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--- blog:2025-01-21 [2025/01/22 03:14] – created pzhou
+++ blog:2025-01-21 [2025/01/23 00:55] (current) – pzhou
@@ Line 5: / Line 5: @@
   * Localized mirror functor. No, not just probing the space using a compact immersed Lagrangian, but with deformation, allowing immersed Lagrangians.
   * Nakajima quiver variety coming from Floer theory
-Then, I am also going to meet with Denis Auroux. His not-so-recent work with Abouzaid is about fibered Lagrangian. There is one thing that is quite interesting to me: consider the very singular fibration
-$f: \C^3 \to \C$, $f=xyz$. Consider a Lagrangian, say living over the line $Re f = -1$, and in the fiber, we pick the 'positive real' slice in $(\C^*)^2$. I am not sure what does 'positive real mean, but it must be cocore to the compact Lagrangian, which I think is well-defiend $|x|=|y|=|z|$ in each fiber. OK, great, then turn on the gradient flow for $Re(f)$, do we get a nice thim
+What is the Crane-Frenkel 4d TQFT? What is the small quantum group? Why we need to be small? Just so the Verma can be defined?