The Picard-Lefschetz theory of complexified Morse functions 1 ...
The Picard-Lefschetz theory of complexified Morse functions 1 ...
The Picard-Lefschetz theory of complexified Morse functions 1 ...
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Complexified <strong>Morse</strong> <strong>functions</strong> 55<br />
and let<br />
N j<br />
2 = ((E2 loc ) j ∩ R 4 ) ∩ f −1<br />
2 ([c2 − 1/2, c2 + 1/2]).<br />
This corresponds to the jth 2−handle <strong>of</strong> N .<br />
Recall from §5.3 that E2 is a certain quotient <strong>of</strong> the disjoint union<br />
[M2 \ (∪ j=k<br />
j=1 φ (L j<br />
2 )′(D r/2(T ∗ S 3 )))] × D 2 (c2) ⊔ ⊔ j=k<br />
j=1 (E2 loc) j ) .<br />
Recall L ′ 4 ⊂ M2 is defined as<br />
L ′ 4 = [L0 \ (∪ j=k<br />
j=1 φj(S 1 × D 2 r/2 ))] ∪ φ (L j<br />
2 )′(Dr(ν ∗ K+)),<br />
where φ j<br />
(L2 )′ identifies D (r/2,r](ν ∗K+) with φj(S1 × D2 (r/2,r] ). Define Ntriv<br />
2 ⊂ E2 by<br />
N triv<br />
2 = [L0 \ (∪ j=k<br />
j=1 φj(S 1 × D 2 r/2 ))] × [c2 − 1/2, c2 + 1/2]<br />
<strong>The</strong>n, N ⊂ E is defined to be the union<br />
⊂ [M2 \ (∪ j=k<br />
j=1 φ (L j<br />
2 )′(D r/2(T ∗ S 3 )))] × D 2 1/2 (c2).<br />
N = N0 ∪ (∪j N j<br />
2 ) ∪ Ntriv 2 ∪ N4.<br />
See figure 1 in §1 for the 2-dimensional version <strong>of</strong> this. (Note that the pieces over-lap.)<br />
<strong>The</strong>orem 8.1 (1) N ⊂ E is a smooth closed exact Lagrangian submanifold.<br />
(2) <strong>The</strong>re is a diffeomorphism α: N −→ N .<br />
(3) π(N) = [c0, c4].<br />
(4) All critical points <strong>of</strong> π lie on N , and in fact Crit(π) = α(Crit(f )).<br />
(5) <strong>The</strong>re is a diffeomorphism β : R −→ R such that<br />
β ◦ π|eN ◦ α = f : N −→ R.<br />
Pro<strong>of</strong> First we prove that N is a smooth manifold diffeomorphic to N . Define<br />
N2 = (∪ j=k j<br />
j=1 N2 ) ∪ Ntriv 2 .<br />
<strong>The</strong> gluing map in the definition <strong>of</strong> E2 is the composite <strong>of</strong><br />
and<br />
Φ 2 : (E 2 loc ) j ∩ (k 2 ) −1 ([4(r/2) 2 , 4r 2 ]) −→ D [r/2,r](T ∗ S 3 ) × D 2 (c2)<br />
φ (L j<br />
2 )′ : D [r/2,r](T ∗ S 3 ) −→ M2.