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--- blog:2023-03-23 [2023/03/23 23:36] – [About comparing exact WKB] pzhou
+++ blog:2023-03-23 [2023/06/25 15:53] (current) – external edit 127.0.0.1
@@ Line 30: / Line 30: @@
 I am deliberately vague about which direction the integral should be done, since this is a formal integral.
-Now, I know I am wrong. Given this holomorphic Lagrangian, we have the holomorphc Legendrian lift, then over every point in hte base
+Now, I know I am wrong. Given this holomorphic Lagrangian, we have the holomorphc Legendrian lift, then over every point in hte base, we can have many points in the fiber Legendrian. For simplicity, we have exact Lagrangian. Locally, over a small ball of $p$, if we pick a Legendrian branch $b$ up there, we can construct $e^{f_b(z)/\hbar} I_b(\hbar, z)$, where we have phase function $f_b(z)$ and amplitude $\varphi_b(z)$. Now we can play the KS formalism for each fixed $z$. If you only know the spectral curve locally at that branch (well by analytic continuatino, you should know everything), you can still do WKB and get formal solution. I am not sure if the Borel plane is the actually the $J^0 C$ fiber. If everything works all, everyone consistent, then we do have Borel function $\hat I_b(u, z)$.
+We can ask, does the Borel resummed function $\hat I_b(u,z)$, as a function of $u$, satisfies any equation?
+don't worry. Assume that you have full analytic continuation of $\hat I_b(u,z)$, and you picked a path in the $u$ space, compatible with the $\hbar$ phase choice so that $u/\hbar$ goes to infinity. You then, just integrate that holomorphic function $\hat I_b(u,z)$ along that path, to get an actual honest convergent solution.
+OK, say, pointwise, you have many ways to cook up honest convergent $\hbar$ solution. You have local solution space with a canonical lattice labelled by thimbles. maybe, for each generic $\theta \in S^1$ a favorite basis.
+Now, the problem is that, how do they talk to each other?
+==== exact WKB and holomorphic disks ====
+last time we were talking about $\hbar$-differential equation, and constructing solutions. Conceptually, given $\hbar \in \C^*$, given a point on the holomorphic Legendrian, given a path in the fiber avoiding the Legendrian to infinity compatible with the half-space defined by $\hbar$, we may perform some fiber-wise integration. And we may do it locally in a neighborhood of $z$.
+Consider stokes ray. Consider the $\hbar$ circle bundle over $C$. Then we have the universal spectral curve on this manifold, induced by the holomorphic Legendrian in $C \times \C$.
+Suppose we are on a stokes curve, that means two phases are of the same size for some $\hbar$. Suppose we can connect the two equal-height points by some path. I assume that we have the period (image) lattice, Where we have the $H_1$ lattice, acting by translation.
+The question is, how to relate $\hbar$-Stokes curve, to $\hbar$ holomorphic curve. Ah, say $\hbar$ is the twister space parameter? or just $\C^*$ variable.
+yes, you can find spectral network is some sort of holomorphic disk weaves.
+But, what is the space of solutions?