universe evolves:
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The end of the GUT era is signaled by the symmetry breaking where the nuclear (strong) and electro-weak forces become distinct forces. This is the event where inflation is driven.
The symmetry breakings are analogous to phase transitions (e.g., liquid water → solid water (ice), liquid water → vapor, etc.). Similar to the phenomenom of supercooling in water, where the phase transition from water to ice is delayed, the phase transition in which the GUT force breaks into the strong nuclear force and the electroweak force can also be delayed. Here, the Universe is trapped in the higher energy state which leads to the repulsive force of inflation. The energy trapped as the Universe lingers in the higher energy phase is abruptly released when the phase transition finally takes place. This effect is nicely demonstrated by supercooled water, freezing water releases heat (Youtube video). The phase transition at the end of the GUT era behaves in this manner.
During inflation, the scale factor of the Universe R(t) evolves as:
In the example, the Universe grows by a factor of more than 1030 in 10-32 sec. The exact rate at which the Universe grows depends on the particular model. The point is, expansion is humongous! (Note that in this example, the Universe expands so quickly that even a light beam emitted from a distant observer cannot reach the Earth; the amount of ground it has to cover grows too fast. If the Universe goes from 10-24 cm to 13 km in 10-32 seconds, the average expansion rate is about 13 km divided by 10-32 seconds = 1.3x1033 km per second. The speed of light is 300,000 km per second. The horizon of the observer clearly gets smaller in the sense that we see less of the Universe as time passes during inflation!)
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This explains the horizon problem.
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Inflation predicts that the Universe should appear flat (that is, Ω = 1, identically). This resolves the flatness problem.
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