Three Roads To Quantum Gravity
Three Roads To Quantum Gravity
Three Roads To Quantum Gravity
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HOW TO WEAVE A STRING<br />
185<br />
What is remarkable ± indeed, what is almost a miracle ± is<br />
that the hardest problem faced by each group was precisely<br />
the key problem that the other had solved. Loop quantum<br />
gravity tells us how to make a background independent<br />
quantum theory of space and time. It offers a lot of scope to<br />
the M theorist looking for a way to make string theory<br />
background independent. On the other hand, if we believe<br />
that strings must emerge from the description of space and<br />
time provided by loop quantum gravity, we then have a lot of<br />
information about how to formulate the theory so that it does<br />
describe classical spacetime. The theory must be formulated<br />
in such a way that the gravitons appear not on their own, but<br />
as modes of excitations of extended objects that behave as<br />
strings.<br />
It is then possible to entertain the following hypothesis:<br />
string theory and loop quantum gravity are each part of a<br />
single theory. This new theory will have the same relationship<br />
to the existing ones as Newtonian mechanics has to<br />
Galileo's theory of falling bodies and Kepler's theory of<br />
planetary orbits. Each is correct, in the sense that it describes<br />
to a good approximation what is happening in a certain<br />
limited domain. Each solves part of the problem. But each<br />
also has limits which prevent it from forming the basis for a<br />
complete theory of nature. I believe that this the most likely<br />
way in which the theory of quantum gravity will be completed,<br />
given the present evidence. In this penultimate<br />
chapter I shall describe some of this evidence, and the<br />
progress that has recently been made towards inventing a<br />
theory that uni®es string theory and loop quantum gravity.<br />
As a ®rst step we can ask for a rough picture of how the two<br />
theories might ®t together. As it happens, there is a very<br />
natural way in which strings and loops can emerge from the<br />
same theory. The key to this is a subtlety that I have so far only<br />
hinted at. Both loop quantum gravity and string theory<br />
describe physics on very small scales, roughly the Planck<br />
length. But the scale that sets the size of strings is not exactly<br />
equal to the Planck length. That scale is called the string<br />
length. The ratio of the Planck length to the string length is a<br />
number of great signi®cance in string theory. It is a kind of