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String Theory and M-Theory

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9.8 Nonperturbative effects in Calabi–Yau compactifications 409<br />

in which a Euclidean M2-brane wraps the circle <strong>and</strong> a holomorphic two-cycle<br />

of the Calabi–Yau.<br />

EXERCISES<br />

EXERCISE 9.14<br />

Show that the submanifold X = X is a supersymmetric three-cycle inside<br />

the Calabi–Yau three-fold given by a quintic hypersurface in £ P 4 .<br />

SOLUTION<br />

To prove the above statement, we should first check that the pullback of<br />

the Kähler form is zero. This is trivial in this case, because X → X under<br />

the transformation J → −J. On the other h<strong>and</strong>, the pullback of J onto the<br />

fixed surface X = X should give J → J, so the pullback of J is zero.<br />

Now let us consider the second condition, <strong>and</strong> compute the pullback of<br />

the holomorphic three-form. The equation for a quintic hypersurface in £ P 4<br />

discussed in Section 9.3 is<br />

5<br />

m=1<br />

(X m ) 5 = 0.<br />

Defining inhomogeneous coordinates Y k = X k /X 5 , with k = 1, 2, 3, 4, on<br />

the open set X 5 = 0, the holomorphic three-form can be written as<br />

The norm of Ω is<br />

Ω = dY 1 ∧ dY 2 ∧ dY 3<br />

(Y 4 ) 4 .<br />

Ω 2 = 1<br />

6 ΩabcΩ abc =<br />

1<br />

ˆg|Y 4 ,<br />

| 8<br />

where ˆg = det g a ¯ b . Using Eqs (9.104) <strong>and</strong> (9.129), as well as Exercise 9.8,<br />

one has<br />

e −K2,1<br />

which implies that<br />

<br />

= i<br />

Ω ∧ Ω = V Ω 2 = 1<br />

8 e−K1,1Ω<br />

2<br />

Ω 2 = 8e 2K ,

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