Differences

This shows you the differences between two versions of the page.

--- blog:2023-04-30 [2023/04/30 17:41] – [Dimer? Quiver? Spectral Curve? 2d Torus?] pzhou
+++ blog:2023-04-30 [2023/06/25 15:53] (current) – external edit 127.0.0.1
@@ Line 1: / Line 1: @@
 ====== 2023-04-30 ======
   * More on quiver gauge theory from toric CY3
+  * Editing the paper
 ===== quiver gauge theory from toric CY3 =====
@@ Line 52: / Line 53: @@
 $$ |\Sigma_X| = \sigma_X \In N_X \Rightarrow \sigma_X^\vee \In M_X $$
 So, I do have things living on $(N_X)_T$ and $(N_X)'_T$.
+==== Toric CY3 X, as the A-side ====
+What kind of superpotential do I want to have on $X$? I want sum of monomials, that pairs-positively with the cone $\sigma_X$, that is, maybe the ray generators of $\sigma_X^\vee$.
+** Ex: $X = \C^3$ **, we want
+$$ \wt W_X = xyz + \epsilon(x+y+z) $$
+** Ex: $X$ is conifold **, say the ray generators of $\sigma_X$ is
+$$ (0,0,1), (1,0,1), (0,1,1), (1,1,1). $$
+with divisors called $D_1, \cdots, D_4$.
+Then, the dual cone has generators
+$$ (1,0,0), (0,1,0), (0,-1,1), (-1, 0, 1). $$
+Let's call these generators $W_1, \cdots, W_4$, with $W_1 W_4 = W_2 W_3$. We want
+$$ W = W_{(0,0,1)} + \epsilon(W_1 + W_2 + W_3 + W_4) $$
+Suppose we have a corner vertex given by intersection of $D_1, D_2, D_3$, then the function looks like
+$$ W = xyz + \epsilon(x+y+xz + yz) $$
+OK, fine.
+==== The 3d and 2d torus on the X-side ====
+$\gdef\La{\Lambda}$
+X is the A-side. Except $X$ is the compactification of $(\C^*)^3$.
+The skeleton $\Lambda_X \In (N_X)_T \times (M_X)_\R$, where its projection $\La_X$ on $(M_X)_\R$ is the dual cone subdivided by a ray $\xi_X$.  And its projection to $(N_X)_T$ is a periodization of $\Sigma_X$.
+I am not sure what am I supposed to do with this setup. This should be called: mirror symmetry with toric CY3 as the A-side, and with superpotential of hierarchy.
+The B-side, $Y$, will have compactification. The moment polytope of $Y$ is the simplest way to describe it, it is just the truncated $\Sigma_X$, with flat bottom. Then, the superpotential is just these monomials, labelled by $A_X$, and the critical loci is the compactified spectral curve.
+We are interested in counting disks ending on a Lagrangian. many ways to cook up Lagrangians here. don't worry.
+What do you want? Restrict to one monomial, and look at all the nearby monomials. That's restrict to some open part of the skeleton.
+OK, in terms of skeleton and 2d torus on the $X$-side, or rather $X' = W_X^{-1}(1)$ side, I am completely happy. But, where is the dimer? Dimer data is the same as the zigzag path (at least in some nice cases)
+** What is a dimer? Dimer is a particular Lagrangian filling of a Legendrian boundary condition. **
+==== Remaining Questions ====
+What is dimer mutation? Well, for a given alternativing Lagrangian, the local system on it only support some $(\C^*)^k$ torus open chart worth of objects among all the allowed guys.
+We are looking at the moduli space of rank $1$ sheaves on the toric stack $Y'$. Basically, we can change the parameters of the coefficients. What's the big deal then?
+What is your starting point? For TWZ or STWZ or STW, their starting point is a singular 2-dimensional skeleton, obtained by gluing disks to a surface. The moduli space of microlocal rank 1 sheaves on it, forms a cluster variety.