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 ...
Create successful ePaper yourself
Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.
54 Joe Johns<br />
Now<br />
Using<br />
V γ 1 4 = τ −1<br />
[c2+1/4,c4−1/4] (V4) ⊂ π −1<br />
2 (c4 + 1/4).<br />
τ −1<br />
[c2+1/4,c4−1/4] = (τ 2 [c2+1/4,c2+1] )−1 ◦ Ψ −1<br />
24 ◦ (τ 4 [c4−1,c4−1/4] )−1<br />
and arguing as we did for Vγ0 one sees that V γ 1 4 satisfies<br />
<strong>The</strong>n<br />
Vγ4<br />
<strong>The</strong>refore, using lemma 7.2, we get<br />
ρ 2 1/4 (V γ 1 4 ) = L′ 4 ⊂ M2.<br />
−1<br />
= τ<br />
γ0 (Vγ1) = τ<br />
4 4 2 −π (Vγ1 4 )<br />
ν 2 −1/4 (Vγ4 ) = (ν2 −1/4 ◦ τ 2 −π ◦ (ρ 2 1/4 )−1 )(L ′ 4) = τ(L ′ 4) = L4 ⊂ M.<br />
8 Construction <strong>of</strong> N ⊂ E<br />
In this section we construct an exact Lagrangian embedding N ⊂ E and prove <strong>The</strong>orem<br />
A (see <strong>The</strong>orem 8.1). We also discuss some ways <strong>of</strong> refining <strong>The</strong>orem A in remark<br />
8.5, and we give a detailed sketch <strong>of</strong> the pro<strong>of</strong> that E is homotopy equivalent to N in<br />
Proposition 8.4.<br />
We first construct a Lagrangian submanifold N ⊂ E and then check that N is diffeomorphic<br />
to N . N ⊂ E will be defined as the union <strong>of</strong> several Lagrangian manifolds,<br />
say Ni, with boundary (sometimes with corners). This decomposition <strong>of</strong> N is essentially<br />
the same as the handle-type decomposition which appears in [M65, pages 27-32].<br />
<strong>The</strong> fact that the union <strong>of</strong> the Ni is diffeomorphic to N is essentially <strong>The</strong>orem 3.13 there.<br />
Let<br />
N0 = ∆ [c0,c2−1/10],<br />
N4 = ∆ [c2+1/10,c4].<br />
<strong>The</strong>se are the <strong>Lefschetz</strong> thimbles over the indicated intervals. <strong>The</strong>y correspond to the<br />
0− and 4− handles <strong>of</strong> N . Let<br />
f2 = q2| E 2 loc ∩R 4 : E2 loc ∩ R 4 −→ R,