blog:2023-07-16
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+ | * planning for the Coulomb branch | ||
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+ | ===== planning ===== | ||
Let me think about my desired statement first. What do I want to state in this section. Yes, I need to discuss about the geometry of the Coulomb branch in this section. What is my point? Don't be bind up by the setup, do your own setup. If I were to rewrite this paper, I would do this: immediately after the introduction, | Let me think about my desired statement first. What do I want to state in this section. Yes, I need to discuss about the geometry of the Coulomb branch in this section. What is my point? Don't be bind up by the setup, do your own setup. If I were to rewrite this paper, I would do this: immediately after the introduction, | ||
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+ | ==== Aside: do we care about codimension 2 guys? ==== | ||
Question: suppose you have a Kahler manifold, that you only know very well up to complex codimension two loci, is that good enough to define a Fukaya category? Hmm, what does codimension two mean? It means that you start with a space, singular maybe, and you deleted something from it. Why it should not matter? Because when we define things, because a (complex) codimension 2 guy intersect a dimension 1 guy is a complex codimension 1 condition. And, when we build things in a family, like, checking associativity condition, one only need to build real one-dimensional disk moduli spaces, so it is OK. You will not see it. | Question: suppose you have a Kahler manifold, that you only know very well up to complex codimension two loci, is that good enough to define a Fukaya category? Hmm, what does codimension two mean? It means that you start with a space, singular maybe, and you deleted something from it. Why it should not matter? Because when we define things, because a (complex) codimension 2 guy intersect a dimension 1 guy is a complex codimension 1 condition. And, when we build things in a family, like, checking associativity condition, one only need to build real one-dimensional disk moduli spaces, so it is OK. You will not see it. | ||
- | Well, if you say so, how do you define the Fukaya category of $T^*\P^1$, which is a resolution of the nilpotent cone of $sl_2$? The singularity downstairs is codimension 2. It is the tip of a cone. | + | Well, if you say so, how do you define the Fukaya category of $T^*\P^1$, which is a resolution of the nilpotent cone of $sl_2$? The singularity downstairs is codimension 2. It is the tip of a cone. In this case, you can certainly imagine a disk bounded by Lagrangian that run through the exceptional divisor. So, it would be a ' |
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+ | Answer: If the ambient space is smooth, then we don't care about codim 2 guy, no matter if it is smooth or not. | ||
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+ | ==== Just write it. in 1 hour ==== | ||
+ | 10:53am now. | ||
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blog/2023-07-16.1689526922.txt.gz · Last modified: 2023/07/16 17:02 by pzhou