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Three Roads To Quantum Gravity

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102 THREE ROADS TO QUANTUM GRAVITY<br />

the idea that matter is made out of atoms; it has to do with<br />

missing information. The entropy of the black hole itself<br />

seems to have nothing to do with either atoms or with<br />

information. It is a measure of a quantity which has to do<br />

with the geometry of space and time: it is proportional to the<br />

area of the black hole's event horizon.<br />

There is something incomplete about a law which asserts a<br />

balance or an exchange between two very dissimilar things. It<br />

is as though we had two kinds of currency, the ®rst of which<br />

was exchangeable into a concrete entity such as gold, while<br />

the other had no worth in terms other than paper. Suppose we<br />

were allowed to freely mix the two kinds of money in our<br />

bank accounts. Such an economy would be based on a<br />

contradiction, and could not survive for long. (In fact,<br />

communist governments experimented with two kinds of<br />

currency, one convertible into other currencies and one not,<br />

and discovered that the system is unstable in the absence of<br />

all sorts of complicated and arti®cial restrictions on the use of<br />

the two kinds of money.) Similarly, a law of physics that<br />

allows information to be converted into geometry, and vice<br />

versa, but gives no account of why, should not survive for<br />

long. There must be something deeper and simpler at the root<br />

of the equivalence.<br />

This raises two profound questions:<br />

. Is there an atomic structure to the geometry of space and<br />

time, so that the entropy of the black hole could be<br />

understood in exactly the same way that the entropy of<br />

matter is understood: as a measure of information about the<br />

motion of the atoms?<br />

. When we understand the atomic structure of geometry will<br />

it be obvious why the area of a horizon is proportional to the<br />

amount of information it hides?<br />

These questions have motivated a great deal of research since<br />

the mid-1970s. In the next few chapters I shall explain why<br />

there is a growing consensus among physicists that the<br />

answer to both questions must be `yes'.

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