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String Theory and M-Theory

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9.10 Heterotic string theory on Calabi–Yau three-folds 415<br />

As a result, W is a T 3 fibration over a base B. By definition, a Calabi–<br />

Yau manifold is a T 3 fibration if it can be described by a three-dimensional<br />

base space B, with a three-torus above each point of B assembled so as to<br />

make a smooth Calabi–Yau manifold. A T 3 fibration is more general than a<br />

T 3 fiber bundle in that isolated T 3 fibers are allowed to be singular, which<br />

means that one or more of their cycles degenerate. Turning the argument<br />

around, M must also be a T 3 fibration. Mirror symmetry is a fiber-wise<br />

T-duality on all of the three directions of the T 3 . A simple example of a<br />

fiber bundle is depicted in Fig. 9.9.<br />

Fig. 9.9. A Moebius strip is an example of a nontrivial fiber bundle. It is a line<br />

segment fibered over a circle S 1 . Calabi–Yau three-folds that have a mirror are<br />

conjectured to be T 3 fibrations over a base B. In contrast to the simple example<br />

of the Moebius strip, some of the T 3 fibers are allowed to be singular.<br />

Since the number of T-dualities is odd, even forms <strong>and</strong> odd forms are interchanged.<br />

As a result, the (1, 1) <strong>and</strong> (2, 1) cohomologies are interchanged,<br />

as is expected from mirror symmetry. Moreover, there exists a holomorphic<br />

three-form on W , which implies that W is Calabi–Yau. The three<br />

T-dualities, of course, also interchange type IIA <strong>and</strong> type IIB.<br />

The argument given above probably contains the essence of the proof of<br />

mirror symmetry. A note of caution is required though. We already pointed<br />

out that there are Calabi–Yau manifolds whose mirrors are not Calabi–Yau,<br />

so a complete proof would need to account for that. The T-duality rules <strong>and</strong><br />

the condition that a supersymmetric three-cycle has to be special Lagrangian<br />

are statements that hold to leading order in α ′ , while the full description of<br />

the mirror W requires, in general, a whole series of α ′ corrections.<br />

9.10 Heterotic string theory on Calabi–Yau three-folds<br />

As was discussed earlier, the fact that dH is an exact four-form implies that<br />

tr(R∧R) <strong>and</strong> tr(F ∧F ) = 1<br />

30Tr(F ∧F ) must belong to the same cohomology<br />

class. The curvature two-form R takes values in the Lie algebra of the

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