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Three Roads To Quantum Gravity

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HOW TO WEAVE A STRING<br />

191<br />

p in the formula for the radiation emitted by these black<br />

holes.<br />

A second idea about a black hole's entropy is that it is a<br />

count, not of the ways to make a black hole, but of the<br />

information present in an exact description of the horizon<br />

itself. This is suggested by the fact that the entropy is<br />

proportional to the area of the horizon. So the horizon is<br />

something like a memory chip, with one bit of information<br />

coded in every little pixel, each pixel taking up a region 2<br />

Planck lengths on a side. This picture turns out to be<br />

con®rmed by calculations in loop quantum gravity.<br />

A detailed picture of the horizon of a black hole has been<br />

developed using the methods of loop quantum gravity. This<br />

work started in 1995 when, inspired by the ideas of Crane,<br />

't Hooft, and Susskind, I decided to try to test the holographic<br />

principle in loop quantum gravity. I developed a method for<br />

studying the quantum geometry of a boundary or a screen. As<br />

I mentioned earlier, the result was that the Bekenstein bound<br />

was always satis®ed, so that the information coded into the<br />

geometry on the boundary was always less than a certain<br />

number times its total area.<br />

Meanwhile, Carlo Rovelli was developing a rough picture<br />

of the geometry of a black hole horizon. A graduate student of<br />

ours, Kirill Krasnov, showed me how the method I had<br />

discovered could be used to make Carlo's ideas more precise.<br />

I was quite surprised because I had thought that this would be<br />

impossible. I worried that the uncertainty principle would<br />

make it impossible to locate the horizon exactly in a quantum<br />

theory. Kirill ignored my worries and developed a beautiful<br />

description of the horizon of a black hole which explained<br />

both its entropy and its temperature. (Only much later did<br />

Jerzy Lewandowksi, a Polish physicist who has added much<br />

to our understanding of loop quantum gravity, work out how<br />

the uncertainty principle is circumvented in this case.)<br />

Kirill's work was brilliant, but a bit rough. He was subsequently<br />

joined by Abhay Ashtekar, John Baez, Alejandro<br />

Corichi and other more mathematically minded people who<br />

developed his insights into a very beautiful and powerful<br />

description of the quantum geometry of horizons. The results

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