blog:2024-12-20
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blog:2024-12-20 [2024/12/21 07:18] – created pzhou | blog:2024-12-20 [2024/12/21 08:28] (current) – pzhou | ||
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We have a few observations: | We have a few observations: | ||
- $End(T_{(k_1, | - $End(T_{(k_1, | ||
+ | - This parabolic subgroup $P_{k_1, k_2}$ is the automorphism subgroup that preserves the partial flag $\C^{k_1} \In \C^k$. | ||
+ | - We have different kinds of flags there. They are different quiver representations of $ \bullet \to \bullet$. For example, consider the injection $j: \C^{k_1}\into \C^k$ as an object in the quiver rep. The moduli stack for this object is $Gr(k_1, k) / GL(k) = pt/P_{k_1, k_2}$, this is because $GL(k)$ acts on $Gr(k_1, k)$ transitively, | ||
+ | - How to think about $T_{2,3} \to T_{1,4}$? We have flag $Fl_1:=( \C^3 \to \C^5)$ and $Fl_2 := (\C^4 \to \C^5)$. We do have map from $Fl_1 \to Fl_2$, just like $T_{2,3} \to T_{1,4}$ admits maps. | ||
+ | Our goal is to build a category living over the Higgs side space. But I don't know what is the ambient space. | ||
+ | |||
+ | One guess is that, the space is still and always is $BGL_k$, and the T-brane sheaf is still $BB \to BG$ pushing forward. But this is like after doing stop removal. How to remember? | ||
+ | |||
+ | Another way of thinking is, we don't have to use $[pt/ | ||
+ | $$ Sh(X) \to Sh(X \times G) \to Sh(X \times G \times G) \to \cdots $$ | ||
+ | |||
+ | |||
+ | But what is $Sh(pt \to pt)$? | ||
blog/2024-12-20.1734765518.txt.gz · Last modified: 2024/12/21 07:18 by pzhou