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> 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.