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String Theory Demystified

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256 <strong>String</strong> <strong>Theory</strong> Demystifi ed<br />

A Statement of the Holographic Principle<br />

The holographic principle was fi rst proposed by Gerard t’Hooft in 1993 and has<br />

been worked on extensively by Leonard Susskind. It can be asserted using two<br />

postulates:<br />

• The total information content in a volume of space is equivalent to a theory<br />

that lives only on the surface area that encloses the region.<br />

• The boundary of a region of space-time contains at most a single degree of<br />

freedom per Planck area.<br />

The holographic principle really applies to gravity and we have already seen it in<br />

action when talking about black holes. Information content, which is another way<br />

of saying entropy, is about counting the number of states in a system and so is<br />

proportional to area. We have already seen that in the case of a black hole that<br />

entropy is proportional to the area of the event horizon:<br />

S<br />

A<br />

=<br />

4G<br />

where G is Newton’s gravitational constant. The area A is measured in Planck<br />

units.<br />

This is a surprising result because we would intuitively expect that the number of<br />

states is proportional to the volume of the enclosed region. Following Susskind, we<br />

illustrate that this is in fact the case when gravity is not involved. Imagine that a<br />

volume V contains a set of spins on a lattice. We take the lattice spacing to be a, and<br />

imagine that the lattice fi lls the entire volume. Then the total number of spins<br />

contained in V is<br />

# spins = V<br />

a 3<br />

The total number of states the system can have is<br />

N<br />

V a<br />

= 2 3<br />

/<br />

Using thermodynamics, we arrive at a relationship between the number of states<br />

and entropy S:<br />

N ∝ exp<br />

S

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