Example 3.28 . [03PL]
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Example 3.28.
Let be a Calabi–Yau -fold for , a compact Lagrangian in , and . In [57], Neves defines another Lagrangian in , which is Hamiltonian isotopic to and coincides with except in a small open neighbourhood of . Here are locally surfaces of revolution on the curves in sketched in Figure 3.7. (Actually Neves restricts to , but the same ideas should work for all .)
Neves’ main result [57, Th. A] is that Lagrangian MCF starting from develops finite time singularities. This is important, as it shows that finite time singularities in Lagrangian MCF are unavoidable in many situations (although note that has phase variation greater than , so this does not show that almost calibrated Lagrangian MCF has finite time singularities).
What actually happens in Lagrangian MCF starting from ? Neves’ proof does not tell us, as he assumes for a contradiction that no finite time singularity occurs. The author expects a Lagrangian MCF with surgeries in with , with two singular times . For looks much like , but as in , the region marked with crosses ‘’ in Figure 3.7 undergoes a ‘neck pinch’. At , as sketched in Figure 3.8, decomposes as , where is a small immersed near with one transverse self-intersection point with , a ‘Whitney sphere’ as in Example 3.23, and looks quite like the original .
Then as increases from to , the component should shrink to a point, until at the second singular time it undergoes ‘collapsing a zero object’ as in Principle 3.25. Meanwhile, the Lagrangian MCF of looks quite like that of the original , and continues for . Thus, at least conjecturally, Neves’ examples [57] are not counterexamples to the programme of §3.2.