blog:2024-09-08
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blog:2024-09-08 [2024/09/09 06:22] – pzhou | blog:2024-09-08 [2024/09/10 16:38] (current) – pzhou | ||
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* additive resolved Coulomb branch is a symplectic resolution of conic symplectic singularity, | * additive resolved Coulomb branch is a symplectic resolution of conic symplectic singularity, | ||
* When Webster did that procedure (char p quantization) for Coulomb branch. If we do it honestly, then we need to consider the convolution algebra of $BFN=map(bubble, | * When Webster did that procedure (char p quantization) for Coulomb branch. If we do it honestly, then we need to consider the convolution algebra of $BFN=map(bubble, | ||
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+ | ok, apparently I still don't know the Webster' | ||
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+ | But that's not my side. I think I will follow Ginzburg' | ||
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+ | It would be nice to just do a summary for the symplectic realization | ||
+ | - finite Hecke algebra, Tian-Yuan-Honda | ||
+ | - affine Hecke algebra (for $GL_n$?) the one with the $S^1 \times \R$, | ||
+ | - double affine Hecke should be on $S^1 \times S^1$. | ||
+ | - this paper: degenerate affine Hecke is Fukaya category of Horizontal Hilb for $\C^* \times \C \to \C$, no superpotential. | ||
+ | - Nil affine Hecke, our last paper, which has potential. | ||
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blog/2024-09-08.1725862933.txt.gz · Last modified: 2024/09/09 06:22 by pzhou