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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> 37<br />

5 Construction <strong>of</strong> three <strong>Lefschetz</strong> fibrations<br />

In this section we review how to construct a <strong>Lefschetz</strong> fibration with any prescribed<br />

symplectic manifold M ′ as the fiber, and with a single vanishing sphere consisting<br />

<strong>of</strong> any prescribed exact Lagrangian sphere L ′ ⊂ M ′ (see lemma 1.10 in [S03A] for<br />

details). We apply this construction for each <strong>of</strong> our local models πi loc , i = 0, 2, 4<br />

to produce three <strong>Lefschetz</strong> fibrations πi, i = 0, 2, 4. If we think <strong>of</strong> the target <strong>of</strong><br />

π : E −→ D2 as containing three real critical values c0 < c2 < c4 corresponding to<br />

those <strong>of</strong> f , then (E,π) will be constructed so that (Ei,πi) is equal to the part <strong>of</strong> (E,π)<br />

lying over a small disk around ci :<br />

(E|Ds(ci),π|Ds(ci)) ∼ = (Ei,πi).<br />

<strong>The</strong> regular fiber <strong>of</strong> πi, say Mi, is a exact symplectomorphic to M (the regular fiber<br />

<strong>of</strong> π) but Mi is in some cases obtained from M by a key twisting operation, which<br />

models the transport map π −1 (c2 − s) −→ π −1 (c2 + s) along a half circle in the lower<br />

half plane.<br />

5.1 A particular choice for h in the definition <strong>of</strong> L4<br />

Before proceding we specify our choice <strong>of</strong> the function h in the definition <strong>of</strong> L4 in<br />

§3.1. Namely we set<br />

h(t) = t/2 − R 1/4(t)<br />

where R 1/4 is from (16). (<strong>The</strong> choice s = 1/4 comes from the choice <strong>of</strong> basepoint<br />

(19), which comes later.)<br />

5.2 Construction <strong>of</strong> π0 : E0 −→ D 2<br />

In this section we construct a <strong>Lefschetz</strong> fibration<br />

π0 : E0 −→ D 2<br />

such that for any 0 < s ≤ 1 there is a canonical exact symplectic identification<br />

ρ 0 s<br />

: π−1<br />

0 (s) −→ M, 0 < s ≤ 1<br />

with the vanishing sphere corresponding to L0. By construction <strong>of</strong> M, we have a<br />

canonical exact Weinstein embedding<br />

D(T ∗ S 3 ) −→ M.

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