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String Theory and M-Theory

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196 T-duality <strong>and</strong> D-branes<br />

Chan–Paton charges, Wilson lines <strong>and</strong> multiple branes<br />

In the preceding construction a single Dp-brane appeared naturally after<br />

applying T-duality to an open string with Neumann boundary conditions.<br />

This section shows that, when several Dp-branes are present instead of a<br />

single one, something rather interesting happens, namely nonabelian gauge<br />

symmetries emerge in the theory.<br />

An open string can carry additional degrees of freedom at its end points,<br />

called Chan–Paton charges. These are degrees of freedom that were originally<br />

introduced, when string theory was being developed as a model for<br />

strong interactions, to describe flavor quantum numbers of quarks <strong>and</strong> antiquarks<br />

attached to the ends of an open string. The original idea was to describe<br />

the global SU(2) isotopic spin symmetry acting on a quark–antiquark<br />

pair located at the ends of the string, but it was eventually realized that the<br />

construction actually gives a gauge symmetry.<br />

n<br />

Fig. 6.3. Chan–Paton charges at the ends of an open string.<br />

The Chan–Paton factors associate N degrees of freedom with each of the<br />

end points of the string. For the case of oriented open strings, which is the<br />

case we have discussed so far, the two ends of the string are distinguished,<br />

<strong>and</strong> so it makes sense to associate the fundamental representation N with<br />

the σ = 0 end <strong>and</strong> the antifundamental representation N with the σ = π<br />

end, as indicated in Fig. 6.3. In this way one describes the gauge group<br />

U(N).<br />

For strings that are unoriented, such as type I superstrings, the representations<br />

associated with the two ends have to be the same, <strong>and</strong> this forces the<br />

symmetry group to be one with a real fundamental representation, specifically<br />

an orthogonal or symplectic group. Each state is either symmetric<br />

or antisymmetric under orientation reversal, an operation that interchanges<br />

the two ends. If the massless vectors correspond to antisymmetric states,<br />

then there are N(N − 1)/2 of them <strong>and</strong> the group is SO(N). On the other<br />

h<strong>and</strong>, if they are symmetric, there are N(N + 1)/2 of them <strong>and</strong> the group is<br />

m _

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