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String Theory and M-Theory

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9.2 Calabi–Yau manifolds: mathematical properties 363<br />

Then, in general, the only components of Qα that are invariant under g are<br />

those whose weights εα have the same sign for all n components, since then<br />

ε a αφ a = 0. In special cases, other components may also be invariant. For<br />

each value of α for which the supercharge is not invariant, the amount of<br />

unbroken supersymmetry is cut in half. Thus, if there is invariance for only<br />

one value of α, the fraction of the supersymmetry that is unbroken is 2 1−n .<br />

This chapter shows that the same fraction of supersymmetry is preserved<br />

by compactification on a Calabi–Yau n-fold. In fact, some orbifolds of this<br />

type are singular limits of smooth Calabi–Yau manifolds.<br />

9.2 Calabi–Yau manifolds: mathematical properties<br />

Definition of Calabi–Yau manifolds<br />

By definition, a Calabi–Yau n-fold is a Kähler manifold having n complex<br />

dimensions <strong>and</strong> vanishing first Chern class<br />

c1 = 1<br />

[R] = 0. (9.7)<br />

2π<br />

A theorem, conjectured by Calabi <strong>and</strong> proved by Yau, states that any compact<br />

Kähler manifold with c1 = 0 admits a Kähler metric of SU(n) holonomy.<br />

As we will see below a manifold with SU(n) holonomy admits a spinor<br />

field which is covariantly constant <strong>and</strong> as a result is necessarily Ricci flat.<br />

This theorem is only valid for compact manifolds. In order for it to be valid<br />

in the noncompact case, additional boundary conditions at infinity need to<br />

be imposed. As a result, metrics of SU(n) holonomy correspond precisely<br />

to Kähler manifolds of vanishing first Chern class.<br />

We will motivate the above theorem by showing that the existence of a<br />

covariantly constant spinor implies that the background is Kähler <strong>and</strong> has<br />

c1 = 0. A fundamental theorem states that a compact Kähler manifold has<br />

c1 = 0 if <strong>and</strong> only if the manifold admits a nowhere vanishing holomorphic<br />

n-form Ω. In local coordinates<br />

Ω(z 1 , z 2 , . . . , z n ) = f(z 1 , z 2 , . . . , z n )dz 1 ∧ dz 2 · · · ∧ dz n . (9.8)<br />

In section 9.5 we will establish the vanishing of c1 by explicitly constructing<br />

Ω in backgrounds of SU(n) holonomy.<br />

Hodge numbers of a Calabi–Yau n-fold<br />

Betti numbers are fundamental topological numbers associated with a manifold.<br />

4 The Betti number bp is the dimension of the pth de Rham cohomology<br />

4 There is more discussion of this background material in the appendix of this chapter.

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