blog:2023-03-10
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blog:2023-03-10 [2023/03/11 05:45] – pzhou | blog:2023-03-10 [2023/06/25 15:53] (current) – external edit 127.0.0.1 | ||
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$$ v \mapsto (T_1 v, T_2 v) \mapsto (T_1 T_1 v, T_1 T_2 v; T_2 T_1 v, T_2^2 v) $$ | $$ v \mapsto (T_1 v, T_2 v) \mapsto (T_1 T_1 v, T_1 T_2 v; T_2 T_1 v, T_2^2 v) $$ | ||
hence, we need to have $T_i^2 = T_i, T_1 T_2=0$. The only chance here is that $(T_1, T_2)= (1,0)$ or $(T_1, T_2) = (0, 1)$. | hence, we need to have $T_i^2 = T_i, T_1 T_2=0$. The only chance here is that $(T_1, T_2)= (1,0)$ or $(T_1, T_2) = (0, 1)$. | ||
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+ | That's only for rank-1 comodule. How about | ||
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You know what is the easiest way to get comodule? Just take the image of $L$. Suppose we have $(V, W)$ upstairs, and we get $V \oplus W$ downstairs. Then, we need to know how does $L (V,W) \mapsto LRL(V,W)$ | You know what is the easiest way to get comodule? Just take the image of $L$. Suppose we have $(V, W)$ upstairs, and we get $V \oplus W$ downstairs. Then, we need to know how does $L (V,W) \mapsto LRL(V,W)$ | ||
- | $$ V \oplus W \to (V_1 \oplus W_1) \oplus (V_2 \oplus W_2). $$ | + | $$ V \oplus W \to (V_1 \oplus W_1) \oplus (V_2 \oplus W_2), (v,w) \mapsto ( (v,0), (0, w)) $$ |
so there is only one reasonable thing to do. | so there is only one reasonable thing to do. | ||
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+ | Summary, what is the comonad structure? It is equip $\Om V$ with the trail of paths (here two paths) as it moves up and down. | ||
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+ | What is the comodule structure? It is dividing $v$ into $v=v_1 + v_2$. Some sort of idempotent projection. | ||
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+ | ==== Another example ==== | ||
+ | Consider the skeleton of a cross, and consider the localization to the vertical line and horizontal line. | ||
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+ | Danny says, these two localization functors preserves limit (left exact), hence satisfies Barr-Beck. | ||
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+ | when you kill a linking disk (cocore to some non-compact component of a skeleton), everybody will do negative Reeb flow to snap on the skeleton again. How do I know if that motion preserves limit? | ||
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+ | The word ' | ||
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+ | So, don't worry about the words if you don't know what it means. Let's just see, if you can understand the comodule. | ||
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+ | So, we understand $\dcal$, which is just $Vect \times Vect$. And the comodules $\Omega$ is doing what? It is | ||
+ | $$ \Omega(V_1 , V_2) = (V_1 + V_2[1], V_2 + V_1) $$ | ||
+ | so it is clear, what is the co-unit map. And what is $\Om (V_1 , V_2) \to \Om \Om (V_1 , V_2)$? First, what is $ | ||
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blog/2023-03-10.1678513533.txt.gz · Last modified: 2023/06/25 15:53 (external edit)