Peng Zhou

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blog:2023-06-27 [2023/06/27 18:11] pzhoublog:2023-06-27 [2023/06/27 18:32] (current) pzhou
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 Now, we turn on $\C^*$ or $S^1$ action. There are many invariant subspaces. We also have $S^1$ action on $S^{2r}$, coming from the suspension of $S^1$ acting on $S^{2r-1}$.  Now, we turn on $\C^*$ or $S^1$ action. There are many invariant subspaces. We also have $S^1$ action on $S^{2r}$, coming from the suspension of $S^1$ acting on $S^{2r-1}$. 
  
-What can we say then? If we want to compute the equivariant cohomology (which is equal to equivariant homology up to shift) of $\C$ acted by $S^1$, then we pass to the Borel model, we form $EG \times_G \C$, $G=S^1$, and we get a line bundle over $BG=\C \P^\infty$. The top dimensional 'homology', or 0-degree (degree = codim) cohomology is defined. +What can we say then? If we want to compute the equivariant cohomology (which is equal to equivariant homology up to shift) of $\C$ acted by $S^1$, then we pass to the Borel model, we form $EG \times_G \C$, $G=S^1$, and we get a line bundle over $BG=\C \P^\infty$. The top dimensional 'homology', or 0-degree (degree = codim) cohomology is defined. That is $[\C_G]$, the fundamental (homology) class of the universal associated bundle.  Then, we can ask, what is the homology of $[0_G]$, the universal zero-section's fundamental class? By Thom isomorphism, we know **it is equivalent to something in the base, times the full fiber of $[\C_G] \to [0_G]$**, by perturbation and stretching. This is equal to computing the self-intersection of the zero-section.  
 +$$ [0_G] = [\C_G] \cdot u $$ 
 +where $u$ is cohomological degree $2$. $ [0_G] = [\C^r_G] \cdot u^r$. This make sense at least degreewise.  
 + 
 +So, the actual non-compact space fundamental class is 
 +$$ [\C^r_G]= \frac{[0_G]}{u^r} $$ 
 + 
 +OK, this summarizes my understanding of equivariant localization between a vector space and the zero section.  
 + 
 +For the abelian case, there should be several approaches, all leading to the correct consistent answers.  
 +BFN and VV both defined some convolution, maybe even BDG.  
 + 
 +==== BFN convolution space ==== 
 +Recall what is matrix multiplication: given matrices of sizes $n_1 \times n_2$, $n_2 \times n_3$, called $M_{12}$ and $M_{23}$, we can form their product, which is given by 
 +$$ (M_{13})_{ij} = \sum_k (M_{12})_{ik} (M_{12})_{kj} $$ 
 + 
 +This can be considered as composing correspondences. We need a way to do composition (multiplication), and a way to do summation (over all possible $k$, intermediate state).  
 + 
 +If we package this in terms of BM homology, we  
 + 
 + 
  
  
blog/2023-06-27.1687889507.txt.gz · Last modified: 2023/06/27 18:11 by pzhou