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String Theory and M-Theory

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7.3 Toroidal compactification 285<br />

Fig. 7.3. Fundamental domain of the torus displaying the discrete identifications.<br />

Points in the τ plane where enhanced symmetries appear for ρ = i are displayed.<br />

Suppose that ρ1 = τ1 = 0, so that B = 0 <strong>and</strong><br />

<br />

ρ2τ2<br />

G =<br />

0<br />

0<br />

ρ2/τ2<br />

<br />

.<br />

If ρ2 = τ2 or ρ2 = 1/τ2 then one of the two entries is one, which means that<br />

one of the two circles is at the self-dual radius, <strong>and</strong> there is an enhanced<br />

SU(2) gauge symmetry for both left-movers <strong>and</strong> right-movers. These two<br />

relations are satisfied simultaneously if<br />

(τ, ρ) = (i, i).<br />

In this case both circles are at the self-dual radius <strong>and</strong> the enhanced symmetry<br />

is SU(2) × SU(2) for both left-movers <strong>and</strong> right-movers giving SU(2) 4<br />

altogether.<br />

Another point of enhanced symmetry appears when<br />

In this case B = 0 <strong>and</strong><br />

(τ, ρ) = (− 1<br />

+ i<br />

2<br />

G = 1 √ 3<br />

2 −1<br />

−1 2<br />

√<br />

3<br />

, i).<br />

2<br />

Here G is proportional to the Cartan matrix of SU(3). (For an introduction<br />

to the theory of roots <strong>and</strong> weights of Lie algebras see the review article by<br />

Goddard <strong>and</strong> Olive.) As a consequence both the left-movers <strong>and</strong> the rightmovers<br />

contain the massless vectors required for SU(3) enhanced gauge<br />

<br />

.

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