ScalingStacks

0PDZ

Proof. It is immediate that d⁡(f1)=0d(f_{1})=0. For the second equality, consider α∈Rξ2−∙​(T,U)\alpha\in R^{\bullet}_{\xi_{2}^{-}}(T,U) and β∈Hom𝒮∙​(Zξ)⁡(S,U)\beta\in\operatorname{Hom}\nolimits_{{\mathcal{S}}^{\bullet}(Z_{\xi})}(S,U). Since α⊗β=(id⊠αξ2−​(−1))⊗(α|U⋅β)\alpha\otimes\beta=(\operatorname{id}\nolimits\boxtimes\alpha_{\xi_{2}^{-}(-1)})\otimes(\alpha_{|U}\cdot\beta), we can assume that α|U=id\alpha_{|U}=\operatorname{id}\nolimits. We have

d(f2)(α⊗β)=α⋅(d(β⊠[ξ1−(−1)→ξ2−(−1)])+d(β)⊠[ξ1−(−1)→ξ2−(−1)]).d(f_{2})(\alpha\otimes\beta)=\alpha\cdot\bigl(d(\beta\boxtimes[\xi_{1}^{-}(-1)\to\xi_{2}^{-}(-1)])+d(\beta)\boxtimes[\xi_{1}^{-}(-1)\to\xi_{2}^{-}(-1)]\bigr).

We have

d(β⊠[ξ1−(−1)→ξ2−(−1)])\displaystyle d(\beta\boxtimes[\xi_{1}^{-}(-1)\to\xi_{2}^{-}(-1)]) =d((id⊠[ξ1−(−1)→ξ2−(−1)])⋅(β⊠idξ1−​(−1)))\displaystyle=d\bigl((\operatorname{id}\nolimits\boxtimes[\xi_{1}^{-}(-1)\to\xi_{2}^{-}(-1)])\cdot(\beta\boxtimes\operatorname{id}\nolimits_{\xi_{1}^{-}(-1)})\bigr)
=(id⊠[ξ1+(1)→ξ2−(−1)])⋅d(idU⊠[ξ1−(−1)→ξ1+(1)])⋅(β⊠idξ1−​(−1))\displaystyle=(\operatorname{id}\nolimits\boxtimes[\xi_{1}^{+}(1)\to\xi_{2}^{-}(-1)])\cdot d(\operatorname{id}\nolimits_{U}\boxtimes[\xi_{1}^{-}(-1)\to\xi_{1}^{+}(1)])\cdot(\beta\boxtimes\operatorname{id}\nolimits_{\xi_{1}^{-}(-1)})
+(id⊠[ξ1−(−1)→ξ2−(−1)])⋅(d(β)⊠idξ1−​(−1))\displaystyle\ \ \ \ +(\operatorname{id}\nolimits\boxtimes[\xi_{1}^{-}(-1)\to\xi_{2}^{-}(-1)])\cdot(d(\beta)\boxtimes\operatorname{id}\nolimits_{\xi_{1}^{-}(-1)})
=(idU⊠[ξ1+(1)→ξ2−(−1)])∑x∈ξ~1−1​(U)(id⊠ξ~1([x→1])⊠ξ~1([−1→x]))\displaystyle=(\operatorname{id}\nolimits_{U}\boxtimes[\xi_{1}^{+}(1)\to\xi_{2}^{-}(-1)])\sum_{x\in\tilde{\xi}_{1}^{-1}(U)}\bigl(\operatorname{id}\nolimits\boxtimes\tilde{\xi}_{1}([x\to 1])\boxtimes\tilde{\xi}_{1}([-1\to x])\bigr)
⋅(β⊠idξ1−​(−1))+d(β)⊠[ξ1−(−1)→ξ2−(−1)]\displaystyle\ \ \ \ \cdot(\beta\boxtimes\operatorname{id}\nolimits_{\xi_{1}^{-}(-1)})+d(\beta)\boxtimes[\xi_{1}^{-}(-1)\to\xi_{2}^{-}(-1)]

hence

d(f2)(α⊗β)=α⋅∑x∈ξ~1−1​(U)(id⊠([ξ1+(1)→ξ2−(−1)]⋅ξ~1([x→1]))⊠ξ~1([−1→x]))⋅(β⊠idξ1−​(−1))d(f_{2})(\alpha\otimes\beta)=\alpha\cdot\sum_{x\in\tilde{\xi}_{1}^{-1}(U)}\Bigl(\operatorname{id}\nolimits\boxtimes\bigl([\xi_{1}^{+}(1)\to\xi_{2}^{-}(-1)]\cdot\tilde{\xi}_{1}([x\to 1])\bigr)\boxtimes\tilde{\xi}_{1}([-1\to x])\Bigr)\cdot(\beta\boxtimes\operatorname{id}\nolimits_{\xi_{1}^{-}(-1)})
=∑x∈ξ~1−1​(U)(id⊠ξ~1([−1→x])⊠(αξ2−​(−1)⋅[ξ1+(1)→ξ2−(−1)]⋅ξ~1([x→1])))⋅(β⊠idξ1−​(−1))\displaystyle=\sum_{x\in\tilde{\xi}_{1}^{-1}(U)}\Bigl(\operatorname{id}\nolimits\boxtimes\tilde{\xi}_{1}([-1\to x])\boxtimes\bigl(\alpha_{\xi_{2}^{-}(-1)}\cdot[\xi_{1}^{+}(1)\to\xi_{2}^{-}(-1)]\cdot\tilde{\xi}_{1}([x\to 1])\bigr)\Bigr)\cdot(\beta\boxtimes\operatorname{id}\nolimits_{\xi_{1}^{-}(-1)})
=f1∘u⁡(α⊗β).\displaystyle=f_{1}\circ u(\alpha\otimes\beta).

The lemma follows. ∎

Original mathematics by the credited authors. Source collection and HTML conversion remain in progress.

Andrew Manion, Raphael Rouquier

Original source: arXiv:2009.09627v2